Reference

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NAT'L INST. OF STAND & TECH

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a NBS TECHNICAL NOTE 1177

U.S. DEPARTMENT OF COMMERCE/National Bureau of Standards

Elements of

Thermography for

Nondestructive Testing

QC«

100

U575i

1177

19^3
NATIONAL BUREAU OF STANDARDS

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/V)£5 Mo^Ol

Elements of Thermography for

Nondestructive Testing

NATIONAL BtTBEAU OF STANDARDS.

LIBRARY

JUN 14 1983

Julius Cohen

Radiometric Physics Division

Center for Radiation Research

National Measurement Laboratory

National Bureau of Standards

Washington, DC 20234

*°»EAV O*

U.S. DEPARTMENT OF COMMERCE, Malcolm Baldrige, Secretary

NATIONAL BUREAU OF STANDARDS, Ernest Ambler, Director

Issued May 1983
National Bureau of Standards Technical Note 1177

Natl. Bur. Stand. (U.S.), Tech. Note 1177, 35 pages (May 1983)

CODEN: NBTNAE

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WASHINGTON: 1983

For sale by the Superintendent of Documents, U.S. Government Printing Office, Washington, DC 20402

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(Add 25 percent for other than U.S. mailing)
PREFACE

Thermography, the process whereby the invisible infrared thermal

radiation from an object or a scene is rendered into a visible image,

is known mainly for its military surveillance and remote-sensing

applications. Nevertheless, thermography has great value also in a variety of non-military applications, and is being exploited in

agriculture, geology, environmental control, meteorology, medicine,

energy conservation, building, and manufacturing industry. In particular, its importance in industry for plant preventive maintenance,

process control, quality control, and nondestructive testing has been

recognized with the recent establishment of several independent

working groups in thermography by different professional societies

such as ASTM, ASNT, and SPIE.

This is intended to be a tutorial paper in thermography, especially as it relates to nondestructive testing, for program managers

and scientists who are unfamiliar with thermal imaging systems and

techniques, and who also may not have a background in infrared

physics and technology. The material offered herein gives a simple,

broad, and mainly qualitative overview which should help the reader

to adjudicate the feasibility of applying thermography for his

specific purpose. Notwithstanding, thermography is a highly sophisticated and complex subject, and readers who wish to delve into the

theory and the design of thermal imaging systems are referred to the

books listed in the bibliography section. The bibliography includes

also a listing of periodicals and reports dealing with applications

of thermography to nondestructive testing.

m
CONTENTS

Page

Preface iii

1. Introduction 1

2. Thermal Imaging Systems 4

3. System Performance Characteristics 7

4. The Target and the Image 15

5. Atmospheric Effects < 18

6. Radiometric Measurement of Temperature 19

7. Applications of Thermography to Nondestructive Testing 21

8. References 23

Bibliography 25

Epilogue 28

IV
List of Figures

Spectral distribution of blackbody radiant power density

at various temperatures. W, is the rad -

per unit wavelength at the wavelength X

at various temperatures. W, is the radiant power density

Page

2. (a), Thermogram of a current-carrying transformer wherein

the light regions signify higher temperatures.

(b), An ordinary photograph of the transformer 3

3. Simplified block diagram of a scanning, thermal imaging system ... 7

4. Targets used for measuring performance of thermal imaging

systems; T is target temperature, T

g

is background temperature, and T > Tg. (a), NEAT. The target is an extended

source of square geometry; (b), MRTD. The target is a periodic 4-bar chart of rectangular geometry, with aspect

ratio of 7:1; (c), MDTD. The target is a square whose

area is equal to the area of the surrounding background

temperature 10

5. Effect of a finite aperture on the image of a point

source (a) and a line source (b) 12

6. Example of the dependence of minimum resolvable temperature

difference (MRTD) and modulation transfer function (MTF) on normalized spatial frequency ... 13
Yet from those flames

No lights but vathev darkness visible.

Milton

VI
ELEMENTS OF THERMOGRAPHY FOR NONDESTRUCTIVE TESTING

Julius Cohen

Radiometric Physics Division

Center for Radiation Research

This paper presents an elementary review of thermal imaging

systems, with emphasis on the application of thermography to non- destructive testing. Topics discussed include heat radiation theory;

early and contemporary thermal imaging systems; performance characteristics; effects of emissivity, background temperature, atmosphere,

and field of view. Examples of various applications of thermography

to nondestructive testing are given. A bibliography is included.

Key words: heat; imagery; infrared; nondestructive testing; passive;

radiation; remote sensing; temperature; thermography.

1 . Introduction

All objects continually emit thermal radiation from their surfaces. Usually

the radiation is in the infrared portion of the spectrum, which is not visible to

the unaided eye. Indeed, the radiation from an object does not become visible

until its temperature exceeds 800 K.

The radiant energy emitted from a heated surface per unit time--i.e., the

power radiated—depends on the nature of the surface, on its area, and on its

temperature, in accordance with the Stefan-Boltzman law,

W = A e a T

4

,

where W is the power radiated [watt]

2

A is the surface area [meters ]

e is the emissivity of the surface (sometimes called emittance)

-8 2 4 a is the Stefan-Boltzman constant = 5.670 * 10 watt/m K

and T is the absolute temperature.

The emissivity, e, is a measure of the radiation efficiency of a body, com- pared to a perfect radiator at the same temperature; thus, e (assumed to be

wavelength independent) is a dimensionless number lying between zero and unity.

For example, for a perfect radiator, termed a blackbody, e = 1; for copper,

e - 0.3.
1 23456789 1011 12131415

A(^m)

Figure 1. Spectral distribution of blackbody radiant power density

at various temperatures. W, is the radiant power density

per unit wavelength at the wavelength X.

The radiant energy is continually being emitted in the form of a mixture of

electromagnetic waves of different wavelengths, and the radiant power is distributed as a continuous function of wavelength. Figure 1 is a graph of the

spectral distribution of the radiant power per unit area from the surfaces of

several blackbodies of different uniform surface temperatures 1

; here W, is the

radiant power density per unit wavelength at wavelength X. Each curve is characterized by a particular wavelength A , a function of temperature, for which W, P A is a maximum. The effect of increasing temperature is seen to shift X to shorter

wavelengths, as well as to increase the value of W, at each wavelength. The

relationship between x_, and temperature of the maximum W, is given by the approxP A imation,

x These spectral distribution curves are obtained from Planck's blackbody radiation

law. The area under a curve, the total power density radiated, would correspond

to the Stefan-Boltzman law, with e = 1.
A - 3000/T .

As a concrete example of spectral distribution of radiant power, a terrestrial object, commonly at ^ 300 K, emits in the 2 ym to 100 ym region, most of

the power is in the 3 ym to 14 ym region, and the power peaks at ^ 10 ym. On the

other hand, for an incandescent filament at ^ 3000 K, A - 1 ym, which is in the near infrared. The filament can be seen to be glowing because of the shorter

wavelengths emitted in the visible region of the spectrum (approximately 0.38 ym

to 0.77 ym).

Although infrared radiation is invisible to the unaided human eye, various means have been devised for detecting and imaging an infrared scene for visualization. Infrared imaging may be classified as active or passive according to

whether the scene is irradiated with an infrared source and the resultant reflected

radiation is imaged, or whether the self-radiation from the scene is imaged. The

latter process, which converts the temperature pattern of a scene into a corresponding contrast pattern, is termed thermography, and the viewed image is termed.

a thermogram; an example is shown in figure 2(a), a thermogram taken of a currentcarrying transformer. For comparison, figure 2(b) is an ordinary photograph of

the same current-carrying transformer.

(b)

Figure 2. (a), Thermogram of a current-carrying transformer wherein

the light regions signify higher temperatures.

(b), An ordinary photograph of the transformer.
Thermography's ability to see scenes, objects, and features otherwise

invisible—sometimes even below a surface—has made it a potent means used in a variety of applications for military, medical, industrial, agricultural, geological, meteorological, and energy conservational purposes. For example, it is used

for military intelligence gathering, early warning systems, and weaponry fire

control; for medical diagnosis of tumors and inflammations; for monitoring

nuclear reactor steam cooling towers; for inspecting refractory linings of

furnaces and ducts; for inspecting electrical power transformers and electrical

rotating machines while under power; for studying soil moisture, crops, and

vegetation decay; for studying volcanoes, glaciers, tides, and tectonic plates,

and for detecting petroleum and mineral deposits; for detecting and mapping

thermal effluent discharges; and for detecting heat losses from residential

buildings, plants, and machinery. These are just some of the myriad ways thermography is being put to use. They are mentioned here only to suggest scope and

usefulness, but will not be elaborated on, as this paper is concerned chiefly

with the applications of thermography to nondestructive testing.

2. Thermal Imaging Systems

John W. Herschel (son of William, the discoverer of the infrared spectrum)

is credited [I,?.] 1 with inventing thermography in 1840, by utilizing differential

evaporation of thin liquid films. This rudimentary apparatus was the prototype

for the Evaporograph, as later (1929) Czerny improved on the concept by substituting thin oil films that changed color with differential evaporation resulting

from the heat of the incident infrared radiation [2]. And in 1959, the Evaporograph was utilized for qualitative nondestructive testing of hot spots. However,

this imaging device was crude and insensitive, with poor repeatability; it is

much more of historical than of practical importance.

An exotic way of producing a thermal image is through the use of certain

temperature-sensitive liquid crystals, applied directly to the surface to be

examined. This technique is sometimes used to examine aerospace structures [3].

However, liquid crystals exposed to the atmosphere have a short lifetime owing to

contamination, and their use is rather restricted.

Thermistors, which are commonly oxidic semiconductors having a large negative

temperature coefficient of resistance, also may be utilized as the detector in

thermal imaging systems. But thermistors have \/ery long time constants, high 1/f

Figures in brackets indicate the literature references at the end of this paper.
noise necessitating chopping of the radiation, and very long scan-frame times,

thus making for inferior real-time display, particularly as regards resolution.

For imaging systems, thermistors are of rather limited applicability. Thermistors

for thermography find their chief use now in infrared microscopes where the

targets are small and the image is produced on a photograph.

Most modern thermal imaging systems use either photon detectors or pyroelectrics, a type of thermal detector, as the infrared sensor which receives the

radiation from the scene or the target and converts it into an electrical signal

for processing and display.

Photon detectors respond to numbers of photons, hence they are wavelength

dependent. Owing to their electronic structure, any given detector responds to

only a very narrow range of wavelengths. Photon detectors responsive to infrared

radiation generally require cooling to 77 K or below, depending on the nature of

the material from which the detector is made. Photon detectors fall into either

of two categories, photoconductive or photovoltaic, and either may be used in a thermal imaging system. Photoconductors are homogeneous semiconductors, while

photovoltaic detectors are junction or barrier devices. The advantages of the

photovoltaic detectors are that they require no application of a voltage bias and

do not generate a significant amount of heat as does a photoconductor, and their

noise may be somewhat lower than photoconductive detectors made of the same material. However, not all materials are utilizable as photovoltaic detectors.

The detectors commonly used in thermal imaging systems are indium antimonide

photovoltaic detectors at 77 K, for the 3 urn to 5.6 ym region, and mercury

cadmium telluride photoconductive and photovoltaic detectors at 77K, for the 8 ym

to 14 ym region. Although a single detector may be used, it is usual to use an array of detectors. In general, single detectors and linear arrays are preceded

by an opto-mechanical scanner, which dissects the scene or target bit by bit for

sequential reception by the detector(s). Opto-mechanical scanners generally

utilize rotating or oscillating mirrors or prisms to generate a rectangular

raster--!". e. , a line-by-line scan of the scene or target--analagous to the formation of a picture on a television screen. On the other hand, focal -plane mosaics

(square arrays of detectors) do not require scanning.

Thermal detectors respond to total radiant power, hence they are relatively

wavelength independent, their response often extending to very long wavelengths,

up to ^ 100 ym. A particularly attractive attribute of thermal detectors is that

they require no cooling. This is not just a convenience; it also reduces size,
weight, cost, and complexity, and does not introduce additional noise (microphonics) owing to any refrigerator vibrations. Pyroelectrics are a special class

of thermal detector; unlike the others they respond only to a change in temperature, rather than to the temperature itself. Hence, pyroelectric devices need to

be panned or nutated, or else the incoming radiation from the scene or target

needs to be periodically interrupted, or chopped, as for example, with a rotating

toothed wheel. However, pyroelectrics will produce a current, or signal, on cooling, as well as on heating, with the polarity of one opposite to that of the

other, so special means are provided in the better systems to overcome the effects

of changing scene polarity. The pyroelectric in a thermal -imaging system is

generally a thin crystal such as triglycene sulfate (although systems employing

polymeric films instead--e.g. , of polyvinyl idene fluoride--are being developed

because of their thinness, cheapness, and superior chemical stability). Pyroelectric thermal -imaging systems are usually of the vidicon type, which means

that the scene is imaged on one face of the pyroelectric, thus producing a pattern

of localized charges on the poorly-conducting pyroelectric material, the magnitudes of which are read by an electron-beam scanning the opposite face of the

pyroelectric, in raster fashion. Pyroelectrics, like photovoltaic detectors, do

not require biasing. On the other hand, compared to photon detectors, pyroelectrics, like thermal detectors in general, have lower specific detectivities 1

and longer response times. Thus, while the performance of pyroelectric thermal

imaging systems can be quite good, the performance of systems with photon detectors can be better. The main attribute of the pyroelectric system, as already

mentioned, is its operability over an extensive range of wavelength, without the

necessity of cooling.

Although the heart of a thermal -imaging system is its infrared detector(s),

the detector is but one of several interacting subsystems which together comprise

a complex system. Figure 3 is a simplified block diagram of a scanning thermal - imaging system. The subsystems are, in general, the following, given in sequence:

1) an optical system for collecting the radiance from the scene or target, spectrally filtering, and focusing it onto the detector(s); 2) a scanning system for

"dissecting the scene" or a chopper for modulating the radiance; 3) a detector

system including any preamplifiers and ancillary circuitry; 4) a signal processor

Specific detectivity (D*) is the signal-to-noise ratio of the detector output

per unit incident power normalized to a unit sensitive detector area and a unit

electrical bandwidth. D* is defined in units of [cm Hz 2/watt].
Collecting

Optics and

Filters

OptoMechanical

Scanner

Detector

Bias and

Preamplification

Circuits

Detector Assembly —»> Video

Processor Video

Monitor

Figure 3. Simplified block diagram of a scanning thermal imaging system,

system for receiving the low-level signal from the detector(s), amplifying it,

limiting the bandwidth, extracting the information the signal contains, and

delivering this information to the display system; and 5) a display system,

generally a video monitor. The signal processor uses techniques similar to that

used for commercial television, so 4) and 5) together may be considered a TV

system. In addition to the aforementioned subsystems, there may be optical

baffles, or stops, to limit field of view and a cooling system such as a dewar,

pressurized gas, or heat pump, for cooling the detector(s) and baffles. Because

of the complexity and sophistication of the modern thermal -imaging system, it is

usually designed by a team of specialists, coordinated by a systems engineer.

The fields which are usually represented are radiation theory and radiometry;

optical design and engineering, including Fourier optics and optical scanning

devices and systems; infrared physics, including detectors, noise theory, and

atmospheric transmission; and television engineering.

3. System Performance Characteristics

Thermal images result primarily from temperature differences and/or emissivity differences in a scene or target (rather than reflections), and it is the

function of a thermal-imaging system to reproduce an acceptable visible image of

the scene or target from its thermal content. Thus, a thermal -imaging system is

required to resolve temperature differences and emissivity differences (apparent

temperature differences). Further, as temperature and emissivity are distributed

spatially in the scene or target, the thermal -imaging system is required to

resolve spatial differences of emissivity or temperature. A system's ability to

reproduce an accurate, sharp image is given by its performance characteristics,

which obviously must include measures of the system's ability to resolve (true

and apparent) temperature differences and spatial variations.

Many measures have been devised for characterizing the performance of a thermal -imaging system and its subsystems, with most being of value only as an aid to the subsystem designer or systems engineer. Nevertheless, several measures
relating to overall system performance may be of importance to the user of a thermographic system, depending on the application. These measures are 1)

[temperature] accuracy

1

, 2) noise-equivalent temperature difference [NEAT or NETD], 3) minimum resolvable temperature difference [MRTD] , and 4) minimum

detectable temperature difference [MDTD]. Item 1) is relevant to remote radiometric temperature measurements, 2) to temperature sensitivity to a broad area target, and 3) and 4) to imaging. It may be noted that measures 2), 3), and

4) are some expression of temperature difference , which certainly is not sur- prising. Not obvious, however, is that these temperature differences are functions

of signal-to-noise ratio, which also should not be surprising as noise imposes

the lower limit of radiative power which may be detected. Each of the above

performance measures will now be discussed in relation to their measurement or determination and to their significance and utility.

1) Accuracy -- For most applications of a thermal -imaging system accurate

temperature measurements are not of concern, and accuracy is seldom mentioned in

thermographic literature or manufacturer's specifications. Further, "highlyaccurate" temperature measurements may be exceedingly difficult to make—particularly under some field conditions. Nevertheless, there appears to be a growing

need for accurate radiometric temperature determinations, e.g., for process

control and for research purposes. Factors which may cause inaccuracy in temperature determination include the original calibration method and inherent operational effects, and effects of atmosphere, emissivity, and reflections (discussed

in subsequent sections). If accurate temperature determinations are required, it

is generally advisable to make an on-site calibration using blackbody targets of

known temperature. 2

^ome imaging systems include temperature measurement capability, other systems

do not.

2 Note added in proof: A forthcoming paper describes some simple procedures for

making qualitative measurements in the field without the need for extensive

ancillary equipment. Although the results are not highly accurate, in many cases they are adequate. See Orlove, G. L., Practical Thermal -Measurement Techniques,

Proceedings of Thermosense V, SPIE, P.O. Box 10, Bellingham, WA 98227 (to be

published).

8
2) Noise-equivalent temperature difference -- This is a convenient measure of an imaging system's thermal sensitivity to a broad area target whose image

completely covers the area of one detector. (Such a target is referred to as an extended source.) If the target is a blackbody at temperature T, and the sur- rounding background, assumed to be a uniform blackbody, is at temperature T

B

, the

noise equivalent temperature difference NEAT is defined as the blackbody targetto-background temperature difference in a standard test pattern which produces a peak signal-to-rms noise ratio (S/N) of unity in the reference electronic filter

(used in the processing of the detector signals) when the system views the test

pattern. The test pattern can be a square area of temperature greater than the

background, as shown in figure 4(a).

Expressed mathematically, noise equivalent temperature difference is given

by

T - T

R AT

NEAT = S/N S/N *

When S/N = 1, NEAT = AT. Thus, to measure the noise-equivalent temperature

difference, one finds the AT which just produces S/N = 1 in the reference electronic filter. Because noise-equivalent temperature difference depends on the

filter and on the background temperature, usually ^ 300 K, these should be specified along with the NEAT value. The measurement of noise-equivalent temperature

difference is not difficult; however, owing mainly to the inaccuracy in measuring

rms noise levels, NEAT is not a \/ery accurate measure. Still, it can be used to

compare the thermal sensitivities of two different systems provided the measurements conform to the same standard and the differences in NEAT are sufficiently

large. Thus, for example, if the NEAT of system A were 0.2°C and that of system

B were 0.25°C, both systems would be considered to have essentially the same thermal sensitivity. Alternatively, if the NEAT of system A were 0.2°C and that

of system B under the same conditions were 0.4°C, system A would be considered to

be the more sensitive system for those conditions.

Noise-equivalent temperature difference is measured at the video signal

output and relates only to the thermal -imaging system exclusive of an image

observer. On the other hand, where imagery itself is concerned, an observer's

visualization capabilities must be included, as is done for the measures, minimumresolvable temperature difference (MRTD) and minimum-detectable temperature

difference (MDTD), discussed next.
(a)

(b)

(c) D

Figure 4. Targets used for measuring performance of thermal imaging systems;

T is target temperature, T

B is background temperature, and T > Tg.

(a), NEAT. The target is an extended source of square geometry;

(b), MRTD. The target is a periodic 4-bar chart of rectangular

geometry, with aspect ratio of 7:1; (c), MDTD. The target is a

square whose area is equal to the area of the surrounding background temperature.

10
3) Minimum-resolvable temperature difference -- MRTD is a measure of the

compound system-observer capability to spatially resolve temperature differences

in a standard target by observing its display on a video monitor. MRTD is a function of target geometry and it is usual practice to use a periodic 4-bar

chart of rectangular geometry and aspect ratio (length:width) of 7:1. MRTD is a function also of the periodicity of the bars, or its inverse, the spatial frequency

1

, so in practice MRTD is measured as a function of the spatial frequency

and shown as a curve. Examples of targets used for these measurements are shown

in figure 4(b). The targets are blackbody radiators of different, but uniform

temperatures. Further, the power of the eye-brain to resolve spatial temperature

differences is a function of signal-to-noise ratio (S/N). For example, the

probability of resolution with a standard target is ^ 50 percent for a display

S/N of roughly 3 and is ^ 90 percent for S/N - 5. Thus, the probability of

detection should be specified along with the MRTD vs. spatial frequency curves.

Qualitatively, MRTD is defined as the image S/N required for an observer to

resolve a defined 4-bar pattern chart that is masked by noise, and it is expressed

as the temperature difference between the bars and the background.

Analytically, the MRTD is directly proportional to the noise-equivalent

temperature difference (NEAT) of the system and inversely proportional to a mathematical 'quantity called the modulation transfer function (MTF); hence, MRTD

can be derived or it can be measured directly. A brief discussion of the modulation transfer function will now be given in order to make clearer the significance

of the minimum resolvable temperature difference.

Consider a target to be decomposed into a vast number of discrete points of

various intensities or radiances--which, in fact, is precisely what the optomechanical scanner accomplishes. If an imaging system were perfect, every point

in the target would be reproduced exactly in the image (with due allowance for

any magnification or inversion), and the target would be reproduced exactly by

the total image. In reality, perfect fidelity is a physical impossibility, owing

mainly to diffraction effects from finite apertures. Examples of finite apertures in imaging systems include lenses, stops, infrared detectors (responsive

areas), and the scanning electron beam spot of the display tube. Thus the image

1 Spatial frequency may be defined in terms of the angle between an observation

point and the normal distance between the centerlines of two adjacent bars. The

usual units are cycles/mrad or (number of) lines/picture height.

11
differs from the object in amplitude (it is attenuated), shape, position, or all

three. The modulation transfer function (the modulus of a Fourier transform)

gives a spatial description of the attenuation in amplitude; the minimum attenuation is denoted by a normalized MTF of unity.

(a)

(b)

Point

*

Line

Focal Plane

Figure 5. Effect of a finite aperture on the image of

a point source (a) and a line source (b).

Figure 5(a) illustrates the effect of the finite aperture of a lens on the

image of a point source. If a point source were focused through a thin (negligible refraction), aberration-free, positive lens, the image in the focal plane,

parallel to the plane of the lens, would be found to be a spread-out spot of non- uniform intensity (intensity is greatest at the centerpoint) and blurred perimeter,

A similar phenomenon would occur if a line source (a rectangular slit of uniform

radiance or intensity) were substituted for the point source, as depicted in

figure 5(b).

The MTF of the overall thermal imaging system includes the individual MTF's

associated with its various apertures and it relates to the ability of the

system to recreate the thermal -spatial frequency content of an object. The

(system) MTF can be determined by measuring the point or line spread (cf figure

5) from a blackbody source using photometric or thermal techniques, and applying

Fourier analysis. (The measurement is quite difficult—aperture dimensions and

12
positions must be precisely determined and temperatures need to be controlled to

within ±0.05°C.)

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0

Target Spatial Frequency

Figure 6. Example of the dependence of minimum resolvable temperature difference (MRTD) and modulation transfer function

(MTF) on normalized spatial frequency.

A modulation transfer function, in general, is a sensitive function of

spatial frequency, as may be noted in the example of figure 6. MTF decreases

with increasing spatial frequency and in fact vanishes at sufficiently high

spatial frequency; i.e., the element (aperture) blocks high spatial frequency

information.

13
Remembering that MRTD <* NEAT/MTF, the dependence of MRTD on spatial frequency can be graphed, as shown in the example of figure 6, where the system MTF

has been included for instructive purposes. The intuitively realizable result

shows that the resolution of closely-spaced lines of high spatial frequency

requires greater contrast, or temperature difference, between a line and the

background, than does widely-spaced lines of low spatial frequency; cf figure

4(b).

Although MRTD is a function of noise-equivalent temperature difference, it

is obvious that NEAT alone cannot be used to compare the performance of two

different systems in spatially resolving temperature differences. For example,

system A can have a lower (better) NEAT than system B, but the MTF of B may be

sufficiently larger (better) than that of A, so that the MRTD of B is lower

(better) than that of A.

4. Minimum-detectable temperature difference -- The minimum-detectable

temperature difference (MDTD) is similar to the minimum-resolvable temperature

difference, except that instead of the 4-bar pattern, the target consists of a uniformly heated square of blackbody temperature T framed by a uniform background, of specified area, at blackbody temperature T„; this target is imaged by

the system and observed under improved conditions of long search time and known

target location. An MDTD target is depicted in figure 4(c); the area of the

square of temperature T is equal to the area of the surrounding background of

temperature Tg. As for MRTD, curves of MDTD as a function of spatial frequency

are obtained, except that spatial frequency is expressed in terms of angle of

view [mrad], rather than lines/picture height.

Where details in imagery are of concern, MRTD would be a more useful measure

than MDTD; however, where detection of small hot spots in a wide expanse is of

concern, as for many nondestructive testing applications, MDTD would be the more

useful measure.

Finally, performance measures are useful indicators, and it is hoped that

they will correlate with field use, so a caveat is in order. The performance

measures are obtained under ideal laboratory conditions such as blackbody targets

and unit transmissivity, and the temperature differences are small, < 1°C. Field

conditions may deviate appreciably, so performance measures must be utilized

cautiously or with modification.

14
4. The Target and The Image

Thermal -imaging systems act on target information and the contents of an image, including the intelligence therein, depend on characteristics of the

target as well as those of the imaging system. The latter has already been

treated in some detail; for optimal use of a thermal -imaging system, it is

necessary to consider also the characteristics of a target. Some basic facts

concerning the target are now listed:

1) The thermal radiation from a target (radiance) emanates from

its surface;

2) A thermal -imaging system responds to irradiance at its entrance

aperture (which one would like to be only radiance from the

target). Thus the imaging system will perceive apparent temperatures or apparent temperature differences present at the

surface of the target. If the target is a uniform blackbody,

the apparent temperature will be the "true" temperature

(neglecting any extraneous effects). If the target is a greybody (an object of uniform emissivity < 1), the apparent temperature will not be the "true" temperature; likewise, the

system will indicate emissivity differences as temperature

differences.

3) A thermal -imaging system, no matter how good, cannot distinguish a target from its background unless there is sufficient

contrast between the target and its background. Contrast is

defined as the difference between the radiances of the target

L and of the background l_ B

, divided by their sum L + L„. As

the ease with which an object can be identified depends on contrast, it is sometimes desirable to increase the contrast,

e.g., by using spectral filters to measure over a limited

spectral region, or by suppressing background radiance, a sophisticated and costly measure.

4) Obviously the spectral response of the system's infrared

detectors must include the spectral radiance of the target.

Optimal detection results when the peaks of both coincide,

but optimal detection is not always necessary; mismatches

may be compensated by large irradiance or high spectral

detectivity.

15
For convenience, targets may be classified according to 1) emissivity and

2) size relative to image size.

1) If the thermal target is a perfect or near-perfect absorber of

radiation over all wavelengths, it is said to be a blackbody,

and the emissivity e - 1 . A target of constant emissivity < 1

is said to be a grey body.

2) If the target fills the field of view of the detector (i.e.,

the image of the target is larger than the area of a single

detector), the target is said to be an extended source. If

the target does not fill the field of view (i.e., the image

of the target is smaller than the area of a single detector),

the target is said to be a nonresolvable source (and considered

to be a point source).

A consideration of the foregoing will show that it is advantageous to

employ targets which are blackbody extended sources:

If the target is an extended source, the radiometric quantity of concern is

radiance,

L - Si

where L is radiance [watt/ cm sr],

2

W is radiant emittance [watt/cm ].

Ignoring attenuation by the atmosphere or the optics, the irradiance at the sensor is independent of distance to the source, and is given by

H = Loo

2

where H is irradiance [watt/cm ]

OJ is the solid angle subtended by the detector [sr]

When two areas differ in radiance, the difference may be due to a difference

in temperature or emissivity, or both, so in general,

AL = AI_ T + AL

E

.

16
If the source is a blackbody

AL = AI_ T

,

and variations in radiance are due only to temperature differences. Therefore,

system temperature-sensitivity performance on an actual (as opposed to test)

target should correlate with the noise-equivalent temperature difference of the

system (which is measured on blackbody test targets).

The noise-equivalent temperature difference may be written

H

NEAT =

u> t L

» a

where H is the noise-equivalent irradiance--i .e. , the irradiance for which the

o

^ signal-to-noise ratio is unity, t is the atmospheric transmissivity (assuming

a negligible atmospheric absorption, t, = 1).

a

It is a property of solids that any material discontinuities in an object—

e.g., cracks, fractures, voids, foreign inclusions—will result in a corresponding

temperature discontinuity if heat is made to flow through the object. While

surface discontinuities may be discernible because of emissivity differences

alone, thermal viewing of infrasurface discontinuities requires that heat flow

through the target. The required heat may be developed from within the targetas with electrical components or running tires—or from without—as by heat

soaking the material just prior to viewing, or by uniformly heating the surface

of the material during viewing. To eliminate spurious results due to emissivity

differences, it is usual practice to paint or spray the surface with a coating of

highly absorbing material, thus approximating a uniform blackbody target.

The temperature discontinuities, or differences, in a heated target may

originate at the surface, the subsurface, or in the interior. In any case,

thermal radiation is emitted only from the surface, so infrasurface temperature

differences must be transmitted to the surface if they are to be perceived by a thermal-imaging system. Whether or not an infrasurface-originating temperature

difference--!*. e. , an infrasurface defect—can be detected depends strongly on its

depth and on the thermal conductivity of the target material. If an infrasurface

temperature difference is produced, heat will diffuse from the warmer to the

cooler regions in all directions, including that of the surface. If the thermal

17
conductivity of the material is low--e.g., ceramics, glass, rubber--the heat will

not readily disperse, so that a temperature difference may be transferred to the

surface. On the other hand, if the thermal conductivity is high--e.g., metal s-- heat will readily disperse and the target will soon acquire a uniform equilibrium

temperature with no temperature difference manifest at the surface.

At this juncture the reader may wish to review the descriptions of the

various targets used for the measurements of performance, and these have been

summarized in figure 4. Additionally, recall that a quoted value of NEAT should

include specifications of the background temperature and the reference electronic

filter in the measurement circuit, while quoted values of MRTD/MDTD should also

include specifications of spatial frequency/angle of view and the probability of

resol ution/detection.

5. Atmospheric Effects

Atmospheric effects are of great importance in airborne thermography where

the source, or target, is far away. The atmosphere may attenuate the radiation

from the target, as well as alter its spatial, temporal, and spectral characteristics, thus degrading the target information received. On the other hand, in

nondestructive testing atmospheric effects are generally of negligible importance

because the source is quite close (< 1 m) and the atmosphere is uncontaminated

with vapors such as smoke, fog, etc. Occasionally, however, nondestructive

testing may involve critical measurements or may have to be made under adverse

conditions--e.g. , the source is distant or the atmosphere is humid--such that

atmospheric effects need to be considered.

Atmospheric effects arise from (1) the interaction of the atmosphere with

the target radiation and (2) from inherent causes. The ways in which atmospheric effects are manifested are

1. Absorption of source radiation by various atmospheric con- stituents, notably water vapor, carbon dioxide, nitrous

oxide, and ozone, of which the first two are prominent.

The absorption is selective with optical frequency,

resulting in an absorption spectrum, and it is important

that the system's infrared detector have spectral response

within an atmospheric "window", where absorption is negligible. As noted above, atmospheric absorption (selectively)

attenuates the target radiation;

18
2. Background thermal radiation from these same atmospheric

constituents which are strong absorbers;

3. Scattering of the source radiation out of the path of the

imaging optics by molecules of the permanent gases and by

aerosols;

4. Scattering of unwanted background radiation into the

imaging optics by these same permanent gases and aerosols;

5. Turbulence in the atmosphere, or atmospheric optical noise.

The most important of the above phenomena is atmospheric absorption, a complex subject which has received considerable study. The practicable mathematical solution of atmospheric transmission problems requires a mathematical

model, of which there are many, and computer aid. For information on some computer programs, see Goodell et al . [4]; for additional discussion on attenuation, and references, see Holter et al . [5], and The Infrared Handbook [6].

In airborne thermography, atmospheric effects may impose a handicap on good

imagery which must be coped with, and mathematical methods of modeling are often

used for this purpose. Although modeling is probably the best, if not the sole

rational means of coping, it can only provide rough estimates because a model is

based on assumptions and the implementing data are uncertain. If atmospheric

absorption were a problem in nondestructive testing, it would be preferable to

calibrate the system on site with the aid of a blackbody target, rather than to

employ modeling.

6. Radiometric Measurement of Temperature

The primary function of a thermal imaging system is to obtain a visual image

of a thermal target. Additionally, however, some systems may be used for remote

determination of target temperature (a minority of sophisticated systems incorporate a blackbody benchmark). Such temperature measurements properly are more

in the realm of radiometry than thermography. Nevertheless, the factors of concern are some of the same factors which are of concern in imagery, viz.

target, background, and atmospheric effects. The manifestations of the factors

differ for the two cases, but unsurprisingly the solutions are the same.

The imaging system, like any radiometric device, responds to the irradiance

at its entrance aperture. If the target is unresolved, the irradiance is a function of distance to the target and its temperature is given by [1]

19
2 R

2

(g) Af) %

a A r D (NA) D' a o

I

4

N J

'

where T

y

R

00

Af

a

A

s

D

oNA

D*

T

a

£

s

is temperature [K]

is distance between target and detector [cm]

is solid angle subtended by detector [sr]

is noise equivalent band pass [Hz]

2 4-, is Stefan-Bol tzman 1 s constant [W/cm K J

2- is target surface area [cm ]

is lens diameter [cm]

is numerical aperture [dimensionless]

^ -1 is specific detectivity [cm(Hz) 2 W ]

is atmospheric transmittance [dimensionless]

is spectral transmittance of detector, including the

optics [dimensionless]

is emissivity [dimensionless]

is signal-to-noise ratio [dimensionless].

If the target is an extended source, the irradiance is independent of the

distance to the target, and its temperature T is given by [1]

a D

Q

(NA) D* t

q xQ

e Af

CO

Note that T is independent of both target distance and target area, a particularly valuable characteristic that is exploited for industrial process control

and for nondestructive testing.

Assuming errors in system calibration to be negligible, the potential sources of error in temperature determination are emissivity variations, atmospheric effects, and background effects. These have already been discussed in

connection with imagery, and those discussions generally carry over.

20
Nevertheless, some additional remarks concerning background effects are worth noting here. As alluded to, above, background is not restricted to the

backdrop; background in general encompasses the entire surround that interferes

with the radiation being received from the target: atmospheric scattering and

emission, radiation from walls and windows, etc. Background radiation which

falls on a greybody target will be reflected. Assuming the target to be opaque,

the reflectivity, or fraction of the impinging radiation reflected, is merely

(1-e). The reflected background radiation results in errors in apparent radiance

hence temperature measurement. For a treatment of errors in passive infrared

imaging systems due to reflected ambient flux, see J. C. Richmond [7]. On the

other hand, if the target is a blackbody, it will absorb all of the impinging

background radiation and none will be reflected. Thus it is practice in non- destructive testing, to coat targets such that they are rendered blackbodies. In sum, there are many advantages to working on blackbody extended sources, rather

than greybodies or unresolved sources, whether for imagery or for radiometry.

For references to various calibration techniques for radiometers, see Hudson [1],

p. 437 (10-15).

7. Applications of Thermography to Nondestructive Testing

Early 'on, it became apparent that the infrared radiative properties of

matter were exploitable, especially militarily. Thus, heat seeking devices for

searching and tracking were already being proposed in 1910. The desire for new

and improved military capabilities, augmented by monetary support, has been the

impetus and the nurture for infrared technology in general, and thermography in

particular. Modern commercial imaging systems are a modified spillover.

Use of thermography for nondestructive testing dates back several decades.

The main application then, as now, was the qualitative detection and location of

hot spots, indicators of incipient failure. As technology advanced, however, and more sophisticated imaging systems became available, their application to non- destructive testing followed suit, and the realm of work expanded into quantitative determinations, especially important for process control and strength of

materials.

Hudson's [1] section 17.4.1 provides an annotated listing of accessible

published literature, covering the years 1946-1977, dealing with the thermographic application to nondestructive testing and inspection. Many of these

papers deal with electronic applications such as the detection of overheated

components on circuit boards. There are also papers on the detection of

21
del ami nations, voids, undesired inclusions, and cracks in motor casings; bonds;

weldments; anti-icing panels; and thermal insulation. Closely allied with

thermography as a tool for nondestructive testing, inspection, and process

control is radiometry, and Hudson's section 17.2.1 gives an annotated listing of

pertinent references.

The September 1968 issue of Applied Optics [8] is dedicated to nondestructive testing with infrared thermal -imaging devices. Some of the applications

reported there are the same as those of the previous listing; other papers report

on bonding/debonding of aerospace structures, fatigue cracks, coatings and bonds,

lamination/delamination, and incipient failure in power line transformers,

motors, embedded heating elements, and electrical connections. These types of

appl ication persist.

Some of the later published literature is referenced herein [9-22]. Further,

readers may wish to peruse the international journal, NDT, for its research and

development articles on nondestructive testing in general, and for its survey of

published literature and patents.

It is apparent that the remote sensing capabilities of thermography and

radiometry can be used effectively for automatic process control and quality

control, and indeed some companies are doing so. Many accounts of such applications are not made public, however, as they are considered to be proprietary.

Finally, in the usual course of events, one is confronted by a problem for

which a means of solution is then sought. With the modest background in thermography presented herein, an investigator with an appropriate knowledge of an intended target should be able to make a rational judgment concerning the feasibility of applying themography. Some test objectives are simple and require only

a simple instrument (imaging system); others are demanding and require a sophisticated instrument. Further, owing to inaccessibility of adverse targets or extraneous effects, thermographic testing may be complicated, and an alternative

method of testing might be better. Usually, however, in the laboratory at least,

conditions can be established favorable to the execution of simple and direct

nondestructive testing by thermography.

22
8. References

[1

[2

[3

[4

[5

[6

[7

[8

[9

[10

[11

[12

[13

[14

[15

[16

Hudson, R. D., Jr., Infrared System Engineering, Wiley-Interscience,

New York, 1978.

Wormser, E. M. , Sensing the Invisible World, Appl Opt. 7_, 1667; 1968.

Woodmansee, W. E., Aerospace Thermal Mapping Applications of Liquid

Crystals, Appl. Opt. 7, 1721; 1968.

Goodell, J. B. et al . , The Fundamentals of Thermal Imaging Systems,

F. Rosell and G. Harvey, eds., NRL Report 8311, Naval Research Laboratory,

Washington, D.C., pp. 21-48; 1979.

Holter, M. R. et al . , Fundamentals of Infrared Technology, MacMillan Co.,

New York, 1962.

Wolfe, W. L. and Zissis, G. J., eds., The Infrared Handbook, Office of

Naval Research, Dept. of the Navy, Washington, D.C., 1978.

Richmond, J. C. , Errors in Passive Infrared Imaging Systems due to

Reflected Ambient Flux, SPIE 226, p. 110; 1980.

Appl. Opt. 7; 1968.

Rosencwaig, A., Thermal -Wave Microscopy, Solid State Technology,

p. 91; March 1982,

Beatty, K. 0., Jr., and Richardson, F. M. , Transfer Thermography,

Mechanical Engineering, p. 42; October 1981.

Hyzer, W. G. , Thermography, Research/Development, p. 44;

February 1978.

Green, D. R. , Thermal and Infrared Nondestructive Testing of Composites

and Ceramics, Materials Evaluation, Vol. XXIX, No. 11, p, 241,

November 1971

Green, D. R. ; Collingham, R. E.; and Fischer, L. H., Infrared NDT of

Electrical Fuel Pin Simulators Used in LMFBR Thermal Hydraulic Tests,

ibid, p. 247.

Dixon, R. D.; Lassahn, G. D. ; and DiGiallonardo, A., Infrared

Thermography of Subsurface Defects, Materials Evaluation, Vol. XXX,

No. 4, p. 73; April 1972.

Lawrence, W. Thompson; A Thermal Method for Measuring Wall Thickness

and Detection of Incomplete Core Removal in Investment Castings,

Materials Evaluation, Vol. XXIX, No. 5, p. 105, May 1971.

Anon., Non-Destructive Infrared Tire Testing, Rubber Age, April 1971.

23
[17] Conant, F. S. ; Hall, G. L. ; and Walter, J. D. , Surface Temperature of

Running Tires Using Infrared Scanning, Society of Automotive

Engineers, Mid-Year Meeting, Detroit, MI, May 18-22, 1970,

Paper No. 700475.

[18] Hesketh, P. M. , Condition Monitoring & Thermography, British Steel

Corp., Scunthorpe Division.

[19] Bernstein, B., Transmission Substations, Hot Spot Detector,

EPRI Journal, p. 46; November 1981.

[20] Westinghouse Electric Corp., East Pittsburgh, PA. On-Line Monitoring

and Diagnostic Systems for Generators, EPRI NP-902, Final Report;

September 1979.

[21] Thermography in Non-Destructive Testing, The Infrared Observer,

No. 7, 1981, AGA Infrared Systems, AB, Danderyd, Sweden.

[22] Malone, M. S. , Silicon Valley's 'Maternity Ward, New York Times,

March 7, 1982, p. 4F [thermal -wave microscopy].

24
BIBLIOGRAPHY

Books

Goodman, J.W., Introduction to Fourier Optics , McGraw-Hill, New York, 1968,

Fourier optics is basic to a detailed understanding of image

format. This slim text is a readable introduction to the subject,

but a knowledge of the mathematics of Fourier transforms is prerequisite.

Hudson, R.D., Jr., Infrared System Engineering , Wiley-Interscience,

New York, 1969.

The joys of system engineering; "down-to-earth".

LaRocca, A.J. (ed.), Infrared Technology : Fundamentals & Systems

Applications , Engineering summer conference, Univ. of Michigan

College of Engineering, 1982.

An uneven assortment of lecture notes for a one-week "crash

course".

Lloyd, J.M. , Thermal Imaging Systems , Plenum Press, New York, 1975.

A lucid introduction to the technology of thermal imaging.

Marshall, G.F., "Scanning Devices and Systems", Applied Optics and

Optical Engineering , Vol. VI, Kingslake, R., and Thompson, B.J.

(eds. ), Academic Press, New York, 1980.

An introductory chapter on the practical engineering of scanning

systems.

Wolfe, W.L. and Zissis, G.J. (eds.), The Infrared Handbook , Chapter 1,

"Radiation Theory"; Chapter 10, "Optical -Mechanical Scanning

Techniques & Devices"; Chapter 13, "Imaging Tubes"; Chapter 18,

"Displays"; Chapter 19, Imaging Systems", Office of Naval

Research, Washington, D.C., 1978.

An exhaustive compendium makes a useful reference.

25
Periodicals & Reports

AGA staff, "Thermography in Non-Destructive Testing", The Infrared

Observer, AGA Infrared Systems AB, Danderyd, Sweden, No. 7,

1981, p. 3.

Astheimer, R.W. and F. Schwarz, "Thermal Imaging Using Pyroelectric

Detectors", Appl . Opt. 7_, 1968, p. 1687.

Beatty, K.O., Jr., and F.M. Richardson, "Transfer Thermography",

Mechanical Engineering, October 1981, p. 42.

Bernstein, B., "Transmission Substations, Hot Spot Detector",

EPRI Journal, November 1981, p. 46.

Borg, S., "Thermal Imaging with Real Time Picture Presentation",

Appl. Opt. 7, 1968, p. 1697.

Conant, F.S. et al . , "Surface Temperature of Running Tires Using

Infrared Scanning", Society of Automotive Engineers, Mid-year

Meeting, Detroit, MI, May 18-22, 1970, Paper No. 700475.

Dixon, R.D. et al . , "Infrared Thermography of Subsurface Defects",

Materials Evaluation, Vol. XXX, No. 4, April 1972, p. 73.

Goodel i , J.B. et al . , "The Fundamentals of Thermal Imaging Systems",

F. Rossell and G. Harvey (eds.), NRL Report 8311, Naval

Research Laboratory, Washington, D.C., 1979.

Green, D.R. , "Thermal and Infrared Non-destructive Testing of

Composites and Ceramics", Materials Evaluation, Vol. XXIX,

No. 11, November 1971, p. 241.

Green, D.R. et al . , "Infrared NDT of Electrical Fuel Pin Simulators

Used in LMFBR Thermal Hydraulic Tests", ibid, p. 247.

Griffin, D.D., "Infrared Techniques for Measuring Temperature and

Related Phenomena of Microcircuits", Appl. Opt. 7_, 1968, p. 1749.

Hesketh, P.M., "Condition Monitoring & Thermography", British Steel

Corp., Scunthorpe Division.

Hyzer, W.G., "Thermography", Research/Development, February 1978, p. 44.

Kubiak, E.J., "Infrared Detection of Fatigue Cracks and Other Near

Surface Defects", Appl. Opt. 7, 1968, p. 1743.

Kutzcher, E.W. and K. H. Zimmerman, "A Scanning Infrared Inspection

System Applied to Nondestructive Testing of Bonded Aerospace

Struct res", ibid, p. 1715.

Lawrence, W.T., "A Thermal Method for Measuring Wall Thickness and

Detection of Incomplete Core Removal in Investment Castings",

Materials Evaluation, Vol. XXIX, No. 5, May 1971, p. 105.

26
Leftwich, R.F. and G. B. Ordway, "Unusual Applications of Infrared

Nondestructive Testing", Appl . Opt. 7, 1968, p. 1853.

Malone, M.S., "Silicon Valley's Maternity Ward", [thermal -wave microscopy], N.Y. Times, March 7, 1982, p. 4F.

Myers, V.I. and W.A. Allen, "Electro-optical Remote Sensing Methods

as Nondestructive Testing and Measuring Techniques in Agriculture",

Appl. Opt. 7, 1968, 1819.

Richmond, J.C., "Errors in Passive Infrared Imaging Systems due to

Reflected Ambient Flux", SPIE, Vol. 26, 1980, p. 110.

Rosencwaig, A., "Thermal -Wave Microscopy", Solid State Technology,

March 1982, p. 91.

Rubber Age Staff, "Non-destructive Infrared Tire Testing", April 1971.

Vogel , P.E.J. , "Evaluation of Bonds in Armor Plate and Other

Materials Using Infrared Nondestructive Testing Techniques",

Appl. Opt. 7, 1968, p. 1739.

Westinghouse Electric Corp. staff, "On-Line Monitoring and Diagnostic

Systems for Generators", EPRI NP-902, Final Report, East

Pittsburgh, PA, September 1979.

Woodmansee, W.E., "Aerospace Thermal Mapping Applications of Liquid

Crystals", Appl. Opt. 7, 1968, p. 1721.

Wormser, E.M., "Sensing the Invisible World", ibid, p. 1968.

Yoder, J.R. , "Temperature Measurement with an Infrared Microscope",

ibid, p. 1791.

27
EPILOGUE

The demands by the military and industrial sectors for new or improved

capabilities are giving rise to rapid expansion of thermal -imaging system technology. Military needs for improved imagery, amply supported, are expected to

result in replacement of discrete detector arrays by monolithic charge coupled

devices (CCD), and to detector materials with broader spectral response capabilities; these improvements should ultimately enter the civilian market. In industry, the application of thermography to plant monitoring (preventive maintenance), process control, robotics, and nondestructive testing is widespread and

growing rapidly as increasing numbers of industries and plants are recognizing

both the capabilities and the cost benefits to be derived. Although qualitative

thermography--the detection of thermal gradients or hot spots--is still the usual

industrial requirement, there is increasing demand for quantitative thermography--

the size and location of defects—as well as for the accurate determination of

temperature, especially for process control where temperature is a critical

parameter.

This introductory work is a simplified treatment of a subject which can be

highly complex and esoteric. The report has aimed to familiarize the reader with

the broad aspects of thermography and to make him aware of various factors which

may have to be considered in the application of thermography. On the other hand,

this report does not attempt to solve the various problems which can ariseindeed, this would require a major work of encyclopedic dimensions—and the

enterprise must reside with the needful reader. Those who intend to pursue

thermography as a career or require additional information might initially

consult the references and bibliography given herein.

28
NBS-114A IREV. 2-8C) U.S. DEPT. OF COMM. BIBLIOGRAPHIC DATA

SHEET (See instructions)

1. PUBLICATION OR

REPORT NO. NBS TO 1177

2. Performing Organ. Report No 3. Publication Date

May 1983

4. TITLE AND SUBTITLE

Elements of Thermography for Nondestructive Testing

5. AUTHOR(S)

Julius Cohen

6. PERFORMING ORGANIZATION (if joint or other than NBS. see instructions)

NATIONAL BUREAU OF STANDARDS

DEPARTMENT OF COMMERCE

WASHINGTON, D.C. 20234

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Final

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J] Document describes a computer program; SF-185, FIPS Software Summary, is attached.

11. ABSTRACT (A 200-word or less factual summary of most significant information. If document includes a significant

bibliography or literature survey, mention it here)

This paper presents an elementary review of thermal imaging systems, with

emphasis on the application of thermography to nondestructive testing. Topics

discussed include heat radiation theory; early and contemporary thermal imaging

systems; performance characteristics; effects of emissivity, background temperature, atmosphere, and field of view. Examples of various applications of

thermography to nondestructive testing are given. A bibliography is included.

12. KEY WORDS (Six to twelve entries; alphabetical order; capitalize only proper names; and separate key words by semicolons)

heat; imagery; infrared; nondestructive testing; passive;

radiation; remote sensing; temperature; thermography.

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characteristics of the products. NBS administers this program as a supplement to the activities of the private sector standardizing

organizations. Consumer Information Series—Practical information, based on N BS research and experience, covering areas of interest to the con- sumer. Easily understandable language and illustrations provide

useful background knowledge for shopping in today's technological marketplace. Order the above NBS publications from: Superintendent of Documents. Government Printing Office, Washington. DC 20402. Order the following NBS publications—FlPS and NBSIR's—from

the National Technical Information Service. Springfield. VA 22161.

Federal Information Processing Standards Publications (FIPS

PUB)—Publications in this series collectively constitute the Federal Information Processing Standards Register. The Register

serves as the official source of information in the Federal Govern- ment regarding standards issued by NBS pursuant to the Federal Property and Administrative Services Act of 1949 as amended.

Public Law 89-306 (79 Stat. 1127), and as implemented by Executive Order 11717(38 FR 1 23 1 5, dated May 11, 1973) and Part 6

of Title 15 CFR (Code of Federal Regulations).

NBS Interagency Reports (NBSIR)—A special series of interim or

final reports on work performed by NBS for outside sponsors

(both government and non-government). In general, initial dis- tribution is handled by the sponsor; public distribution is by the National Technical Information Service , Springfield, VA 22161,

in paper copy or microfiche form.
U.S. Department of Commerce

National Bureau of Standards

Washington, D.C. 20234

Official Business

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