ELECTRO-OPTIC VOLTAGE SENSOR

Abstract: An electro-optic voltage sensor for achieving voltage measurement without significant error contributions from neighboring conductors or environmental perturbations. The voltage sensor includes a transmitter (1), a sensor (4), a detector (43, 44) and a processor (62). The transmitter (1) produces a beam of electromagnetic radiation which is routed into a sensor (4). Within the sensor (4), the beam undergoes the Pockels electro-optic effect. The electro-optic effect produces a modulation of the beam's polarization, which is in turn converted to a pair of independent conversely-amplitude-modulated signals, from which the voltage of the E field is determined by the processor (62). The use of converse AM signals enables the signal processor (62) to better distinguish signal from noises. The sensor (4) converts the beam by splitting the beam in accordance with the axes of the beam's polarization state (an ellipse whose ellipticity varies between -1 and +1 in proportion to voltage) into at least two AM signals. These AM signals are fed into a signal processor (62) and processed to determine the voltage between ground conductor and the conductor (2) on which voltage is being measured.

Description: ELECTRO-OPTIC VOLTAGE SENSOR BACKGROUND OF THE INVENTION 1. The Field of the Invention. The present invention pertains generally to the field of voltage sensors and more particularly to a voltage sensor system which utilizes the Pockels electro-optic effect to measure voltage. 2. The Background Art . High-accuracy measurement of high voltage has traditionally been accomplished using iron-core ferro¬ magnetic potential transformers. These devices have substantially limited dynamic range, bandwidth, linearity, and electrical isolation. During electrical fault conditions these transformers can conduct dangerous levels of fault energy to downstream instrumentation and personnel, posing an additional liability. A variety of optic sensors for measuring voltage have been developed in attempts to offer the power industry an alternative to the conventional transformer technology. Generally, these voltage sensor systems require that direct electrical contact be made with the energized conductor. This contact is made necessary by the use of a voltage divider which is utilized to connect the sensing element with the energized conductor on which a measurement is to be made. Direct electrical contact with the conductor may alter or interrupt the operation of the power system by presenting a burden or load. In addition to the disadvantages associated with direct electrical contact with the energized conductor, prior art voltage sensor systems are typically bulky, particularly in extremely high voltage applications. This is true because the size of the voltage divider required is proportional to the voltage being measured. The size of such systems can make them difficult and expensive to install and house in substations. Many prior art sensors are based upon the electrostrictive principle which utilize interferometric modulation principles. Unfortunately, interferometric modulation is extremely temperature sensitive. This temperature sensitivity requires controlled conditions in order to obtain accurate voltage measurements. The requirement of controlled conditions limits the usefulness of such systems and makes them unsuited for outdoor or uncontrolled applications. In addition, interferometric modulation requires a highly coherent source of electromagnetic radiation, which is relatively expensive. Open-air E-field based sensors have also been developed, but lack accuracy when used for measuring voltage because the open-air E-field used varies with many noisy parameters including ambient dielectric constant, adjacent conductor voltages, moving conductive structures such as passing vehicles, and other electromagnetic noise contributions. Systems which utilize mechanical modulation of the optical reflection within an optic fiber have also been developed. Among other drawbacks, the reliance of such systems on moving parts is a significant deterrent to widespread use. It would therefore be an advantage in the art to provide a system which does not require direct electrical contact with the energized conductor, is compact, operates m a variety of temperatures and conditions, is reliable, and is cost effective. OBJECTS AND SUMMARY OF THE INVENTION It is therefore an object of the present invention to provide an electro-optic voltage sensor system which does not require contact with a conductor. It is a further object of the present invention to provide such an electro-optic voltage sensor system which is capable of use m a variety of environmental conditions It is a still further object of the present invention to provide such an electro-optic voltage sensor system which can be employed to accurately measure high voltages without use of dedicated voltage division hardware. It s an additional object of the present invention to provide such an electro-optic voltage sensor system which minimizes the electronics needed for implementation. It is a further object of the present invention to provide a sensor system capable of being integrated with existing types of high voltage power transmission and distribution equipment so as to reduce or eliminate the need for large stand-alone voltage measurement apparatus . It is yet another object of the present invention to provide a sensor system capable of being integrated with existing types of power transmission and distribution equipment . These and other objects of the present invention will become more fully apparent from the following description and appended claims or may be learned by the practice of the invention as set forth herein. While the present invention is described m terms of a sensor system, it is to be understood that the subject apparatus and method may be used m any field of electrical or optical application. Those having ordinary skill in the field of this invention will appreciate the advantages of the invention, and its application to a wide variety of electrical uses. The above objects and others not specifically recited are realized in a specific illustrative embodiment of an Electro-Optical Voltage Sensor System whereby one may measure the voltage difference (or electrical potential difference) between objects or positions Voltage is a function of the electric field (hereinafter "electric field" shall be indicated "E-field") and the geometries, compositions and distances of the conductive and insulating matter. Where, as m the present invention, the effects of an E-field can be observed, a voltage measurement can be calculated. The invention employs a transmitter, a sensor, a detector, and a signal processor The transmitter produces a beam of electromagnetic radiation which is routed into the sensor Although this electromagnetic radiation used m the present invention can comprise any wavelengths beyond the visible spectrum, the term "light" will be used hereinafter to denote electromagnetic radiation for the purpose of brevity The beam undergoes polarization before it undergoes an electro-optic effect m transducer material which is included in the sensor. In the polarized beam, the light has at least two components which propagate along at least two orthogonal axes, thus forming at least two orthogonal planes within the beam. The electro-optic effect occurs when the sensor, and m particular the transducer material, is placed m an E- field, and is observable as a differential phase shift of the orthogonal beam components (the two components are shifted m opposite directions) . The planes of propagation are the object of the differential phase shift, also called phase modulation The differential phase shift causes a corresponding change m the beam's polarization The polarization change is m turn converted into a set of amplitude modulated (AM) signals of opposing polarity that are transmitted out of the sensor The detector converts the set of optical AM signals into electrical signals from which the voltage is determined by the signal processor. The sensor processes the beam by splitting the beam m accordance with the components of the orthogonal polarization planes into at least two AM signals In the preferred embodiment, these AM signals are then converted into digital signals, fed into a digital signal processor and mathematically processed into a signal proportional to the voltage which produced the E-field. In a preferred embodiment of the sensor, the beam is routed through the transducer material along an initial axis and then reflected by a retroreflector back along a second axis generally parallel to the initial axis. BRIEF DESCRIPTION OF THE DRAWINGS The above and other objects, features and advantages of the invention will become apparent from a consideration of the subsequent detailed description presented m connection with the accompanying drawings m which: FIG 1 is a diagram of the electro-optical voltage sensor system shown m a generalized high voltage application scenario The diagram was made in accordance with the principles of the present inventio . FIG. 2 is a diagram of an alternative embodiment of the electro-optical voltage sensor system (m the same generalized application scenario) made m 6 accordance with the principles of the present invention. FIG. 3 is a diagram of the light polarizing beam splitter of FIGS. 1 and 2. FIG. 4 shows a partially sectioned side view of a collimator of FIG. 2 and also FIGS 7 and 8, below. FIG. 5 is a diagram of one embodiment of tne transducer of FIGS. 1 and 2, wherein transducing material m only one orientation is shown. FIG. 6 is a diagram of one embodiment of the transducer in FIGS. 1 and 2, wherein transducing material m two orientations is shown. FIG. 7a is a top-down schematic view of one embodiment of the sensor head of FIG. 2. FIG. 7b is a top-down schematic view of one embodiment of the sensor head of FIG. 2. FIG. 7c is a top-down schematic view of one embodiment of the sensor head of FIG. 2. FIG 8 is a top-down schematic view of one embodiment of the sensor head of FIG. 1. FIG. 9 is a cross-sectional, schematic view of one embodiment of the E-field originator of FIGS. 1 and 2, as a shielded joint. FIG. 10 is a top perspective, partially schematic view of one embodiment of the E-field originator of FIGS. 1 and 2, as a terminator. FIG. 11 is a cross-sectional side view of one embodiment of the E-field originator of FIGS. 1 and 2, as a bushing. FIG. 12 is a sectional, partially schematic, side view of one embodiment of the E-field originator of FIGS. 1 and 2, as a shielded bus or shielded cable. FIG. 13 is a sectional, partially schematic, side view of one embodiment of the E-field originator of FIGS. 1 and 2 , as a gas or oil-insulated switchgear FIG. 14 is a sectional, partially schematic, side view of one embodiment of the E-field originator of FIGS. 1 and 2 , as a duct-enclosed bus. FIG 15 is a side view of one embodiment of the E-field originator of FIGS. 1 and 2, as a clamp-on apparatus. FIG. 16 is an alternative embodiment of the electro-optical voltage sensor of FIG. 1 having a current detector. DETAILED DESCRIPTION A preferred embodiment in accordance with the present invention is illustrated m FIG. 1, which is a diagram of the electro-optical voltage sensor system There is shown a transmitter 1, which is a transmitting means that transmits a beam of electromagnetic radiation (the beam is not shown m FIG 1 but generally designated as 12 elsewhere) and a sensing means, shown in FIG. 1 as a sensor head 4 In the preferred embodiment the beam is routed from the transmitter 1 to the sensor head 4 by a polarization maintaining (PM) fiber 18. In an alternative embodiment the PM fiber 18 is replaced by low- birefrmgence fiber. Another alternative embodiment whose cost/performance characteristic may be quite different and better suited to certain applications, entails replacement of the PM fiber 18 by single-mode or multi-mode optic fiber. The PM fiber 18 directs the beam from the transmitter 1 into the sensor head 4. Optical signals are routed from the sensor head 4 by a pair of either single-mode or multi-mode optical fibers, shown as 37 and 38. The optical fibers 18, 37, and 38 electrically isolate the sensor head 4 from the transmitter 1 and the rest of the detection system, providing further protection to personnel and equipment from the dangers of high voltage systems The sensor head of the preferred embodiment of FIG. 1 is shown in greater detail in the top-down schematic view of FIG. 8, where the preferred embodiment of the sensor head is generally depicted at 4. The sensor head 4 comprises a polarizer 6, a translucent medium 13, a transducer 5, a retro- reflector generally depicted at 10, a polarizing beam splitter 80 and beam reflector 14. A collimator 26 is connected to the PM fiber 18 and transmits the beam 12 from the PM fiber 18 into the polarizer 6. The polarizer 6 polarizes the beam 12 when the beam 12 is transmitted from the collimator 26; thus, the polarizer 6 polarizes the beam 12 if the beam 12 is not polarized when it is transmitted from the collimator 26, or re-polarizes the beam 12 if the beam 12 is polarized when it is transmitted from the collimator 26. As a practical matter, the polarizer 6 could be eliminated or placed anywhere between the transducer 5 and the transmitter of the beam 12, including anywhere along the PM fiber 18. In an alternative embodiment the PM fiber 18 can be aligned with sufficient precision with respect to the optical axes of the transducing medium, to perform the function of (and eliminate the need for) the polarizer 6. The beam 12 passes from the polarizer 6 through the translucent medium 13 and into the transducer 5. The translucent medium 13 comprises a non-conductive, non-birefringent material, such as fused quartz or a similar substance, which provides a pathway for the beam from the polarizer 6, which is preferably situated outside the E-field, to the transducer 5, which must reside within the E-field. The source of this E-field will be discussed shortly. When the transducer 5 (also called the transducing medium) is in a non-zero E-field (not shown) it induces a "differential phase shift" to orthogonal beam components of the beam 12 through the Pockels electro-optic effect, which will now be explained. In the polarized beam 12 the light has at least two components which propagate along at least two orthogonal planes, respectively, thus forming at least two orthogonal planes within the beam 12. The phase of the components in each plane of propagation are the object of a shift, relative to the phase of the component in the other plane, in the transducer 5. The Pockels electro-optic effect, which takes place in transducer 5, changes the relative phases of the beam components by altering their respective velocities, and is observed in Pockels transducing crystals and similar media. The magnitude of the phase shift, called the "differential phase shift", is proportional to the magnitude of the E-field. Thus, the Pockels electro-optic effect is observed as a "phase differential shift" of the orthogonal beam components which is proportional to the magnitude of the E-field. Due to the fixed coaxial structure of the devices in which the sensor head is to be installed, the magnitude of the E-field is proportional to the voltage. Therefore, the differential phase shift is proportional to (and can be used to measure) the voltage of the E-field between energized conductor and ground conductor. In the preferred embodiment, the transducer 5, or transducing medium, comprises a material which exhibits the Pockels electro-optical effect. In the present invention the transducer 5 is preferably Lithium Niobate (LiNb0 3 ) Pockels, although other materials, such as Ammonium Dihydrogen Phosphate (NH 4 H 2 P0 4 ) , Ammonium Dideuteriu Phosphate (NH 4 D 2 PO„) , Potassium Dideuterium Phosphate (KD 2 P0 4 ) , MgO-doped Lithium Niobate (MgO-LiNb0 3 ) , electro-optic polymers, organic materials, and others may be used. The phase shift between orthogonal components further manifests itself as an alteration of the beam's polarization Therefore, the beam may be considered either to be a differential phase shifted signal or an optical polarization modulation signal The polarization modulation signal is used in the present invention because it can be detected using low-cost, components that are less susceptible to temperature, mechanical perturbations, and optical incoherence than those components that would be required to sense the differential phase shift directly. In the practice of the present invention, the sensor head 4 or the transducer 5 may be encased m a dielectric buffering material, not shown, to smooth the transition geometry between the permittivity of the transducer 5 and the permittivity of the surrounding media, which m most cases will be an insulator The dielectric buffering material promotes uniformity in the E-field, particularly around the edges of the transducer 5 This enhances uniform phase shift m the beam 12 passing through the transducer 5, and minimizes voltage stress on the materials in and surrounding the sensor head 4 as well, thereby increasing the probable maximum operating lifetime of the entire system. After the beam 12 has passed sequentially through the polarizer 6 (FIG. 8) , translucent medium 13 and transducer 5, it enters into the retro-reflector 10 The retro-reflector 10 comprises a reflector material 9 which induces the beam to reflect and causes a quarter-wave retarding of the beam 12. The quarter- wave retarding property of the reflector material 9 induces a 1/4 wavelength shift m the orthogonal planes of the beam 12. The 1/4 wavelength shift can be achieved by reflection of the beam 12 alone, if the material 9 is non-birefnngent , alternatively, the material 9 can comprise birefringent reflector material wherein the properties of the material help achieve the shift. If a reflector material 9 having birefringence is used, the phase shifting occurs when orthogonal components of the electromagnetic waves of the beam are shifted (here by 1/4 a wave length) with respect to one another. This birefringence, which is inherent m some materials, is not dependant upon the E-field In the preferred embodiment, a reflector material 9 is used which exhibits a reflection-induced retardation to differentially shift the relative phases of the beam components m orthogonal planes m the beam 12 by ιτ/2 radians. The polarization of the beam 12 incident upon the retro-reflector 10 depends upon the E-field present when the beam 12 makes a first pass through the transducer 5. If there is an E-field present then there will be some differential phase shift already present m the beam 12. The 7r/2 retardation withm the retro-reflector 10 biases the sensor's overall resultant polarization such that zero E-field (and hence zero voltage) corresponds to circular-polarized light, as no differential phase shift is mduced upon the beam 12 by the transducer 5 However, due to the location of the retro-reflector 10 in the sensor head 4, if the transducer 5 is a non-zero E-field and induces a differential phase shift m the beam 12, then the retro-reflector 10 will not convert light from linear to circular-polarization, rather it will induce elliptical-polarization upon the beam 12, whose ellipticity will vary m proportion to the voltage. While laser light is used m the preferred embodiment, other forms of electromagnetic radiation could also be used the practice of the mvention The reflection of the beam 12 m the retro- reflector 10 is accordance with the principle of the angle of incidence being the same as the angle of reflection. In the practice of the preferred embodiment of the present invention, the retro- reflector 10 is configured to cause a 180° change m the direction of the beam 12, thereby sending the beam back mto the transducer 5. Upon each reflection, a beam 12 may be induced to undergo a 1/8 wave length phase shift to produce a total of 1/4 wave phase shift, as m the preferred embodiment. One skilled in the art could further induce a 1/4 wave length shift in beam 12 by combining reflection and birefringence. When the beam 12 reenters the transducer 5, it undergoes further phase shift from the Pockels electro-optic effect. As shown in FIG. 8, the beam 12 then passes through the translucent medium 13 and enters into the polarizing beam splitter 80. In the polarizing beam splitter 80, (also called an analyzer m the art) , the beam 12 is separated accordance with the respective axes of its polarization ellipse into AM signals 35 and 36. The said polarization ellipse will exhibit an ellipticity ranging between -1 and +1, in proportion to voltage at any given time. Those skilled the art will note that an elliptic polarization whose ellipticity ranges between -1 and +1 can be described as ranging from a linear polarization along one axis to a linear polarization along a second axis perpendicular to the first axis, wherein the point at which ellipticity equals 0 corresponds to circular polarization. As shown in FIG. 3, the major and minor axes of the polarization ellipse of beam 12 can be represented by two orthogonal components, indicated generally at 83. The beam splitter 80 then separates the beam 12 mto two components 84 and 85 which comprise the intensities along each of the two axes of the polarization ellipse shown as orthogonal components 83. The intensity of beam components 84 and 85 will modulate conversely to one another in response to modulations in the ellipticity of the beam's polarization. The beam components 84 and 85 are two AM signals shown as 35 and 36, respectively, which are routed as shown in FIG. 1 into photo-detectors 43 and 44, respectively. The AM signals 35 and 36 are then passed by colli ators 27 and 28, shown in FIG. 8, and routed through multi-mode or single-mode optic fibers 37, 38. A beam reflector 14 may be used to aid in routing the AM signals 35 and 36. As shown in FIG. 1, first and second routing means, shown as optic fibers 37 and 38, are used to route the AM signals 35 and 36 from the sensing means into the detecting means. First the AM signals 35 and 36 are routed into the photodetectors 43 and 44 through the first and second routing means, shown as the first and second translucent fibers 37 and 38, respectively. In the preferred embodiment the first and second translucent fibers 37 and 38 comprise at least one optic fiber, wherein the optic fiber is selected from the group consisting of : a single-mode optic fiber, and a multi-mode optic fiber. In the photodetectors 43 and 44 the AM signals 35 and 36 become electrical signals 45 and 46. The electrical signals 45 and 46 are routed into a signal processor 62, the final component of the detecting means, wherein a desired E-field characteristic is determined, particularly that of voltage. To determine the voltage in the practice of the preferred embodiment of the present invention the signal processor 62 is designed to sample each AM signal at substantially regular intervals and substantially simultaneous times, process the signals to produce a display signal (not shown) which is then displayed on a readable display such as: digital, hardcopy, video, software, computer memory displays or an audible indicator. While it is possible to actually measure the relative phases of the orthogonal components of the beam 12 after exiting the transducer, the relative phase shift can also be derived from the intensities of the AM signals 35 and 36 shown in FIG. 8 without using complex and costly approaches as involved in direct phase measurements. Therefore, in the present invention, when the two AM signals 35 and 36 are separated from a single differential phase shifted signal using a properly oriented polarizing beam splitter 80, the beam's polarization state is analyzed to obtain AM intensity signals. The AM signals 35 and 36 extracted from the beam's polarization state by the splitter 80 are transmitted to and used in the signal processor 62 where their complementary nature facilitates rejection of common mode noise and minimizes effects of temperature dependent intrinsic birefringence that may reside in the transducing medium or other optical components within the system. This feature of the present invention substantially enhances accuracy and practicality of the system and represents an additional advancement over much of the prior art . The signal processor 62 performs these functions while converting the received AM signals 35 and 36 into a single, highly accurate voltage measurement . In addition to measuring the voltage of a device, the invention may be used in conjunction with a device for measuring current to provide information regarding power, power factor angle, and energy on the conductor of interest. As mentioned, each AM signal, 35 and 36 (FIG. 8) is converted by a photo-detector 43 and 44 (FIG. 1) into a electrical signal 45 and 46 (FIG. 1) which can be processed by the signal processor 62. The photo- detector comprises an optic-to-electronic conversion means for converting said AM signals into analog electronic signals. Preferably, the analog electronic signals comprise low-level analog voltage signals or current signals . In the preferred embodiment of the present invention the electrical signals 45 and 46 are electronic signals transmitted to the signal processor 62 which correspond to the intensity of the AM signals 35 and 36. Thus, in the practice of the present invention, a series of AM signals are manipulated by the signal processor 62, as each of the electrical signals 45 and 46 corresponds to intensity of eacn AM signal 35 and 36. The electrical signals 45 and 46 are sampled by the signal processor 62 at regular intervals and substantially simultaneously with one another. The sampled signals are the instantaneous intensity for each AM signal, 35 and 36 These intensity signals will be discussed below as (A) and (B) , respectively. In the signal processor 62 (FIG 1) the instantaneous intensity signal for each beam component is sampled sequentially and stored, thereby forming a data base of stored signals which represents each AM signal over time The stored signals are then converted into a displayable signal regarding the voltage of E-field at the transducer 5 (FIG 8) In the preferred embodiment signals are manipulated the following manner. First, an average intensity for each independent amplitude modulated signal is calculated. This is done by summing the instantaneous intensities of the signals which have been sampled over a pre-determined time interval and dividing by the number of samples taken m the mterval. In the preferred invention this is accomplished by taking the average of the signals over time for each beam component by summing the signals of each beam component and dividing the sum by the number of signal samples taken Mathematically, the average intensity for the AM signal (A) is expressed as follows: A = (1/L) Σ where the average intensity is (A) , the instantaneous AM signal is (A , the number of samples is (L) , the samples are taken and stored at uniform time intervals d) , and the average is calculated usmg samples between present time index n and past time index (n- L) Similarly, the average intensity for the AM signal (B) is expressed as follows- B 1/L) B, l-n where the average intensity is (I) , the instantaneous AM signal is (BJ , with the other values being as above. Next, an adjusted instantaneous intensity for each signal is found by comparing the most recent instantaneous signal intensity with the average signal intensity of the correspondmg AM signal Thus, for the beam component correspondmg to AM signal (A) , the adjusted instantaneous intensity (I n ) is: I n = -A,, ; Where at (A is the instantaneous intensity of AM signal (A) at the present time index Similarly, for AM signal (B) , the adjusted instantaneous intensity (J n ) is: J n = B-B n Where (B n ) is the instantaneous intensity of signal (B) at the present time It will be recognized by those skilled in the art that because signals (A) and (B) each represents a different axis on the polarization ellipse, their amplitudes will change in opposite directions from one another for a given change m polarization. Thus where the intensity of one signal increases there will be a decrease of intensity of equal magnitude in the other signal. Therefore, the adjusted instantaneous intensity signals (I n ) and (J n ) must be computed as indicated above in order to preserve sign. The adjusted average instantaneous intensity signal for both signals (A) and (B) compensates for any temperature induced birefringence that may exist within the transducer. Temperature mduced birefringence causes a change m the intensity of the AM signals over time, as the transducer heat or cools. The variation in the intensity due to temperature- dependant intrinsic birefringence of the transducer appears as a modulation or variation in the average intensity. Thus, by comparing the instantaneous intensity with the average intensity of the signals, and deducting the average intensity from the instantaneous intensity, temperature induced variations of the signal due to the birefringence m the transducer are compensated for in the adjusted instantaneous intensity signals (I n ) and (J n ) . An additional manipulation of the adjusted instantaneous intensity signals (I n ) and (J n ) compensates for intensity fluctuations and other common mode noise. This is accomplished by comparing the average of the adjusted instantaneous intensity signals (I and (J 1 ) for the signals (A) and (B) . This comparison entails calculating the average between (I n ) and the sign-reversed value of (J r ) . K n = _ ι n __ι n _ . 2 This average (KJ is directly proportional to the voltage. This is so because the Pockels electro-optic effect induces a differential phase shift in the orthogonal planes of the beam 12 (FIG. 8) which is directly proportional to the E-field, and the E-field is directly proportional to voltage. Thus, for a sampling of interest (n) , the average instantaneous intensity signal (K n ) for the signals (A) and (B) is directly proportional to the actual instantaneous voltage (V n ) between energized conductor and ground, varying only by a scaling constant (k) . v n = kκ n = k H n ^J n l 2 The scaling constant (k) is determined by applymg a precisely known voltage to the device of interest and adjusting the scaling constant (k) until the value measured as the actual instantaneous voltage (V n ) is equivalent to the precisely known voltage being applied. In a typical general application of the present invention, shown in FIG. 1, the sensor head 4 is placed in an insulator 50 between a conductor 52 and a grounded conductor 48. When voltage is applied to the conductor 52 an E-field is created between the conductor 52 and the grounded conductor 48, m the insulator 50. Determination of the scaling constant (k) is accomplished by applying a precisely known voltage to the conductor 52. Once the scaling constant (k) is known the electro-optical voltage sensor system may be operated to determine additional actual instantaneous voltages applied to conductor 52. An alternative embodiment m accordance with the present mvention is illustrated FIG. 2, which is a diagram of the electro-optical voltage sensor system. Wherever practicable, components in the alternative embodiment which are equivalent those discussed above have the same reference numbers. In this embodiment there is shown a transmitter 1, which comprises a laser (not shown) , a polarizer 6, and a wave plate 9. The laser emits an electromagnetic radiation beam 12. The electromagnetic radiation beam 12 passes first through a polarizer 6 and then a wave plate 9, producing a polarized beam 12 which may be circular- polarized. The beam 12 enters mto a PM optic fiber 18 through a collimator 20. The PM optic fiber 18 may further comprise a low-birefrmgence optic fiber The optic fiber 18 routes the beam 12 to a sensor head generally designated at 16 It is important to note that the sensor head 16 m this alternative embodiment shown m FIG. 2 differs from the sensor head 4 of the preferred embodiment shown m FIG. 1. The detector generally depicted at 8, as shown m FIG. 2, comprises a polarizing beam splitter 80, at least two photo-detectors 43, 44, a signal processor 62. The beam 12 is routed from the sensor head 16 through another PM optic fiber 19 through a collimator 23 and into the polarizing beam splitter 80. Again, as shown m FIG. 3, the polarizing beam splitter 80 separates the polarized beam 12 m accordance with the respective separate wave components propagating the orthogonal axes of the polarization ellipse mto AM signals 35, 36. In the embodiment shown m FIG 2, the AM signals 35, 36 which are analog optic signals, are routed through multi-mode or smgle-mode optic fibers 37, 38 to the photo-detectors 43, 44. The photo-detectors convert the AM signals 35, 36 into electrical signals 45, 46 which can be analyzed m the signal processor 62. Prior to discussing the sensor head 16, consider the collimators 20, 21, 22, 23, 24, 25 in FIGS. 2, 7a, 7b, and 7c and collimators 26, 27 and 28 in FIG. 8, which each are generally represented by the collimator 29, shown in FIG. 4. Generally, a collimator 29 comprises a lens 30 and a transparent end 31 which can pass a beam 12 mto or out of the core 32 of an optic fiber 40. A collimator used to couple light mto the core of an optic fiber is sometimes also referred to as a "coupler" m the art, but the term "collimator" is used herein for simplicity. In the preferred embodiment, the optic fiber 40 is a PM optic fiber 18, which may also take the form of low-birefringence fiber. Referring to FIGS. 7a, 7b, and 7c, these alternative embodiments of the sensor head 16 comprise a transducer 5 and a reflector 17. In FIG. 7a the beam 12 enters into the sensor head 16, through a collimator 21 which is attached to a PM fiber 18. The beam 12 then passes through the transducer 5 and upon being reflected by a beam reflector 17 enters into a second collimator 22. The second collimator 22 is connected to an optical fiber 19 by which the beam 12 is routed away from the sensor head 16. In this embodiment (and that in FIG. 7b) , the beam only passes through the transducer once . Similarly, in the practice of the alternative embodiment of FIG. 7b, the beam 12 enters into the sensor head 16, through a collimator 21 which is attached to a PM fiber 18, following which it is reflected by the beam reflector 17 into the transducer 5. The beam 12, after passing through the transducer 5 would enter into a second collimator 22 connected to an optical fiber 19 and be routed away from the sensor head 16. Likewise, in the practice of the alternative embodiment of FIG. 7c, the beam 12 enters into the sensor head 16, following which it travels through the transducer 5. The beam 12 is then reflected by the beam reflector 17 back through the transducer 5, and into a second collimator 22 connected to an optical fiber 19. The beam 12 is then routed away from the sensor head 16. In the embodiments of FIGS. 1 and 2, the sensor heads 4 and 16 each have a cross-sectional area of only approximately fifty millimeters squared (50 mm 2 ) or less, and a length of approximately twenty five centimeters (25 cm) or less, depending upon the particular apparatus in which the sensor head is embedded. There are two alternative embodiments of the transducer 5 which vary according to intrinsic birefringence. The first embodiment of the transducer 5, as shown in FIG. 5, is particularly appropriate where the transducer material 5 does not exhibit intrinsic birefringence along the propagation axis, shown as z. The beam 12 propagates along axis z. The transducer 5 in the presence of the E-field 90 causes differential phase modulation in the orthogonal planes of the beam 12. The embodiment shown in FIG. 5 is preferred where the transducer 5 exhibits no intrinsic birefringence. It is desirable to avoid intrinsic birefringence, as it is typically temperature dependant . The second embodiment for the transducer 5 which exhibits intrinsic birefringence is shown in FIG 6. Here, the transducer 5 and a second transducer 11, have matched intrinsic birefringence to one another along the propagation axes, shown as y' . The transducer 5 is aligned with the second transducer 11 such that the optic axes y' are rotated ninety degrees (180°) with respect to one another. The E-field 90, aligned along the z axes, achieves a reverse polarity in the second transducer 11. The orientation of the beam 12 with respect to the optic axes y' is preserved by the rotation of the beam 12 by ninety degrees (90°) . This rotation of the orientation is achieved by placement of a 90° polarization rotator 7 between the first transducer 5 and the second transducer 11. This configuration achieves cancellation of the effects of intrinsic temperature dependant birefringence, while yielding a differential phase shift in each transducer 5, 11. Thus, in this embodiment, the beam 12 goes through the transducer 5 to the 90° polarization rotator 7, and thence through the second transducer 11. There are a number of expressions of the E-field originator 96 which will now be discussed. The first, shown in FIG. 9, is a shielded joint 100. A shielded joint 100 is used to connect shielded conductors 52 to one another, and may take the form of either a splice or pre-molded connector. In the preferred embodiment the two conductors 52 connected to one another are each enclosed within insulation 50, around which is a semi-conducting jacket 109 and a cable ground shield 111. Around the conductor connecting means 104 is a layer of shielded joint insulation 108 and a joint ground shield 102. The joint ground shield 102 is supported in place by the end caps 115. A ground shield connector 113 can be used to maintain a common ground potential upon the cable ground shields 111 and the joint ground shield 102. The cable ground shields 111 are electrically connected by conductive wire 106 attached to ground shield connector 113. Alternatively, the cable ground shields 111 can be physically connected to the joint ground shield 102 at the intersection points without use of a ground shield connector 113 or conductive wire 106. The sensor head 4 is disposed between the joint ground shield 102 and the conductor connecting means 104. The optical fibers 18, 37, 38, route the beam to and from the sensor head 4. The E-field of interest, and into which the sensor head 4 is introduced, arises between the joint ground shield 102 and conductor connecting means 104 when an electric voltage is present upon the conductor connecting means 104. Another expression of the E-field originator 96 is the terminator 118 shown in FIG. 10. In the preferred embodiment showing a terminator 118, a conductor 52 is enclosed within insulation 50 forming a transition span. The insulation 50 is enclosed within a voltage gradient control means 120. A cable ground shield 111 may partially enclose the voltage gradient control means 120. The sensor head 4 is disposed between the conductor 52 and the voltage gradient control means 120. Optical fibers 18, 37, 38 route the beam to and from the sensor head 4. The E- field of interest, and into which the sensor head 4 is introduced, arises between conductor 52 and the voltage gradient control means 120 when a voltage is present upon the conductor 52. Another expression of the E-field originator 96 of FIGS. 1 and 2 is the through-hole insulator 124, here shown as a transformer bushing in FIG. 11. In the preferred embodiment showing a through-hole insulator 124, a conductor 52 is enclosed within insulation 50, which is enclosed within a grounded conductor 48. The through-hole insulator shown here as a transformer bushing has a mounting flange 126 for mounting the bushing and creepage distance skirts 128 which extend from the grounded conductor 48. The sensor head 4 is disposed between the conductor 52 and the grounded conductor 48. Optical fibers 18, 37, 38 route the beam to and from the sensor head 4. The E- field of interest, and into which the sensor head 4 is introduced, arises between the conductor 52 and the grounded conductor 48 when a voltage is present upon the conductor 52. Another expression of the E-field originator 96 of FIGS. 1 and 2 is the shielded cable or bus 129, shown in FIG. 12. In the preferred embodiment of a shielded cable or bus 129, a conductor 52 is enclosed within insulation 50, which is enclosed within a grounded conductor 48. The sensor head 4 is disposed between the conductor 52 and the grounded conductor 48. Optical fibers 18, 37, 38 route the beam to and from the sensor head 4. The E-field of interest, and into which the sensor head 4 is introduced, arises between the conductor 52 and the grounded conductor 48 when a voltage is present upon the conductor 52. Whereas FIG. 12 shows a bus having a round cross- section, an alternative and equivalent embodiment comprises a rectangular (or square) cross-section. Another expression of the E-field originator 96 shown in FIGS. 1 and 2 is the gas or oil-insulated switchgear 132, shown in FIG. 13. In the preferred embodiment showing a gas or oil-insulated switchgear 132, a conductor 52 is enclosed within gas or oil insulation 134, by a grounded conductive or se i- conductive containment means 140 for containing the gas or oil insulation. The sensor head 4 is disposed between the conductor 52 and the grounded containment means 140. Optical fibers 18, 37, 38 route the beam to and from the sensor head 4. The E-field of interest, and into which the sensor head 4 is introduced, arises between the conductor 52 and the grounded containment means 140 when a voltage is present upon the conductor 52. Another expression of the E-field originator 96 is the duct-enclosed bus 142, shown in FIG. 14. In the preferred embodiment of a duct-enclosed bus 142, a conductor 52 is enclosed within insulation 50 of sufficient thickness to minimize possibility of flash- over. The insulated bus is enclosed within a grounded duct or other grounded at least semi-conducting means 144. Those skilled in the art will appreciate that by the term "at least semi-conducting", it is meant all semi-conducting and conducting means, by which the bus can be grounded. The sensor head 4 is disposed between the conductor 52 and the grounded semi¬ conducting means 144. Optical fibers 18, 37, 38 route the beam to and from the sensor head 4. The E-field of interest, and into which the sensor head 4 is introduced, arises between the conductor 52 and the grounded semi-conducting means 144 when a voltage is present upon the conductor 52. Another expression of the E-field originator 96 is the clamp-on apparatus 147, shown in FIG. 15. In the preferred embodiment of the clamp-on apparatus, a conductor 52 is enclosed within a coaxial conductive grounded surrounding means 149. In the practice of the invention, the conductor 52 is preferably a nonshielded transmission line, a nonshielded cable, or a nonshielded bus. The conductor 52 is separated from the conductive grounded surrounding means 149 by insulated standoff means 151. The sensor head 4 is disposed between the conductor 52 and the coaxial conductive grounded surrounding means 149. Optical fibers 18, 37, 38 route the beam to and from the sensor head 4. The E-field of interest, and into which the sensor head 4 is introduced, arises between the conductor 52 and the coaxial conductive grounded surrounding means 149 when a voltage is present upon the conductor 52. FIG. 16 is an alternative embodiment of the electro-optical voltage sensor of FIG. 1, having a current detector 153 disposed substantially in common with the sensor head. The current detector 153 detects the current, not shown, passing through the conductor 52 by detecting the magnetic field, not shown, associated with the current. The current detector provides a current signal, not shown, which is routed through a current signal routing member 156 to the signal processor 62. In one embodiment the optical current signal routing member 156 consists of optic fiber, photodetection means, and electrical connecting means, none of which are shown. Where voltage (V) and current (I) are known, the power (P) can be determined by the signal processor by multiplying the current (I) by the voltage (V) as follows : P= IV A combination of at least two sensors of the present invention may be used to achieve a line-to- ground voltage measurement on separate conductors of a multi-source system. "Multi-source system" is meant a to include both a multi-phase as well as a multi-line system. In such a system, line-to-ground measurements may also be used to calculate line-to-line voltages through simple subtraction of line-to-ground values. The present invention represents a significant advance over the prior apparatus, methods and art of voltage measurement . The present invention does not require any additional electronics to bias the transducing material to determine voltage, such as a voltage divider. Voltage is determined in the present invention by utilizing the E-field that exists within many types of devices to transmit and distribute power, often these power distribution devices are co- axial, which simplifies the application of the present invention. The E-field, which is proportional to voltage, is used to bias a transducing element in order to induce a differential phase shift in the orthogonal planes of the beam, which as modulated optic signals, is proportional to voltage. It is noted that many of the advantages of the present invention accrue due to the simplified structure of the sensor head, which is sufficiently small so as to be conveniently installed in devices in which E-fields arise, or built in as part of a sensor. Although the prior art apparatus and methods for voltage measurement have attempted to use the electro- optical effect in materials having either a Pockels or Kerr coefficient, they have typically required a separate compensator crystal with a known reference voltage or a separate voltage divider directly connected to the energized conductor in order to make a voltage measurements The result has been devices which were bulky and required additional electronics for measuring the known reference, or required extra hardware presenting size, weight, expense, reliability, and other problems By using the sensor head of the present invention, which may be installed or built mto the described voltage transmission and distribution apparatus, voltage measurement is achieved without the use of a large, dedicated, stand-alone voltage division device. Real estate withm Power substations s at a premium, thus this sensor system offers a substantial economic advantage due to space savings In addition, contact with the energized conductor is substantially reduced and in most cases altogether eliminated with the practice of the present invention This is advantageous, as an energized conductor can present significant life and health risks among other hazards where high voltages are involved Further, the practice of the present invention does not interfere with the apparatus being measured, and avoids various other problems associated with the use of the voltage dividers in the prior art Those skilled m the art will appreciate from the preceding disclosure that the objectives stated above are advantageously achieved by the present mvention It is to be understood that the above-described arrangements are only illustrative of the application of the principles of the invention. Numerous modifications and alternative arrangements may be devised by those skilled m the art without departing from the spirit and scope of the present invention and the appended claims are intended to cover such modifications and arrangements.

Claims: CLAIMS What is claimed: 1. A sensor for sensing voltage in an E-field, said voltage sensor comprising: transmitting means for transmitting at least one beam of polarized electromagnetic radiation, said beam having at least two components propagating along at least two orthogonal planes, respectively, to form at least two orthogonal beam components; sensing means for sensing the presence of an E- field and inducing a differential phase shift on the orthogonal beam components when said sensing means is in said E-field; detecting means for detecting said differential phase shift of said orthogonal beam components; and first and second routing means, said first routing means including a first translucent element for routing said beam from said transmitting means to said sensing means, and said second routing means including a second translucent element for routing said beam components from said sensing means to said detecting means. 2. The sensor as in claim 1, wherein said routing means further comprises: first reflection means for reflecting said beam between said sensing means and said second translucent element, wherein said second translucent element routes said beam from said sensing means to said detecting means. 3. The sensor as in claim 1, wherein said routing means further comprises: second reflection means for reflecting said beam between said first translucent element and said sensing means, wherein said first translucent element routes said beam from said transmitting means to said sensing means 4. The sensor as in claim 1, wherein said first and second translucent elements each comprise at least one optic fiber, wherem said at least one optic fiber comprises an optic fiber selected from the group consisting of: (1) a single-mode optic fiber, and (2) a multi-mode optic fiber. 5. The sensor as in claim 4 , wherein at least one of said optic fibers comprises a polarization maintaining (PM) optic fiber for routing said beam with decreased loss of polarization of the beam. 6. The sensor as in claim 4, wherein at least one of said optic fibers comprises a low birefringence optic fiber for routing said beam with decreased loss of polarization of the beam. 7. The sensor as m claim 1, wherem said sensing means further comprises: beam separation means for separating orthogonal beam components oriented along the axes of the beam's polarization ellipse (whose ellipticity varies between -1 and +1 proportion to voltage) and forming at least two independent amplitude-modulated signals therefrom, respectively. 8. The sensor as m claim 1, wherein said detectmg means further comprises. beam separation means for separating orthogonal beam components oriented along the axes of the beam's polarization ellipse (whose ellipticity varies between -1 and +1 m proportion to voltage) and forming at least two independent amplitude-modulated signals therefrom, respectively; processmg means for converting said independent- amplitude modulated signals mto at least one display signal proportional to the voltage of said E-field. 9. The sensor as m claim 8, wherein said processing means further comprises. optic-to-electronic conversion means for converting said AM signals into analog electronic signals, wherein said analog electronic signals comprise signals selected from the group consisting of: (1) low-level analog voltage signals, and (2) current signals. 10. The sensor as in claim 9, wherein said processmg means further comprises: analog-to-digital conversion means for converting said analog electronic signals into at least one digital electronic signal. 11. The sensor as m claim 1, wherein said sensor further comprises at least one shielded cable joint, said shielded cable joint comprising. at least two conductors, at least one conductor connecting means, and at least one ground shield; said at least two conductors are connected to one another by said at least one conductor connecting means, wherein said sensing means is disposed between said at least one conductor connecting means (or said conductors) and said at least one ground shield 12. The sensor as m claim 1, wherein said sensor further comprises at least one terminator, said at least one terminator comprising: at least one conductor, insulating means for insulating said conductor, said insulating means forming a transition span, and voltage gradient control means for a smoothing and controlling of the voltage gradient across the transition span, wherein said sensing means is disposed m said insulating means. 13. The sensor as m claim 1, wherein said sensor further comprises at least one through-hole insulator, said through-hole insulator comprising: at least one conductor, at least one grounded conductor, and insulating means for insulating said conductor, said insulating means residing between said at least one conductor and said at least one grounded conductor, wherein said sensing means is disposed in said insulating means between said conductor and said grounded conductor. 14. The sensor as m claim 1, wherem said sensor further comprises at least one shielded bus, said shielded bus comprising: conducting means for conducting electricity, wherein said conducting means comprises a bus, and at least one grounded co-axial conductor disposed co-axially with respect to said bus, wherein said sensing means is disposed between said conducting means and said grounded co-axial conductor. 15. The sensor as in claim 1, wherein said sensor further comprises at least one shielded cable, said shielded cable comprising: conducting means for conducting electricity, wherein said conducting means comprises a center conductor, and at least one grounded co-axial conductor disposed co-axially with respect to said center conductor, wherein said sensing means is disposed between said conducting means and said grounded co-axial conductor 16. The sensor as m claim 1, wherein said sensor further comprises at least one insulated switchgear, said insulated switchgear comprising: at least one conductor; insulation, wherein said insulation comprises a material selected from the group consisting of : (1) oil, and (2) gas; and grounded containment means disposed around said conductor for containing said insulation in a surrounding position around said conductor, said insulation functioning to insulate said conductor, wherein said sensing means is disposed between said conductor and said grounded containment means 17. The sensor as m claim 1, wherein said sensor further comprises at least one duct-enclosed bus, said bus comprising: conducting means for conducting electricity, wherem said conducting means comprises a bus, insulation means, said insulation means is disposed around said conducting means and havmg sufficient thickness to minimize flash-over, and grounded at least semi-conductive means for a grounded shield, wherein said grounded semi-conductive means is disposed around said conducting means and said insulation means, wherein said sensing means is disposed outside of said conducting means, withm said insulation and said grounded semi-conductive means 18. The sensor as m claim 1, wherein said sensor further comprises at least one clamp-on apparatus, said clamp-on apparatus comprising, at least one conductor, wherein the conductor comprises a conductor selected from the group consisting of: (1) a nonshielded transmission line, (2) a nonshielded cable, and (3) a nonshielded bus; conductive co-axial grounded surrounding means havmg a cross-sectional shape correspondmg to said conductor and a size larger than said at least one conductor; and insulated standoff means for separating said surrounding means from said conductor and for holding said surrounding means when said surrounding means is placed around said conductor, wherein said sensing means is disposed between said at least one conductor and said surrounding means . 19. The sensor as in claim 1, wherein said sensing means further comprises: first sensing means having a first optical propagation orientation; second sensing means havmg a second optical propagation orientation, said propagation orientation of said second sensing means being oriented at a 180 degree angle to said first optical axis of the first sensing means; and ninety degree polarization rotator means disposed between said first sensing means and said second sensing means for receivmg the beam from the first sensing means, rotating said beam ninety degrees, and passing said beam into said second sensing means. 20. The sensor of claim 1, wherein said sensor further detects the presence and magnitude of a magnetic field caused by a current, wherem said sensor further comprises: current detection means for detectmg said magnetic field and determining the current therefrom, said current detection means being disposed substantially common with said sensing means. 21. The sensor of claim 1, wherein said sensor further comprises: buffering means for buffering the sensing means to uniformly transition the E-field mto the sensing means, wherein said buffering means include a dielectric buffering material whose dielectric properties are substantially similar to those of the sensing means, disposed substantially m common with the sensing means . 22 A combination of at least two sensors of claim 1, wherein each said sensor achieves a l e-to- ground voltage measurement on a separate conductor of a multi-source system wherein said line-to-ground measurements may be further used to calculate line-to- line voltages m said system by simple subtraction of line-to-ground values 23. A method of using a sensor head as part of a system for sensing voltage in an E-field, said sensor head having an electro-optical sensing means for inducing a differential phase shift of at least two beam components propagating m at least two orthogonal planes as electromagnetic wave components of a beam of electro-magnetic radiation when said sensor head is an E-field of an apparatus having a voltage the E- field, said method comprising the steps of (a) transmitting an electromagnetic radiation beam having at least two beam components propagating along at least two orthogonal planes, respectively; (b) routing said beam from said transmitting means to said sensor head to induce a differential phase shift of the beam components; (c) routing said beam from said sensor head to processing means; and, (d) processing said beam components by converting said beam components into at least one electrical signal, wherein said signal is proportional to the voltage of the E-field at the sensor head. 24. The method as defined in claim 23, wherein the routing of step (c) further comprises: separating specific beam components from said beam into at least two independent amplitude modulated signals, each independent amplitude modulated signal comprising a beam component. 25. The method as defined in claim 23, wherein the processing of step (d) further comprises the steps of: (e) sampling the electrical signal at substantially regular intervals, said sampling occurring substantially simultaneously for all beam components; (f) storing said sampled signal; and (g) manipulating said sampled signal of each beam component so as to convert said signals into a display signal, said display signal being proportional to the voltage of said E-field. 26. The method of claim 25, in which the manipulating of step (g) further comprises the steps of: (h) determining an average electrical signal for each beam component by summing the sampled electrical signals of each beam component over a specified time mterval and dividing said sum by the number of samples of the beam component taken in that mterval, (1) determining an adjusted instantaneous signal for each beam component by comparing the most recent electrical signal of the beam component sampled with the most recently calculated average electrical signal of the beam component and taking the difference thereof ; ( ) determining an adjusted average instantaneous signal for all beam components by summing the adjusted instantaneous signal of each beam component and dividing the same by the number of beam components; and (k) determining a scaled adjusted average instantaneous signal by proportionally mcreasmg the scaled adjusted average instantaneous signal by multiplying said adjusted average instantaneous signal by a scaling constant; said scaled adjusted average instantaneous signal is a display signal representing voltage between ground and the energized conductor on which the voltage measurement is being taken. 27 The method of claim 25, further comprising the step of : (1) displaying said display signal on display means, wherein said display means for displaying said display signal is selected from the group consisting of: (1) a digital display; (2) a hardcopy display, (3) a video display; (4) a software display; (5) a computer memory; and (6) an audible indicator 28 The method of claim 23 wherein said steps are performed on each of at least two sensors, and further comprising the step of (m) calculating l e-to-lme voltage between at least two energized conductors by subtracting the lme-to-ground voltages of the conductors of interest. 29. A method for measuring voltage using the electro-optic effect of electromagnetic radiation on matter, comprising the steps of: transmitting at least one beam of polarized electromagnetic radiation having at least two beam components propagating along at least two orthogonal planes, respectively, routing said at least one beam through at least one translucent element into sensing means; modulating said at least one beam as it passes through said sensing means so as to cause a differential phase shift of said at least two beam components m said at least two orthogonal planes of said at least one beam when said sensing means is m an E-field, wherein said differential phase shift produces a correspondmg change in said beam's polarization state, separating at least two beam components mto at least two independent amplitude modulated signals correspondmg to conversely modulating intensities along the two orthogonal axes of beam's said polarization ellipse whose elliptocyte modulates between -1 and +1 proportion to voltage; converting said at least two independent amplitude-modulated signals mto at least one display signal, said at least one display signal being proportional to the voltage of said E-field; and displaying said display signal such that the voltage of the E-field may be ascertained. 30. A sensor head for use in combination with at least one beam of electromagnetic radiation for detecting presence and magnitude of E-field and voltage, said sensor head comprising: polarizing means for polarizing said at least one beam such that said at least one beam comprises at least two beam components in at least two orthogonal planes; transducing means for receiving said at least one beam from said polarizing means and inducing a differential phase shift of the beam components which varies in magnitude in response to the magnitude of an E-field; and first reflecting means for receiving said at least one beam from said transducing means and reflecting said beam back into said transducing means. 31. The sensor head as in claim 30, wherein the sensor head further comprises: quarter wave retarding means for biasing the beam's polarization such that zero E-field magnitude on the transducer corresponds to a circular polarization state. 32. The sensor head as in claim 30, wherein said reflecting means comprises a material having at least one surface, a reflective coating disposed on at least one surface of said reflecting means wherein said reflective coating accomplishes reflection of said beam. 33. The sensor head as in claim 31, wherein said quarter wave retarding means resides within said reflecting means, said reflecting means further comprising: phase shifting means for shifting the phase of at least one of said beam components to thereby achieve a differential phase shift between said beam components of one-quarter of a wavelength, said quarter wavelength shift comprising at least a single order shift. 34. The sensor head as in claim 31, wherein said quarter wave retarding means comprises: a quarter wave plate disposed at a point within the path of said beam following said polarizing means for shifting the phase of at least one of said beam components one-quarter of a wavelength, said quarter wavelength shift comprising at least a single order shift . 35. The sensor head as in claim 30, wherein said transducing means further comprises a Pockels transducing material. 36. The sensor head as in claim 35, wherein said Pockels transducing material is a material selected from the group consisting of: Lithium Niobate (LiNb0 3 ) , Ammonium Dihydrogen Phosphate (NH 4 H 2 P0 4 ) , Ammonium Dideuterium Phosphate (NH 4 D 2 P0 4 ) , Potassium Dideuterium Phosphate (KD 2 P0 4 ) , MgO-doped Lithium Niobate (MgO-LiNb0 3 ) , Lithium Tantalate (LiTa0 3 ) , Electro-optic polymers, and Organic material . 37. The sensor head as in claim 30, wherein said sensor head further comprises: translucent means disposed between the polarizing means and the transducing means for receiving said at least one beam from said polarizing means and transmitting said beam to said transducing means. 38. The sensor head as claim 37, wherein said translucent medium further comprises a material that is substantially non-birefnngent and nonconductive. 39. The sensor head as m claim 30, wherein said sensor head further comprises : beam separation means for separating the beam components correspondmg to the major and minor axes of the polarization ellipse of said at least one beam, forming at least two signals therefrom. 40. The sensor head as m claim 39, wherein said sensor head further comprises translucent means disposed between the transducing means and the separation means for receiving said at least one beam from said transducing means and transmitting said beam to said separation means 41. The sensor head as m claim 39 wherein said at least two signals comprise independent converse amplitude-modulated signals. 42. The sensor head as m claim 38 wherein said translucent means comprises at least one material selected from the group consisting of: fused quartz, fused silica, and nonconductive translucent media. 43. The sensor head as m claim 38 wherein said translucent means comprises at least one fiber selected from the group consisting of. colli ator- coupled low-birefnngence fiber and polaπzation- mamtam g optic fiber. 44. A sensor head for use m combination with at least one beam of electromagnetic radiation for detecting an E-field, said sensor head comprising polarizing means for polarizing said at least one beam such that said at least one beam comprises at least two beam components m at least two orthogonal planes; transducing means for receiving said at least one beam from said polarizing means and inducing a differential phase shift of the beam components which varies in magnitude in response to the magnitude of an E-field, and second reflecting means for receiving said at least one beam from said polarizing means and reflecting said beam mto said transducing means. 45. The sensor head as in claim 44, wherein the sensor head further comprises: quarter wave retarding means for biasing the beam's polarization such that zero E-field magnitude on the transducer corresponds to a circular polarization state . 46. A sensor head for use m combination with at least one beam of electromagnetic radiation for detectmg an E-field, said sensor head comprising- polarizing means for polarizing said at least one beam such that said at least one beam comprises at least two beam components m at least two orthogonal planes,- transducing means for receivmg said at least one beam from said polarizing means and inducing a differential phase shift of the beam components which varies m magnitude in response to the magnitude of an E-field; beam separation means for receiving said at least one beam and separating the beam components and forming at least two signals therefrom, and third reflecting means receiving said at least one beam from said transducing means and reflecting said beam into said beam separation means 47. The sensor head as in claim 46, wherem the sensor head further comprises. quarter wave retarding means for biasing the beam's polarization such that zero E-field magnitude on the transducer corresponds to a circular polarization state. 48 A method for detecting an E-field using at least one beam of polarized electromagnetic radiation having at least two beam components propagating m at least two orthogonal planes, comprising the steps of: (a) imposing an E-field upon at least one transducing means by disposing said transducing means mto an apparatus containing electric flux proportional to voltage; (b) passing said beam through said at least one transducing means, (c) inducing a differential phase shift between the beam components when said beam passes through said transducing means said E-field, said differential phase shift indicating the presence and magnitude of said E-field; (d) reflecting said beam after said beam has passed through the transducing means with a reflective means, so that said beam is directed back into the transducing means, thereby causing said beam to reenter the transducing means; (e) separating beam components mto at least one pair of converse amplitude modulated (AM) signals, said AM signals corresponding to the major and minor axes of said beam's polarization ellipse, whose ellipticity modulates between -1 and +1 proportion to voltage, wherem intensity along each of said axes modulates conversely to the intensity exhibited along the other axis; (f) transmitting said AM signals, whereby the E- field magnitude (and hence voltage) can be ascertained.

Inventors: RENAK TODD W, WOODS GREGORY K, RENAK, TODD, W., WOODS, GREGORY, K.
Applicants: LOCKHEED IDAHO TECHNOLOGIES CO, LOCKHEED IDAHO TECHNOLOGIES COMPANY
Application year: 1996
Main classification: G01R19
IPC codes: G01R1, G01R15, G01R19