Electro-optic voltage sensor for sensing voltage in an E-field

Electricity: measuring and testing – Measuring – testing – or sensing electricity – per se – Using radiant energy

Reexamination Certificate

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Details

C324S750010

Reexamination Certificate

active

06362615

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention The present invention relates generally to an electro-optic high voltage sensor for sensing and/or measuring an E-field produced by an energized conductor. More particularly, it concerns an electro-optic voltage sensor which utilized the Pockels electro-optic effect to measure voltage.
2. 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.
U.S. Pat. No. 5,892,357, issued Apr. 6, 1999, and assigned to the same assignee of the present invention, discloses an electro-optic voltage sensor which may be disposed in an E-field between an energized conductor and a grounded conductor without contacting the energized conductor. The electro-optic voltage sensor utilizes a Pockles crystal or transducer which is sensitive to the E-field and induces a differential phase shift on a beam of electro-magnetic radiation traveling through the sensor in response to the E-field. Although the electro-optic voltage sensor solves many of the problems with the prior art, it still has some drawbacks. For example, the electro-optic voltage sensor disclosed in the above mentioned co-pending application utilizes a beam splitter to separate orthogonal polarization components of the electro-magnetic radiation. The beam splitter directs one component out of the sensor in one direction, for example along a longitudinal axis of the sensor, and directs the other component out a different direction, perpendicular to the longitudinal axis of the sensor. Therefore, either both components exit the sensor from different sides, making the sensor difficult to locate between the conductor and grounded conductor, or an additional reflector is required to direct the other component so both components exit the same side, making the sensor large.
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 in 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 flier object of the present invention to provide such an electro-optic voltage sensor system which is capable of use in 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 is 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.
It is yet another object of the present invention to provide a sensor system with a sensor that is of small size.
While the present invention is described in terms of a sensor system, it is to be understood that the subject apparatus and method may be used in 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 device and 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 in the present invention, the effects of an E-field can be observed, a voltage measurement can be calculated.
The sensor device may be utilized to sense or measure an E-field using a source beam of electromagnetic radiation. The sensor device comprises a sensor body disposed in the E-field. The sensor has an input for receiving the source beam into the sensor body. The sensor body also has first and second outputs.
A polarization beam displacer is disposed in the sensor body and is optically coupled to the input. The polarization beam displacer separates the source beam into a first beam having substantially a first linear polarization orientation and a second beam having substantially a second linear polarization orientation. The polarization beam displacer also directs the first beam along a first path and the second beam along a different second path. The second beam may be discarded.
A wave plate is disposed in the sensor body and is optically coupled to the polarization beam displacer for rotating the first polarization of the first beam to a rotated polarization with major and minor axes.
A transducer is disposed in the sensor body and is optically coupled to the wave plate. The transducer induces a differential phase shift on the major and minor axes of the rotated polarization in response to the E-field when the transducer is exposed to the E-field.
A reflecting prism

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