; NIST

PUBLICATJONS AuiDs 3S5t5p ^^^^H United Ststes Department of Commerce

Technology Administration iMisr National Institute of Standards and Technology

NIST Technical Note 1425

Gases for Electrical Insulation and Arc Interruption:

Possible Present and Future Alternatives to Pure SFe

L. G. Christophorou, J. K. Olthoff, and D. S. Green

QC

100

1U5753

1997
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NIST Technical Note 1425

Gases for Electrical Insulation and Arc Interruption:

Possible Present and Future Alternatives to Pure SFe

L. G. Christophorou

J. K. Olthoff

D. S. Green

Electricity Division

Electronics and Electrical Engineering Laboratory

and

Process Measurements Division

Chemical Science and Technology Laboratory

National Institute of Standards and Technology

Gaithersburg, MD 20899-0001

^^et^^o^co^^

1^ ^Q^ "tL ff ^.v -^ %

November 1997

U.S. Department of Commerce

William M. Daley, Secretary

Technology Administration

Gary R. Bachula, Acting Under Secretary for Technology

National Institute of Standards and Technology

Raymond G. Kammer, Director
National Institute of Standards U.S. Government Printing Office For sale by the Superintendent of and Technology Washington: 1997 Documents

Technical Note 1425 U.S. Government Printing Office

Natl. Inst. Stand. Technol. Washington, DC 20402

Tech. Note 1425

48 pages (Nov. 1997)

CODEN: NTNOEF
Bibliographic Information

Abstract

The electric power Industry's preferred gaseous dielectric (besides air), sulfur hexafluoride (SFg), has been

shown to be a greenhouse gas. In this report we provide information that is useful In Identifying possible

replacement gases, in the event that replacement gases are deemed a reasonable approach to reducing the use of SFg in high voltage electrical equipment. The report focuses on the properties of SFg as a dielectric gas

and on the data available for possible alternatives to pure SFg (i.e., SFg alone). On the basis of published

studies and consultation with experts in the field, it was attempted to identify alternative dielectric gases to pure SFg for possible immediate or future use in existing or modified electrical equipment. The possible

alternative gases are discussed as three separate groups: (i) mixtures of SFg and nitrogen for which a large

amount of research results are available; (ii) gases and mixtures (e.g., pure Nj, low concentrations of SFg in Ng, and SFg-He mixtures) for which a smaller yet significant amount of data are available; and (iii) potential

gases for which little experimental data are available.

Keywords

gaseous dielectrics; gas mixtures; gas recycling; global warming; nitrogen; SFg; SFg-Ng mixtures; sulfur

hexafluoride

Ordering

Copies of this document are available from the National Technical Information Service, 5285 Port Royal Road,

Springfield, VA 22161, at (800) 553-6847 or (703) 487-4650.

ACKNOWLEDGMENTS

The authors benefitted greatly from the suggestions and comments provided by individuals in industry, academia, and

government. Shown below are the individuals who contributed by providing information relevant to the report, or by

reviewing and commenting on draft materials. While these individuals influenced the development of this document, the authors are solely responsible for the views expressed in the document. The presence of a reviewer's name here is not intended to suggest endorsement or agreement with all of the views contained in this report.

Christophe Boisseau

Phil Bolin

Lowell Brothers

John Brunke

Ian Chalmers

Alan Cookson

Steinar Dale

Benjamin Damsky

Armin Diessner

Elizabeth Dutrow

Lois Ellis

Fumihiro Endo

Michael Frechette

Yoshikazu Hoshina

Edmund Kuffel

Richard LaLumondier

Donald Martin

Hugh Morrison

Koichiro Nakanishi

C. M. A. Nayar

Lutz Niemeyer

Marshall Pace

Reinhold Probst

Bryan Smith

Xavier Waymel

Howard Withers

Roy Wootton

Electricite de France, FRANCE

Mitsubishi Electric Power Products, Inc., USA

Southern Company Services, Inc., USA

Bonneville Power Administration, USA

University of Strathclyde, U.K.

National Institute of Standards and Technology, USA

ABB Power T&D Company, Inc., USA

Electric Power Research Institute, USA

Siemens, GERMANY

US Environmental Protection Agency, USA

Allied Signal, Inc., USA

Hitachi, JAPAN

Hydro-Quebec, CANADA

Toshiba, JAPAN

University of Manitoba, CANADA

National Electrical Manufacturers Association, USA

G&W Electric Co., USA

Ontario Hydro, CANADA

Mitshubishi Electric Corporation, JAPAN

GEC ALSTHOM, FRANCE

ABB Corporate Research, SWITZERLAND

University of Tennessee, USA

DILO Company, Inc., USA

Cryoquip, Inc., USA

Electricite de France, FRANCE

Air Products and Chemicals , Inc., USA

Formerly at Westinghouse, USA

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST

Section 1 - Introduction

Gases for Electrical Insulation and Arc Interruption:

Possible Present and Future Alternatives to Pure SFg

Contents 1. Introduction

1. Introduction 1

1.1 Sulfur Hexafluoride 2

1 .2 Principal Uses of SF^ by the Electric Power Industry 2

1.3 Concentrations of SFf,in the Environment ... 3

1 .4 SFf, is a Potent Greenhouse Gas 4

1.5 SF(i Substitutes 5

1 .6 Scope of this Report 6

2. Properties of Gaseous Dielectrics 6

2.

Intrinsic Properties 6

2.1.1 Basic Physical Properties 7

2.1.2 Basic Chemical Properties 8 2.2 Extrinsic Properties 8

2.2.1 Reactions and Byproducts 8

2.2.2 Electrical Discharge and Breakdown . . 8

2.3 Other Requirements for Commercialization . 9

2.4 Properties of Gaseous Insulators for Specific Industrial Uses 9

2.4.1 Circuit Breakers 9

2.4.2 High Voltage Insulation 9

2.4.2.1 Gas-insulated Transmission

Lines 9

2.4.2.2 Gas-insulated Transformers .10

3. Required Performance and Testing of Gases .... 10

4. Possible "Universal-Application" Gas Mixtures ..11

4.1 Insulation 12

4.1.1 Gas-insulated Transmission Lines ...12

4. 1 .2 Gas-insulated Transformers 15 4.2 Interruption 16

4.3 Gas Handling, Storing, Recycling,

and Recovering 22

4.4 Discussion 22

5. Other Promising Gases or Mixtures 23

5.1 High-Pressure N2 23

5.2 Low-Concentration SF^-Nj Mixtures 25

5.3 SF(i-He Mixtures 26

6. Other Possible Substitutes: Future R&D 27

7. Conclusions and Recommendations 28

8. References 29

Appendix A - Sales of SF^ 35

Appendix B - Issues 37

Appendix C - Potential Barriers 39

Sulfur hexafluoride (SF^), the electric power

industry's presently preferred gaseous dielectric (besides

air), has been shown to be a greenhouse gas. Concerns

over its possible impact on the environment have

rekindled interest in finding replacement gases. In this report we provide information that is useful in identifying

such gases, in the event that replacement gases are deemed a reasonable approach to controlling emissions of

SFft from high voltage electrical equipment. The report

focuses on the properties of SF^ as a dielectric gas and on

the data available for possible alternatives to pure SF^

(i.e., SFfi alone). On the basis of published studies and

consultation with experts in the field, we attempt to identify alternative dielectric gases to pure SF^ for possible immediate or future use in existing or modified

electrical equipment.

This report first describes the properties that make

a good gaseous dielectric, and the tests and measurements

that are necessary to demonstrate and document the appropriateness of a gas as a high voltage insulating

medium, or for use as an arc or current interrupting

medium. An effort has been made to gather expert

opinion regarding the possible adoption of likely SF^, substitutes and the additional tests that are needed to effect their acceptability by electric equipment

manufacturers and by the electric power industry. During

the preparation of the report, we consulted with a broad

spectrum of experts (see Acknowledgments) via a series of meetings on the subject matter and by correspondence.

Representatives from electric equipment manufacturers,

electric utilities, gas handling and manufacturing

companies, and academic institutions were consulted.

An attempt was made during the preparation of this report to identify a gaseous mixture that could be adopted

for "universal use" as an immediate replacement of pure

SFf,. The large amount of available physical and

laboratory data suggest that a 40%SF(,-60%N2 mixture'

may exhibit dielectric characteristics suitable for use as insulation in high voltage equipment. However, it is realized that there are difficulties in using this mixture for arc or current interruption, and as a replacement gas in

'All references in this report to mixtures and

concentrations are by volume.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 1.1 - Sulfur Hexafluoride

already existing equipment. The reasons for and against

the use of this "universal-application" gas mixture are discussed.

The report also discusses other possible substitutes for which a significant but smaller amount of data exists. These include high-pressure pure Nj and dilute SFj^-N^

mixtures (concentrations of SF^ in the mixture less than

about 15%) as likely gaseous media for electrical insulation, and SFj^-He mixtures as a possible medium for arc interruption. Other gases and mixtures are also discussed for which the available data are too few to allow an assessment of their utility as a substitute, but which

suggest some promise. The need for a future R&D

program in these areas is indicated and suggestions are made as to possible elements of such a program. While

the literature search utilized in this report was not intended to be complete, it is extensive and can serve as a guide to critical work on alternatives to pure SFj^. This report concentrates on specific uses of SFf, by

the electric power industry. However, much of the discussion is appropriate for other uses of SF^j as a high

voltage insulating and current interrupting medium.

1.1 Sulfur Hexafluoride

Sulfur hexafluoride is a man-made gas which

became commercially available in 1947 [1]. It is one of

the most extensively and comprehensively studied

polyatomic molecular gases because of its many

commercial and research applications.' Its basic physical

and chemical properties, behavior in various types of gas

discharges, and uses by the electric power industry have

been broadly investigated (see, for example, [2-7]). In its normal state, SF^ is chemically inert, non-toxic,

non-flammable, non-explosive, and thermally stable (it does not decompose in the gas phase at temperatures less than 500 "C). Sulfur hexafluoride exhibits many

properties that make it suitable for equipment utilized in the transmission and distribution of electric power. It is a strong electronegative (electron attaching) gas both at room temperature and at temperatures well above

ambient, which principally accounts for its high dielectric strength and good arc-interruption properties. The

breakdown voltage of SF^, is nearly three times higher than

air at atmospheric pressure [6]. Furthermore, it has good

^Besides the use of SF^, by the electric power industry, other uses of SFsinclude: semiconductor processing, blanket gas for magnesium casting, reactive gas in aluminum recycling to reduce

porosity, thermal and sound insulation, airplane tires, spare tires, "air sole"shoes, scuba diving voice communication, leak checking,

atmospheric tracer gas studies, ball inflation, torpedo propeller

quieting, wind supersonic channels, and high voltage insulation for many other purposes, such as AWACS radar domes and X-ray

machines.

heat transfer properties and it readily reforms itself when

dissociated under high gas-pressure conditions in an

electrical discharge or an arc (i.e., it has a fast recovery

and it is self-healing). Most of its stable decomposition

byproducts do not significantly degrade its dielectric strength and are removable by filtering. It produces no

polymerization, carbon, or other conductive deposits

during arcing, and it is chemically compatible with most

solid insulating and conducting materials used in electrical equipment at temperatures up to about 200 "C. Besides its good insulating and heat transfer

properties, SF^ has a relatively high pressure when

contained at room temperature. The pressure required to liquefy SF^ at 21 "C is about 2100 kPa [5, 8]; its boiling

point is reasonably low, -63.8 "C, which allows pressures of 400 kPa to 600 kPa (4 to 6 atmospheres) to be

employed in SFf^-insulated equipment. It is easily

liquefied under pressure at room temperature allowing for compact storage in gas cylinders. It presents no handling

problems, is readily available, and up until recently has

been reasonably inexpensive.^ The electric power

industry has become familiar and experienced with using

SF(; in electrical equipment.

However, SF^, has some undesirable properties: it forms highly toxic and corrosive compounds when

subjected to electrical discharges (e.g., SjF.q, SOFj); nonpolar contaminants (e.g., air, CF4) are not easily removed

from it; its breakdown voltage is sensitive to water vapor, conducting particles, and conductor surface roughness;

and it exhibits non-ideal gas behavior at the lowest

temperatures that can be encountered in the environment,

i.e., in cold climatic conditions (about -50 "C), SF^; becomes partially liquefied at normal operating pressures (400 kPa to 500 kPa). Sulfur hexafluoride is also an

efficient infrared (IR) absorber and due to its chemical

inertness, is not rapidly removed from the earth's atmosphere. Both of these latter properties make SF^ a potent greenhouse gas, although due to its chemical

inertness (and the absence of chlorine or bromine atoms

in the SF^ molecule) it is benign with regard to stratospheric ozone depletion.

1.2 Principal Uses of SFg by the Electric

Power Industry

Besides atmospheric air, sulfur hexafluoride is the

electric power industry's preferred gas for electrical

'From 1960 to 1994 the price ofSF^ in quantity purchases

remained basically constant at about $3.00 per pound (one pound

= 0.4536 kg). The current price of SF^ for quantity purchases in the United States varies from as low as $12 per lb to over $37 per pound ($ 82/ kg) [Private communication, P. Bolin, 1 997; P. Irwin, Electrical World, February 1997, pp. 27-30].

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFf; / NIST
Section 1 - Introduction

insulation and for arc quenching and current interruption

equipment used in the transmission and distribution of

electrical energy. Generally, there are four major types of

electrical equipment which use SF^, for insulation and/or

interruption purposes: gas-insulated circuit breakers and

current-interruption equipment, gas-insulated transmission

lines, gas-insulated transformers, and gas-insulated

substations. It is estimated [9-11] that for these

applications the electric power industry uses about 80%

of the SF(i produced worldwide, with circuit breaker

applications accounting for most of this amount. These

estimates are consistent with a recent tabulation of SF^; production worldwide [12] (See Appendix A). Gasinsulated equipment is now a major component of power

transmission and distribution systems all over the world

and employs SF^ almost exclusively. It offers significant

savings in land use, is aesthetically acceptable, has

relatively low radio and audible noise emissions, and

enables substations to be installed in populated areas close

to the loads. Depending on the particular function of the gasinsulated equipment, the gas properties which are the most

significant vary. For circuit breakers the excellent thermal conductivity and high dielectric strength of SF^,

along with its fast thermal and dielectric recovery (short

time constant for increase in resistivity), are the main

reasons for its high interruption capability. These

properties enable the gas to make a rapid transition between the conducting (arc plasma) and the dielectric

state of the arc, and to withstand the rise of the recovery

voltage. SFfi-based circuit breakers are presently superior

in their performance to alternative systems such as high- pressure air blast or vacuum circuit breakers. For gas-insulated transformers the cooling ability,

compatibility with solid materials, and partial discharge

characteristics of SF^ - added to its beneficial dielectric characteristics - make it a desirable medium for use in

this type of electrical equipment. The use of SF,; insulation has distinct advantages over oil insulation,

including none of the fire safety problems or environmental problems related to oil, high reliability, flexible layout, little maintenance, long service life, lower

noise, better handling, and lighter equipment.

For gas-insulated transmission lines the dielectric strength of the gaseous medium under industrial conditions is of paramount importance, especially the behavior of the gaseous dielectric under metallic particle

contamination, switching and lightning impulses, and fast transient electrical stresses. The gas must also have a high

efficiency for transfer of heat from the conductor to the enclosure and be stable for long periods of time (say, 40

years). SF(;-insulated transmission lines offer distinct advantages: cost effectiveness, high-carrying capacity,

low losses, availability at all voltage ratings, no fire risk.

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\ \ 1 r O U. Denver (32°N) • ATMOS/SL3(3rN)

ATMOS/AT1 (28-8. 54''S)

-- Fit to measurements

r

f

1982 1984 1986 1988 1990

Date Of Observation

1992

Fig. 1. Average SF^ concentration (pptv = parts per trillion = parts in 10'^ by volume) between 12 km and 18 km altitude as a function of time [16]. o University of Denver balloon-borne infrared measurements at 32° N

latitude; • Spacelab 3 ATMOS data at 31" N latitude; Average of ATMOS ATLAS 1 data at 28° S and 54" S [16].

reliability, and a compact alternative to overhead highvoltage transmission lines in congested areas that avoids

public concerns with overhead transmission lines. Finally, in gas-insulated substations (GIS), the entire substation (circuit breakers, disconnects, grounding

switches, busbar, transformers, etc., are interconnected) is insulated with the gaseous dielectric medium and, thus, all of the abovementioned properties of the dielectric gas are

significant.

1.3 Concentrations of SFg in the Environment

Because of the many and increasing commercial uses of SFfi, there has been an increased demand for it. The

estimated world production of SF,; has increased steadily

since the 1970s to approximately 7000 metric tons per

year in 1993 [9-11, 13, 14].'' In turn, this has resulted in an increased concentration of SF,, in the atmosphere [11,

13-18]. As seen in Fig. 1, measurements [16, 18] have

shown that the amount of SF^ in the atmosphere has been

increasing at a rate of approximately 8.7% per year, from

barely measurable quantities a decade ago to current

levels near 3.2 pptv (3.2 parts in 10'^ by volume). More

recent measurements indicate atmospheric concentrations

"This figure is compatible with a compilation of worldwide SF^ sales data by end-use markets from six companies

from the USA, Europe, and Japan (see Appendix A). The total figures listed in Appendix A, however, must be higher than shown,

since countries such as China and Russia were excluded from the survey [12].

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 1 .4 - SF. is a Potent Greenliouse Gas

of SF(; ranging from 3.18 pptv (at 8 km) to 2.43 pptv (at 27 km) [ 1 7a], an atmospheric lifetime of 1 937 years [ 1 7a],

and a global growth rate for atmospheric SF^

concentrations of 6.9% for 1996 [17b]. While the

uncertainties in these numbers make extrapolations

difficult, it is clear that the atmospheric concentration of

SFf, is increasing and could reach 10 pptv by the year 2010

[11, 15, 16, 18], depending upon the assumptions of

release rates (see Fig. 2). In some industrial applications SF^ is not easily

recoverable, e.g., in aluminum manufacturing. Releases

of SFf, into the environment by the electric power industry come from normal equipment leakage, maintenance,

reclaiming, handling, testing, etc.-^ Without disposal

methods that actually destroy SF,,, it can be expected that

all of the SFf, that has ever been or will ever be produced

will eventually enter the atmosphere. This is so even if the present SF^ leak rate from enclosed power-system

equipment is only 1% per year or is improved to < 0.5%

per year. It has been suggested [9] that impure, used SF^

removed from "retired" electrical equipment can be

destroyed by thermal decomposition in industrial waste

treatment furnaces at elevated temperatures (T > 1 1 00 "C),

but no records are available indicating that this has ever been done at a significant level. However, decreasing the rate of SF,^ leakage and

increasing the level of recycling are high priorities since

they both curtail use and production needs of SF^, and thus

reduce the quantities of SF^; that are eventually released

into the environment. Indeed, efforts have recently been

undertaken by the electric power industry to reduce and

monitor better the amount of SF^ released into the environmentfromSFf,-insulatedequipment[9-l 1]. These

efforts include:

• minimizing SF^ releases by improved methods to quantify and stop leakages, gradual replacement of older

equipment which normally leaks at higher rates, implementation of a sound overall policy of using,

handling, and tracing SF^, better pumping and storage

procedures, efficient recychng and setting of standards for recycling [19], and destruction of used SF^,

• reducing the amount of SF^^ used by

manufacturing tighter and more compact equipment,

development of sealed-for-life electrical apparatus, and

replacing SF^ where possible by other gases or gas mixtures (see later in this report).

These efforts are partially motivated by the prospect

'^We acknowledge private discussions on theseissues with

P. Bolin of Mitsubishi Electric Power Products Inc. (USA),

J. Brunke of Bonneville Power (USA), H. Morrison of Ontario Hydro (Canada), M. F. Frechette of IREQ (Canada), L. Niemeyer

of ABB Research Corporation (Switzerland), A. Diessner of Siemens AG (Germany), K. Nakanishi of Mitsubishi Electric Corporation (Japan), and F. Endo of Hitachi (Japan).

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6

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4

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Full release:

7000 metric

tons/year

Full release:

5000 metric

tons/year

30% release:

7000 metric

tons/year

30% release:

5000 metric

tons/year

Installed

Electrical

installationl_

1970 1990 2010

Year

Fig. 2. Atmospheric SF^ concentration (pptv = parts in 10'^ by volume) as a function of time. The solid curve represents

the estimated cumulative total SF^ from gas-insulated equipment in the past, the open points are measured

atmospheric trace concentrations, the solid point labeled

"installed" is the estimated concentration assuming that all

SFft enclosed in electrical equipment throughout the world in 1990 has been released into the atmosphere, and the broken

lines are projected increases under various assumptions [11].

of regulation and the possibility of imposition of controls on the use and transport of SF^ [11, 14, 20] (also see Appendix B for a summary of the current status of

regulatory issues related to SF(; use). The overall concern

is motivated by virtually one reason only: SFf^ is a potent

greenhouse gas with an extremely long atmospheric

lifetime.

1 .4 SFg is a Potent Greenhouse Gas

Greenhouse gases are atmospheric gases which

absorb a portion of the infrared radiation emitted by the

earth and return it to earth by emitting it back. Potent greenhouse gases have strong infrared absorption in the wavelength range from ~ 7 pm to 13 |am. They occur

both naturally in the environment (e. g., HjO, CO2, CH4,

N2O) and as man-made gases that may be released [e. g., SF^; fully fluorinated compounds (FFC); combustion

products such as CO2, nitrogen, and sulfur oxides]. The

effective trapping of long-wavelength infrared radiation

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 1 - Introduction

from the earth by the naturally occurring greenhouse

gases, and its re-radiation back to earth, results in an

increase of the average temperature of the earth's surface. Life on earth depends on a normal greenhouse effect to provide the appropriate temperature for its support. An

imbalance in the earth's normal greenhouse effect occurs when the man-made, or anthropogenic, emissions of

greenhouse gases contribute to an enhanced greenhouse

effect which shifts the balance between incoming and

outgoing radiation so that more radiation is retained, thus causing changes in the climate system.

Sulphur hexafluoride is an efficient absorber of

infrared radiation, particularly at wavelengths near

10.5 /um [21]. Additionally, unlike most other naturally

occurring greenhouse gases (e. g., CO,, CHJ, SF^ is largely immune to chemical and photolytic degradation;

therefore its contribution to global warming is expected to be cumulative and virtually permanent. Although the determination of the atmospheric lifetime'' of SF^; in the environment is highly uncertain because of the lack of

knowledge concerning the predominant mechanism(s) of

its destruction, it is very long; estimates range from 800

years to 3200 years [11, 14, 17, 22-24], with the higher

values being the most likely estimates. The strong

infrared absorption of SFf, and its long lifetime in the environment are the reasons for its extremely high global

warming potential which for a 100-year time horizon is estimated to be -24,000 times greater (per unit mass) than

that of CO2, the predominant contributor to the greenhouse effect [22]. The concern about the presence

of SFfi in the environment derives exclusively from this very high value of its potency as a greenhouse gas. While the potency of SF^, as a greenhouse gas is extremely high, the amount of SF^ in the atmosphere

compared to the concentrations of the naturally occurring

and other man-made greenhouse gases are extremely low.

Estimates of the relative contribution of SF^ to non-natural

global warming -using 1993 estimated SF^-concentration

levels - range from 0.01% [11] to 0.07% [9, 10]. In 100

years this value could become as high as 0.2% [9]. However, it is feared that SF^; and other small-volume

emissions may have a significant combined influence, and

that environmental effects not yet anticipated may be

exacerbated by their long lifetime in the atmosphere.

Government and environmental protection agencies,

electrical, chemical and other industries using or

interested in the use of SFj; [6, 11, 13, 14, 20] have

expressed concerns over the possible long-term

environmental impact of SF,,, and the electric power

industry is responding in a multiplicity of ways to better control SFfi usage than in the past and to reduce emissions

into the environment [9-11]. Because SF^, is already

widely used, there are obvious economic implications

about any attempts to regulate or control its production,

use, and eventual disposal.

Sulfur hexafluoride is an superior dielectric

gasfor nearly all high voltage applications. It

is easy to use, exhibits exceptional insulation

and arc-interruption properties, and has

proven its performance by many years of use and investigation. However, the extremely

high global warming potential of SF^

mandates that users actively pursue means to minimize releases into the environment, one of

which is the use ofother gases or gas mixtures

in place ofSF^.

The time taken for a given quantity of SF^, released into the atmosphere to be reduced via natural processes to -37% of the

original quantity.

1.5 SFg Substitutes

Gaseous insulation must be environmentally

acceptable, now and in the future. Therefore, the best

response to the concerns over the possible impact of SF^ on global warming is to prevent the release of SF^ into the environment. Clearly the most effective way to do this, is not to use SF^ at all. While such a proposition might be

environmentally attractive, it is difficult to envision the near term elimination of the use of SF^ in view of the

industrial reliance on the gas and demonstrated societal value of its use. This environmentally-friendly solution

does highlight the need for a search for alternative gaseous insulation and perhaps also the need for

alternative high-voltage insulation technologies.

SF^-substitute gaseous dielectrics are more difficult

to find than it seems on the surface, because of the many

basic and practical requirements that a gas must satisfy

and the many studies and tests that must be performed to allow confident use. For example, the gas must have a high dielectric strength which requires the gas to be

electronegative; however, strongly electronegative gases

are usually toxic, chemically reactive, and

environmentally damaging, with low vapor pressure, and

decomposition products from gas discharges that are extensive and unknown. Non-electronegative gases which

are benign and environmentally ideal, such as N,,

normally have low dielectric strengths. For example, N,

has a dielectric strength about 3 times lower than SF^ and

lacks the fundamental properties necessary for use by

itself in circuit breakers. Nonetheless, such

environmentally friendly gases might be used by

themselves at higher pressures, or at comparatively lower

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF^ / NIST
Section 1 .6 - Scope of this Report

pressures as the main component in mixtures with

electronegative gases, including SFf^, at partial

concentrations of a few percent.

The search for SF^ substitutes traces back many

years. It was especially intense in the 1970s and 1980s

when gases "superior" to SF^, were being sought. A

number of studies conducted mainly during this time

period, produced a large body of valuable information

(see, for example, Refs. 2 and 3) which needs to be

revisited and be reassessed not from the perspective of

finding "better" gaseous dielectrics than SF^, but rather from the point of view of finding gases or gas mixtures

which are environmentally acceptable and comparable in dielectric properties and performance to SF^. A rekindled

interest in "new" gaseous insulators may also direct itself toward finding gases or gas mixtures which are not

necessarily universally optimum for every high-voltage

insulation need, but which can be optimized for a

particular application.

Any program on substitutes needs to address

comprehensively the issues involved and evaluate possible

substitutes within the framework of the total environment.

Besides the obvious requirements of high gas pressure,

non-toxicity, non-flammability, availability and cost, there should be basic, applied, and industrial testing to assess

the thermal and electrical properties of other gaseous

dielectrics. Performance under various voltages (DC, AC,

impulse, transients), field configurations, and particle

contamination must be tested. Gas decomposition under

prolonged electrical stress, corona, breakdown, and arc must be investigated, along with gas aging and the influence of spacer and other materials. Gas mixtures in particular need to be looked at anew. Efforts must be

made to address concerns regarding mixtures which

include difficulties in handling, mixing, maintaining

constant mixture composition, reclaiming of mixture's

constituents, possible inferior performance with regard to thermal, insulation, and current interruption properties,

and the associated equipment design changes that such

use may entail. It must be emphasized, however, that gas mixtures should be tested under conditions (e.g., pressures, equipment design) where they are likely to perform well, not simply under conditions for which SF^

is better. It must also be stressed that historically resources have not been as abundant for the study of gas mixtures as they had been for the study of pure SF,;

.

of the electric power industry.

2. The tests required to document the suitability and

acceptability of a dielectric gas for the intended

application(s).

3. The feasibility of a "universal" gas mixture that could substitute for pure SF^ and help reduce the current levels of SF^ utilized by the electric power industry.

4. Alternate gases or gas mixtures for which a

significant amount of data are available

supporting their possible use in newly-designed

industrial equipment.

5. Possible gases or gas mixtures for which little physical data are presently available, but which

are sufficiently promising to justify further

research.

6. Recommendations on substitutes and future R&D

aimed at the development of environmentally

acceptable alternatives to pure SF^. Items 1 to 6 are respectively discussed in Sections 2

to 7 of this report.

2. Properties of Gaseous Dielectrics

The properties of a gas that are necessary for its use

in high voltage equipment are many and vary depending on the particular application of the gas and the equipment.

They are also interconnected and coupled. In their optimum combination one may achieve distinctly

desirable synergisms with regard to dielectric strength, for

instance, which clearly show that a gas mixture may be more than just the partial-pressure-weighted addition of

the dielectric strength of the individual mixture

components [2, 3, 25]. In the following sections, the gaseous dielectric properties which are of particular

importance in high voltage applications are identified. For the purpose of this report the properties of a gaseous dielectric are divided into four groups:

• intrinsic properties (physical and chemical);

• extrinsic properties (reactions, gas byproducts,

discharge and breakdown);

• other requirements for commercial use; and

• specific properties required for arc interruption,

transmission lines, and transformers.

1 .6 Scope of this Report

It is the purpose of this report to provide information

regarding the following:

1 . The required or desirable properties of any

dielectric gas for use in the various applications

2.1 Intrinsic Properties

Intrinsic properties are those properties of a gas which are inherent in the physical atomic or molecular

structure of the gas. These properties are independent of

the application or the environment in which a gas is placed.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 2 - Properties of Gaseous Dielectrics

2.1.1 Basic Physical Properties

One of the desirable properties of a gaseous

dielectric is high dielectric strength (higher, for instance,

than air). The gas properties that are principally

responsible for high dielectric strength are those that reduce the number of electrons which are present in an

electrically-stressed dielectric gas. To effect such a reduction in the electron number densities, a gas should:

• be electronegative (remove electrons by

attachment over as wide an energy range as possible); it should preferably exhibit increased electron attachment

with increasing electron energy and gas temperature since electrons have a broad range of energies and the gas temperature in many applications is higher than ambient;

• have good electron slowing-down properties

(slow electrons down so that they can be captured

efficiently at lower energies and be prevented from

generating more electrons by electron impact ionization);

and

• have low ionization cross section and high

ionization onset (prevent ionization by electron impact).

The significance of these parameters, especially electron attachment, in determining the dielectric strength of the

Table 1. Relative DC uniform-field breakdown strengths V," of some

dielectric gases.'

Gas Comments

SF« 1 Most common dielectric gas to date besides air

C3F8 0.90 Strongly and very strongly n-QF,„ 1.31 electron attaching gases. C-C4F8 -1.35 especially at low electron 1,3-C,F, -1.50 energies C-C4F, -1.70

2-C4F, -1.75 2-QF, -2.3 c-QF,3 -2.4

CHF, 0.27 Weakly electron attaching; CO, 0.30 some (CO, N,0) are effective in CF4 0.39 slowing down electrons CO 0.40 NjO 0.44

Air -0.30

Hj 0.18 Virtually non-electron attaching

N, 0.36 Non-electron attaching but

efficient in slowing down

electrons

Ne 0.006 Non-electron attaching and not Ar 0.07 efficient in slowing down

electrons "Based on Table 2 of Ref. 25.

"" Some of the values given are for quasi-uniform fields and may thus be somewhat lower than their uniform-field values.

"•' The relative values listed in the table can be put on an absolute scale by

multiplying by 3.61 x 10 ''^ V cm\ the uniform-field breakdown field, (£W)„„„ of SR.

gaseous medium can be seen from the representative data

for different gases in Table 1. It is evident in this table

that some gases actually exceed the dielectric strength of

SFfi. However, they all exhibit negative properties as to make them less desirable gaseous insulators in practical

systems as presently designed. Figure 3 illustrates the basic physical properties of electron attachment,

ionization, and scattering as they relate to the dielectric strength [25]. The most critical property of a gaseous

dielectric for high dielectric strength is a large electron

attachment cross section over a wide electron energy

range. The second most significant property is a large electron scattering cross section at low electron energies

to slow electrons down so that they can be captured more

efficiently and be prevented from generating more

electrons in collisions with the dielectric gas molecules.

Furthermore, the gas properties must be such that electron detachment from negative ions is prevented since

electron detachment is a major source of electrons that trigger gas breakdown. The negative ions that are formed

(through the formation of negative ions by electron attachment) must be as stable as possible. Detachment of

electrons from negative ions can occur via a number of

processes, foremost by autodetachment, collisional detachment, and photodetachment. Especially the former

process is a strong function of gas temperature [26].

The measurements needed to quantify the intrinsic physical properties of a gaseous dielectric for insulation

include:

• electron attachment cross sections;

• electron scattering cross sections;

• electron impact ionization cross sections;

• electron detachment cross sections

(photodetachment, collisional detachment, and

the associated processes of clustering and ionmolecule reactions ); and

• coefficients for electron attachment, ionization,

effective ionization, and transport.

Besides the above properties, there are a number of

other basic properties which are necessary for the complete characterization of the dielectric gas behavior

and its performance in practice. These include:

• secondary processes such as electron emission

from surfaces by ion and photon impact;

• photoprocesses;

• absorption of photoionizing radiation (this is a controlling factor in discharge development in non-uniform fields);

• dissociation under electron impact

decomposition;

• ion-molecule reactions;

• reactions with trace impurities; and

• reactions with surfaces.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 2.2 - Extrinsic Properties

T T

O ' z o

< :i

llAy-^''^ r(e.E/N)(eV'i-N2

I , \X (E/N)|,„= ).3«10-'5v-cr

.'/ M ^E/N= 1.24 « 10'^ Vcm^

////////////////////////////////// GAS

E/N

HV -

(1.5MV;')

-J e

8 10 12 ELECTRON ENERGY. C (eV)

16 18

Fig. 3. Total ionization cross section Oj (e) for Nj (—) and SF^ (-•-) close to the ionization onset. Total electron scattering cross section o,(t) as a function of electron energy, e, for Nj (—), and total electron attachment cross section a,(z) for SF^ (-•-). Electron energy distribution functions in pure Nj for two values of the density, N, reduced electric field E/N: at a value of 1 .24 X 10""' V cm^ about ten times lower than the E/N value at which breakdown occurs under a uniform electric field, and at the

limiting value of EJN (= 1.3 x 10"'^ V cm') at which breakdown occurs under a uniform electric field. The shaded areas designated by \\ and a are, respectively, a measure of the electron attachment and electron impact ionization coefficients for SF, (from [25]).

2.1.2 Basic Chemical Properties

The dielectric gas must have the following

"chemical" properties:

• high vapor pressure;

• high specific heat (high thermal conductivity) for gas cooling;

• thermal stability over long periods of time for temperatures greater than 400 K;

• chemical stability and inertness with regard to conducting and insulating materials;

• non-flammable;

• non-toxic; and

• non-explosive.

When used in mixtures, it must have appropriate

thermodynamic properties for mixture uniformity,

composition, and separation (see Appendix C).

2.2 Extrinsic Properties

Extrinsic properties are those which describe how a gas may interact with its surroundings, or in response to external influences, such as electrical breakdown and

discharges.

2.2.1 Reactions and Byproducts

To be used in electrical applications, a dielectric gas

should:

• undergo no extensive decomposition;

• lead to no polymerization;

• form no carbon or other deposits; and

• be non-corrosive and non-reactive to metals,

insulators, spacers, and seals. In addition it should have:

• no major toxic or adversely-reactive byproducts;

• removable byproducts; and

• a high recombination rate for reforming itself, especially for arc interuption.

Finally, the gas must be environmentally friendly, e.g., it must not contribute to global warming, must not deplete

stratospheric ozone, and must not persist in the environment for long periods of time.

2.2.2 Electrical Discharge and Breakdown

Properties

Specific properties of the gas under discharge and

breakdown conditions include:

• a high breakdown voltage under uniform and

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 2 - Properties of Gaseous Dielectrics

non-uniform electric fields;

• insensitivity to surface roughness or defects and

freely moving conducting particles;^

• good insulation properties under practical

conditions;

• good insulator flashover characteristics

• good heat transfer characteristics;

• good recovery (rate of voltage recovery) and self- healing;

• no adverse reactions with moisture and common

impurities; and

• no adverse effects on equipment, especially on

spacers and electrode surfaces. Also some knowledge must be available concerning its discharge mechanisms (corona, breakdown, arc) and

discharge characteristic behavior, and its decomposition

under arc and various types of discharges.

2.3 Other Requirements for

Commercialization

Commercial use of a dielectric gas requires certain non-physical characteristics, including widespread

availability, reliable supply, and long-range stability of

supply.

2.4 Properties of Gaseous Insulators for

Specific Industrial Uses

2.4.1 Circuit Breakers - Arc Quenching and

Current Interruption

An electric arc is the most crucial switching element

in a circuit breaker. It has the unique ability to act as a rapidly changing resistor such that during the AC current, high conductance is maintained. As the current approaches zero, the conductance decreases rapidly, and

finally, at zero current, the resistance rises to prevent re- ignition. Commercial circuit breakers utilize air, oil, SF^,

solid state, or vacuum as interrupting media. The arc properties for gas-based circuit breakers are a strong

function of the arcing gaseous medium. The most

significant required gas properties for arc interruption are:

• High dielectric strength comparable to that of

sulfur hexafluoride - This is one of the most essential properties characterizing a good interrupting medium.

• High thermal conductivity - This is another

'The optimum design of a gas-insuiated system requires

tiiis knowledge. Perhaps one can determine this through the so- called figure of merit, i.e., from basic measurements of {a-T\)IN

versus E/N. It would certainly be desirable to have a gas for which

these effects are less troublesome than for SF^.

important required property. The arc is initially hot

(temperatures in excess of 10,000 K), and it must be

quickly cooled down by removing energy from it by the

gas. Additionally, the arc must have a short time constant

for the increase in resistivity. For these requirements, the gas must have high thermal conductivity at high

temperatures and also should capture quickly free electrons when the gas is hot and the electrons fast. These

two properties - high thermal conductivity and high

electron attachment - lead to a high interruption

capability, i.e., enable a rapid transition between the

conducting state (arc plasma) and a dielectric state able to withstand the rise of recovery voltage. SF^ is known to have a time constant 100 times shorter than air and is used

in circuit breakers for two main reasons: it has a high

thermal conductivity at high temperatures which enables

it to rapidly cool down; SF^ and its decomposition

products are electronegative and thus enhance the

disappearance of electrons even when the gas is hot.

• Fast gas recovery - At the high temperatures

involved, the gas molecules are dissociated into their constituent atoms (atomized). They must quickly

reassemble, preferably to form their original molecular

structure. (Besides SF^, this is a property shared by a number of molecules with top symmetry such as a-bonded

perfluoroalkanes).

• Self-healing /dielectric integrity - This limits the

preferred gases to those that are either atomic in nature or molecular with very compact and stable structure, such as

SFj;, CF4, and other compounds, which when "atomized"

under the high temperature arc conditions reform

themselves with high efficiency, that is, the original

molecules are the main decomposition product.

2.4.2 High Voltage Insulation

There are two important types of basic gas-insulated

apparatus used by the electric power industry: gas- insulated transmission lines and gas-insulated

transformers. In this section are outlined some of the

principal properties a gaseous dielectric needs to be used

in such applications. Other applications with similar

needs include buses and disconnects in gas-insulated

substations.

2.4.2.1 Gas-insulated Transmission Lines - Here the

dielectric strength of the gas and its long-range stability

and inertness, along with its heat transfer properties at temperatures much lower than in circuit breakers

(£l 10 "O, are important gas requirements. Specifically, the required properties include:

• high dielectric strength (in uniform fields, non- uniform fields, in the presence of electrode

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF^ / NIST
10 Section 2.4 - Properties of Gaseous Insulators for Specific Industrial Uses

roughness and conducting particles, and for various geometries including co-axial

configurations);

• high vapor pressure at operating and ambient

temperature;

• chemical inertness;

• high thermal conductivity [but at temperatures far below those encountered in arcs (a few hundred

degrees above ambient)];

• no thermal aging (long-term, 40 years or more);

• no deposits (no carbon deposits, no

polymerization, and no decomposition);

• easily removable, non-harmful byproducts;

• no hazards (fire, explosion, toxicity, corrosion).

2.4.2.2 Gas-insulated Transformers - In very early

transformers, air was the most commonly used insulating

medium, but as the voltages were increased, oil was

substituted for air. While oil is presently widely used and

has many advantages, it bums when exposed to flame or heated to ignition point in the presence of air. Also,

certain mixtures of oil vapor and air explode on ignition

when confined. Additionally, breakdown due to charge

accumulation on insulating parts by ions transported by

the cooling pumps may occur, and flashovers due to particulate contaminants may be caused.

There are distinct advantages in using gas insulation

in transformers. Firstly, the use of a gas instead of oil completely removes the undesirable characteristics of oil just mentioned. Secondly, gas-filled transformers are

lighter, have better noise characteristics (since gas

transmits less vibration than oil), and are easier to handle.

Compared to oil, however, the gas is not as good for cooling (needs special techniques to remove the heat) and

thus gas-insulated transformers presently are unable to meet the highest ratings achieved by oil transformers. The

properties of the gas required for this application include:

• high dielectric strength at reasonable (e. g., 500 kPa) pressures;

• low boiling point (low condensation temperature,

high vapor pressure);

• low toxicity;

• chemical inertness;

• good thermal stability (because transformers are operated in a wide temperature range);

• non-flammable;

• high cooling capability (heat transfer is important

in transformers which frequently get quite hot);

• good compatibility with solid materials (because

the gas must coexist with many different solid materials in the gas-insulated transformer);

• good partial discharge characteristics (because of

the high possibility of partial discharges in the transformer);

useable over a range of temperatures (basic

properties as a function of temperature);

safe, easy to handle, inexpensive, securely

available.

3. Required Performance and

Testing of Gases

At first consideration one may be tempted to adopt

an extreme position for new gases.- ALL that has been

done on SF^ has to be repeated. While there is a need for any new gas "to be proven," this approach is unrealistic,

impractical, and perhaps unwise and unnecessary.

Clearly, before any testing is done, the gas must:

• be environmentally acceptable, or confined for

life,

• have no serious known health-related risks and

serious safety-related problems (toxicity,

flammability, etc.),

• have a high pressure (to be useful as a unitary gas

or as an additive in mixtures), and

• be available, stable, and thermally and chemically

inert. These requirements must be satisfied whether one is looking for potential gas substitutes on which tests have

already been made or for new gaseous systems for which

tests will be made, independently of the intended use. The list of other tests that are also useful and

desirable is long (see Sec. 2 on required properties) and

includes:

• breakdown tests as a function of pressure, field,

types of voltage, and time;

• comprehensive dielectric strength tests using

practical-size systems and voltages and

waveforms (i.e., DC, AC, lighting and switching

impulse, fast transients). Since the design of the high voltage insulation system is usually

determined by the lighting impulse test level (BIL), the lighting impulse test is a crucial test;

• effects of surface roughness and conducting

particles. Practical design levels for the dielectric strength are normally much lower than the

"theoretical" dielectric strength of a gas insulator,

because the dielectric strength of gases, especially

those for strongly electronegative gases, are very

sensitive to field perturbations such as those

caused by conductor surface imperfections and

by conducting particle contaminants;**

• dielectric strength measurements at high gas

"The design levels for SF,, have been quoted [27] to be of

the order of 37% of the theoretical strength of SFf, for lighting

impulse and 1 9% of the 60 Hz factory test for these stated reasons.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 4 - Possible "Universal-Application" Gas Mixtures 11

pressures (this is one type of measurement that has generally been lacking and is crucial);

• long-time tests;

• flashover voltages of insulators;

• thermal stability in the presence of other materials

(long-time stability with metals and resins), and

thermal aging;

• corona inception'^ and extinction

• thermal cooling.

• mass and light spectroscopy to identify the discharge products and their reactions for a number of purposes including diagnostics;

• measurement of dielectric strength as a function

of gas pressure, especially for weakly electron attaching gases or mixtures;

• scaling data on small laboratory equipment to large practical systems, and extrapolating data

taken over short time scales to the expected long

life times of industrial systems (e.g., 40 years);

• byproducts and possible health effects.

The list of desirable tests for use of a gas under arc or current interruption applications must also include:

• tests of arc and current interruption properties;

• recovery tests; and

• nozzle design and behavior.

4. Possible "Universal-Application"

Gas Mixtures

The most desirable SFf, substitute would be a gas that could be put in all existing SF^-equipment, requiring little or no change in hardware, procedures or ratings. Such a gas we refer to as a "universal-application" gas and we

define it as a gaseous medium which can be used instead

of pure SFft in existing equipment without significant

changes in practice, operation, or ratings of the existing

gas-insulated apparatus. It is a useful exercise to determine if such a substitute can be identified from the existing gaseous dielectric data. Of the many unitary, binary, and tertiary gases or gas mixtures that have been tested over the last three decades

or so, SF(;-N2 mixtures seem to be the most thoroughly

characterized [yet not completely tested, especially at high

'It has been pointed out by Wootton [28] that in tests on

a full size GIS with a fixed particle, typically less than 10% of the breakdowns occur without corona stabilization. Based on this information, Dale et al. [27] suggested that in practical apparatus it would be the corona inception level and not the corona stabilized breakdown level which is important. However, the strong corona

stabilization characteristics of electronegative gases can be

advantageous.

pressures (greater than 0.5 MPa)] gaseous dielectric media

besides pure SF^ [2-4, 6-8, 14, 25, 29-34]. There is broad acceptance of the view that these mixtures may be

good replacements of pure SF^. The main reasons are:

• they perform rather well for both electrical insulation applications and in arc or current interruption

equipment,

• they have lower dew points and certain advantages

especially under non-uniform fields'" over pure SF^,,

• they are much cheaper than SF^ especially after the recent large increases^ in the price of SFf,, and

• industry has some experience with their use. The relevant question, therefore, is: does an optimum

mixture composition and total pressure exist that allows

the use of this mixture as a "universal-application" gas, and could the industry readily use such a mixture? While

the answer to this question is complex, it is desirable to attempt to identify, on the basis of existing knowledge, a

particular mixture composition that may be best suited for consideration by the electric power industry for their needs. If such mixture can be identified, it can perhaps be

standardized in composition. Although it would be

desirable to have such a standard mixture prepared and

sold by chemical companies for direct use in the field, this may not be feasible, and the two gases would probably

have to be mixed to the standard composition at the point

of use (see Appendix C).

Based upon research conducted world-wide over the

last three decades or so, it appears that the optimum

composition of an SF^ -N, mixture for use by the electric power industry in place of pure SF^, for both high voltage

insulation (for gas-insulated transmission lines and gasinsulated transformers) and arc or current interruption

purposes may be in the range of 40% to 50%SFft in N,.

Thus, possible standard mixtures that can reasonably be

considered are 40%SF6-60%N2 or 50%S¥(-50%n,.

The savings" of replacing pure SF^ by a 40%SF(;-

60%N2 gas mixture are potentially large. If it is assumed

that 80% of the -8,000 metric tons of SFf, produced

annually is used by the electric power industry (Sec. 1.2; [12]), at a price'^ of $20 / lb (~$42 / kg) for SF„ the total annual savings in the cost of SF^ will be about $150

million.

'"The more electronegative the gas is, the larger the reduction of its dielectric strength under non-uniform tleld conditions and in the presence of conducting particles.

"Perhaps even higher savings may be possible if the percentage of SFf, is lowered further by increasing the total operating pressure of the mixture. Limited measurements on the arc interruption capability of pure SF,, in the pressure range 0.41 MPa

to 0.72 MPa ([3], p. 51) indicate that it increases almost as the square of the till pressure.

'^Based on the spectrum of prices, it seems logical to assume a price of about $20 per lb ($42 / kg).

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
12 Section 4.1 - Insulation

>

uu

1 1 1 1

<i<b..'' O^,-' 80 ~

V'-'''

60 -

40

'^-

20 0^ -

1

1 1 1

800

20 40 60

PERCENT ADDITIVE TO Ng

80 100

BY VOLUME

Fig. 4. DC breakdown voltage as function of electron attaching additive

to nitrogen (uniform and quasi-uniform electric fields; the total gas pressure

is 66.66 kPa and the electrode gap is 7 mm). The broken curves are extrapolations (from [35, 36]).

The feasibility analysis of a universal application

mixture for insulation applications, and arc and current

interruption purposes is based on information obtained

from a number of sources, the most significant of which

are briefly discussed below. Additional pertinent

information related to mixtures with even lower

concentrations of SF^, is presented in Sec. 5.2.

4.1 Insulation

4.1.1 Gas-insulated Transmission Lines

Existing information suggesting the use of SFfi-Nj

mixtures for insulation purposes has been summarized and

discussed in a number of recent publications (see, for example, Refs. [3, 6, 14, 33, 34]). In this section we refer

to and supplement the work summarized in those reports,

which indicates the possibility of adopting the 50%SFfi50%N2 mixture as a standard gas option for gas-insulated

transmission lines. Most of the information presented also supports the use of such mixtures for gas-insulated

transformers (Sec. 4. 1 .2) and possibly also circuit breakers

(Sec. 4.2). It has been known for a long time that the breakdown voltage of SF^-Nj mixtures saturates as the percentage of SF^ in the binary mixture is increased above

about 40%. This is seen from DC measurements ([35,

36], Fig. 4), AC measurements ([37], Fig. 5), and impulse

measurements ([37], Fig. 6). Above this saturation level,

addition of more SF^ to N2 yields limited returns for

insulation applications. This has been shown by many

0.2 0.4 0.6 0.8 SFg CONTENT PER UNIT, R1.0

Fig. 5. Measured (symbols) and calculated (solid lines) 60-Hz breakdown

voltage values for SFf,-N2 in coaxial electrode geometry (from [37]).

Studies. For instance, Bouldinetal. [30, 31] conducted an assessment of the potential of dielectric gas mixtures for

industrial applications based mostly on DC uniform and

quasi-uniform field data at pressures less than a few

hundred kPa. They concluded that a 50%SF6-50%N2

mixture, operated at 15% higher pressures, exhibits the same dielectric strength as 100% SF^, but at -35% lower

cost (calculated using a price of SFg more than ten times

lower than it is today). A 50%SF(;-50%N2 mixture was

listed as having 0.88 the dielectric strength of pure SF^ at the same pressure and a condensation point 20 "C lower.

Malik and Qureshi [38] reviewed the work on

electrical breakdown in mixtures of SF^ and other gases

1400

1200

1000

800

600

400

200

J i L

0.2 0.4 0.6 0.8 1.0 SFg Content - Per Unit

Fig. 6. Negative lightning impulse breakdown voltages for SF^-Nj

mixtures. The solid curves are semiempirical fits to the measurements (from [37]).

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF^; / NIST
Section 4 - Possible "Universal-Application" Gas IVIixtures 13

including N2. They state: "SF^-Nj mixtures containing

50% to 60% of SFfi have dielectric strength of up to 85%

to 90% that of pure SFf;. Such mixtures can have

improved impulse and power-frequency breakdown

strength in highly non-uniform field gaps and therefore

are expected to be less sensitive (than pure SF^) to the presence of free conducting particles and electrode surface

roughness." Furthermore, the mixtures can be operated at pressures considerably higher than 600 kPa which is the upper limit for SF^-insulated apparatus [39] and at considerable reduction in cost [38]. In view of the superior insulation properties of N2 at higher pressures and in non-uniform fields compared to pure SFfi, the advantage of the 50-50 mixture over pure

SF(i may be even greater. For example, non-uniform

(positive point-plane electrode geometry) DC breakdown

measurements [36] as a function of the total pressure showed that the dielectric strength of a 30%SFf;-70%N2

mixture at -600 kPa is somewhat higher than that of pure

SFfi under the same conditions. Similarly, Nakanishi [40]

concluded that "a gas mixture of SFfi-Nj (and SFf^-air) is thought to be the most promising candidate for application

to high power apparatus. SF^-Nj (and SFfj-air) mixtures

have breakdown properties superior to pure SF^ at non- uniform fields." A recent example [41] of the voltage versus pressure

characteristic of SF^ and a 75%SFf;-25%N2 mixture is shown in Fig. 7. Included in the figure are measurements

of both the breakdown and the corona onset voltages for the two gases. The measurements were made using

nonuniform fields and lightning impulse voltage. The

corona onset for SF^ and the SF^^-Nj mixture scales with

the respective uniform field breakdown voltages of the two gases, but the breakdown voltage exhibits the usual corona stabilization region which varies with mixture

composition. Depending on the mixture composition

there are total pressures for which the breakdown voltage

of the mixture exceeds that of pure SF^;. Similar conclusions have been reached by other

impulse breakdown studies. Lightning and switching

impulse breakdown measurements in the pressure range

between 0. 1 MPa and 0.7 MPa by Cookson and Pedersen

[37] led them to conclude that "the SF^, mixtures with N2

(or air, or CO2) look promising for compressed gasinsulated transmission (CGIT) applications with a 50-50

mixture at a typical pressure of 0.54 MPa being able to replace SF,; at 0.45 MPa without loss of breakdown

strength." Similarly, Cookson [42] concluded that mixtures of SF,; with Nj can be readily applied in practical

CGIT lines at a cost savings over SF^. Rein and Kulsetas

[43] studied lightning and switching impulse breakdown

of SF(,-N2 mixtures using electrode configurations

representative of open disconnectors and earthing

switches and concentric cylinder systems, and pressures

80

60

J

40

r-l

20

x:75%SF6/25%N2

o:SF,

.r^x^

^'y Breakdown

Corona onset

0.1 0.2 0.3 0.4 Pressure (MPa)

Fig. 7. Voltage versus pressure characteristic of SF,, anda75%SF^

-25%N2 mixture for a point-plane gap and lighting impulse (+1 .2 / 50 us) (from Qiu and Feng [41]]).

ranging from 0.5 MPa to 1.5 MPa. They concluded that "compared to pure SF^ of 1 .0 MPa, a 50%-50% mixture

of SFfi and Nj with the same total pressure retains about

85% of the dielectric strength. An increase of Nj content

to a total pressure of 1 .5 MPa gives a dielectric strength

equal to that of 1.0 MPa SF^. The condensation

temperature is thereby lowered from - 15 "C to -40 "C." Furthermore, Fatheddin et al. [44] investigated the

breakdown properties of SF^-Nj mixtures using lighming

and switching impulses of both polarities, a point-plane

geometry, and total pressures between 0.05 MPa and

0.5 MPa. From Figs. 1 to 5 of their paper it appears that a40%SF(;-60%N2 mixture is an excellent choice. For this mixture, the impulse polarity had negligible effect with

lightning surges. However, the negative polarity V50 (V50

is the peak voltage with 50% breakdown probability)

values were higher and the positive V50 values were lower

for the (slower) switching surge pulse. Interestingly, their positive DC point-plane geometry measurements (Figs. 6

and 7B of their paper) showed a 30%SFft-70%N2 mixture

to be at least as good as pure SF^ for total pressure greater

than 500 kPa.

Very importantly, a number of studies [3, 29, 45-52]

have shown that in the presence of particles a number of

SFfi-Nj mixtures perform well compared to pure SF^. They

have also indicated that the effect of particles on the breakdown strength of such mixtures depends on the total pressure and on the partial pressure of the component

gases (Fig. 8; Table 2). The data in Table 2 are

particularly interesting. They show that for certain

conditions (DC, cylindrical electrodes, in the presence of

conducting particles as contaminants) the highest

breakdown voltage for a 50%SF(,-50%N2 mixture

corresponds to a total pressure of about 608 kPa (~ 6 atm)

(see Table 2), which is a reasonable pressure for use in

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF,-, ' NIST
14 Section 4.1 - Insulation

3UU NI

r 1 1

s "? ^SFs

i

/fii ^""""^f^^^iy /~ ^°°^° '^2

^°°^° ^^B

KDOWN

VOLTAGE,

kV

-•

to

8

S

/' -~-~-\y...A }

,'kj

>••• -/ Iv"" -^""""^ - ^ 98% Nj + 2% SFg <

•" 1 1 1 5 10 15 PRESSURE, Atm, Abs.

Table 2. DC breakdown voltages of SF^-N^ mixtures with cylindrical

electrodes and particle contamination [52]

SF,-Nj V,,(kV) V,,(kV) V,,(kV) V,,(kV) V,,(kV)

303.9 kPa 405.2 kPa 607.8 kPa 810.4 kPa 1013 kPa

FIG. 8. AC breakdown voltage in SF^-Nz mixtures with 0.043 cm (0.017

in) diameter copper wires, 0.635 cm (0.25 in) long in a 7.62 cm (3 in) plane gap [3, 45, 46]. The 60%SFs-40%N2 data are shown by the broken

line.

gas-insulated equipment. However, more work is needed

on particle-contaminated SF6-N2 gas mixtures. Present

data are not sufficient to fully characterize the behavior of

such mixtures as a function of partial or total pressure. The solid-gas interface has its own breakdown

characteristics. Generally, the breakdown voltage is lowered by the presence of a spacer. A 50%SFfi-50% Nj

mixture has about 90% the flashover voltage of pure SF^

in the presence of spacers [31] (see also [53]). Similar

conclusions have been reached by other researchers. For

instance, Nakanishi [40] cited work by M. Hara et al. on

the flashover characteristics of a cylindrical spacer on which a conducting particle was affixed in an SF^-Nj gas

mixture which "showed that the flashover properties can be improved by mixing 20%SFfi into N2."'^ Furthermore, Eteiba et al. [54] measured the breakdown voltage of particle-contaminated spacers using

60-Hz and negative lighting impulse voltages. Figure 9

compares the dielectric strength of a clean spacer (curves

A) to that obtained with a 2-mm long aluminum wire of

0.8 mm diameter particle attached on the spacer interface 2.6 mm from the center conductor (curves B) and from the outer envelope (curves D). The authors concluded that their results show no significant difference in the 60-Hz

withstand voltage between pure SF^ and the 50%SF(;-

50%N2 mixture for either the clean or the particle

contaminated system and the 50%SFfi-50%N2 mixture has

only a slightly lower impulse ratio than pure SF,;. However, the breakdown characteristics of spacers for SFft and SF(i-N2 mixtures as well as their cooling efficiencies need further investigation in order to quantify the performance of the mixtures under practical conditions, as has been pointed out by Endo [55].

100/0 59.6 62.1 70.0 67.5 60.0

80/20 45.7 49.0 59.6 58.6 50.1

60/40 50.7 54.1 66.0 62.4 61.2

40/60 24.3 39.5 55.7 50.9 43.5

20/80 26.3 38.5 37.2 41.9 33.4

'^M. Hara et al. as quoted by Nakanishi [40].

Similarly Blankenburg [56] found that the flashover

behavior of cylindrical insulators in SF^-Nj mixtures

subjected to AC voltage was found [88] to be qualitatively

similar to that in pure SF^ independently of the amount of

SFg in the mixture (even when the mixture contained as

little as 1%SF6).

Additionally, according to Waymel and Boisseau

[57] recent dielectric tests on real-size gas insulated

transmission line (GITL) compartments confirmed the good industrial performance of SF^-Nj mixtures. Partial conclusions could be reached by them in the particular case of buried 400 kV GITL. They concluded that "compared to pure SFf,, SF6-N2 mixtures offer good

compromise with the diameter of busbar required by the

thermal design of buried GITL."

Interestingly, the uniform field breakdown strength

of SFfi has been found [58] to increase by ~1 1% in the

temperature range 300 K to 600 K. Because the presence

of N2 in SF6-N2 mixtures is not expected to change the

dissociative electron attachment properties of SFf; which

are responsible for this increase, a similar increase in the

dielectric strength of SF6-N2 mixtures with increasing

temperature might be anticipated.

The behavior of a 50%SF(;-50%N2 mixture under fast transient conditions has been investigated by Pfeiffer and

co-workers. They found no significant difference in the behavior of the mixture compared to pure SF^ (e. g, see

Pfeiffer et al. [59] ; see also discussion in [6]). Concerning the decomposition of SF^-Nj mixtures,

there exist only limited data on the decomposition

products of SFfi-Nj mixtures (see discussion in [6]). These

data are mainly of corona decomposition. They show that there is very little chemical interaction between SF^ and

N2 in discharges and that the predominant oxidation

byproducts are those seen in SF^ (SO2, SOF2, SO2F2, and

SOF4). However, the presence of Nj may reduce the

ability of SF^, to reform itself following an arc or a discharge and thus it may inhibit its recovery. This needs

further investigation.

Finally, to our knowledge there is only one

toxicological study [60] on SF^-Nj mixtures, which

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 4 - Possible "Universal-Application" Gas IVIixtures 15

0,1 OZ 03 Ol4 Gai pman (MR))

(a)

hardly affected, but the ahmentary systems are generally

influenced.

For gas-insulated transmission lines, SF^-Nj

mixtures in general and the 40%SF6-60%N2 mixture in particular have great industrial potential. Depending upon

the test, mixtures of SF(i-N2 appear to perform at least at levels of 80% of pure SF^;, and in some cases SF^i-Nj

mixtures exceed pure SF^ performance. Indeed, some

members of the electric power industry are in the process

ofdesigning and/or building GITL using SFfi-Nj mixtures

for insulation purposes. The use of SFf;-N2 mixtures in existing GITL designed for pure SFf;is more problematic

due to the need for possible equipment changes and

derating or recertification of existing equipment.

4.1.2 Gas-insulated Transformers

440 -

400

360

_320

>t280

?

1 240

I

200 S£ 160

8 120

80

40

Portidi posiNan EpoiyipiMr

Outtr MfMlop*

• 100%SF,

X 50%SfB*50i;(toi , a WOUNj

'Porlidi poilhon^ 8

0,1 0,2 0,3 Gas pressure (MPo)

0.4

(b)

360

330

300

270

240

210 5

I 180 £

120 I

90

60

30

Fig. 9. (a) Variation of the AC voltage in SF^, N^, and the mixtures 50%SF,-50%N2and 75%SF,-25%N2 (from Eteibaet al. [54]). (b) Variation of the 50% negative impulse breakdown voltage for SF^, Nj, and the mixture 50%SF,-50%N2 (from Eteiba et al. [54]).

concentrates on the toxicological action of arc- decomposed SF(;-N2 mixtures (and pure SF^;). Its main

conclusions are: (i) the lung, liver, and kidney can be

attacked by arc-decomposed SF^ gas and the alimentary

system also can be influenced by the arced SF^;; and (ii) arced SF^-Nj mainly attacks the lungs of the animals

exposed to the gas; livers, kidneys, and other organs are

As was indicated in Sec. 2.4.2.2 of this report, heat

dissipation is a significant requirement for gas-insulated

transformers (GIT) in addition to the gas dielectric insulation characteristics. A number of recent studies [55,

61-65] considered SF(;-N2 mixtures as the insulating and

heat transfer medium for gas-insulated transformers in spite of the fact that their insulating and heat-transfer (cooling) capabilities are somewhat lower than for pure

SFfi. A recent study on the temperature distribution in SF6-N2 mixtures-insulated existing transformers [63] has

led to the conclusion that "SFf,-N2 mixtures-GIT meets the

standards completely and it can be applied in electric power systems." This same study found that a mixture

ratio 55%SF(i-45%N2 has "good characteristics." Similar

studies [61, 62] concluded that: (i) the application of SF^-

N2 mixtures as the insulating and heat-transfer medium is feasible, (ii) with the same construction as for pure SF,;, SFfi-Nj mixtures can be selected with composition as high

as 55%SF6-45%N2 with good insulation characteristics,

and (iii) for 10 kV class SFj^-Nt mixtures GIT, the heattransfer characteristics of the gas mixtures are the

controlling factor in the design of insulation construction.

Because the temperature rise [55, 64, 65], of a 50%SF6-50%N2 mixture over that of pure SF^ is significant (approximately 15 "C to 20 "C) [63], it was

suggested [64] that amorphous steel construction may

help alleviate the heat transfer problem and allow use of

a lower percentage of SF^ in the SF^-Nj mixtures. The use

of SFft-Nj mixtures may, thus, need to be coupled to the use of more heat resistant materials and modification of

the transformer cooling design.

Overall, in spite of the difficulties mentioned in this section regarding the cooling capabilities of the SF^-Nt

mixtures, a 50%SF6-50%N2 mixture can be a potentially useful gas-insulated transformer medium and further

studies are indicated.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFf; / NIST
16 Section 4.2 - Interruption

4.2 Interruption^^

As discussed in Sec. 2, for arc and current

interruption, the dielectric, switching, and thermal

properties of the gas are important. Characterization of

the cooling capacity of an interrupting gaseous medium

involves consideration of the specific heat and specific

thermal conductivity of the gas, as well as its ability to dissipate heat by convection. Nitrogen (and other light gases such as He) supplement SF^; in this regard, SFj;

being efficient at the very high temperatures (say,

10,000 K to 3,000 K) and N2 (or He) at the relatively

lower temperatures (say, below 3,000 K). Table 3 lists the

specific heats, specific thermal conductivities, and

coefficients of viscosity of SF^;, Nj, and He.

There have been a number of studies on the arc and

current-interruption capabilities of SF^i-Nj mixtures and

their performance in comparison to pure SFf^. Most such

studies on circuit breakers used either of two types of gas

circuit breakers (GCB). One is a double pressure type,

and the other is a puffer type. Their structures and thus

current-interruption capabilities are different. In the double pressure type GCB, high pressure gas is always

stored in a high pressure vessel and the compressed gas in this vessel is blasted as soon as the contacts are separated.

In the puffer type GCB, it is necessary to compress a gas

in a puffer cham>ber during the opening stroke. The

compressed gas is blasted to arc through an insulation

nozzle. In this type of operation, the pressure increase and

its duration are crucial variables for current-interruption

capability. Most current GCBs are of the puffer type.

A comprehensive review and discussion of gases for

arc interruption prior to 1982 was given in [3]. One of the

significant results of this study is the observed strong

dependence of the arc interruption performance of a gaseous medium on the total gas pressure, P. The rather limited data in this report [3] indicated that the arc interruption capability of SF^ increased superlinearly with

increasing pressure. This is significant because a small

increase in the total pressure of an SFf^-N, mixture may

compensate for the reduction in the arc interruption

capability of the mixture relative to pure SF,;. This

work [3] also concluded that: "For general purpose high

voltage gas circuit breaker applications, SF,; will be the

interruption medium. However, there are applications for which other media can be viable alternatives. For

example, a European manufacturer offers SFf,-N2 as part

of the puffer line with about 20% current derating in

Table 3. Specific heat, specific thermal conductivity, and coefficient of

viscosity for SFn, N;, and He.

'"See Ref. [3] for a list of patents up to 1980 on gases for

electrical arc interruption. Also see Chervy et al. ([66, 67, 68]) for information on the arc interruption capabilities of SFs-CF4and SF^

-CjFf, mixtures, Nakagawa et al. [69] for the interruption capability of SFfi-CF4 mixtures in puffer type gas-blast circuit breakers, and Middleton et al. [70] for work on SFf,-CF4 circuit breakers.

Gas Specific heat"

(cal g' K-')

Thermal

conductivity" (W m' K')

Coefficient of

viscosity'' (poise)

SF, 0.157 0.0155 161 X 10-''(25°C)

N2 0.248 0.0238 163 X 10-'(0''C)

He 1.242 0.150 189xlO-'^(0°C)

"Data provided by Endo [55] (Toshiba Corporation). 'From Clark [71].

interrupting capability for applications in extreme low

temperature environment ( < -40 "C). Our data confirms

that our puffer interrupters can be applied without design

alteration. Furthermore, with interrupters designed

specifically for SF^-Nj, no derating is necessary with

benefits of less SF,; gas required, elimination of special

heaters, and because of overall lower gas mass for a given

pressure level, lower mechanical energy to operate the

breaker. The combination can offer a lower cost

interrupter with wider operating temperature range. Additional data on interrupter development specifically for SFfi-Nj will be required to be more quantitative in regard to the economic advantages of SF^-Nj interruption

medium."

Another significant study is that of Grant et al. [72]

who compared the performance of SF(;-N2 mixtures as interruption media of gas-blasted arcs for various mixture

compositions and total pressures of 500 kPa, 600 kPa, and

700 kPa. They measured the rate of rise of the recovery

voltage (RRRV) capability, as a function of concentration

of added Nj (or He) to SF,;. Their results along with

similar measurements by Garzon [73] are shown in Fig. 10. They show that the peak in the RRRV versus SFg

percentage moves towards lower SF^ concentrations at higher total pressures. These investigations also showed

that the addition of appropriate amounts of Nj (or He) to

SFf; can result in improved RRRV performance of up to 40% above that of pure SF^; (Fig. 11). The measurements

of Grant et al. [72] on SF^-Nj mixtures and Garzon [73] on SFfi-N, and SFf^-He mixtures are listed in Table 4. The

measurements of Leeds et al. [74] on SFj^-air mixtures are

also listed in Table 4 for comparison. As can be seen from Table 4, the measurements of Garzon [73] on the

rate of rise of recovery of voltage (RRRV) for a synchronous interrupter show that the performance of SF(; -N2 mixtures having 50%SF(; by volume at pressures of

1300 kPa to 1900 kPa is approximately 1.39 times better than for pure SF^,. Garzon also found that the recovery

capability of a non-synchronous circuit breaker using this gas mixture was at least as good as when pure SF^ was

used. The optimum interrupter performance, judged in terms of its voltage recovery capability, is observed to

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 4 - Possible "Universal-Application" Gas Mixtures 17

Table 4. Recovery performance factors^ normalized to pure SF, as listed

in [69]).

N, N, N, N, He Air %SF, 500 600 700 1700 600 1000 kPa kPa icPa kPa kPa kPa

[72] [72] [72] [73] [73] [74]

100 1.0 1,0 1.0 1.0 1.0 1.0

90 1.32 1.07 1.13 1.02 0.98 -

75 1.03 1.24 1.46 1.08 1.12 -

65 - - 1.52 1.17 - -

60 - 0.93 - 1.22 1.13 -

50 1.0 0.82 0.86 1.33 1.14 0.52

40 - - - 1.39 - -

25 0.56 0.38 0.52 0.90 1.08 0.28

"Ratio of the RRRV for a given mixture to the RRRV for pure SF^.

occur when the mixture composition is roughly 50%SFf,-

50%N2 (Fig. 10). Garzon pointed out that these results using a double pressure type cannot be generalized for the design of all circuit breakers, but in applications where

conditions are similar to those of his experiments, "it will be safe to assume that the use of a 50%-50% mixture of

Nj and SF^ will serve to improve the dv/dt recovery

capability of the interrupter." While this conclusion is for higher pressures than are normally encountered in practice, Grant's data in Fig. 10 and the data in Table 4

clearly support this statement for lower total pressures as

well. The results of Garzon were obtained with a synchronously operated interrupter, and "therefore it is conceivable that non-synchronous operation may alter some of the findings." However, Garzon states that "it is our experience that the recovery capability of a non- synchronous breaker using a 50%SF(;-50%N2 mixture was

at least as good as when 100%SF(; had been used." Their

results taken between 1.38 MPa and 1.93 MPa indicate

improved capability with increasing total pressure and this finding is consistent with earlier results [3]. Studies on full-size puffer interrupters using pure SF^

and SFft-Nj mixtures by Solver [75] led him to conclude

that "a mixture of 69% SF^, and 3 1 % N2 had considerably

higher recovery speed than pure SF^ at the same SF^

partial pressure."

As mentioned previously, Malik and Qureshi [38]

reviewed the work on electrical breakdown in mixtures of

SFfi and other gases including Nj. They pointed out that previous work [72, 73, 76-78] shows that it is possible to further enhance the excellent arc interruption properties of

SFfi by using SF^ mixed with lighter gases such as nitrogen or helium

Naganawa et al. [79] investigated the DC

interruption by a spiral arc in SF^-Nt gas mixtures in the pressure range 0.1 MPa to 0.8 MPa . The mixtures they

2.5

2.0

1.5 -

1.0

0.5 -X25 50 75 tSF,

100

Fig. 10. RRRV as a function of SFft-Nj mixture ratio. Curves 1-3 are the data of Grant et al. [72] and Curve 4 are the data of Garzon [73] (adapted from Fig. 2 of [72]). The measurements of Garzon were made at a pressure of nOOkPa.

Studied contained a constant partial pressure of SF^, equal

to 0. 1 MPa. The voltage-current characteristic curve of

the spiral arc for the mixture 50%SFf;-50%N2 was slightly

below the similar curve for pure SF,; at the same total pressure (0.8 MPa). They recommended SFft-N2 as "an

extinguishing medium of switch gear to avoid the

liquefying phenomena of pure SF,; gas of high pressure under extremely low temperature and to reduce gas costs." However, other studies (see below) indicated that the 50%SF(i-50%N2 mixtures performed not as well as pure

SFj; as arc or current interrupting media.

A comprehensive evaluation of and measurements on gases for arc interruption (puffer-type interrupter, current range -10-15 kA) was conducted by Lee and

Frost [80]. They concluded that "the results of previous

investigators reaffirmed the overall excellent arc

interruption ability of SFj^, while other gases and gas

mixtures can have comparable performance in some

aspects of interruption." They themselves screened about

250 gases and out of these they selected 40 gases and gas

mixtures for experimental evaluation. In Table 5 are given the arc interruption capabilities they measured for

SF(,-N2 mixtures, SFf,-He mixtures, and pure SF,; for two

values of the load line Zq. These data show that the

relative interruption capability of a 50%SF(;-50%N2

mixture is only about 70% that of pure SF^,. This seems to be at variance with the studies mentioned above and

points to the need for further studies. Nakagawa et al. [69] performed calculations aimed

at examining SF(;-N2 gas mixtures in a buffer-type GCB.

Their theoretical study showed that (i) the current

interruption capability of the mixture depends on the

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF^^ / NIST
18 Section 4.2 - Interruption

Table 5. Measured arc interruption capabilities" of gases and gas mixtures

at 0.6 MPa (Lee and Frost [80])

Gas or mixture

Zo = 450 Q

I.. (kA)

Z,, = 450 Q

Relative

interruption

capability

Z,, = 225 Q

Relative

interruption capability

Z„ = 225 Q

Ic (kA)

100%

SF,

21.0 100 100 26.3

75%SF,

25%N2

17.8 85 78 20.4

50%SF,

50%N2

14.9 71 65 17.2

75%SF,

25%He

15.4 73 78 70.4

50%SF,

50%He

14.7 70 75 19.7

The critical current I^, can be defined as that current where the critical RRRV line intersects the load line Z„. Higher I^ corresponds to higher

interruption capability. For practical transmission and distribution power

circuits, a Z,, of 450 Q is typical.

partial pressure of SF^ in the mixture, and (ii) that SF^-Nj

gas mixtures are inferior to pure SF^. The interrupting

abihty of the SF^-Nj gas mixtures containing a given

amount of SF^ was found to deteriorate when Nj was

added to the mixture. For instance, the interrupting

capability of 300 kPa of pure SF^ was higher than that of a mixture of 300 kPa SF^ + 200 kPa N2. The no-load

characteristics of 300 kPa SF^ + 200 kPa Nj gas mixtures

showed that the rate of pressure rise was higher than that of pure 300 kPa SF^ , and that in spite of the higher value

of the total pressure of the SFf;-N2 mixtures, the pressure

fall occurred faster in the mixture than in pure SF^;

These findings are at variance with the work of Grant

et al. [72] who reported that the interrupting abilities of

SFfi-N2 gas mixtures become higher at certain mixture

ratio (see Figs. 10 and 11) but are consistent with the calculations of Tsukushi et al. [81] who examined the curtent interruption capability of SF,; gas mixtures using

puffer-type GCB. According to Tsukushi et al. for currents of -15 kA, a 300 kPa SF^ -1- 200 kPa Nj showed

76% of di /dt of pure SF^ . Their calculation of the puffer pressure rise of gas mixtures in puffer-type gas blast

circuit breakers for SF^ and SFfi-N2 mixtures indicated

that the SF^ partial pressure in a mixture was lower than

the pure SF^; pressure when the pure SF^, filling pressure equaled that of the SF^, partial pressure in the mixture.

This was attributed to increases in the mass flow of SFf; caused by the Nj gas. Thus these calculations showed that the pressure characteristics in a puffer chamber are

different for SF,, and SFfi-N2 mixtures. This seems to be

bom out by other calculations discussed below [82-87].

The interruption capability of SFfi-N2 mixtures has

2.0

a. >

1.5

1.0

SFg/He_-7-

/

^

oc 0.5 /

1

SFg/Nj

1 1

-

25 50 75 100 ISF,

FIG. 11. RRRV as a function of SF^-Nj and SF^-He mixture ratio for an upstream pressure of 600 kPa (from Grant et al. [72]).

been investigated by Gleizes et al. [82-87] in a series of

papers. Specifically, Gleizes et al. [82-84] reported

measurements of the axial temperature in a steady state arc plasma burning in SF^^-Nj as a function of current

intensity. They found that the axial temperature value is a complex function of radiation, thermal, and electrical conductivities and it may not be intermediate to those of

pure SF(5 and pure Nj. At high currents the energy losses were found to be dominated by radiation. In another

paper Gleizes et al. [81] calculated thermodynamic

properties and transport coefficients for SF^-Nj mixtures

in the temperature range 1000 K to 3000 K under the

assumption that the number densities involved in the

computation are those of a plasma under local thermodynamic equilibrium. Figure 12 shows some of

their results on the dependence of the thermodynamic

properties of N2, SF,; , and SF^-Nj mixtures. It seems that the thermodynamic properties of the 40%SF^ -60%N2 are not significantly different than those of pure SFf;. Gleizes et al. [84] also performed calculations on the

variations of temperature and conductance during the

extinction of nonblown, atmospheric pressure, wallstabilized arcs and concluded that "the use of SF^-Nj

mixtures as a gas fill for circuit breakers will be efficient

(i.e., will largely preserve the interruption properties of

SFfi) when the proportion of SF,; is higher than 50%." See

Refs. [85-87] for further calculations on the various

parameters of significance in the performance of gas

circuit breakers depending on type and gas medium and

on the role of plasma convection.

Sasao et al. [88] simulated the arc dynamic behavior

of gas-blasted arcs using SF(;-N2 mixtures. Their

simulations indicate that the use of SF(;-N2 mixtures may

require design changes of the arc chamber in order to optimize the arc quenching capability, and that these

changes would depend on gas composition. They did not, however, indicate the "optimum" mixture composition.

They found that the arc quenching ability of the SFfi-N2

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFe / NIST
Section 4 - Possible "Universal-Application" Gas Mixtures 19

40% SF -60% N

e 2

10 20

Temperature(10 K)

(a)

20

1^

bJD

&10

= 2 atm

PURE N2

*07l SF6-eOK N2

PURE

10 15 20 25

Temperature(10 K)

(b)

15

i4

ft 10

o

40;: sF6-so% N2

10 15 20 25

Temperature(10^ K)

(c)

0)

6

CM2 4

P=2 atmospherea //

^^^ y

• / '<'"

. PITRB N?

/

•-V 40% sra-60x nj

/

PUKE SFS 1

10 15 20 25

Teinperat\ire(10 K)

(d)

Fig. 12 a, B, C, D. Calculations by Gleizes et al. [83] of the variation of enthalpy with temperature and pressure of a 40%SF^-60%N2 mixture (Fig.

1 2a); variation of the constant-pressure specific heat, Cp, with temperature for pure Nj, pure SF^, and 40%SF^-60%N, mixture (Fig, 1 2b); evolution of the peaks of the constant-pressure specific heat with pressure of a 40%SFs-60%Nj mixture (Fig. 12c) ; and variations of the speed of

sound, V, as a function of temperature for pure Nj, pure SF^, and 40%SFs-60%N2 mixture (Fig. 1 2d). Note that these parameters for pure SF^ and

the 40%SFfi-60%N2 mixture are rather close.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
20 Section 4.2 - Interruption

10

o

-^ 1

I

10°

G

ou

-3 10"'

o

uS

10"^

S^.

/

40% SF6-^60X N2

1

f

1

P=l atm

P=2 >tm

P=6 atm

P=10 atm ':

10'

10 15 20 25

a

4-> u

-d

C5o

o

I—

01a

10

|P=8 ttmoapherei

PURE N2

40?! SF8-60J! N2

PtniE SF6

Temperature(10 K)

10 15 20 25

Teinperature( 10 K)

(e) (f)

WIO

i

o\

••^ 1 >10

'*-> o

:i

(3o

o

I—

a)§10°

0) Xi

40% SFe-60% N,

p-:1 atm — p=:2 atm — p=:6 atm

p=:10atm

10 15 20 25

, 3 . Temperature(10 K)

10-^

• " '-T- P=l atmosphere

^ii^=^^^^\\

f \\

f \\

\ \

%

Dlmv er*a

• ~ 405? SF6-607S NZ — PURE N2

\

10 15 20 25

Temperature(10 K)

(g) (h)

Fig. 12 E, F, G, H. Calculations by Gleizes et al. [83] for the electrical conductivity of a 40%SF^-60%N2 mixture as a function of temperature and

pressure (Fig. 12e); variation of the total thermal conductivity with temperature for pure Nj, pure SF^, and 40%SF,,-60%N2 mixture at a total pressure of

6 atm (Fig. 12f); variation of the total thermal conductivity with temperature and pressure for 40%SFf,-60%N2 mixture (Fig. 12g); and variation of

viscosity with temperature forpure Nj, pure SF^, and 40%SF^-60%N2 mixture at a total pressure of 1 atm (Fig. 12h).

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF^ / NIST
Section 4 - Possible "Universal-Application" Gas Mixtures 21

103

CD DC

50 100

Percent of SFq by Volume

Fig. 13. Relative thermal interrupting capability of mixtures of He, Nj, CF4, and CjF, with SF, [70].

mixtures (including pressure rise and decrease) depends

significantly on the configuration of the arc chamber and

interruption current in addition to the arc quenching

properties of the mixture itself. Hence, these studies indicate that the actual performance is a function of many design variables. Thus

a "drop-in" gas mixture (i.e., a gas mixture for use in existing equipment) does not appear to be feasible for GCBs designed specifically for use with pure SF^. However, the concept of new circuit breakers designed for use with a mixture, rather than for pure SF^, must be

explored and tested before the possibility of a replacement

mixture for circuit breakers is ruled out. According to Waymel and Boisseau [57], gasinsulated substation circuit breakers require high arc- breaking properties that are not compatible with Nj or low percentage SFfi-N2 mixtures and for this reason SF,,- Nj mixtures are not considered for switchgear and other

gas-insulated equipment existing or re-designed.

Similarly, Middleton et al. [70] concluded that the use of SFfi-Nj mixtures for circuit breakers involves

significant derating of the circuit breakers under short line

fault because of their reduced thermal capability compared

to pure SFft. These authors reported the relative thermal

switching capabilities of various gas mixtures shown in Fig. 13 which indicate a poor performance for Nj and a good performance for CF4. As other studies have shown,

the build up pressure is higher for the SF^j-Nj mixture

than for the SF(;-CF4 and both are higher than for pure SF,,.

It may thus be inferred from the studies mentioned above

that the performance deficiencies of SF^-Nj mixtures in circuit breakers are principally due to thermal effects.

o

o

<z> u.COo

o

E

CO

Z

o

HO

o

cc

a.a

111 N

_j<

:e

a:O

SFe/N2

P = 200 kPa

I = 40|jA

10-

10

1.0

''SO2

_i I L. 20 40 60 80 100

PERCENT N2

Fig. 14. Production rates normalized to the SF^ content vs N,

percent volume in SF^-Nj mixtures for negative point-plane corona in gas at a total absolute pressure of 200 kPa and a constant discharge current of 40 ^A [6, 89].

Finally, Christophorou and Van Brunt [6] reviewed

the limited data on the decomposition of SF^-N, mixtures.

Their conclusion, based on corona decomposition

measurements, was that "there is little chemical

interaction between SF^ and Nj in discharges, and the predominant oxidation byproducts are those seen in pure

SFf, such as SOj, SOF^, SOjFj, and SOF4." These

byproducts are principally formed via interactions of SF^

decomposition fragments with oxygen and water

impurities [6]. The relative abundances of these

byproducts may, however, be different, especially that of

SO2 which is much larger for the 40%SF(;-60%N2 mixture

compared to pure SF,; (see Fig. 14). The very much larger

concentrations of SO2 in a 40%SF(,-60%N2 mixture

compared to pure SF^ may be useful for diagnostic purposes. It might be noted also that the presence of N2

may affect the ability of SFf, to reform itself in arc or discharge decomposition.

Overall, the data for use of SFf,-N2 mixtures in circuit breakers are contradictory, thus suggesting the need for additional research. It seems clear that SFf,-N2 mixtures

may not be used in existing breakers designed specifically for pure SF,,, but new designs may make effective use of

SF^-N, mixtures.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF,, / NIST
22 Section 4.3 - Gas Handling, Storing, Recycling, and Recovery

4.3 Gas Handling, Storing, Recycling,

and Recovering

Clearly, if an SF^-Nj mixture is to be used in existing

electrical equipment, a number of other issues need to be

addressed and one of them pertains to information on

handling, storing, recycling, and recovering SF^; from the

SFf,-N2 mixtures. In this connection, Mitchel et al. [8] investigated the practical thermodynamics of SF^ recovery

from SF(,-N2 (and SFf,-air) mixtures. They discussed

recovery of SF^ from mixtures with various noncondensible gases using a compressor/refrigerator system,

and presented simulation results showing SF^ recovery

efficiency and capacity in terms of cooling temperature,

total pressure, and gas composition. This study indicated

that SFfi extraction from a 50%SF(,-50%N2 mixture

presents no real problems. However, Probst [90] argues

that SFfi-Nj mixtures have problems in terms of

recyclability and reusability and that economic factors may be significant (see Appendix C for additional

discussion of this issue). The SF^, gas can be reclaimed

from the mixture but at a cost. Thus it seems reasonable

to conclude that recycling of mixtures can be done, but the technologies used need to be improved. CIGRE 23.10

Task Force just published a document [19] dealing with

SFfi recycling, reuse of SF^, gas in electrical equipment

and final disposal. Unfortunately, no such work has been

done on mixtures.

The data presented in earlier sections of this report

suggest that there can be considerable tolerance for variation of the percentage of SF^; in Nj for a proposed

50%SF(;-50%N2 mixture without significant effect on the

dielectric performance of the mixture. This is because the properties of the mixture are not generally a strong

function of the SF^; concentration at this mixture

composition. Certainly a tolerance in the percentage of

SFf; content of ±5% seems reasonable. It should also be

noted that the removal of byproducts from the mixture is not expected to be much different than in pure SF^,. Furthermore, there seem to be no serious problems in making a standard gas mixture or in recovering the SF^

from the mixture (see Appendix C).

medium. This "universal-application" mixture has no

apparent physical or chemical problems, but the fact that

its dielectric performance is only 85% to 90% of that of

pure SF(; would require equipment recertification along

with hardware changes or derating. This is nearly

impossible for equipment already in service, and would be

costly for new equipment presently certified only for pure

SFg use. Thus it would appear that the development of a replacement gas for use in existing equipment (a "drop-in"

gas) is not presently a viable alternative. However, the

application of standard gas mixtures to newly designed

equipment is certainly worthy of further consideration.

Questions must also be raised with regard to the recovery, reusability, recycling, separation, and

transportation of gas mixtures using existing technologies.

These points are discussed in Appendix C of this report.

The electric power industry clearly prefers to use pure SFfi for arc interruption. While still more work is necessary to resolve open questions and differences in published work, the standard mixture seems to have the

potential to perform well even in circuit breakers,

especially if used in new equipment designed specifically for use with a particular mixture. Nonetheless, it appears

that industry is hesitant to consider SF^-Nj mixtures for

arc interruption. Some of the reasons given [55, 91, 92],

in addition to those mentioned above for insulation

applications, are:

• Thermal derating would be required for many

applications.

• The pressure rise during an internal failure arc in equipment will be much faster and higher with the mixture. This may be limited by rupture disk properties,

which presents a possible safety issue.

• Some studies indicate significant reduction in the

performance of mixtures, as compared to pure SF^, in current circuit breaker designs, thus indicating the

possible need for substantial breaker redesign.

• Recycling of mixtures will be more expensive and

would require new equipment.

• Benefits of SF^^ substitutes can only be adequately

judged by complete life cycle analysis of the equipment

which is used, including the effects of different materials.

4.4 Discussion

The electric power industry seems willing to consider

SFf,-N2 mixtures for insulation, for instance, in new gasinsulated transmission lines. Indeed, much work is being

conducted world-wide in this area. Most such studies

focus on low concentration mixtures (10% to 15%) for

insulation, although work is also being done on higher

concentration SF(;-N2 mixtures for circuit breaker use. A

40%SF6-60%N2 mixture performs well as an insulating

In general, the physical and chemical

properties of a 40% or 50% mixture ofSF^ in N2 suggest that it may be appropriate as a

"universal application" gas mixture in new

equipment, particularly ifdesigned specifically

for use with SF^-N2 mixtures. However, the practical difficulties of using SF^-N2 mixtures

in existing equipment seem to be particularly

large at present.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 5 - Other Promising Gases or Mixtures 23

5. Other Promising Gases or

Mixtures

In the previous section we have attempted to identify a gas mixture that would be acceptable as a "universalapplication" replacement of SFf, for both high voltage

insulation and arc interruption. In this section we focus on gases or mixtures which are likely substitutes for

specific high voltage insulation or arc interruption

applications,'-^ and are thus worthy of immediate

exploration (i.e., sufficient data are presently available to demonstrate their potential, but not to sufficiently prove

their performance). Their possible use may require

changes in equipment designs. We focus on three such

gaseous dielectric media for which a significant amount of

data are available:

• high-pressure pure Nj for high voltage insulation;

• low concentration SF^j-Nj mixtures for insulation

and arc interruption; and

• SF(i-He mixtures for arc interruption.

Besides the gaseous media mentioned above, there are many other unitary gases, and binary and tertiary gas

mixtures which are superior in dielectric strength to pure

SFft and can potentially be used in high voltage needs

(e.g., see [2, 3, 27, 31-33] and Table 1). However, the overwhelming preponderance of these gaseous dielectrics are not acceptable for various reasons such as their environmental impact, toxicity, or flammability, or because they cannot satisfy one or more of the required

overall properties discussed in Sec. 2. From the long list of these we have identified a number of the most

promising. These are discussed in Sec. 6.

5.1 High-Pressure N2 for Insulation

As mentioned earlier [6, 14], nitrogen is an ideal gas

to use: it is abundant, cheap, inert, non-toxic, non- flammable, and unquestionably environmentally

acceptable.

However, nitrogen is a non-electronegative gas (it does not attach electrons) and for this reason its dielectric strength is rather low. Nitrogen, however, is a strong

electron-slowing down gas and this property accounts for

its relatively good dielectric properties in non-uniform

fields and in the presence of conducting particles, and for

its excellent performance in mixtures with electronegative

''Depending on a particular application, the mixture,

composition, or pressure of the replacement gas will be varied to maximize the performance of the equipment.

4.0 -

760 mm ,0

o

>

O) £

LUO

<o

>

o

o

Q

Z

o

o

3.0

2.0

1.0

152 mm

- G

O O

line spark

term limit /.

SF,

P/ M

t

.J3

2 4 6 8 GAS PRESSURE (atm)

Fig. 15. DC breakdown voltage applied to the conductor as a function of

gas pressure for SF,; and Nj using coaxial geometry (152 mm / 776 mm

system; positive or negative polarity). The data represented by the solid and open symbols are for breakdowns at two locations as indicated in the figure. The solid symbols correspond to breakdown in the line and the open

symbols are those cases where line sparks were not the limiting factor (see

[95]).

gases [6, 25, 29]. Its thermal conductivity (Table 2)

makes it a good cooling gas, especially at temperatures

less than a few thousand degrees. In this regard, it nicely

complements SF^. Existing measurements [3, 6, 14, 34, 37, 51] show

that:

• Under uniform field conditions and low pressures

(less than about 300 kPa) Nj has about one third [25, 93]

the dielectric strength of pure SFg.

• The breakdown voltage (DC or AC) of N,

increases with pressure as does that of SF^ (see Figs. 4 and

15) [37, 48, 50, 94, 95], but it turns toward saturation at high pressures. The falling of the breakdown voltages for both Nj and SF^ below the linearly projected dielectric strength as the pressure increases, is due to the "magnification" at high pressures of the field nonuniformity due to surface roughness and imperfections.

Such effects are more pronounced for SF,, (and other

electronegative gases) for which the effective ionization

coefficient increases with the field much faster than does

the ionization coefficient of the non-electronegative gas Nj [6, 25, 93]. In Fig. 16 are shown the results of a recent comparison of AC and DC measurements using

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
24 Section 5.1 - High Pressure Ng for Insulation

1400 T

1200-

1000

— 800 >

600 -

400-

200-

100% N2

EOF data (peak AC) {1996CEIDP)

Cooke & Velazquez data (DC)

COAX [D^(mm)/D2(mm)]

Cookson & Pedersen data (peak AC)

200 400 600 800 1000 1200

pr (bar mm)

22

20

|,e

I"

ID 12

0)

iJ- 10 o

o

LU

I -1 1 1 Negative Impulse1 1

Nitrogen

y^'^^

/ EDF-95 ' £5 185/400 -

A °

• Lightning -

CP-79

/ ° 89/226 -

•

° o Ligiitnlng -

' B

a Switching -

1 ... 1 1 1 1 1 4 6 8 10 Pressure (bar)

12 14

Fig. 16. Breakdown voltage ErvsPr(r is tiie radius of the inner conductor)

for cylindrical electrode geometries (similarity plot) for pure nitrogen [34]

Data of Pace et al. [34], Cooke and Velazquez [95], and Cookson and

Pedersen [37].

cylindrical electrodes. '^•'^•'*' Pace et al. [34] argued that when the area effect is taken into consideration, the recent

Electricite de France measurements [96] are compatible

with the DC measurements of Ref. [37]. The limited

lightning impulse measurements of Medeiros et al. [97] are consistent with the rest of the data in Fig. 16. Breakdown voltages of 1 MV are possible for values of

the product P x r ( pressure times radius of inner

conductor) of 8 MPa cm. The level of voltage is a function of the system dimensions and the total pressure. According to Pace et al., a rough estimate of the level of

voltage may be determined by employing similarity

rules.

"^

• Impulse breakdown studies [37, 96] with co-axial

electrodes of various inner and outer conductor radii have

been made and they vary with the ratio of the inner to outer conductor radius (see Fig. 17). The measurements

of Cookson and Pedersen [37] with lightning impulse, are

in excellent agreement with the recent measurements of

"'We are thankful to M. O. Pace for Figs. 1 5, 1 6, and 1 9, and to X. Waymel and C. Boisseau for their permission to reproduce the EDF measurements. "The similarity rule helps consolidate data from various experimental set ups. Two experiments are "similar" if one can be

converted to the other by a change in scale. For example, two

coaxial cylinder experiments are similar if the corresponding radii and lengths are all in the same ratio from one system to another [34, 98].

"*The measurements of Refs. [36, 50, 94, 95] were made

on coaxial geometries with various inner and outer conductor

diameters.

Fig. 17. Lightning impulse breakdown stress in nitrogen using cylindrical electrodes as a function of gas pressure [34, 96]. •, Lightning data of

Elecricite de France [34, 96]; o. Lightning data of Ref. 36; D, Switching

data of Ref. 37. The ratio of the diameters of the two coaxial electrodes is given in the figure.

Electricite de France as reported by Pace et al. [34, 96].

For a coaxial electrode arrangement with 185 mm inner

and 400 mm outer conductor radius, electric fields as high

as 19 kV/mm can be sustained for nitrogen pressures of

about IMPa.

• The dielectric strength of Nj is less sensitive to non-uniform fields than that of SF^. This is understood

from basic physical measurements such as the variation of

the effective ionization coefficient with E/N close to

(£:/V)ij„ [14, 25, 93, 99, 100]. Similarly, Nj is less sensitive than electronegative gases to conductor

roughness. In practice, surface roughness effects are a

strong function of the cable system size.

• Under conditions of conductive particle

contamination and high pressures (about 1.0 MPa), Nj

performs very well compared to pure SF,^ (Fig. 8).

• The arc interruption capability of pure Nj is significantly inferior to that of pure SF^, although at high

pressures (> 1 MPa) there may well be some use of pure

The physical data presented here suggest that high

pressure (2; IMPa) Nj may be a good alternative to pure

SFg for certain electrical insulation purposes. However, more work on practical systems at high pressures (high P

X r) is desirable to check its performance stability in industrial equipment. Also the question of environmental

and economic impact of designing and constructing the required high pressure vessels must be investigated.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 5 - Other Promising Gases or Mixtures 25

5.2 Low-Concentration SFg-Nj Mixtures for

Insulation^^

There have been many studies aimed at the development of nitrogen-based gaseous dielectrics. In Sec. 4 of this report we attempted to identify an "optimum" mixture of SF^ and N2 and in so doing we

referenced many literature sources dealing with SF^-Nj

mixtures as a function of SF,; concentration. In this section we focus on the possibility of developing lowconcentration SFf;-N2 mixtures for possible use in electrical insulation. By low concentration is meant a percentage of SF,; in Nj of less than 15%. The available

information on such mixtures is outlined below (see also. Sect. 4).

• Small amounts of electron attaching gases such as SFg in N2 substantially increase the dielectric strength of

the mixture (Fig. 4). Depending on the electron attaching

properties of the electronegative gas which is added to N2, the increase in the dielectric strength of the mixture may

or may not saturate as the electronegative gas

concentration is increased [25, 42].

• Pace et al. [34, 96] compared the AC

measurements of Cookson and Pedersen [37] with the measurements of EDF for co-axial cables. Their results are shown in Fig. 18 for 5% and 10% mixtures. A similar

comparison was made by them for the negative lighting

impulse breakdown voltage as a function of pressure for a number of gas mixture compositions. An example of

these measurements and comparisons are given in Fig. 1

9

for a 10% mixture. The data [34, 96] are in reasonable

agreement when the similarity law for cylinders is applied

(Fig. 19). It should be noted, however, that the increase

in the breakdown voltage with pressure is not linear and

any simple extrapolation to higher pressures of these

results may be in error.

• Malik et al. [101] measured the breakdown

properties of low concentrations (< 1 .5%) of SF^ in Nj in a highly non-uniform field arrangement (rod-plane

geometry). Their results for negative polarity clearly

show a large increase in dielectric strength even at very low concentrations ( < 0.3%). Such mixtures may be

useful for filling substations. In such situations there are

parts that have special requirements in terms of higher

'^See, also, Volume 2 of the Proceedings of the 10th

International Symposium on High Voltage Engineering, August

25-29, 1997, Montreal, Quebec, Canada. For instance, H. I. Marsden, S. J. Dale, M. D. Hopkins, and C. R. Eck III, "High

Voltage Performance of a Gas Insulated Cable with Nj and Nj-SF^

Mixtures," pp. 9-12; T. B. Diarra, A. Beroual, F. Buret, E. Thuries, M. Guillen, and Ph. Roussel, "Nj-SF^ Mixtures for High Voltage Gas Insulated Lines," pp. 105-108; and X. Waymel, V. Delmon, T. Reess, A. Gibert, and P. Domens, "Impulse Breakdown in Point- Plane Gaps in SFs-Nj Mixtures," pp. 289-292.

25 n

S20

b

EE

<D o

<

c

o

a2 5-

15-

10-

100%

T I

' ' ' I T

4 6 8 10

pressure, bar

12

Fig. 18. Measured breakdown fields in coaxial cables of diameters 185 mm/400 mm (EDF-95 [96], solid curves), and 89 mm / 226 mm ([37], dashed curves). The percentage of SF^ in mixtures with nitrogen is indicated

in the figure [34, 96].

levels of insulation. These can be separately insulated

with gases or mixtures containing higher percentages of

SFfi or even with pure SF^ if indeed this is necessary. They certainly can be used for transmission of lower level voltages.

• A lightning impulse (1.2 / 50 |as) study [102] of

SF(i-N2 mixtures with 0.15% to 0.2% SF,; content for rod/plane gaps with both positive and negative voltages

showed that for both polarities the effect of the addition of

SFft to N2 is dependent on both the gas pressure and gap

spacing. Maxima in voltage versus SF^ percentage curves were observed which were a function of the total pressure.

Coaxial Geometry (D^(mm)/D2{mm)] 10% SFg/No

2000

1800

1600

1400 ^ 1200

""' 1000

UJ 800

600

400

200

Negative impulse

• EDF-95

1 85/400 O CP-79

89/226

100 200 300 400 500 600 p r (bar mm)

Fig. 19. The product Er as a function of the product Pr for a IO%SF^- 90%N2 mixture for lightning impulse breakdown (E is the electric field, r is the radius of the inner cylinder of the coaxial cylinder electrode geometry, and P is the total pressure) [34, 96].

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF,- / NIST
26 Section 5.3 - SFg-He Mixtures for Arc Interruption

For positive polarity voltages the maximum in breakdown

strength occurs when the SF^, content in the mixture is about 0.5% at 100 kPa, 5% at 300 kPa, and 10% at 500 kPa.

• Qiu and Kuffel [103] investigated the increase in dielectric strength of nitrogen (and helium) mixtures due

to 1% SF(i additive. Table 6 shows their data on the

'^mixture / ^gas of the breakdown voltage for the mixmre to the breakdown voltage of the buffer gas (N2, or He). It is seen that even 1 % SF^ in Nj significantly improves the

dielectric strength, and that this improvement varies with

the t}'pe of apphed voltage.

• Yializis et al. [104] studied impulse breakdown

and corona characteristics of SF^-N, mixtures with less than 1% of SF(i content using rod-plane gaps. Measurements of 50% impulse breakdown voltage were made mainly in SF^i-N, mixtures containing 0.1% SF,^ content by pressure over the range of 100 kPa to 500 kPa

and gap lengths of 10 mm to 50 mm using positive and

negative polarity 1.8/50 |is and 310 / 3500 |is pulses.

Their results show that the positive impulse breakdown of

Nt in the pressure region of 100 kPa to 250 kPa increases

considerably with the addition of small traces of SF^;

.

• Naganawa et al. [73] made measurements on DC

interruption by spiral arc in SF^-Nt mixtures (0. 1 MPa to 0.8 MPa). They recommended SF^-Nj mixtures as an

extinguishing mediumof switchgear to avoid liquefication

of pure SFf, at high pressure under extremely low

temperatures and to save on gas cost. They concluded

that compared to the case of pure SF^ "even a small content of SF^; in the mixture is effective to decrease the magnitude of interrupting overvoltages with the arcing

time unchanged." On the other hand, Wootton and

Cookson [51] found that "addition of trace amounts of SF^

(e.g., 2%) to nitrogen at high pressures (e.g., 1.2 MPa)

can reduce the breakdown strength (by -40%), while

increasing the strength at low pressures.

• Finally, according to Bolin [105], recent reports

from ABB and Siemens show that GITL are being

designed for use with low percentage SF^, mixtures

(containing less than 20% SFg).

Table 6. Vfj,,„^,^ I Vq^^, for a mixture of 1 % SF^ in either Nj or He for various types of applied voltage [103],

Table 7. Breakdown strength of mixtures of SF^, and He [106]

Applied Voltage (400 kPa) (200 kPa)

He N,

-1.5/40^5 1.35 1.55

+ 1.5 /40 ms 1.92 1.70 AC 2.59 2.79

Strength Maximum Minimum

relative to SF^ strength relative strength relative (quasi-uniform to SF^ (non- to SF^ (non- Gas field ; sphere- uniform field ; uniform field ; mixture plane electrodes pin protrusion; pin protrusion;

at 150 kPa) 100kPa<P 100kPa<P

<500 kPa) <500 kPa)

100% SF,

100% He

75% SF, 25% He

50% SF, 50% He

25% SF, 75% He

100

78

56

33

100

130

126

101

100

71

58

41

5.3 SFg-He Mixtures for Arc Interruption

SF(;-He mixtures are considered for use in circuit breakers. Helium has a very low dielectric strength (~ 3%

that of SFf; in uniform fields. Table 7) and contributes

virtually nothing to the dielectric strength of the mixture.

Unlike the SF^-Nj mixtures which exhibit substantial

synergism in terms of their dielectric strength, the SFfj-He

mixtures show no such synergism.

Helium, however, complements SF,; in terms of its cooling capability because it is very light. Its specific heat

and thermal conductivity are very large (see Table 3). Helium is an inert gas and does not react chemically with

either SF^, or the gas impurities present in commercial

SFf;, or the system components.

Grant et al. [73] investigated the recovery

performance of SFf;-He mixtures as a function of the SF^

content in the mixture. Their results were presented

earlier in Table 4 and show the performance of SF^-He

mixtures which for a total pressure of 0.6 MPa seem to be

-10% higher than pure SFf, for virtually all mixture

compositions from 75% to 25% SFg (see Fig. 1 1). Basile et al. [107] found that SF^-He mixtures show

a synergistic maximum in the 50% breakdown voltage at a percentage of He around 30%. At the maximum content

of He used in these tests (50%), the breakdown voltage of

a rod-plane electrode system was still higher than in pure

SFfi. This suggests that SFf^-He mixtures could be

considered as an alternative to pure SFf, in operating

conditions of low temperature.

Wootton and Cookson [51] measured the 60-Hz

dielectric strength of SFf,-He mixtures in a plane-parallel

electrode system with particle contamination (free 6.4 mm

long X 0.45 mm diameter copper and aluminum particles).

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 6 - Other Possible Substitutes: Future and Long-term R&D 27

0.5 1.0 PressureiMPal

|)00

Breakdown - 100* Sf,

Breakdmn Breakdwn ^

?0%Sfj Tf

£

f

^

200 - X^Vi / H^

^]'

\y^^ -:;>i15% 5F. 4 6 ^ / i //

\A h

"t"-'"''^ ltSF6_,^

100

n

L ^

1 1

(a)

1.5

this and earlier sections (e. g., Table 4, Figs. 1 and 11 ) on

arc interruption - would suggest that SF^-He mixtures

containing 0.29 MPa of SF^ at total pressures in excess

of about 1 MPa may be suitable for arc/current interruption

applications. However, Niemeyer [108] points out that the published data on SFg-He synergisms in switchgear

only refer to the initial thermal recovery under short line

fault switching where the dielectric stress is still low and

not to terminal fault interruption where the dielectric

stress is high. Clearly, there are still a number of issues

regarding the SF^-He mixtures which include gas compression, separation and leakage which need to be

addressed.

The data presented here strongly suggest that pure N2 and mixtures of low concentration of

SF^ in N2 may be appropriate for many

insulating applications. The data also suggest

that SF^-He mixtures may be viablefor use in gas-insulated circuit breakers. Further

research on their use in practical systems must

still be performed.

PressureiMPal

FIG. 20. Dielectric strength for SF^-He mixtures with 1%, 5%, 20% and 50% SFf, for copper (Fig. 20 a) and aluminum (Fig. 20 b) particles [51],

Figure 20 shows the dielectric strength for mixtures with

1%, 5%, 20% and 50% SF^ for copper (Fig. 20a) and

aluminum (Fig. 20b) particles. While the breakdown

strength of helium in uniform fields is only a small

fraction of that of SF^ and mixtures of the two gases in uniform fields have dielectric strengths which are intermediate to those of the two gases, the data in Fig. 20

show that the dielectric strength of the He-SF^ mixtures

under particle contamination is equal to or greater than

that of SFfi at its optimum pressure of about 0.29 MPa.

Further analysis of these data by Wootton and Cookson

showed that the maxima in the curves for total pressures of 1 .43 MPa, 1 . 1 MPa, 0.77 MPa, and 0.43 MPa occurred

at a partial pressure of SF^; of about 0.3 MPa. It was also found that for mixtures with the optimum partial pressure of SFf; (0.29 MPa), addition of He increases the breakdown strength linearly, in contrast to addition of SF^

which decreases the breakdown strength. The data in Fig.

20b show that a 20%SFfi-80%He mixture at total pressures

greater than 0.7 MPa is superior in performance to pure

SFf,. Even a 5%SFft-95%He mixture at a total pressure

greater than 1.3 MPa performs better than pure SF^

.

This work on particles - and the work discussed in

6. Other Possible Substitutes:

Future Long-term R&D

As mentioned previously, other gases exist for which

there are data that indicate some potential for use as a gaseous dielectric or interruption medium. Some of those

with the most potential are listed in Table 8, and an

investigation of these gases could form the core of a future long-term research and development effort to develop

acceptable substitute gaseous media for the various needs

of the electric power industry. This program could

include efforts in the following specific areas:

• A search for single gases at high pressure (besides

N2) for insulation purposes , including CO^, N.O, and

SO2 [2, 3, 6, 14, 30, 31, 109-111]. These "are weakly

electronegative gases and their electron attaching

properties and dielectric strength may increase with gas

density [110, 111].

• A search for binary mixtures (other than SF^-N,

and SFfi-He) suitable for particular applications [3, 2, 25,

30, 31, 42, 51, 53, 80, 11 2-1 23], including: SF^ -1- Ar, SF^

-t- CF4, SFft + CjFfi, and He + an electronegative

component gas (for arc and current interruption); N, +

SO,, N, + C-C4F8, SO2 -I- SFf,, SF(, +CO2 , and N.O +SFfi

(for insulation).

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF,, / NIST
28 Section 7 - Conclusions and Recommendations

Table 8. Gases and gas mixtures, for possible use in insulation and arc and current interruption applications, which may be appropriate for further research based upon presently known information.

Insulation Interruption

Possible • 40% SF, + 60% Nj • 40% SF, + 60% N2

Universal • 50% SF, + 50% Nj • 50% SF^ + 50% N2

Mixtures

Near Term • High pressure Nj • SF, + He

Research • Lx)w concentration SF, in Nj

Long Range •COj • SF, + Ar

Research •SO2 • SF, + CF/

•N2O . SF, + C,F/

. Nj + SO2 • SF, + Nj + He

•N. + c-QF/ • SF, + Nj + Ar

• SO2 + SF, • He + electronegative

• SO2 + C-C4FS gases

• SF, + CO2

''These are also greenhouse gases, but their global warming potentials are about one third that of SF^. Over a 100-year time horizon the global warming potentials of C-C4F8, CF4, CjF^, and SF^ are respectively 8,700,

6,500, 9,200, and 23,900 [22].

• A search for ternary mixtures, including the

following systems: SF^; + N. + He and SF^ + N2 + Ar [3, 2,30,31, 124, 125].

While a large amount of effort was expended in the 1970s and 1980s to search for gases exhibiting better

dielectric performance than SF^, the emphasis of any new

research program would be to identify gases with

acceptable dielectric properties, and minimal

environmental impact. This could include a search for new synthetic gases, better additives than SF^, better buffers than N2, and gases with an IR window near 10 \xm

to avoid any contribution to global warming. It could even be suggested that an investigation of gaseous media

that are detrimental to the environment is justified, if the gas has superior performance properties for a particular

application where its release into the environment could

be absolutely prevented.

Other areas of productive investigation that are suggested by the research presented in this report include

the following:

• the role of humidity and impurities on dielectric gas properties;

• electron attachment and detachment in low

concentration SF^-Nj mixtures;

• decomposition of SF^-Nj mixtures as a function of

concentration, impurity content, and type of discharge;

• dielectric behavior of gas mixtures at high gas

pressures;

• thermal and electrical conductivities of SF^-Nj

mixtures; thermodynamic properties, thermal

conductivities, and viscosities of gas mixtures under the conditions they are used in electrical equipment;

• the role of particles and improved particle control

methods;

• interface phenomena and partial discharge

behavior;

• assessment of available data;

• life cycle analysis of the overall environmental

gain by using mixtures instead of pure SFj;

;

• handling, storage, recovery, and disposal of gas

mixtures;

• ways to reduce the cost of recovery of SF^; from

gas mixtures;

• new equipment designed specifically to eliminate

emissions;

• improved recycling procedures;

• relaxation of equipment constraints that would

make other gases acceptable;

• alternative technologies not requiring gaseous

dielectrics, such as high temperature superconductors and

solid state switching.

A significant amount of research must be

performedfor any new gas or gas mixture to be used in electrical equipment. Such a program necessarily would require the systematic study of potential replacements,

including their physical, chemical, and

performanceproperties. A concerted national or international effort in this area by

equipment manufacturers, utilities,

government labs, universities and gas

manufacturing companies would be beneficial.

7. Conclusions and

Recommendations

Sulfur hexafluoride is an superior dielectric gas for nearly all high voltage applications. It is easy to use, exhibits exceptional insulation and arc-interupption

properties, and has proven its performance by many years of use and investigation. It is clearly superior in performance to the air and oil insulated equipment which was used prior to the development of SF^-insulated

equipment. However, the extremely high global warming

potential of SF^ mandates that users actively pursue means

to minimize releases into the environment, one of which

is the use of other gases or gas mixtures in place of SF^;.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Section 8 - References 29

An evaluation of the results of the last two decades,

and a detailed analysis of the data presented in this report,

indicate that no replacement gas is immediately available

for use as an SF^-substitute ("drop-in gas") in existing

electric utility equipment. For gas insulated transmission

lines and gas insulated transformers, the limitation is primarily due to the need for re-certification and possible

re-rating of equipment that is already in use. For gas

insulated circuit breakers there are still significant

questions concerning the performance of gases other than

pure SF(;. However, various gas mixtures show considerable

promise for use in new equipment, particularly if the equipment is designed specifically for use with a gas

mixture:

• Mixtures of nearly equal amounts of SF^ and Nj

exhibit dielectric properties that suggest that they could be

used as a "universal application" gas for both electrical insulation and arc/current interruption purposes. In this connection, standard procedures for mixture handling,

use, and recovery would need to be further developed.

• Mixtures of low concentrations (<15%) of SF^, in N2 show excellent potential for use in gas insulated

transmission lines, although further work on their performance in practical systems is necessary.

• Pure high pressure nitrogen may be suitable for some electrical insulation applications. Consideration of

the use of such environmentally friendly gases where SF^

is not absolutely required should be investigated and

promoted.

• A mixture of SF,; and helium has shown promise

when used in gas insulated circuit breakers, and should be

investigated further. Finally, it is clear that a significant amount of

research must be performed for any new gas or gas

mixture to be used in electrical equipment. Such a program necessarily would require the systematic study of

potential replacements, including their physical, chemical,

and performance properties (see for example Sections 3 and 6). A concerted effort in this area by equipment

manufacturers, utilities, government labs, universities, and

gas manufacturing companies would be beneficial.

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1980.

81. M. Tsukushi, Y. Nakagawa, K. Hirasawa, and Y. Yoshioka, "Application of Theoretical Calculation for Puffer Pressure Rise of Gas Mixtures in Puffer Type

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September. 22-24, pp. 198-202, 1981.

82. A. Gleizes, M. Razafinimanana, and S. Vacquie,

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1987.

83. A. Gleizes, M. Razafinimanana, and S. Vacquie,

"Calculation of Thermodynamic Properties and

Transport Coefficients for SF^/Nj Mixtures in the Temperature Range 1,000-30,000 K," Plasma

Chemistry and Plasma Processing, Vol 6, pp. 65-78,

1986.

84. A. Gleizes, I. Sakalis, M. Razafinimanana, and S. Vacquie, "Decay of Wall Stabilized Arcs in SFf^/Nj

Mixtures," J. Appl. Phys., Vol. 61, pp. 510-518, 1987.

85. A. Gleizes, A. M. Rahal, H. Delacroix, P. V. Doan,

"Study of a Circuit Breaker Arc with Self-Generated

Flow: Part I - Energy Transfer in the High-Current

Phase," IEEE Transactions on Plasma Science, Vol.

16, pp. 606-614, 1988.

86. A. Gleizes, M. Mitiche, P. V. Doan, "Study of a Circuit-Breaker Arc with Self-Generated Flow: Part HE

- The Post-Arc Phase," IEEE Transactions on Plasma

Science, Vol. 19, pp.12-19, 1991.

87. A. Gleizes, M. Razafinimanana, and S. Vacquie,

"Theoretical and Experimental Study of an Arc

Discharge in a SF^/N; Mixture," 7th International Conference on Gas Discharges and Their Applications, 31 August- 3 September, 1982, London, pp. 85-88,

1982.

88. H. Sasao, S. Hamano. Y. Ueda, S. Yamaji, and Y. Murai, "Dynamic Behavior of Gas-Blasted Arcs in SF(;-N2 Mixtures," IEEE Transactions on Power

Apparatus and Systems, Vol. PAS-101, pp. 4024-4029, 1982.

89. M. C. Siddagangappa and R. J. Van Brunt,

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SF^/Oj Mixtures", Proc. 8th Int. Conf. on Gas

Discharges and Their Applications, Leeds University

Press, pp. 247-250, 1985.

90. R. Probst, DILO Company, Inc. (Private

Communication, June 1997).

91. P. Bolin, Private Communication, June 1997.

92. L. E. Brothers, Southern Company (Private

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Section 8 - References 33

Communication, July 1997).

93. Th. Aschwanden, "Swarm Parameters in SF^ and

SFf,/N2 Mixtures Determined from a Time-Resolved

Discharge Study," in Gaseous Dielectrics IV, L. G.

Christophorou andM. O. Pace (Eds.), Pergamon Press, New York, pp. 24-33, 1984.

94. H. C. Doepken, Jr. "Compressed-Gas Insulation in Large Coaxial Systems," IEEE Trans. Power Appar.

and Syst., Vol. PAS-88, pp. 364-369, 1969.

95. C. M. Cooke and R. Velazquez, "The Insulation of

Ultra-HV in Coaxial System Using Compressed SF^, Gas," IEEE Trans. Power App. Syst. PAS-96, p. 1491-1497, 1977.

96. X. Waymel and C. Boisseau, Electricite de France,

Private communication, 1997.

97. P. T. Medeiros, S. R. Naidu, and K. D. Srivastava,

"Lighting Impulse Breakdown of Cylindrical Coaxial

Gaps in Nitrogen," IEEE Intern. Symp. Electr. Insul., Washington, D. C, 1986, pp. 210-212, 1986.

98. T. Nitta, Y. Shibuya, Y. Arahata, and H. Kuwahara,

"Statistical Approach to the Breakdown Characteristics of Large Scale Gas-Insulated Systems," in Gaseous

Dielectrics, Oak Ridge National Laboratory Report,

CONF-78030 1 , L. G. Christophorou (Ed.), Oak Ridge,

TTM, pp. 338-354, 1978.

99. A. Pedersen, in Gaseous Dielectrics II, "Evaluation of

the Effect of Surface Defects on Breakdown in Strongly Electronegative Gases or Gas Mixtures,"L. G.

Christophorou (Ed.), Pergamon Press, New York, pp. 201-208, 1980.

100. J. Berril, J. M. Christensen, and A. Pedersen,

"Measurement of the Figure of Merit Related to the Effect of Electrode Surface Defects on Breakdown for Strongly Electronegative Gases or Gas Mixtures," in Seventh Intern. Conf. on Gas Discharges and Their

Applications, 31 August- 3 September 1982, London,

pp. 266-269, 1982.

101. N. H. Malik, A. H. Qureshi, and G. D. Theophilus,

"Static Field Breakdown of SF^^/Nj Mixtures in Rod/Plane Gaps," IEEE Trans. Electr. Insul., Vol. EI14, pp. 61-69, 1979.

102. D. Raghavender and M. S. Naidu, "Lighting Impulse

Study of SF,/N2 Mixtures With 0.1% to 20% SF,

content for Rod/Plane Gaps with both Positive and

Negative Voltages," 1986 Annual Report, Conference on Electrical Insulation and Dielectric Phenomena,

Claymont, Delaware, pp.327-332, 1986.

103. Y. Qiu and E. Kuffel, "The Breakdown Strengths of

Gas Mixtures Containing a Small Amount of

Electronegative Gas in Non-Uniform Field Gaps,"

Seventh Intern. Conf. on Gas Discharges and Their

Applications, 3 1 August- 3 September, 1982, London,

pp. 215-218, 1982.

104. A. Yializis, N. H. Malik, A. H. Qureshi and E. Kuffel,

"Impulse Breakdown and Corona Characteristics for

Rod/Plane Gaps in Mixtures of SF^ and Nitrogen with

less than 1% of SF,, Content," IEEE Trans. Power

Appar. and Systems, Vol. PAS-98, pp. 1832-1840,

1979; E. Kuffel and A. Yializis, "Impulse Breakdown

of Positive and Negative Rod/Plane Gaps in SF^/Nj

Mixtures," IEEE Trans. Power Appar. Systems, Vol.

PAS-97, pp. 2359-2366, 1978.

105. P. Bolin, Private Communication, August 1997.

106. R. E. Wootton and S. J. Dale, "60-Hz Breakdown

Characteristics of SF,, and its mixtures with CF3SF5,

CF3CFCF2, and He in Non-uniform Fields,"

Publication 189, pp. 228-231, 1980.

107. G. Basile, I. Gallimberti, M. Lissandrin, G. Marchesi,

and F. Penon, "Interruption Performances of Circuit Breakers Containing SF^ Gas Mixtures," IX Intern. Conf. on Gas Discharges and Their Applications,

Venice, 19-23 September 1988, pp. 135-138, 1988.

108. L. Niemeyer, ABB Switzerland, Private

Communication, August 1997.

109. J. Dutton, F. M. Harris, and D. B. Hughes, "Electrical Breakdown of NjO, SF„ and NjO/SF, Mixtures,"

Proceedings lEE, Vol. 121, pp. 223-226, 1974.

110. K. Nakanishi, D. R. James, H. Rodrigo, and L. G.

Christophorou, "The Pressure Dependence of the

Dielectric Strength of SO2 and n -C4F,o," J. Phys. D

17, pp. L73-L76, 1984.

111. S. R. Hunter and L. G. Christophorou, "Pressure- Dependent Electron Attachment and Breakdown

Strengths of Unitary Gases, and Synergism of Binary

Gas Mixtures: A Relationship," in Gaseous Dielectrics

IV, L. G. Christophorou and M. O. Pace (Eds.),

Pergamon press. New York, 1984, pp. 1 15-126.

112. A. H. Cookson and B. O. Pedersen, "High Voltage

Performance of Mixtures of SF^ with N2, Air and CO2

in Compressed-Gas-Insulated Equipment," Fifth International Conference on Gas Discharges,

Liverpool, lEE Conference Publication 165, pp. 161-164, 1978.

113. Y. Qiu and D. M. Xiao, "Dielectric Strength of the SFfi/COj Gas Mixture in Different Electric Fields,"

Ninth International Symposium on High Voltage

Engineering, Graz, Austria, 2255-1-2255-4, 1995.

114. Y. Qiu, S. Y. Chen, Y. F. Liu, and E. Kuffel,

"Comparison of SF^/N, and SFf,/C02 Gas Mixtures

Based on the Figure-of Merit Concept," 1988 Annual

Report, Conference on Electrical Insulation and

Dielectric Phenomena, October 16-20, 1988, Ottawa,

Canada, pp. 299-304, 1988.

115. R. E. Wootton, S. J. Dale, and N. J. Zimmerman.

"Electric Strength of Some Gases and Gas Mixtures,"

in Gaseous Dielectrics II, L. G. Christophorou (Ed.),

Pergamon Press, New York, pp. 137-147. 1980.

116. J. Berg and E. Kuffel, "Breakdown Voltage

Characteristics of SF^CFj Mixtures in Uniform and

Non-Uniform Field Gaps," 1995 Annual Report.

Conference on Electrical Insulation and Dielectric

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
34 Section 8 - References

Phenomena, 95CH35842, pp. 126-129, 1995.

117. M. Akbar and N. H. Malik, "Electrical Breakdown of

NjO/SF,, N2O/CCI2F2, and Np/COj Gas Mixtures,"

ffiEE Trans. Electric. InsuL, Vol. EI-20, pp. 581-585,

1985.

118. Y. A. Safar, N. H. Malik and A. H. Qureshi, "Impulse

Breakdown of Negative Rod-Plane Gaps in SF^/Nj,

SFf,/Air, and SF^/COj Mixtures," IEEE Trans. Electric. Insulation, Vol. EI- 17, pp. 441-450, 1982.

119. N. H. Malik, A. H. Qureshi, and Y. A. Safar, "DC

Voltage Breakdown of SF^/Air, and SF^/COj Mixtures

in Rod-Plane Gaps," IEEE Trans. Electr, Insul., Vol. EI-18,pp. 629-636, 1983.

120. C. C. Chan, M. O. Pace, and L. G. Christophorou, "DC

Breakdown Strengths of Some Multicomponent Gas

Mixtures in Concentric Cylinder Geometries," in Gaseous Dielectrics II, L. G. Christophorou (Ed.),

Pergamon Press, New York, 1980, pp. 149-159, 1980.

121. Y. Qiu and Y. P. Feng, "Investigation of SF6/N2,

SFfi/COj, and SF^/Air as Substitutes for SF^

Insulation," Conference Record of the 1996 IEEE

International Symposium on Electrical Insulation,

Montreal, Quebec, Canada, June 16-19, 1996, pp. 766-769, 1996.

122. Y. Qiu and D. M. Xiao, "Dielectric Strength of the SFfi/COj Mixture in Different Electric Fields," Ninth

International Symposium on High Voltage

Engineering, Vol. S2, 1995, paper 2255-1 - 2255-4.

123. J. Berg and E. Kuffel, "Breakdown Voltage

Characteristics of SFfyCF4 Mixtures in Uniform and

Non-Uniform Field Gaps," IEEE 1995 Annual Report:

Conference on Electrical Insulation and Dielectric Phenomena, October 22-25, 1995, Virginia Beach,

VA, pp. 126-1 29, 1995.

124. L. G. Christophorou, D. R.. James, I. Sauers, M. O.

Pace. R. Y. Pai, and A. Fatheddin, "Ternary Gas

Dielectrics," in Gaseous Dielectrics III, L. G. Christophorou (Ed.), Pergamon Press, New York,

pp.151-165, 1982.

125. D. Raghavender and M. S. Naidu, "A Comprehensive

Study of Lightning Impulse Breakdown and Cost / Benefit Analysis of Ternary Gas Mixtures Containing

Two Electronegative Gases," 1995 Annual Report,

Conference on Electrical Insulation and Dielectric Phenomena, 95CH35842, pp. 141-144, 1995.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF^ / NIST
Appendix A - Survey of SFg by End-Use Application 35

Appendix A

Sales of SFft by end-use application [12] (This survey excludes contributions from China and Russia).

YEAR Utilities and

Accelerators

Original Equip. Manufacturers Magnesium

Industry

Electronics Industry

Utilizing SF,

Adiabatic Prop.

All Other Uses TOTAL

(units in metric tons)

1961 91 91

1962 14 145 159

1963 14 181 9 204

1964 18 204 14 14 250

1965 32 231 23 18 304

1966 61 233 27 2 5 23 374*

1967 63 239 32 5 9 27 392*

1968 63 256 36 5 14 32 428*

1969 84 269 41 7 14 36 496*

1970 140 277 44 9 14 44 606*

1971 468 289 71 10 14 72 1,018*

1972 515 263 63 11 14 64 1,017*

1973 700 355 83 11 14 84 1,385*

1974 732 334 46 12 14 72 1,378*

1975 937 559 120 13 14 111 1,754

1976 1,236 760 195 13 14 126 2,344

1977 1,299 924 214 13 14 151 2,615

1978 1,473 1,019 256 13 20 134 2,915

1,979 1,962 1,267 312 15 32 188 3.776

1980 1,861 1,542 321 16 35 216 3.991

1981 2,055 1,397 320 17 54 210 4.053

1982 2,096 1,550 360 18 59 246 4.329

1983 1,966 1,421 374 17 80 233 4.091

1984 2,348 1,859 397 16 108 232 4,960

1985 2,440 1,734 437 20 111 254 4.996

1986 2,717 1,666 431 38 no 300 5.262

1987 2,784 1,641 4! 5 73 146 265 5.324

1988 2,654 1 ,649 398 100 162 307 5.270

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF^ / NIST
36 Appendix A - Survey of SFg by End-use Application

1989 2,832 1.753 363 117 270 323 5,658

1990 3,323 1.722 385 140 220 435 6,225

1991 3,414 2.022 357 151 260 682 6,886

1992 3,312 2,173 266 201 290 645 6,887

1993 3,523 1,847 274 229 290 658 6,821

1994 3,295 2,402 354 262 325 587 7,225

1995 3,126 2.659 399 300 356 617 7,457

1996 3,139 2,795 544 307 344 442 7,571

Subtotal 56,696 39,728 7,972 2,161 3,426 7,857 118,512

1997 3,669 2,155 426 342 472 257 7,321 E

1,998 3,870 2,118 388 378 502 235 7,491 E

1,999 3,711 2,270 362 417 559 212 7,531 E

2,000 3,709 2,281 347 461 584 189 7,571 E

TOTAL 71,655 48,552 9,495 3,759 5,543 8,750 148,426

* For the years 1966-1974, some companies could not provide a breakdown by end use. TOTAL SALES includes an additional 672

metric tons sold in these years. The sum of sales by end use does not equal total sales.

^ Manufacturers provided projections for sales in 1997-2000.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF,^ / NIST
Appendix B - Status of Environmental, Economic and Policy Issues 37

APPENDIX B

Status of Environmental, Economic, and Policy Issues

Driving SFg Reduction

This appendix is a brief summary primarily of the policy (or regulatory) issues that may drive the need for reduction of SFf, use and emissions by industry.

Environmental concern is a significant motivation

toward improved SF^; management or use of alternatives. Pure SFg has a greater ability to absorb infrared radiation

than most other gases and it has a very long atmospheric

lifetime. These properties make SF^ a potent global

warming gas. To put this in perspective, the long-term

radiative effect of 1 kg of SF^ emitted exceeds that of 1 kg

of CO2 by a factor of 23,900. This number refers to the

direct Global Warming Potential (GWP),oo, that is, the

extra amount of long wavelength radiation absorbed over

a 100-year period.

In recent years, the price of SF^ has increased, thus

promoting the possibility of using alternate gases or gas

mixtures. An evaluation of the total cost for switching

from one gas to another, requires performing a technology

impact assessment including a full life-cycle analysis.

Among the economic factors to be considered are (/) the

price of the compounds and material resources consumed,

(//) the costs of new and modified equipment, (Hi) the

costs during equipment operation, including energy

dissipated, emissions control, repair and servicing, (iv) the

cost and effectiveness of recycling, and (v) the cost of

additional personnel and training. Other factors to consider include (/) availability and life of the alternative

gas, (//) electrical reliability, certification and testing of

equipment, (///) health hazards and safety, and (iv) equipment size and land use. Global emission control measures for

perfluorocompounds (PFCs) and SF^ are at present

following the general course set for the "major"

greenhouse gases in the Framework Convention on

Climate Change (FCCC) and the ongoing Conference of

the Parties (COP) meetings. In the United Nations'

efforts to develop an international protocol (under the FCCC) for stronger controls of greenhouse gas emissions,

the European Union (EU) proposed to the Ad Hoc Group

on the Berlin Mandate (AGBM) that fluorocarbon control be incorporated into the final treaty. The EU proposal

suggested policies and measures that include:

• product standards with respect to leakages of

emissions

• use of selected low GWP (global warming

potential) instead of high GWP chemical

• reducing emissions through improved equipment

and practices in the electrical equipment industry.

The concern over emissions of SF^ was further addressed in 1 996 as the Second Conference of the Parties

formally directed countries to inventory SF^ emissions and

report them to the internal governing body. The

Intergovernmental Panel on Climate Change has proposed

methods for countries to consider for use in inventorying

emissions of SF^ from electric power equipment.

Individual countries are developing proposals to shape stronger climate protocols under development for COP-3 (scheduled for late 1997). The European Union

proposal specifically highlights HFCs

(hydrofluorocompounds), PFCs (perfluorocompounds),

and sulfur hexafluoride in the list of greenhouse gases that countries would be able to control under the protocol.

The current intent of the COP-3 meeting is to produce a protocol for greater control of greenhouse gas emissions

worldwide.

While several important issues remain unresolved, it appears likely that "the U.S. will propose that negotiations

for post-2000 year emissions reductions focus on realistic, binding commitments that will produce real environmental

benefits. ... the United States will continue to seek

market-based solutions that are flexible and cost effective.

. . . international cooperation of this challenge remains

critical to any effective response."' It is important to recognize that alternatives taking the form of SF^-

containing mixtures or any other PFC gas or mixture will be subject to these evolving regulations.

In the meantime, the U.S. Environmental Protection

Agency (EPA) is continuing with the development of a voluntary program for users of SF^ in electric power

equipment. EPA's goal for the program is to reduce U.S. emissions of the gas from equipment through voluntary means. The program is expected to incorporate best work

practices, capture and recycling of used gas, and design of

business plans for replacement of obsolete equipment with

uncontrollable SF^ leaks. In the long term, EPA desires to work with industry to eliminate emissions. Elimination of

emissions will require cooperation from the users of

'Statement to Industry/NGOs on U.S. Intervention at Climate Change Negotiations by T. E. Worth, U.S. Department of

State

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF^ / NIST
38 Appendix B - Status of Environmental, Economic, and Policy Issues

equipment as well as the manufacturers of such devices.^

For further information on the voluntary program, contact Elizabeth Dutrow of EPA at (202) 233-9061 or at <dutrow. elizabeth @epamail. epa. gov>

.

"Private communication from Elizabeth Dutrow,

Environmental Protection Agency, September 29, 1997.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Appendix C - Potential Barriers to Using Gas Mixtures 39

APPENDIX C

Potential Barriers to Using Gas Mixtures as a Gaseous Dielectric

1 . Perceived Disadvantages

There are several potential barriers to using even

simple mixtures in electrical equipment. These are:

• more difficult gas supply, recovery and recycling

procedures,

• monitoring and maintaining proper

concentrations,

• challenge of handling leaks and emergencies,

• unknown long-term stability and performance,

• difficult disposal, and

• cost-of-ownership.

The applicability or significance of the perceived

disadvantages listed above will depend on the application.

It is simple to fill up equipment with a mixture, but for some applications routine maintenance requires the gas to be removed, recycled, refilled, or disposed. This

maintenance routine may entail pumping, purging,

filtering and separation of the mixture components,

replacement of the gases in the desired ratio, and volume

percentage analysis. Such a routine must be reliable and

rapid, minimizing down time. To accomplish this task

will require different chemical management practices and

associated technologies from those used for pure SF^. In particular, this may require more training, equipment

development, process automation, and other higherfunction gas handling equipment. However, there seem to be no fundamental limitations to the use ofgas mixtures.

2. Mixed Gas Availability and Costs

It is not viable economically or physically for gas

suppliers to provide large quantities of certified mixtures.

This is due to the fact that a mixture cannot be

significandy compressed and still maintain the appropriate

concentrations in the gas phase. Therefore transportation

of mixtures would require large tanks of gas mixtures in the gas phase. Similarly, there are limitations associated

with certification, storage, and transport of mixtures.

Instead, suppliers recommend that gas be delivered

certified pure, then stored and mixed on-site as needed

[CI].

Major SF(; producers are in the USA, Italy, Japan,

and Germany, see Table CI [CI , C2]. SF,, is prepared for

commercial and industrial use in various grades

(minimum 99.8 mole percent pure) and delivered in a wide range of volumes and pressures. The most

commonly found impurities, include air, nitrogen, water

vapor, carbon dioxide, CF4, SO2, HF, HjS, SOjFj, SOF^,

COS, and trace metal oxides and metal fluorides. Pure

SFfi is readily available in a wide range of volumes and

pressures. At present, only small quantities of calibrated

mixtures of SF^ with other gases can be purchased from a limited number of gas-suppliers. Dilute mixtures such as 1% to 5% SFf, in air, helium or nitrogen, and in various

grades, are routinely available from most gas-suppliers.

Other mixtures are typically treated as specialty orders and

prepared in small quantities (single cylinders or lecture

bottles of desired partial pressure) to specified tolerance

and certification accuracy.

SF(i is shipped, under the appropriate regulations, in cylinders or in tube trailers in liquid form. The maximum

filling density permitted for SF^; in cylinders is 120 % (i.e. percent water capacity by weight). Nitrogen gas is shipped in cylinders, tube tank cars, and tube trailers according to regulations. Liquid nitrogen is shipped as a cryogenic fluid in vacuum-insulated cylinders, and in insulated portable tanks, tank trucks, and tank cars. Storage standards would be recommended if gas mixtures were to be routinely handled, recovered, recycled or

transported.

While there is no limitation to the availability of the

gases, cost and policy considerations cannot be

overlooked. Costs of servicing are relatively high for compounds that are restricted under national or

international regulations. Consequently, the choice of

replacements must consider the dynamics of

environmental policy (as discussed in Appendix B). An

evaluation of the total cost for recover/recycle and

switching from one gas to another, requires performing a

Table Cl. Major producers of sulfur hexafluoride [C1.C2]. Company Counlp,

Air Products and Chemicals Inc. IS A

AliiedSignal Chemicals USA

AGA Gas AB Sweden

Kanto Denka Kogyo Co. Japan

Asahi Glass Co. Japan Ausimont (Montecatini Edison) Italy Solvay (Kali-Chemie) Cicrnuin\

Source: C. M. A. Nayar, GEC Alsthoin, France

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SF^ NIST
40 Appendix C - Potential Barriers to Using Gas Mixtures

technology impact assessment including a full life-cycle

analysis. Among the costs to be considered are (1) the compounds and material resources consumed, (2) the new

and modified equipment required, (3) equipment

operation, including energy dissipated, emissions control,

repair and servicing, and (4) additional personnel and

training. The cost of using gas mixtures will depend on

the relative quality and quantity of the alternative gas

required to meet the necessary certification tests and

operating specifications. In addition, new equipment

would need to be purchased for storage, gas cooling,

pumping, leakage testing, mixing, refilling and other

servicing practices.

3. Preparing Gas Mixtures and l\/laterial

Compatibility

Refilling of equipment with mixtures can be time

consuming and take considerable time to verify or certify to the accuracy desired. Similarly, to "top-off equipment

that has suffered a loss of pressure, i.e., to restore the

original pressure and gas composition, is a greater

challenge than for systems containing a single gas. The

filling and maintenance of any electrical equipment with gas mixtures will require development of concentration

range standards, preparation tolerances, and analytical

accuracy specifications. For example, when preparing a mixture of 40%SF(;-60%N2 an acceptable concentration

range of 10% might require a preparation tolerance of 5%

of component and a 2% analytical accuracy of component.

Studies examining the chemical and physical

properties of SF^-Nj mixtures have been partially

motivated by an interest in the ability to reduce

condensation (effective dew point) of SF,; in equipment

located in cold climates [C3, C4]. The temperature at which SFfi liquefies depends on the gas pressure. Miners

et al. [C3] demonstrated that SFf^-Nj gas mixtures are nonideal. From a practical standpoint a manufacturer who

uses ideal gas assumptions to predict the mixture dew

point temperatures at system-fill pressures of 100 kPa to 500 KPa would under-predict the temperature by as much

as 10 "C. These results suggested that similar

considerations be given to all SFf,-containing mixtures. In some cases electrical equipment may require designs

incorporating heaters to ensure SF^ fractions remain above

the liquefaction temperature (this is, of course,

undesirable). But liquefaction is only one among many

parameters to be considered when refilling with a selected mixture and re-rating the pressure of the electrical equipment and application.

While SFf,-N2 mixtures are relatively inert, other

mixtures of gases with known stability problems may

require special techniques such as passivation or surface

preparation to eliminate the degradation of the unstable

component, generation of undesirable byproducts,

chemical attack of surfaces or general corrosion. In the case of pure SF^, considerable progress has been made in improving the reliability of seal and gasket design and

protection against environmental conditions, resulting in proven long-term performance. When determining what

materials can be used with a gas mixture, it is important

that design and manufacture value compatibility with each

of the components of the mixture separately as well as all of the components when they are combined. This implies

careful choice of material composition, surface finish and

contact methods for walls, spacers, inserts, shields,

electrodes, 0-ring seals, or use of epoxy formulations,

glues and resins. Modes of equipment operation and

location for use must be considered to design for temperature, pressure, and humidity variations or

gradients. For example, equipment with SFj^-Nj mixtures

should be designed for or maintained at temperatures that

will prevent water and SF^ from condensing, thereby

losing performance and homogeneity. If a mixture with a condensable component has been subjected to temperatures at or below its saturation temperature, it will need to be re-homogenized prior to the withdrawal of any

of the gas. Various techniques have been developed for the latter purpose. Since SF,; is packaged as liquefied gas, special

precautions need to be observed when filling equipment.

This applies to both to a new mixture and the processed

gas after recovery and recycling. One concern is particulate matter generated in storage or transfer leading

to the recommendation to filter use to protect

contamination of the electrical equipment. Another issue

is the enhancement of chemical transfer rate by the common practice of warming the gas cylinder or storage

vessel. Warming the storage container during transfer minimizes the refrigeration effect caused by the evaporation of SF^ while allowing its transfer in the

gaseous state. If liquid phase transfer of SF^ is employed,

care is required to ensure the gas is completely vaporized

before it enters the equipment to avoid over-pressurization

or undesirable refrigeration.

4. Mixed Gas Recovery and Recycling

Recovery, recycling, and destruction of SF,; is possible, such that there is no need for deliberate release

into the atmosphere. However, it appears that current

practices are such that economical separation of SF^ from

nitrogen is not possible without some venting of SFf, into the atmosphere. In the event that end-of-life disposal is required, all regulations governing air emissions and

waste management should be followed. SF^ can be

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Appendix C - Potential Barriers to Using Gas Mixtures 41

destroyed by thermal decomposition at elevated

temperatures (>1 100 °C). Such thermal waste treatment furnaces process the sulfur and fluorine constituents to produce naturally occurring materials, e.g. gypsum and

fluorspar.

Choice of alternatives should consider the

availability of internal treatments to the electrical equipment, including gas absorbent filters, desiccants, and

particle filters used in an effort to stabilize the gases and

aid recovery and recycling. Gases, whether initially pure

or mixed, can be expected to degrade with time due to a

variety of factors including contamination caused by

moisture and decomposition products. The composition

and concentration of potentially toxic by-products is unknown for most mixtures and will be quite variable

between applications and equipment.

Lower fluorides of sulfur formed by the decomposition of SF,; may be removed by gas

scrubber/filter systems. Gaseous decomposition products

may be absorbed on molecular sieves or on soda lime

(50/50 mixture of NaOH and CaO), or on activated

alumina (specially dried AI2O3). The quantity of

decomposition products and the amount of absorbent

required to capture all of the products will need to be

determined. It has been suggested that a practical rule-of- thumb is to use a weight of absorbent corresponding to 10% of the weight of gas [C5]. The absorbent should be

located in the equipment to maximize gas contact, unless

both liquid and gas phases are present. In the latter it may

be necessary to locate the absorbent in contact with both

phases or only the liquid phase. The effectiveness and

saturation of absorbents, desiccants and filters will depend

on the equipment design, maintenance schedules,

temperature, as well as consequence of equipment faults and contamination.

The gas from a faulted breaker, leaking transmission

line or transformers, or gas-insulated substation, once

treated to remove decomposition products and moisture,

may be reused if the material meets device specifications.

The key to continued reusability of the gas is to establish

purity standards, certification requirements, and recovery

/ recycling protocols to performance specifications. It takes a combination of factors to achieve this goal:

• Contamination minimization must be built in to electrical equipment design and operation;

• Contamination minimization must be built in to delivery, mixing, recover, and recycle equipment design,

operation and chemical management practices; and

• Monitoring of gas condition including electrical properties and chemical properties (e.g., purity,

decomposition products, moisture content) must be

available; and

• Quality of chemical equipment manufacture,

equipment maintenance, and chemical management

practices must be continuously improved.

The desired purpose of gas recycling is to recover the

original gas, remove any undesirable byproducts (such as moisture, oil, and particles), verify and possibly correct the mixture composition, and return the gas back to the

electrical equipment in a satisfactory certifiable state. A

moisture specification of around 30 ppmv (parts-permillion-volume) is typical while the lEC Standard 376 for new SFf, gas specifies an oil content not to exceed 5 ppmw

(parts-per-million-weight). Two international committees

(CIGRE WG 23-10 TF 01 and lEEE-EI S32; [C6]) are attempting to define purity standards for on-site recycled

SFfi. The standards and protocols for recovery and

recycling of alternatives could be developed in a similar manner. Draft standard EEEE P 1403, which compares air- insulated substations and gas-insulated substations (GIS),

mentions that recent advances in GIS construction include

sophisticated equipment to reprocess SFj^. Similar

integrated technology could be developed for dealing with

. the potential alternatives. In Japan, the Task Committee on the Standardization

of the Use of SF,; Gas for Electrical Power Equipment is currently examining the practices for recycling and

handling of SFf; gas. Among the targeted voluntary

actions is the reduction of releases of SF^ at all stages of

equipment development, installation, and testing. Targets

for recovery are 97% of the purchased gas by the year 2005. This is to be accomplished by the development of

economical and large capacity recycling systems which

evacuate vessels to higher vacuum. Similar recovery and

recycle practices could be implemented for mixtures but

have not been explicitly discussed by this task force. Control of the temperature and pressure is critical to successful reclamation in gas mixtures. In the case of

recovering SF,; from SF^-Nj mixtures, the Nj typically

represents a compressible but non-liquefiable component

that reduces the overall extraction efficiency, unless

higher operating pressures or lower temperatures can be

attained. It should be noted that very little thermodynamic

data on SF^-containing mixtures are available in the

scientific literature. Computational tools are currently

available to help predict some of these missing data [C7].

Efforts to employ these tools may enhance efforts to implement the chemical management of SF^-containing

mixtures as alternative gases. Studies by Mitchel et al. [C8] calculated the SF^, liquid / SF,; gas / N. gas phase

equilibrium assuming a constant volume for an initial fill of various blends at several initial pressures at 20 "C,

subsequently cooled to -50 "C. They concluded that reclamation of SF,, from SF^-N^ and SF^-air mixtures is best accomplished by a combination of compression and

refrigeration to liquefy the SF^. Volumetric efficient handling of mixtures is considered to require cooling

assisted high-pressure (rather than low-pressure) devices.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
42 Appendix C - Potential Barriers to Using Gas Mixtures

Generally, more dilute SF^; mixtures require lower

temperatures and/or higher pressures. To date, commercially available gas reclamation

technology for the electrical industry has been designed

primarily for separation, processing, analysis, and

compression of nearly pure SF^ gas. Much of this work

has been done by companies specializing in SF,; processing, working in cooperation with one or more

manufacturers of SF^ insulated equipment. In most cases, gas carts use pressurized liquefaction of SF^^ (via

compressors) to minimize the necessary volumetric

storage required [C8-C10]. When the stored gas is nearly

100% pure SFfi this method of reclamation is highly

satisfactory and recovery rates greater than 99% yield are possible [C5, CIO]. Losses of SF^ to the environment

depend strongly on the SF^; percentage in the mixture, the operating pressure, the extent of cooling, and the residual pressure remaining in the evacuated volume. Table 2C

shows the losses predicted by Probst [CIO], using

currently available technology based on a two-cycle

distillation process operating at high pressure (5000 KPa)

and low temperature (-40 "C), where liquid SF^ is withdrawn and the remaining gas cushion is vented, when

the purity of liquid gas is to be better than 99%.

Conventional SF^; gas reclamation carts have limited

capability for processing SF^ containing Nj, air or decomposition byproducts at levels exceeding a few

percent [C5, C9]. If gases are heavier than Nj (for

example CF4) then the SF^ losses can be substantial. On

conventional carts, SF^; is cycled and liquefied but the nitrogen gas cannot be liquefied. Liquefaction lowers the

total pressure in the process tank. Each cycle consists of

adding mixed gas until the total pressure equals the initial pressure, followed by additional cooling. If the on-board

volumetric storage tank is not sufficiently large, the

potential exists for N^ gas to shut down the compressor at some limiting high pressure. The ultimate capacity of the

cart storage is reached when the residual gas is compressed to the maximum safe pressure. At this point

the volume being evacuated inside the electrical equipment may still contain some unknown ratio of mixed

gas and the storage tank will hold liquefied SF^ and

gaseous Nj. The protocol used to minimize evaporative

loss of SFf, recommends always reaching full capacity

before emptying the tank, and when emptying to first transfer the SF^ liquid and then purge the residual gas [C5,

'C8]. Practical applications of SF^-Nj mixtures where Nj

gas is the predominant gas requires refrigeration to separate and recover the SF^ efficiently. B. Smith [C5]

recommends that in some instances it may be more

appropriate to use low pressure-assisted cooling operation

instead of high pressure devices [CIO]. In this case, pumps are configured to maximize the quantity of gas

Table 2C. Estimated losses for recover/recycling procedures

SF^ Percentage in Mixture Expected Losses >98%

>90%

>80%

>70%

>60%

>50%

10

12

15

20

30

50

Source: R. Probst, DILO company. Inc. [CIO]

withdrawn from the electrical equipment (reaching base

pressures on the order of 100 Pa) [C5]. Commercial

refrigeration systems are available that use an initial liquefaction of the reclaimed gas (e.g., SF^ and

contaminants), followed by a further liquefaction of the gas phase by sub-cooling of the gas/liquid mixture in a

separate column. Nitrogen gas and contaminants can be

slowly vented while the entrained SF^; can be re-liquefied

and stored. Continuous sub-cooling of the liquid SF^

further separates the gases. Once isolated the SF^ can be

continuously recycled to dry and purify the gas. To assure efficient SF^-Nj mixing, the recommended

protocol for returning recycled gas to the electrical equipment should be to start with nitrogen gas transfer [C5]. As pressure is equalized between the equipment

and SF(i storage tank, heated SF^ gas can be transferred from storage tank to electrical equipment until the desired

mixing ratio (partial pressure) is obtained. The uniformity

of mixing among gas components is important when

refilling with recycled gas. This can be accomplished by

allowing sufficient time for diffusion, designing

equipment with several carefully selected points of gas

injection, and by creating turbulence during the mixing

period. The rate of recovery varies with process used, for example the recovery can be quite slow (on the order of

10-400 Ibs/hr) using conventional gas carts. Such

limitations may not exist with refrigeration systems. More

complex, low pressure gas carts are typically faster, and

recover more gas, then comparable high pressure systems

[C5]. Refill and storage does not appear to be a problem.

Refilling of any container with or without refrigeration

devices or heat exchangers is commercially viable.

If a replacement gas mixture cannot be recovered and

recycled in a safe, cost effective, and environmentally

protective manner, then no real improvement has been

achieved [Cll]. Additional study of the chemical and

physical properties associated with recovery and recycle

of possible replacement gas mixtures needs to be pursued

to accelerate the recommendation, testing, and

implementation of any alternatives to pure SF^.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
Appendix C - Potential Barriers to Using Gas Mixtures 43

5. Retrofit 6. Monitoring and Analysis

A number of manufacturers of electrical equipment

and specialty companies have developed methods to

retrofit circuit breakers and other devices with vacuum

and SFfi interrupters. Depending on the type of

application and equipment it may be reasonable to retrofit equipment with modified gas manifolds, heaters, storage

compartments, material coatings, filters and traps, etc. This concept of retrofitting technology has been proven

reliable and cost effective in certain specific applications. Past experience in this area can be used to help retrofit devices for use of alternatives. In some applications, the use of replacement gas mixtures would require considerably higher operating

pressures than pure SF,; requires. Specific equipment

designs, construction, and manufacture will have to be

evaluated for the ability to accommodate such pressure changes. Otherwise, to maintain similar electrical properties at the same operating pressure, larger and more

robust equipment might be required. Larger insulating

clearances, improved rupture disks, or whatever the

retrofit for pressure requires may only be readily

introduced in the design of new equipment. In other

cases, the changes in operation may be associated with

thermal changes, transport properties, or other

mechanisms not readily addressed via retrofitting. The

feasibility of electrical and/or thermal derating of existing

equipment while purchasing additional equipment will have to be carefully examined. Further research and

development into material properties along with gas thermodynamics and kinetics is needed to recommend and

implement the retrofit of the installed base of electrical devices.

Any change from the original equipment design,

such as substituting a new insulating gas or gas mixture,

in existing equipment would require complete resetting

and certification of the equipment. Again, there are no

fundamental limitations to such testing but there are economic concerns. The testing procedures are described

in a number of international and national standards. For

example with circuit breakers, the required tests are defined in IEEE Standard C37.09-1979 (Reaff 1988)

"Standard Test Procedure for AC High-Voltage Circuit

Breakers Rated on a Symmetrical Current Basis." Current

practices are such that complete type testing on high

voltage electrical equipment can be prohibitively

expensive with estimated costs reaching from $500,000 to $1,000,000 for each type of breaker tested [CI 1]. The move to alternate gases would require research,

development, and policy changes. These would be

intended to provide more cost-effective, rapid and

accurate testing and certification procedures.

Monitoring and analysis are primarily used to determine when maintenance is required and to evaluate

the equipment condition and gas quality. This includes

monitoring of gas adsorbent column, desiccants, particle

filters, and gas scrubbers. Monitoring equipment

designed specifically for pure SF^ applications is currently

available and may be useful to monitor SF^-or alternative gas mixtures. Research and development may be

warranted to certify the performance of such equipment

with mixtures and advance microprocessor technologies

for multiple gas sensing. In all cases, multi-gas testing

would measure moisture content and trace contaminants.

Because moisture is the most detrimental contaminant in pure SFft applications, careful monitoring of humidity will remain an issue with fluorocompound-containing

mixtures.

Monitoring equipment for SF^-containing mixtures

or other alternatives must be sensitive to key byproducts

and be reliable over long periods of time. In the case of

large equipment, such as substations, automated and

multipoint sampling would be valuable. To safeguard the environment against leaks from installed and newly

manufactured equipment, use of alternatives may require

that monitoring systems be developed for installation at transformer and switch-gear stations.

7. References to Appendix C

Cl. H. Withers, Air Products and Chemicals,

Allentown, PA, private communication 1997.

C2. C. Kroeze, Fluorocarbons and SF^,: Global

Emission Inventory and Options for Control,

[Report No. RIVM-773001007] National Instimte

of Public Health and Environmental Protection

(RIVM), Bilthoven, The Netherlands, 1995.

C3. K. B. Miners, M. J. Mastroianni, P. N. Sheldon,

and D. P. Wilson, "Dew Points of SF^ / N, Gas

Mixtures," in Gaseous Dielectrics III [L. G.

Christophorou, Ed., Pergamon Press, NY 1982]

pp. 509-516.

C4. N. G. Trinh and N. Cuk, "Practical Considerations

for Industrial Applications of SF,,/ N, Mixtures,"

Canadian Electrical Association Engineering and

Operating Div. Trans., Vol. 23, Pt.l. 84-A-60.

Canadian Electrical Association. Montreal, 1984

C5. B. Smith, "Mixed Gas Reclamation," Cryoquip

Technical Bulletin, Murrieta, CA 1996; Sulfur

Hexafluoride Gas Recycling Handbook Cryoquip,

Murrieta, CA 1997. C6. G. Mauthe, L. Niemeyer, B. M. Pryor, R. Probst. H. Brautigam, P. A. O'Connell, K. Pettersson. H.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST
44 Appendix C - Potential Barriers to Using Gas Mixtures

C7.

C8.

D. Morrison, J. Poblotzki, D. Koenig, "SF^, and the Global Atmosphere," CIGRE Working Group

23.10. "Gas Insulated Substations," Electra No.

164, pp. 121-131, 1996; L. Niemeyer, R. Probst,

G. Mauthe, H. D. Morrison, J. Poblotski, P. Bolin, B. M. Pryor, CIGRE WG 23-10 Task Force 01,

"SF(; Recycling Guide," 1996.

D. Friend, NIST, Boulder, personal

communication, 1997.

G. R. Mitchel, J. Castonguay, N. G. Trinh,

"Practical Thermodynamics of SF^ Recovery from

SFj^/Nj or SF(,/Air Mixtures," in Gas-Insulated

Substations [S. A. Boggs, F.Y. Chu, N. Fujimoto,

Eds., Pergamon Press, NY 1985] pp. 437-442.

C9. R. Probst, SF^ Maintenance Equipment, DILO

Company, Inc., Oldsmar, FL. CIO. R. Probst, "Recycling of SF^i/Nj Mixtures," DILO

Company, Inc., Oldsmar, FL, personal

communication, 1997.

CI 1. P. Bolin, Mitsubishi Electric Power Products, Inc. and L. Brothers, Southern Company Services, Inc., personal communication 1997.

Gases for Electrical Insulation and Arc Interruption: Possible Present and Future Alternatives to Pure SFg / NIST


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