# Patent

## Title
Method and apparatus for the detection of high pressure conditions in a vacuum-type electrical device

## Abstract

A method for detecting a high pressure condition within a high voltage vacuum device includes detecting the position of a movable structure such as a bellows. The position at high pressures can be detected optically by the interruption of a light beam reflected by a hemispherically shaped reflector. The hemispherical reflector allows the source light fiber to oriented parallel to the detection light fiber, providing a more compact and efficient fiber routing.

## Background
CROSS REFERENCE TO RELATED APPLICATIONS
This application is a continuation of non-provisional application Ser. No. 11/504,138 filed Aug. 14, 2006, now U.S. Pat. No. 7,313,964 entitled METHOD AND APPARATUS FOR THE DETECTION OF HIGH PRESSURE CONDITIONS IN A VACUUM-TYPE ELECTRICAL DEVICE, which is a continuation in part of non-provisional application Ser. No. 11/305,081 filed Dec. 16, 2005, now U.S. Pat. No. 7,302,854 entitled METHOD AND APPARATUS FOR THE DETECTION OF HIGH PRESSURE CONDITIONS IN A VACUUM-TYPE ELECTRICAL DEVICE, which is a continuation in part of non-provisional application Ser. No. 10/848,874 filed May 18, 2004, now U.S. Pat. No. 7,225,676 entitled METHOD AND APPARATUS FOR THE DETECTION OF HIGH PRESSURE CONDITIONS IN A VACUUM SWITCHING DEVICE, and claims benefit thereof. The aforementioned applications are herein incorporated by reference in their entirety.


BACKGROUND OF THE INVENTION
1. Field of the Invention.
This invention relates to detection of failure conditions in high power electrical switching devices, particularly to the detection of high pressure conditions in high voltage vacuum interrupters, switches, and capacitors.
2. Description of the Related Art
The reliability of the North American power grid has come under critical scrutiny in the past few years, particularly as demand for electrical power by consumers and industry has increased. Failure of a single component in the grid can cause catastrophic power outages that cascade throughout the system. One of the essential components utilized in the power grid are the mechanical switches used to turn on and off the flow of high current, high voltage AC power. Although semiconductor devices are making some progress in this application, the combination of very high voltages and currents still make the mechanical switch the preferred device for this application.
There are basically three common configurations for these high power mechanical switches; oil filled, gas filled, and vacuum. These switches are also known as interrupters. The oil filled switch utilizes contacts immersed in a hydrocarbon based fluid having a high dielectric strength. This high dielectric strength is required to withstand the arcing potential at the switching contacts as they open to interrupt the circuit. Due to the high voltage service conditions, periodic replacement of the oil is required to avoid explosive gas formation that occurs during breakdown of the oil. The periodic service requires that the circuits be shut down, which can be inconvenient and expensive. The hydrocarbon oils can be toxic and can create serious environmental hazards if they are spilled into the environment. Gas filled versions utilize SF6 at pressures above 1 atmosphere absolute. Leaks of SF6 into the environment are not desirable, which makes use of the gas filled interrupters less attractive as well. If an SF6 filled interrupter fails due to leakage, the resulting arc can generate an over pressure condition, or explosive byproducts which can cause breach of containment and severe local contamination. Another configuration utilizes a vacuum environment around the switching contacts. Arcing and damage to the switching contacts can be avoided if the pressure surrounding the switching contacts is low enough. Loss of vacuum in this type of interrupter will create serious arcing between the contacts as they switch the load, destroying the switch. In some applications, the vacuum interrupters are stationed on standby for long periods of time. A loss of vacuum may not be detected until they are placed into service, which results in immediate failure of the switch at a time when its most needed. It therefore would be of interest to know in advance if the vacuum within the interrupter is degrading, before a switch failure due to contact arcing occurs. Currently, these devices are packaged in a manner that makes inspection difficult and expensive. Inspection may require that power be removed from the circuit connected to the device, which may not be possible. It would be desirable to remotely measure the status of the pressure within the switch, so that no direct inspection is required. It would also be desirable to periodically monitor the pressure within the switch while the switch is in service and at operating potential.
Perhaps at first blush it may appear that measurement of pressure within the vacuum envelope of these interrupter devices would be adequately covered by devices of the prior art, but the reality of the circumstances under which these devices operate has made a practical solution of this problem difficult to achieve prior to this invention. A main factor in this regard is that the device is used for controlling high AC voltages, with potentials between 7 and 100 kilovolts above ground, and extremely high currents. This makes application of prior art pressure measuring devices very difficult and expensive. Due to cost and safety constraints, complex high voltage isolation techniques of the prior art are not suitable. What is needed is a practical method and apparatus to safely and inexpensively measure a high pressure condition in a high voltage vacuum device, such as an interrupter, preferably remote from the device, and preferably while the device is at operating potential. It would be of further interest to be able to monitor the pressure status of these vacuum devices while they are powered down, on standby, or in storage prior to use.
FIG. 1 is a cross sectional view 100 of a first example of a vacuum interrupter of the prior art. This particular unit is manufactured by Jennings Technology of San Jose, Calif. Contacts 102 and 104 are responsible for the switching function. A vacuum, usually below 10−4 torr, is present near the contacts in region 114 and within the envelope enclosed by cap 108, cap 110, bellows 112, and insulator sleeve 106. Bellows 112 allows movement of contact 104 relative to stationary contact 102, to make or break the electrical connection.
FIG. 2 is a cross sectional view 200 of a second example of a vacuum interrupter of the prior art. This unit is also manufactured by Jennings Technology of San Jose, Calif. In this embodiment of the prior art, contacts 202 and 204 perform the switching function. A vacuum, usually below 10−4 torr, is present near the contacts in region 214 and within the envelope enclosed by cap 208, cap 210, bellows 212, and insulator sleeve 206. Bellows 112 allows movement of contact 202 relative to stationary contact 204, to make or break the electrical connection.
SUMMARY OF THE INVENTION
It is an object of the present invention to provide a method for detecting a high pressure condition within a high voltage vacuum device, including providing a gas tight envelope for containing gas pressure within the high voltage vacuum device; providing a collapsible device, enclosed within the gas tight envelope, having a first surface and a second surface, the first surface fixed relative to the gas tight envelope, the second surface movable relative to the first surface with an increase in the gas pressure within the gas tight envelope; and, providing a shaft, having a first end and a second end, the first end attached to the second surface of the collapsible device. The method further includes transmitting an optical beam to a first location on a hemispherically shaped reflecting surface; reflecting a portion of the optical beam from the first location to a second location on the hemispherically shaped reflecting surface; blocking the portion of the optical beam being reflected from the first location to the second location with a portion of the shaft, at said high pressure condition; and, providing an output responsive to blocking a portion of the optical beam.
It is another object of the present invention to provide an apparatus for detecting high pressure within a high voltage vacuum device, including a gas tight envelope for containing the gas pressure within the high voltage vacuum device, the gas pressure defining a vacuum pressure condition; a collapsible device, enclosed within the high voltage vacuum device, having a first surface and a second surface, the first surface fixed relative to the high voltage vacuum device, the second surface movable relative to the first surface with an increase in the gas pressure within the high voltage vacuum device; a shaft, having a first end and a second end, the first end attached to the second surface of the collapsible device; a sensor for detecting the position of the second end of the shaft; and, electrical contacts located within the gas tight envelope, mounted for relative movement between a first position in which the electrical contacts are positioned closely adjacent, and a second position in which the electrical contacts are spaced apart from each other, with the vacuum pressure condition in the high voltage vacuum device preventing electrical arcing between the electrical contacts when they are moved between the first and second positions, wherein movement of the shaft is independent of movement of the electrical contacts between first and second positions.
It is yet another object of the present invention to provide a vacuum bottle-type electrical device with a vacuum pressure loss detection feature including a bottle defining a vacuum pressure condition at the interior of the bottle; electrical charge members in the bottle mounted for relative movement between a first position in which the electrical charge members are positioned closely adjacent and a second position in which the electrical charge members are spaced apart from each other, with the vacuum pressure condition in the bottle preventing electrical arcing between the electrical charge members when they are moved between their first and second positions at voltage potentials in excess of 1000V; a first optical cable, positioned to transmit an optical beam to a first location on a hemispherically shaped reflective surface; a second optical cable, positioned to receive at least a portion of the optical beam transmitted from the first optical cable, reflected from a second location on the hemispherically shaped reflective surface; a collapsible device, enclosed within the bottle, having a first surface and a second surface, said first surface fixed relative to the bottle, the second surface movable relative to the first surface with an increase in gas pressure within the bottle; a shaft, having a first end and a second end, the first end attached to the second surface of the collapsible device, wherein the second end of the shaft extends through an aperture in the hemispherically shaped reflective surface, the aperture being located between the first location and the second location, the shaft operative to block at least a portion of the optical beam reflected from the first location to the second location at a loss of vacuum pressure within the vacuum bottle-type electrical device.



BRIEF DESCRIPTION OF THE DRAWINGS
The present invention will be better understood when consideration is given to the following detailed description thereof. Such description makes reference to the annexed drawings, wherein:
FIG. 1 is a cross sectional view of a first example of a vacuum interrupter of the prior art;
FIG. 2 is a cross sectional view of a second example of a vacuum interrupter of the prior art;
FIG. 3 is a partial cross sectional view of a device for detecting arcing contacts according to an embodiment of the present invention;
FIG. 4 is a partial cross sectional view of a cylinder actuated optical pressure switch in the low pressure state, according to an embodiment of the present invention;
FIG. 5 is a partial cross sectional view of a cylinder actuated optical pressure switch in the high pressure state, according to an embodiment of the present invention;
FIG. 6 is a partial cross sectional view of a bellows actuated optical pressure switch in the low pressure state, according to an embodiment of the present invention;
FIG. 7 is a partial cross sectional view of a bellows actuated optical pressure switch in the high pressure state, according to an embodiment of the present invention;
FIG. 8 is a partial cross sectional view of an optical device for detecting sputtered debris from the electrical contacts, according to an embodiment of the present invention;
FIG. 9 is a partial cross sectional view of a self powered, optical transmission microcircuit, according to an embodiment of the present invention;
FIG. 10 is a partial cross sectional view of a self powered, RF transmission microcircuit, according to an embodiment of the present invention;
FIG. 11 is a schematic view of a diaphragm actuated optical pressure switch in the low pressure state, according to an embodiment of the present invention;
FIG. 12 is a schematic view of a diaphragm actuated optical pressure switch in the high pressure state, according to an embodiment of the present invention;
FIG. 13 is a partial cross sectional view of a high voltage vacuum switch with an externally mounted pressure sensing bellows and a transmission optical detector, according to an embodiment of the present invention;
FIG. 14 is a partial cross sectional view of a high voltage vacuum switch with an externally mounted pressure sensing bellows and a reflective optical detector, according to an embodiment of the present invention;
FIG. 15 is a partial cross sectional view of a high voltage vacuum switch with an externally mounted pressure sensing bellows and a contact closure sensing microcircuit, according to an embodiment of the present invention;
FIG. 16 is a partial cross sectional view of a high voltage vacuum switch with an externally mounted pressure measuring chamber and a contact closure sensing microcircuit, at low pressure, according to an embodiment of the present invention;
FIG. 17 is a partial cross sectional view of a high voltage vacuum switch with an externally mounted pressure measuring chamber and a contact closure sensing microcircuit, at high pressure, according to an embodiment of the present invention;
FIG. 18 is a schematic cross sectional view of a hemispherically shaped reflector for optical detection of a high pressure condition in a high voltage device, according to an embodiment of the present invention;
FIG. 19 is a schematic cross sectional view of a hemispherically shaped reflector showing a ray trace analysis for narrow optical beam widths, according to an embodiment of the present invention;
FIG. 20 is a schematic cross sectional view of a hemispherically shaped reflector showing a ray trace analysis for broad optical beam widths, according to an embodiment of the present invention:
FIG. 21 is a partial cross sectional view of an externally located bellows pressure detection device coupled to a hemispherically shaped optical reflector, at a low pressure condition, according to an embodiment of the present invention;
FIG. 22 is a partial cross sectional view of an externally located bellows pressure detection device coupled to a hemispherically shaped optical reflector, at a high pressure condition, according to an embodiment of the present invention;
FIG. 23 is a partial cross sectional view of a high voltage switching module, according to an embodiment of the present invention;
FIG. 24 is a partial cross sectional view of a vacuum interrupter module and a bellows actuated pressure sensing device coupled to a hemispherical optical detector assembly, according to an embodiment of the present invention;
FIG. 25 is a partial cross sectional view of a bellows actuated pressure sensing device coupled to a hemispherical optical detector assembly of FIGS. 23 and 24, according to an embodiment of the present invention;
FIG. 26 is a partial cross sectional view of a cylinder actuated pressure detection device coupled to a hemispherically shaped optical reflector, at a low pressure condition, according to an embodiment of the present invention;
FIG. 27 is a partial cross sectional view of a cylinder actuated pressure detection device coupled to a hemispherically shaped optical reflector, at a high pressure condition, according to an embodiment of the present invention;
FIG. 28 is a partial cross sectional view of an internally located bellows pressure detection device coupled to a hemispherically shaped optical reflector, at a low pressure condition, according to an embodiment of the present invention; and,
FIG. 29 is a partial cross sectional view of an externally located bellows pressure detection device coupled to a hemispherically shaped optical reflector, at a high pressure condition, according to an embodiment of the present invention.



DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
The present invention is directed toward providing methods and apparatus for the measurement of pressure within a high voltage, vacuum interrupter. In this disclosure, the terms “vacuum interrupter” and “high voltage vacuum switch” are synonymous. In common usage, the term “vacuum interrupter” may imply a particular type of switch or application. Those limitations do not bear upon embodiments of the present invention, as the disclosed embodiments of the present invention may be applied to any high voltage device utilizing internal gas pressures below 1 atm (absolute) as an aid to insulating opposing high voltage potentials. “High voltages” are AC (alternating current) voltages preferably greater than 1000 volts, and more preferably greater than 5000 volts. As an example, various embodiments described subsequently are employed with or within the interrupter shown in FIG. 1. This by no means implies that the inventive embodiments are limited in application to this interrupter configuration only, as the illustrated embodiments of the present invention are equally applicable to the device shown in FIG. 2 or any similar device such as high voltage, vacuum insulated capacitors, for example.
FIG. 3 is a partial cross sectional view 300 of a device for detecting arcing contacts according to an embodiment of the present invention. As the pressure in region 114 rises, arcing between contacts 104 and 102 will occur, due to the ionization of the gasses creating the increased pressure. An electrically isolated photo detector 310 is employed to observe the emitted light 304 generated in gap 306 as contacts 104 and 102 separate. Photo detector 310 may be a solid state photo diode or photo transistor type detector, or may be a photo-multiplier tube type detector. Due to cost considerations, a solid state device is preferred. The photo detector 310 is coupled to control and interface circuitry 312, which contains the necessary components (including computer processors, memory, analog amplifiers, analog to digital converters, or other required circuitry) needed to convert the signals from photo detector 310 to useful information. Photo detector 310 is optically coupled to a transparent window 302 by means of a fiber optic cable 308. Cable 308 provides the required physical and electrical isolation from the high operating voltage of the interrupter. Generally, cable 308 is comprised of an optically transparent glass, plastic or ceramic material, and is non-conductive. Window 302 is mounted in the enclosure for the interrupter, preferably in the insulator sleeve 106. Window 302 may also be mounted in the caps (for example 108) if convenient or required. Window 302 is made from an optically transparent material, including, but not limited to glass, quartz, plastics, or ceramics. Although not illustrated, it may be desirable to couple multiple cables 308 into a single photo detector 310 to monitor, for example, the status of any of three interrupters in a three phase contactor. Likewise, it may also be desirable to couple three photo detectors 310, each having a separate cable 308, into a single control unit 312. One advantage of the present embodiment, is that both the control unit 312 and/or photo detector 310 may be remotely located from the interrupter. This allows convenient monitoring of the interrupter without having to remove power from the circuit. It should be noted that elements 308, 310, and 312 are not to scale relative to the other elements in the figure.
Although the measurement of light 304 produced by the arcing of contacts 102, 104 is an indirect measurement of pressure in region 114, it is nonetheless a direct observation of the mechanism that produces failure within the interrupter. At sufficiently low pressure, no significant contact arcing will be observed because the background partial pressure will not support ionization of the residual gas. As the pressure rises, light generation from arcing will increase. Photo detector 310 may observe the intensity, frequency (color), and/or duration of the light emitted from the arcing contacts. Correlation between data generated by contact arcing under known pressure conditions can be used to develop a “trigger level” or alarm condition. Observed data generated by photo detector 310 may be compared to reference data stored in controller 312 to generate the alarm condition. Each of the characteristics of light intensity, light color, waveform shape, and duration may be used, alone or in combination, to indicate a fault condition. Alternatively, data generated from first principles of plasma physics may also be used as reference data.
FIG. 4 is a partial cross sectional view 400 of a cylinder actuated optical pressure switch 404 in the low pressure state, according to an embodiment of the present invention. FIG. 5 is a partial cross sectional view 500 of a cylinder actuated optical pressure switch 404 in the high pressure state, according to an embodiment of the present invention. In these embodiments, a pressure sensing cylinder device 404 comprises a piston 406 coupled to spring 410. Chamber 408 is fluidically coupled to the interior of interrupter 402 for sensing the pressure in region 416. A shaft 412 is attached to piston 406. Attached to shaft 412 is a reflective device 414, which may any surface suitable for returning at least a portion of the light beam emitted from optic cable 418 to optic cable 420. At low pressure, shaft 412 is retracted within cylinder 404, tensioning spring 410, as is shown in FIG. 4. Fiber optic cables 418 and 420, in concert with photo emitter 422, photo detector 424, and control unit 426, detect the position of shaft 412. At high pressure, spring 410 extends shaft 412 to a position where reflective device 414 intercepts a light beam originating from fiber optic cable 418 (via photo emitter 422), sending a reflected beam back to photo detector 424 via cable 420. An alarm condition is generated when photo detector 424 receives a signal, indicating a high pressure condition in interrupter 402. The pressure at which shaft 412 is extended to intercept the light beam is determined by the cross sectional area of piston 406 relative to the spring constant of spring 410. A stiffer spring will create an alarm condition at a lower pressure. Fiber optic cables 418 and 420 provide the necessary electrical isolation for the circuitry in devices 422-426. While the previous embodiments have shown the fiber optic cables transmitting and detecting a reflected beam, it should be evident that a similar arrangement can be utilized whereby the ends of each optical cable 418 and 420 oppose each other. In this case, the end of shaft 412 is inserted between the two cables, blocking the beam, when in the extended position. An alarm condition is generated when the beam is blocked.
FIG. 6 is a partial cross sectional view 600 of a bellows actuated optical pressure switch in the low pressure state, according to an embodiment of the present invention. FIG. 7 is a partial cross sectional view of a bellows actuated optical pressure switch in the high pressure state, according to an embodiment of the present invention. Bellows 602 is mounted within interrupter 402, and is sealed against the inside wall of the interrupter such that a vacuum seal for the interior of the interrupter 402 is maintained. The inside volume 604 of the bellows is in fluid communication with the atmospheric pressure outside the interrupter. This can be accomplished by providing a large clearance around shaft 606 or an additional passage from the interior of the bellows 602 through the exterior wall of the interrupter (not shown). Bellows 602 is fabricated in such a manner as to be in the collapsed position shown in FIG. 7 when the pressure inside the bellows is equal to the pressure outside the bellows. When a vacuum is drawn outside the bellows, the bellows is extended toward the interior of region 416 of interrupter 420. At the alarm (high) pressure condition shown in FIG. 7, shaft 606 is extended, placing reflective device 608 in a position to intercept a light beam from cable 418, and reflect a least a portion of the beam back through cable 420 to detector 424. The “stiffness” of the bellows relative to its diameter, determines the alarm pressure level. A stiffer bellows material will result in a lower alarm pressure level. Fiber optic cables 418 and 420 provide the necessary electrical isolation for the circuitry in devices 422-426. While the previous embodiments have shown the fiber optic cables transmitting and detecting a reflected beam, it should be evident that a similar arrangement can be utilized whereby the ends of each optical cable 418 and 420 oppose each other. In this case, the end of shaft 606 is inserted between the two cables, blocking the beam, when in the extended position. An alarm condition is generated when the beam is blocked.
FIG. 8 is a partial cross sectional view 800 of an optical device for detecting sputtered debris from the electrical contacts, according to an embodiment of the present invention. As the pressure increases inside the interrupter, arcing will occur in gap 306 between contacts 102 and 104. The arcing will “sputter” material from the contact surfaces, depositing this material on various interior surfaces. In particular, sputter debris will be deposited on surface 802, and on window 302 interior surface 808. A light beam emitted from optic cable 418 is transmitted through window 302 to reflective surface 802. Reflective surface 802 returns a portion of the beam to optic cable 420. The amount of sputtered debris on window surface 808 will determine the degree of attenuation of the light beam 806. If the beam is attenuated below a certain amount, an alarm is generated by control unit 426. Additionally, sputter debris may also cloud reflective surface 802, resulting in further beam attenuation. Ports 804 are placed in the vicinity of window 302, to aid in transporting any sputtered material to the window surface. This embodiment has the capability of providing a continuous monitoring function for detecting slow degradation of the vacuum inside the interrupter. Beam intensity can be continuously monitored and reported via controller 426, in order to schedule preventative maintenance as vacuum conditions inside the interrupter worsen.
FIG. 9 is a partial cross sectional view 900 of a self powered, optical transmission microcircuit 902, according to an embodiment of the present invention. Microcircuit 902 contains a substrate 904, a photo transmission device 906, a pressure measurement component 908, amplifier and logic circuitry 910, and an inductive power supply 912. Microcircuit 902 can be a monolithic silicon integrated circuit; a hybrid integrated circuit having a ceramic substrate and a plurality of silicon integrated circuits, discrete components, and interconnects thereon; or a printed circuit board based device. The pressure within the interrupter in regions 114 and 114′ are measured by a monolithic pressure transducer 908, interconnected to the circuitry on substrate 904. Amplifier and logic circuitry 910 convert signal information from the pressure transducer 908 for transmission by optical emitter device 906. The optical transmission from device 906 is delivered through window 302 to control unit 426 via optical cable 420, situated outside the interrupter. The optical transmission can be either analog or digital, preferably digital. Microcircuit 902 can deliver continuous pressure information, high pressure alarm information, or both. The inductive power supply 912 obtains its power from the oscillating magnetic fields within the interrupter. This is accomplished by placing a conductor loop (not shown) on substrate 904, then rectifying and filtering the induced AC voltage obtained from the conductor loop. Photo transmission device 906 can be a light emitting diode or laser diode, as is known to those skilled in the art. Construction of the components on substrate 904 can be monolithic or hybrid in nature. Since none of the circuitry in device 902 is referenced to ground, high voltage isolation is not required. High voltage isolation for devices 424, 426 is provided by optical cable 420, as described in previous embodiments of the present invention.
FIG. 10 is a partial cross sectional view 1000 of a self powered, RF transmission microcircuit 1002, according to an embodiment of the present invention. Microcircuit 1002 contains a substrate 1004; a pressure measurement component 1006; amplifier, logic, and RF transmission circuitry 1008; and an inductive power supply 1010. Microcircuit 1002 can be a monolithic silicon integrated circuit; a hybrid integrated circuit having a ceramic substrate and a plurality of silicon integrated circuits, discrete components, and interconnects thereon; or a printed circuit board based device. The pressure within the interrupter in regions 114 and 114′ are measured by a monolithic pressure transducer 1006, interconnected to the circuitry on substrate 1004. Amplifier and logic circuitry convert signal information from the pressure transducer 1006 for transmission by an RF transmitter integrated within circuitry 1008. The RF transmission from device 906 is delivered through insulator 106 to receiver unit 1014, situated outside the interrupter. Various protocols and methods are suitable for RF transmission from integrated circuitry, as are well known to those skilled in the art. For purposes of this disclosure, RF transmission includes microwave and millimeter wave transmission. Receiver unit 1014 may be located at any convenient distance from the interrupter, within range of the transmitter contained within microcircuit 1002. Receiver unit may set up to monitor the transmissions from one or a plurality of microcircuits resident in multiple interrupter devices. Unit 1014 contains the necessary processors, memory, analog circuitry, an interface circuitry to monitor transmissions and issues alarms and other information as required. The inductive power supply 1010 obtains its power from the oscillating magnetic fields within the interrupter. This is accomplished by placing a conductor loop (not shown) on substrate 1004, then rectifying and filtering the induced AC voltage obtained from the conductor loop.
FIG. 11 is a schematic view 1100 of a diaphragm actuated optical pressure switch in the low pressure state, according to an embodiment of the present invention. FIG. 12 is a schematic view 1200 of a diaphragm actuated optical pressure switch in the high pressure state, according to an embodiment of the present invention. A low cost alternative embodiment for detecting high pressures within the interrupter can be obtained through use of a diaphragm 1101. Diaphragm 1101 is fixed to structure 1104, which is generally hollow and tubular in shape. Structure 1104 is in turn fastened to a portion of interrupter segment 1106. Alternatively, diaphragm 1101 could be attached directly to an outer surface of the interrupter, if convenient. Due to the fragile nature of the thin dome material, structure 1104 acts as a weld or braze interface to the thicker metal structure of the interrupter. Possibly, structure 1104 could be brazed to a port in the insulator section (for example, ref 106 in prior figures) as well. At low pressures inside the interrupter, dome 1101 would reside in the collapsed position, as shown in FIG. 11. At high pressure, dome 1101 would be in the extended position of FIG. 12. The pressures at which the dome transitions from the collapsed position to the extended position would be within the range of 2 to 14.7 psia, preferably between 2 and 7 psia. The dome position is detected by components 418-426. In the low pressure state, the collapsed dome produces a relatively flat surface 1102. A light beam generated by emitter device 422 is transmitted to surface 1102 via optical cable 418. A reflected beam is returned from surface 1102 to optical detector device 424 via optical cable 420. At a high pressure condition, the dome snaps into an approximately hemispherical expanded shape, having significant curvature in its surface 1202. This curvature deflects the light beam emitted from the end of optical cable 418 away from the receiving end of cable 420, causing a loss of signal at detector 424, and generating an alarm condition within the circuitry of device 426. It is also be possible to reverse the logic by using optical cables 418 and 420 to detect the near proximity of the dome in its extended position, creating a loss of signal when its pulled down into an approximately flat position. Alternatively, the position of the dome may be detected by a mechanical shaft (not shown) placed in contact with the dome's outer surface, the opposite end of the shaft intercepting and optical beam as is shown in the embodiments of FIGS. 4-7.
FIG. 13 is a partial cross sectional view 1300 of a high voltage vacuum switch 1301 with an externally mounted pressure sensing bellows 1306 and a transmission optical detector, according to an embodiment of the present invention. This embodiment allows the measurement of a high pressure condition (or loss of vacuum) utilizing an externally mounted bellows container 1306, which is in fluid communication with the internal pressure of vacuum switch 1301 via connecting tube 1302. Bellows container 1306 is designed to be extended in length at higher internal pressures, and contracted in length at low internal pressures. The spring force required for the extension of the bellows may be provided by springs situated inside or external to bellows 1306 (not shown), and attached to the bellows by methods known to those skilled in the art. Preferably, the bellows container 1306 is constructed in a manner wherein the extension spring force is built in to the bellows container's wall structure, either by the material chosen or by method of fabrication, or both. Optionally, the extension of bellows container 1306 may be tuned or modified by the addition of external springs, directed to enhance or oppose the extension, so as to optimize the response for a specific vacuum switch pressure range, or to compensate for various atmospheric pressure conditions (not shown). Bellows container 1306 may be constructed of any suitable gas impermeable material, including plastics, glass, quartz, and metals. Preferably, metals are used. More preferably, stainless steel alloy 321 or alloys of nickel are used. Alignment device 1304 aids in housing bellows container 1306 and provides support for attachment of optical transmission devices 1312 and 1308. Optical transmission devices 1312 and 1308 are preferably fiber optic cable, constructed of dielectric materials such as plastic, ceramic, or glass, or their combination. Structure 1310, affixed to one end of bellows container 1306, moves in response to the extension of bellows 1306. At low pressures (high vacuum) inside switch 1301, bellows container 1306 is in a compressed (non-extended) state, wherein structure 1310 is positioned such that the optical path between transmission devices 1312 and 1308 is unobstructed, allowing transmission of a light beam there between. At high pressures (low vacuum), bellows container 1306 is extended in length, moving structure 1310 into the light path between transmission devices 1312 and 1308, blocking or attenuating the light beam. The detection of the blocked light beam may be provided by, for example, photo emitter 422, photo detector 424, and control unit 426 (not shown) in embodiments previously disclosed.
FIG. 14 is a partial cross sectional view 1400 of a high voltage vacuum switch 1301 with an externally mounted pressure sensing bellows 1306 and a reflective optical detector, according to an embodiment of the present invention. Optical transmission devices 1402 and 1404 are mounted in alignment device 1304. In this particular embodiment, structure 1310 comprises a reflective surface 1406. When bellows 1306 is extended at a high pressure condition, reflective surface 1406 is placed in a position to reflect a light beam emanating from one optical transmission device (for example, 1402) into the other optical transmission device (for example, 1404). The detection of the transmitted light beam between devices 1402 and 1404 may be provided by, for example, photo emitter 422, photo detector 424, and control unit 426 (not shown) in embodiments previously disclosed. Optical transmission devices 1402 and 1404 are preferably fiber optic cable, constructed of dielectric materials such as plastic, ceramic, or glass, or their combination.
FIG. 15 is a partial cross sectional view 1500 of a high voltage vacuum switch with an externally mounted pressure sensing bellows 1506 and a contact closure sensing microcircuit 1514, according to an embodiment of the present invention. Bellows container 1506 is designed to be extended in length at higher internal pressures, and contracted in length at low internal pressures. The spring force required for the extension of the bellows may be provided by springs situated inside or external to bellows 1506 (not shown), and attached to the bellows by methods known to those skilled in the art. Preferably, the bellows container 1506 is constructed in a manner wherein the extension spring force is built in to the bellows container's wall structure, either by the material chosen or by method of fabrication, or both. Optionally, the extension of bellows container 1506 may be tuned or modified by the addition of external springs, directed to enhance or oppose the extension, so as to optimize the response for a specific vacuum switch pressure range, or to compensate for various atmospheric pressure conditions (not shown). Bellows container 1506 may be constructed of any suitable gas impermeable material, including plastics, glass, quartz, and metals. Preferably, metals are used. More preferably, stainless steel alloy 321 or alloys of nickel are used. Alignment device 1504 aids in housing bellows 1506 and provides support for attachment of microcircuit 1514 attached to micro circuit support 1512. Structure 1510, affixed to one end of bellows container 1306, moves in response to the extension of bellows 1506. If the bellows is constructed of a non-conductive or dielectric material, structure 1510 is preferably constructed of a electrically conductive material which is bonded to the remaining bellows 1506 using adhesives, glues, press fitting, or any other suitable attachment technique known in the art. Structure 1510 may also be constructed of a non-conductive base material whose upper surface is plated with a conductor utilizing a suitable coating process, such as electroplating or vapor deposition. Electrical contacts 1508, electrically coupled to microcircuit 1514, are positioned to detect the extended position of bellows 1506 (a high pressure condition) when the conductive surface of structure 1510 engages two or more contacts, causing electric current flow in microcircuit 1514 which can be detected by methods well known to those skilled in the art.
Microcircuit 1514 contains a power supply, communication/transmission circuitry, and current sensing circuitry. Microcircuit 1514 is of suitable construction, such as a monolithic silicon integrated circuit; a hybrid integrated circuit having a ceramic substrate and a plurality of silicon integrated circuits, discrete components, and interconnects thereon; or, a printed circuit board based device with through hole or surface mounted components. The power supply is of a suitable construction, such as an inductive device, deriving power from either the current flowing in the high voltage vacuum switch (as previously disclosed in embodiments above), or preferably an RF device receiving power from an external RF source transmitting RF signals to the device. Use of an external RF power transmission source allows the microcircuit to remain dormant until queried, and can be utilized even if the vacuum switch is powered down, offline, or in storage. Alternatively, power may be supplied by batteries, solar cells, or other suitable power sources that can be integrated within microcircuit 1514 or attached to support 1512. The communication/transmission circuitry can be RF transmission based or optical transmission based. RF transmission includes microwave and millimeter wave transmission. Optical transmission may be accomplished with solid state light sources integrated within microcircuit 1514 or attached to substrate 1512 (not shown). An optical receiving device (not shown), such as the embodiments shown in FIG. 9, may be utilized to detect optical transmissions from microcircuit 1514. Such a receiver can be coupled to circuit 1514 directly with optical cable, or be positioned to pick up transmissions by line of sight. An RF receiver unit (not shown) may be located at any convenient distance from the vacuum switch, within range of the transmitter contained within microcircuit 1514. The RF receiver unit may or may not contain RF transmission capability. Both types of receiver units (optical or RF) may set up to monitor the transmissions from one or a plurality of microcircuits resident in multiple high voltage vacuum devices, and may be stationary or mobile. Receivers contain the necessary processors, memory, analog circuitry, an interface circuitry to monitor transmissions and issues alarms and other information as required. Microcircuit 1514 can be programmed to immediately transmit a signal when a high pressure is sensed in the vacuum switch, or wait until circuit 1514 is queried by a signal transmitted to it. On main advantage of the present embodiment is that microcircuit 1514 is floating at the potential of the vacuum switch, and that transmission of information (and power) to and from the microcircuit is not compromised by high voltage potentials in the switch.
FIG. 16 is a partial cross sectional view 1600 of a high voltage vacuum switch with an externally mounted pressure measuring chamber 1604 and a contact closure sensing microcircuit 1514, at low pressure, according to an embodiment of the present invention. FIG. 17 is a partial cross sectional view 1700 of a high voltage vacuum switch with an externally mounted pressure measuring chamber 1604 and a contact closure sensing microcircuit 1514, at high pressure, according to an embodiment of the present invention. Pressure measuring chamber 1604 is fluidically coupled to the pressure inside of the high voltage vacuum switch via conduit 1602. A movable structure 1606 is placed within a portion of the containment walls of chamber 1604. Movable structure 1606 deflects outwardly (ref 1702) at high pressures within chamber 1604. Structure 1606 is generally a thin diaphragm or membrane, constructed of any suitable material, preferably metal or a non-metallic material having an upper coating of metal or other electrically conductive material. Contacts 1508 are placed in close proximity to structure 1606, so that small deflections can be detected by electrical continuity through at least two contacts. Structure 1606 is fabricated in such a manner as to produce a dome shape at low differential pressures. As pressure outside the dome increases (or pressure inside the dome decreases), the dome is forced into an approximately planar shape. The amount of deflection for a given pressure differential is dependent on the wall thickness, type of material, and other material properties as is well known in the art. An advantage to this embodiment is that very small deflections can be detected by placing substrate 1512 in near contact with structure 1606, resulting in increased pressure sensitivity.
The description and limitations of microcircuit 1514 have been recited above.
In an alternative embodiment of the present invention, the deflection of movable structure 1606 is detected by a strain gauge device fixed to the outer surface of structure 1606 (not shown). Microcircuit 1514 contains the power supply and communication/transmission circuitry previously disclosed, the contact closure sensing circuitry being replaced with the appropriate circuitry for interface with the strain gauge device. The strain gauge device may be connected to microcircuit 1514 by wires, or communication with microcircuit 1514 may by wireless techniques such as optical transmission or RF transmission. Alternatively, the strain gauge device may be integrated with other circuitry, such as power supply and transmission/reception circuitry, on the same substrate, which is fixed to the surface of structure 1606. An advantage to this embodiment of the present invention is that very small deflections can be detected, providing a high sensitivity to pressure changes within the high voltage vacuum device. This embodiment also allows continuous (or periodic) measurement and monitoring of the pressure as a function of time, which can be utilized to provide advance warning of potential failure conditions, allowing users to take pro-active action to identify and remove leaking devices from service prior to actual failure.
Optical detection of the high pressure condition offers significant advantages due to the simplicity and low cost of the components, coupled with good dielectric isolation from the high operating potentials. However, previously described embodiments require careful alignment of the transmitting and detecting optical fiber components, or alignment of mirrors and reflecting surfaces. In practice, this can be difficult or expensive, and may lead to reliability issues if these components get out of alignment during use. It would be useful to have a monolithic, self aligning reflector system that cannot get out of adjustment, and provides a more compact packaging geometry. A hemispherically shaped reflector, in accordance with embodiments of the present invention, provides these advantages.
FIG. 18 is a schematic cross sectional view 1800 of a hemispherically shaped reflector for optical detection of a high pressure condition in a high voltage device, according to an embodiment of the present invention. A hemispherically shaped reflector surface 1802 can provide two 90 degree reflections for a source beam 1804, if the source beam is oriented parallel to the axis of symmetry 1803 and is located at a radial position of R√{square root over (2)}/2, where R is the radius of the hemisphere. This location can be derived by constructing two equilateral right triangles 1808, 1810, having sides of length R√{square root over (2)}/2, and hypotenuse of R. Incoming ray 1822 reflects off inside surface of hemispherically shaped reflector 1802 at a 45 degree angle, at a point where right triangle 1814 is tangent to reflector surface. Reflected ray 1824 is directed horizontally (normal to the axis of symmetry 1803) to a second reflection point where right triangle 1812 is tangent to hemispherically shaped reflecting surface 1802. Exiting ray 1826 leaves parallel to incoming ray 1822 at a location R√{square root over (2)}/2 from axis 1803. An opaque flag 1820, inserted through an aperture in hemispherically shaped reflecting surface 1802, will intercept and block the reflected ray 1824 at a distance 1816 of R(1−√{square root over (2)}/2), from where axis 1803 intersects surface 1802 at the pole of the hemisphere. Since this dimension is only dependent on the radius of the hemisphere 1802, it can be precisely fixed once the hemispherically shaped surface 1802 is manufactured. Flag 1820 can be attached to any device whose movement is responsive to pressure inside the high voltage device, as described previously or in the figures below. The preceding analysis indicates that there is a single location where two 90 degree reflections occur. However, real optical beams have a finite width, and it is often desirable to focus these beams to increase their intensity. The spherical reflector, in accordance with the present invention, provides an unexpected benefit for optical beams less than specified widths, in that these beams can be focused for improved detection.
FIG. 19 is a schematic cross sectional view 1900 of a hemispherically shaped reflector 1802 showing a ray trace analysis for narrow optical beam widths, according to an embodiment of the present invention. Arrows 1904a and 1906a represent the boundaries of an incoming light beam. The center of the beam is located at R√{square root over (2)}/2, or 0.707 R (ref 1902) from axis 1803, as shown in FIG. 18. The boundaries are located at distances RM (ref 1908) and RL (ref 1910) from axis 1803. The ray trace of an incoming ray 1904b shows a first reflected ray 1904c and a second reflected ray 1904d. The ray trace of incoming ray 1906b shows a first reflected ray 1906c and a second reflected ray 1906d. Both reflected rays 1904d and 1906d intersect at focal point 1912. An optical detector placed at this location 1912, will receive a signal of increased intensity, due to the focusing action of the hemispherically shaped reflector.
However, for incoming optical beams of broad width, a divergence effect occurs, as shown in the ray trace analysis of FIG. 20. FIG. 20 is a schematic cross sectional view 2000 of a hemispherically shaped reflector 1802 showing a ray trace analysis for broad optical beam widths, according to an embodiment of the present invention. Arrows 2002a and 2004a represent the boundaries of a broad incoming light beam. The center of the beam is located at R√{square root over (2)}/2, or 0.707 R (ref 1902) from axis 1803. The boundaries are located at distances Rmin (ref 2008) and Rmax (ref 2006) from axis 1803. The ray trace of an incoming ray 2002b shows a first reflected ray 2002c and a subsequently reflected rays 2002d, 2002e, and 2002f. The ray trace of incoming ray 2004b shows a first reflected ray 2004c and a second reflected ray 2004d. The directions of exiting rays 2002f and 2004d indicate the divergence of the incoming beam. To minimize the divergence effect, the incoming beam width (Rmax−Rmin) should be less than about 0.26 R, preferably less than 0.06 R.
FIG. 21 is a partial cross sectional view 2100 of an externally located bellows pressure detection device 2116 coupled to a hemispherically shaped optical reflector 2110, at a low pressure condition, according to an embodiment of the present invention. The interior of hollow bellows 2116 is fluidically coupled to the interior of a high voltage vacuum electrical device (not shown) via conduit 2118, as is shown, for example, in FIGS. 13, 14, and 15. Flag 2114, an opaque structure, moves through aperture 2122 in response to an increase in pressure inside bellows 2116. Source optical fiber 2102 and sense optical fiber 2104 are oriented in the proper direction and at the proper location by fittings 2106 and 2104, whose construction is well known to those skilled in the art. At sufficiently low pressures in bellows 2116 (and in the high voltage device connected thereto), a light beam 2112 is reflected via spherical reflector 2110 from source fiber 2102 to detection fiber 2104, due to the recessed position of flag 2114. Pressure sensitivity can be adjusted by the properties of the bellows combined with the pressure inside cavity 2120, if desired. Due to the enclosed nature of the structure, a reference pressure below atmospheric can be easily maintained if fittings 2108 and 2106 are gas tight. An inert gas environment may also be maintained, which is useful in preventing contamination of the reflector surface. FIG. 22 is a partial cross sectional view 2200 of an externally located bellows pressure detection device coupled to a hemispherically shaped optical reflector, at a high pressure condition, according to an embodiment of the present invention. At high pressure, bellows chamber 2116 extends a distance sufficient to block the reflected light beam with flag 2114.
FIG. 23 is a partial cross sectional view 2300 of a high voltage switching module 2302 according to an embodiment of the present invention. A bellows actuated pressure sensing device coupled to a hemispherically shaped optical detector assembly 2304, is shown mounted on a high voltage vacuum interrupter 2306. An optical fiber cable 2308, containing both source and sense optical fibers, is routed down through module 2302 to sensing device 2304. In this figure, it is clear why both source and sense optical fibers need to be parallel to each other and parallel to the axis of extension of the bellows. An optical path where source and sense fibers are perpendicular to extension axis of the bellows (as, for example, in FIGS. 13 and 14) would be difficult to package in module 2302. FIG. 24 is a partial cross sectional view 2400 of a vacuum interrupter module 2306 and a bellows actuated pressure sensing device coupled to a hemispherically shaped optical detector assembly 2304 according to an embodiment of the present invention.
FIG. 25 is a partial cross sectional view 2500 of a bellows actuated pressure sensing device coupled to a hemispherically shaped optical detector assembly 2304 of FIGS. 23 and 24 according to an embodiment of the present invention. Hollow conduit 2516 fluidically couples the interior of bellows chamber 2514 to the internal volume of high voltage vacuum device 2306. Flag 2512 intercepts the optical beam transmitted between optical fibers 2506 and 2508, the optical beam being reflected by hemispherically shaped surface 2510. Optical fibers 2506 and 2508 are held in place via fittings 250 and 2504.
FIG. 26 is a partial cross sectional view 2600 of a cylinder actuated pressure detection device coupled to a hemispherically shaped optical reflector, at a low pressure condition, according to an alternative embodiment of the present invention. In this embodiment, the bellows chamber is replaced with a piston 2604 and spring 2606 assembly, similar to the embodiment shown in FIGS. 4 and 5. Conduit 2608 is fluidically coupled to the interior volume of a high voltage vacuum device (not shown). The vertical location of flag 2602 is determined by the pressures inside volumes 2612 and 2610, in conjunction with the force generated by spring 2606. At low pressures (shown), flag 2602 is recessed and does not block transmission of the optical beam. FIG. 27 is a partial cross sectional view 2700 of a cylinder actuated pressure detection device coupled to a hemispherically shaped optical reflector, at a high pressure condition, according to an alternative embodiment of the present invention. At high pressure, flag 2602 blocks the optical beam as shown. As in the case for the bellows chamber previously described, the pressure sensitivity may also be adjusted by the differential pressures in volumes 2612 and 2610, combined with the spring constant of spring 2606.
FIG. 28 is a partial cross sectional view 2800 of an internally located bellows pressure detection device coupled to a hemispherically shaped optical reflector, at a low pressure condition, according to an alternative embodiment of the present invention. This embodiment is similar to that described previously in FIGS. 6 and 7. In this case bellows chamber 2804 is mounted inside the high voltage vacuum device 2808. The bellows is sealed against the surface of wall 2802, which is the outer wall of the high voltage vacuum device. Hemispherically shaped reflector 2110 is machined into the outer wall 2802. The interior of the bellows chamber 2804 is in fluid communication with the pressure inside the chamber bounded by the hemispherically shaped reflector 2110, which may be atmospheric or some other reference pressure. At low pressure (shown), flag 2806 is recessed and does not block the optical beam. FIG. 29 is a partial cross sectional view 2900 of an externally located bellows pressure detection device coupled to a hemispherically shaped optical reflector, at a high pressure condition, according to an alternative embodiment of the present invention.
The present invention is not limited by the previous embodiments or examples heretofore described. Rather, the scope of the present invention is to be defined by these descriptions taken together with the attached claims and their equivalents.

## Claims

1. A method for detecting a high pressure condition within a high voltage vacuum device, comprising:
providing a gas tight envelope for containing gas pressure within said high voltage vacuum device;
providing a collapsible device, enclosed within said gas tight envelope, having a first surface and a second surface, said first surface fixed relative to said gas tight envelope, said second surface movable relative to said first surface with an increase in said gas pressure within said gas tight envelope;
providing a shaft, having a first end and a second end, said first end attached to said second surface of said collapsible device;
transmitting an optical beam to a first location on a hemispherically shaped reflecting surface;
reflecting a portion of said optical beam from said first location to a second location on said hemispherically shaped reflecting surface;
blocking said portion of said optical beam being reflected from said first location to said second location with a portion of said shaft, at said high pressure condition; and,
providing an output responsive to blocking said portion of said optical beam.

2. The method as recited in claim 1, wherein said high voltage vacuum device is operating at an AC voltage greater than 1000 volts.

3. The method as recited in claim 1, wherein said high voltage vacuum device is a high voltage vacuum switch.

4. The method as recited in claim 1, wherein said high voltage vacuum device is a high voltage vacuum capacitor.

5. The method as recited in claim 1, wherein said second end of said shaft extends through an aperture in said hemispherically shaped reflective surface, said aperture being located between said first location and said second location.

6. The method as recited in claim 1, wherein the output is generated when there is a partial loss of vacuum pressure in the high voltage vacuum device.

7. The method as recited in claim 1, wherein the output is generated only when there is a full loss of the vacuum pressure in the high voltage vacuum device.

8. The method as recited in claim 1, further comprises providing electrical contacts located within said gas tight envelope, mounted for relative movement between a first position in which said electrical contacts are positioned closely adjacent, and a second position in which said electrical contacts are spaced apart from each other, with the vacuum pressure condition in the high voltage vacuum device preventing electrical arcing between said electrical contacts when they are moved between said first and second positions, wherein movement of said shaft is independent of movement of said electrical contacts between said first and second positions.

9. An apparatus for detecting high pressure within a high voltage vacuum device, comprising:
a gas tight envelope for containing gas pressure within said high voltage vacuum device, said gas pressure defining a vacuum pressure condition;
a collapsible device, enclosed within said high voltage vacuum device, having a first surface and a second surface, said first surface fixed relative to said high voltage vacuum device, said second surface movable relative to said first surface with an increase in said gas pressure within said gas tight envelope;
a shaft, having a first end and a second end, said first end attached to said second surface of said collapsible device;
a sensor for detecting a position of said second end of said shaft; and,
electrical contacts located within said gas tight envelope, mounted for relative movement between a first position in which said electrical contacts are positioned closely adjacent, and a second position in which said electrical contacts are spaced apart from each other, with the vacuum pressure condition in the high voltage vacuum device preventing electrical arcing between said electrical contacts when they are moved between said first and second positions, wherein movement of said shaft is independent of movement of said electrical contacts between said first and second positions.

10. The apparatus as recited in claim 9 wherein said sensor comprises:
a first optical cable, positioned to transmit an optical beam to a first location on a hemispherically shaped reflective surface;
a second optical cable, positioned to receive at least a portion of said optical beam transmitted from said first optical cable, reflected from a second location on said hemispherically shaped reflective surface;
wherein said second end of said shaft extends through an aperture in said hemispherically shaped reflective surface, said aperture being located between said first location and said second location, said shaft operative to block a least a portion of said optical beam reflected from said first location to said second location at said high pressure condition within said high voltage vacuum device.

11. The apparatus as recited in claim 10, wherein said first location and said second location are positioned approximately on a circle inscribed on said hemispherically shaped reflective surface, said circle being defined by an intersection of a planar surface and said hemispherically shaped reflective surface, wherein said planar surface is perpendicular to an axis of symmetry of said hemispherically shaped reflective surface, and a radius of said circle is equal to a radius of said hemispherically shaped reflective surface multiplied by one half the square root of 2.

12. The apparatus as recited in claim 10, wherein said optical beam is focused by reflection from said hemispherically shaped reflective surface, prior to reception by said second optical cable.

13. The apparatus as recited in claim 9 wherein said high voltage vacuum device is a high voltage vacuum switch.

14. The apparatus as recited in claim 9 wherein said high voltage vacuum device is a high voltage vacuum capacitor.

15. A vacuum bottle-type electrical device with a vacuum pressure loss detection feature comprising:
a bottle defining a vacuum pressure condition at the interior of the bottle;
electrical charge members in the bottle mounted for relative movement between a first position in which the electrical charge members are positioned closely adjacent and a second position in which the electrical charge members are spaced apart from each other, with the vacuum pressure condition in the bottle preventing electrical arcing between the electrical charge members when they are moved between their first and second positions at voltage potentials in excess of 1000 V;
a first optical cable, positioned to transmit an optical beam to a first location on a hemispherically shaped reflective surface;
a second optical cable, positioned to receive at least a portion of said optical beam transmitted from said first optical cable, reflected from a second location on said hemispherically shaped reflective surface;
a collapsible device, enclosed within said bottle, having a first surface and a second surface, said first surface fixed relative to said bottle, said second surface movable relative to said first surface with an increase in said gas pressure within said bottle; and,
a shaft, having a first end and a second end, said first end attached to said second surface of said collapsible device, wherein said second end of said shaft extends through an aperture in said hemispherically shaped reflective surface, said aperture being located between said first location and said second location, said shaft operative to block at least a portion of said optical beam reflected from said first location to said second location at a loss of vacuum pressure within said vacuum bottle-type electrical device.

16. The device as recited in claim 15, further comprising:
first components optically coupled to said first optical cable, operative to provide radiation for said optical beam; and,
second components optically coupled to said second optical cable, operative to sense the blockage of said portion of said optical beam reflected from said first location to said second location, further operative to issue an alarm when the loss of vacuum pressure exceeds a predetermined value.

17. The apparatus as recited in claim 15, wherein said first location and said second location are positioned approximately on a circle inscribed on said hemispherically shaped reflective surface, said circle being defined by an intersection of a planar surface and said hemispherically shaped reflective surface, wherein said planar surface is perpendicular to an axis of symmetry of said hemispherically shaped reflective surface, and a radius of said circle is equal to a radius of said hemispherically shaped reflective surface multiplied by one half the square root of 2.

18. The apparatus as recited in claim 15, wherein said optical beam is focused by reflection from said hemispherically shaped reflective surface, prior to reception by said second optical cable.

19. The apparatus as recited in claim 15, wherein said high voltage vacuum device is a high voltage vacuum switch.

20. The apparatus as recited in claim 15, wherein said high voltage vacuum device is a high voltage vacuum capacitor.