Abstract:
Described are improved transmissive magneto-optical sensors that may be used to determine the magnitude and phase of a magnetic field surrounding a conductor, and when in contact with the conductor, the surface temperature of the conductor. The magneto-optical sensor may be made to be symmetric around the direction of propagation of the internal light, enabling ease of manufacturing as well as automated assembly and calibration. The magneto-optical sensor may also be made to be symmetric about the plane determined by the Faraday rotator material, thus enabling reciprocating optical paths for increased vibration and birefringence immunity. The disclosed sensors preferably include cylindrically symmetrical components, thereby making the sensor readily mass-producible.

Description:
[0001]    This application claims the benefit of U.S. patent application Ser. No. 60/331,385, filed Nov. 15, 2001, the entire disclosure of which is hereby incorporated herein by reference. 
     
    
     
       BACKGROUND OF THE INVENTION  
         [0002]    1. Field of the Invention  
           [0003]    The invention relates in general to optical sensors that detect the Faraday effect in crystal media, and more specifically, the class of transmissive optical sensors that rotate the plane of polarization of light traveling through a crystal media that is under the influence of external quantities such as magnetic fields, electrical currents which give rise to magnetic fields, or temperature fluctuations.  
           [0004]    2. Related Art  
           [0005]    More than 150 years ago, Michael Faraday discovered that when linearly polarized light travels through flint glass that is exposed to a magnetic field, its plane of polarization rotated. This property, now known as the Faraday effect, is widely used in the fiber optic telecommunications field, specifically to prevent reflected light energy from coupling back into a light source and changing source parameters such as frequency or power output. In sensor systems that exploit the Faraday effect, a sensor assembly is placed into a magnetic field. By monitoring the rotation of the incident polarization state, a direct measurement of the magnetic field intensity can be inferred. The relationship governing this phenomenon is best stated as:  
           Θ= VHl    EQN(1)  
           [0006]    where Θ is the measured angle of rotation of the field, V is a constant known as Verdet&#39;s constant, H is the applied magnetic field, and l is the optical path length. All materials exhibit the Faraday effect, but the magnitude varies greatly. For example, the Verdet constant for a SiO 2  crystal is approximately 3.2e−4 (deg/cm-Oe), while in ferromagnets such as the value can be on the order of 6.0e+5 (deg/cm-Oe).  
           [0007]    When an optical path completely encircles a conductor, a numerical integration can be performed about the optical path, which results in the ability of relating the Faraday rotation directly to the current flowing through the optical path. In this instance, the rotation is related to current I by a form of Ampere&#39;s Law:  
           Θ= VHdl    EQN(2)  
           Θ= VI    EQN(3)  
           [0008]    Finally, if N optical paths exist around the conductor, the total current in the conductor is  
             I   =     Θ   VN             EQN                   (   4   )                                 
 
           [0009]    Optical fiber is one material that exhibits a small Faraday effect. Based upon this, devices have been known and used for measuring the amount of current flowing through a conductor. By wrapping multiple turns of optical fiber around the conductor and applying Ampere&#39;s Law, the amount of current can be directly measured. Sensitivity is controlled in this fashion: applications requiring higher sensitivity wrap a higher number of turns around the conductor being monitored.  
           [0010]    Unfortunately, using optical fiber as a sensor is often impractical in many applications because it is not feasible to interrupt power by disconnecting the conductor, installing the fiber coil assembly, then reconnecting the conductor. Another disadvantage of an all-fiber sensor is that in practical use, the loops that encircle the conductor can be no smaller than 4-5 cm in diameter. Violation of this condition typically results in tremendous temperature sensitivity, which then appears as an undesired rotation of the state of polarization of the desired signal.  
           [0011]    Bulk glass is another material that exhibits a Faraday effect. An advantage of the use of bulk glass is that the sensor can be fabricated from materials with a higher Verdet constant, which improves the sensitivity to the influencing magnetic field. These bulk crystals can be annealed, which can release internal stresses, thereby reducing linear birefringence. By themselves, bulk-glass sensors are relatively mechanically stable in both temperature and mechanical handling. Bulk glass can be made relatively inexpensively, which portends well for mass production concepts using these sensors.  
           [0012]    Bulk-glass sensors suffer from their own set of limitations. The transducers manufactured from bulk glass are large, relatively on the same order as the all-optical fiber sensors previously described. Bulk glasses are not ferromagnetic, hence their Verdet constants are lower, which restricts their applications to extremely high current measurement. Obtaining multiple circular paths around a bulk-glass arrangement in order to increase the sensitivity of the sensor has been accomplished by some researchers, but there are limitations of using this configuration in applications that experience tremendous temperature fluctuations. Finally, assembly and alignment of bulk-glass sensors has historically been performed by hand, resulting in tremendous labor costs that preclude their widespread use.  
           [0013]    Ferromagnetic materials, such as bismuth- and terbium-doped yttrium-iron-garnet (BiTb 2 Y 3 Fe 5 O 12 ) for example, have much larger Verdet constants per unit thickness. This results in a much smaller Faraday rotator to measure a given magnetic field strength, and the outcome is that a whole class of reduced size magneto-optical transducers is enabled. Methods to grow these materials are well established and directly support other markets, specifically optical telecommunications, hence tremendous economies of scale are realized that surpass that of bulk-glass and rival the cost of optical fiber. Packaging of the transducer becomes smaller with the introduction of high-Verdet constant materials, and thus manufacturing costs are significantly less than what is available with all-fiber or bulk-glass designs.  
           [0014]    Applications for a reduce-sized magneto-optic transducer continue to grow. For example, the electric utility industry is experiencing tremendous pressures as consumer and regulatory demands upon the industry increase. Consumers, with expanding telecom, data processing, and other energy needs, are demanding “high-nines” reliability. Utilities are attempting to respond, but are doing so with an antiquated infrastructure that has an average age of 31 years. Regulatory pressures have created large uncertainties in the future ownership of assets, and hence infrastructure improvements have fallen sharply since the mid 1990&#39;s. Additionally, many utilities operate under rate caps and cannot pass costs onto consumers. Not surprisingly, the industry is looking to conserve capital, and is doing so by pushing equipment harder without fully understanding the long-term consequences, as well as deferring maintenance until corrective action is required. Even small percentage changes in distribution system operating efficiencies can result in hundreds of millions of dollars a year in savings. Hence, many utilities are reviewing technologies that can provide efficiency and reliability improvements.  
           [0015]    Optical sensor technologies for utility applications promise to deliver lower-cost monitoring solutions to the industry. These technologies provide an entirely new means of measuring electrical current, conductor temperature, voltage, and combustible gasses. When combined with the latest wireless and network topologies, automated data delivery and control is possible, resulting in improved operations. Optical sensory systems which cost less than current state-of-the-art transformer-based systems gives utilities the key to unlocking information by which they can manage their systems much more efficiently, resulting in improved reliability and improved system efficiencies. Furthermore, widespread use of these technologies will result in the immediate notification and location of power faults and outages, potentially saving the utility industry and it&#39;s customers 100&#39;s of millions of dollars in outage costs.  
           [0016]    U.S. Pub. No. US2001/0043064A1 to Bosselmann et al. discloses a pi-shaped transmissive polarimetric sensor that is comprised of a polarizer, a sensor element, and an analyzer. An output optical waveguide with a core diameter of at least 100 μm is used. The input light is uncollimated and unfocused. The sensor requires the use of a prism to steer the light from the input fiber to the sensor element, and correspondingly, from the sensor element to the output optical waveguide.  
           [0017]    U.S. Pat. No. 6,404,190 (2002) to Itoh et al. discloses a pi-shaped transmissive polarimetric sensor that is comprised of an input optical fiber, a polarizer, a magneto-optical device, a second polarizer comprising an analyzer, and an output optical fiber. Itoh et al. present three embodiments: one that uses spherical or hemispherical lens at each of the fibers, one that omits the polarizers and uses fiber to provide the polarization/analyzer function, and one that uses plastic optical fiber.  
           [0018]    U.S. Pat. No. 6,347,885 (2002) to Duncan discloses the use of rare-earth iron garnet magneto-optical films in reflection-type magneto-optical sensors as well as presenting several optical and signal processing topologies that can be used to measure the Faraday rotation due to a changing magnetic field.  
           [0019]    U.S. Pat. No. 6,370,288 (2002) to Itoh et al. discloses a pi-shaped transmissive polarimetric sensor that is arranged as a confocal optical system comprised of a input optical fiber, a drum lens, a polarizer, a magneto-optical device, a second polarizer comprising an analyzer, a second drum lens, and an output optical fiber. In this disclosure, one holder contains both the input drum lens and the output drum lens.  
           [0020]    U.S. Pat. No. 6,160,396 (2000) to Itoh et al. discloses a pi-shaped transmissive polarimetric sensor that is comprised of an input optical fiber, a first lens, a first mirror, a polarizer, a magneto-optical device, an analyzer, a second mirror, a second lens, and an output fiber. Integrated holders are used to hold the discrete optical components.  
           [0021]    U.S. Pat. No. 5,861,741 (1999) to Itoh discloses a linear, transmissive polarimetric sensor that uses multimode optical fiber for the input and output fibers. Only one rod lens is used to couple the energy from the input fiber to the output fiber.  
           [0022]    U.S. Pat. No. 5,742,157 (1998) to Ishizuka et al. discloses a pi-shaped transmissive polarimetric sensor that uses one GRIN lens to launch and recover the optical energy in a configuration similar to that disclosed by Itoh et al. in U.S. Pat No. 6,160,396.  
           [0023]    U.S. Pat. No. 5,485,079 (1996) to Itoh discloses a linear, transmissive polarimetric sensor comprised of a first lens, a polarizer, a magneto-optical element, an analyzer, and a second lens. Itoh further discloses that this sensor system is a light converging optical system.  
           [0024]    U.S. Pat. No. 5,475,298 (1995) to Rogers discloses a reciprocal optical system that dynamically compensates for external perturbations that change the properties of an optical wavefront traveling within an optical fiber.  
           [0025]    U.S. Pat. No 5,321,258 (1994) to Kinney discloses a pi-shaped optical sensor unit that is capable of being manufactured as a small sensor package as a result of a novel housing used to align the magneto-optical sensing element with the incoming wavefront. The design eliminates the need for mirrors, prisms, or collimating lenses.  
           [0026]    U.S. Pat. No. 5,202,629 (1993) to Seike et al. discloses a pi-shaped magneto-optical sensor having a magneto-optical element, a polarizer, an analyzer, and a substrate to which these elements are bonded. Seike et al. assert that the disclosed sensor is temperature stable from −20° C. to +80° C., and that this is due to a specialized synthetic resin that is used in the bonding process.  
           [0027]    U.S. Pat. No. 5,008,611 (1991) to Ulmer, Jr. discloses a method and apparatus for measuring a target electric current utilizing the Faraday effect in an optical medium.  
           [0028]    In “Vibration Compensation Technique for an Optical Current Transducer”, Opt. Eng. 38(10), October 1999, pp 1708-1714, Niewczas et al. discuss a technique for compensation of vibration-induced noise in a optical current transducer. Their method uses two light sources as well as two photodetectors.  
           [0029]    In “A High-Accuracy Optical Current Transducer for Electric Power Systems” Power Delivery, IEEE Transactions on, Volume: 5 Issue: 2 , April 1990 Page(s):  892-898 , Ulmer, E. A., Jr. discusses the use of non-45 degree orientations between an incident polarizer and an accompanying analyzer.  
           [0030]    In “A Common-Mode Optical Noise-Rejection Scheme for an Extrinsic Faraday Current Sensor”,  Meas. Sci. Technol.  7 No 5 (May 1996) pp. 796-800, Fisher, N E and Jackson, D A discuss a method to eliminate optical noise induced by fiber optic vibration. Their experiment utilizes a linear, non-reciprocal magneto-optical transducer that places a beam splitter directly onto the sensor assembly.  
           [0031]    In “Improving the Sensitivity of a Faraday Current Sensor by Varying its Operating Point”,  Meas. Sci. Technol.   — 6 No 10 (October 1995) pp. 1508-1518, Fisher, N E and Jackson, D A discuss a method to improve the performance of a Faraday sensor. Their experiment utilizes a linear, non-reciprocal arrangement of a polarizer, Faraday rotator, and another polarizer, and they discuss the effect of varying the polarization angles between the two polarizers.  
         OBJECTS AND SUMMARY OF THE INVENTION  
         [0032]    It is an object of the invention to provide an improved optical sensor for measuring polarization rotation of optical wavefronts.  
           [0033]    It is a further object of the invention to provide an improved optical sensor for measuring the temperature of the sensor element as well as the temperature of the conductor in which the sensor is in contact.  
           [0034]    It is a further object of the invention to provide an improved optical sensor that mechanically self-aligns the entire optical path during the manufacture of the device.  
           [0035]    It is a further object of the invention to provide an improved optical sensor that can be used in reciprocal mode, e.g., with counter-propagating optical wavefronts simultaneously entering and leaving each fiber.  
           [0036]    It is yet a further object of the invention to provide an improved optical sensor that can be easily mass-produced through automation, with minimization or complete elimination of the difficulties of alignment and characterization of the said optical components.  
           [0037]    In a preferred embodiment, the invention provides optical sensors that use Faraday rotator materials, e.g., crystalline materials such as rare-earth garnets for example, as to measure magnetic fields, corresponding electrical currents, or temperature fluctuations. The invention may be provided in the form of a fiber optic sensor system preferably comprising an optical fiber coupled to a graded index (GRIN) lens, a polarizer, a Faraday rotator material, another polarizer, another GRIN lens coupled to an optical fiber, an optical detector, and an electronic circuit to analyze the output of the detector. 
       
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0038]    The foregoing and other objects, features, and advantages of the invention will be apparent from the following more particular description of preferred embodiments as illustrated in the accompanying drawings, in which reference characters refer to the same parts throughout the various views. The drawings are not necessarily to scale, emphasis instead being placed upon illustrating principles of the invention.  
         [0039]    [0039]FIG. 1 shows a schematic of a fiber optic magneto-optic sensor assembly in accordance with a preferred embodiment of the invention;  
         [0040]    [0040]FIG. 2 shows an exploded view of components that make up the fiber optic magneto-optic sensor assembly;  
         [0041]    [0041]FIG. 3 shows a representative small-signal linearity of the magneto-optic sensor assembly in a 60-Hz, AC magnetic field.  
         [0042]    [0042]FIG. 4 shows a representative large-signal linearity of the magneto-optic sensor assembly in a 60-Hz, AC magnetic field.  
         [0043]    [0043]FIG. 5 shows a representative single-ended-schematic used to process magnetic field or temperature information and is comprised of a semiconductor driver, semiconductor light source, the magneto-optic sensor assembly, a single photodiode, and signal processing electronics.  
         [0044]    [0044]FIG. 6 shows a representative schematic used to process magnetic field or temperature information and is comprised of a semiconductor driver, a semiconductor light source, the magneto-optic sensor assembly, a polarizing beamsplitter, dual photodiodes, and signal processing electronics.  
         [0045]    [0045]FIG. 7 shows a representative schematic used to process temperature and magnetic field information and is comprised of a semiconductor driver, dual semiconductor light sources, a fiber optic coupler, the magneto-optic sensor assembly, a polarizing beamsplitter, dual photodiodes, and signal processing electronics.  
         [0046]    [0046]FIG. 8 shows a representative reciprocating path schematic used to process magnetic field and temperature information and is comprised of a semiconductor driver, two semiconductor sources, three optical couplers, the magneto-optic sensor assembly, dual beam splitters, four photodiodes, and signal processing electronics.  
         [0047]    [0047]FIG. 9 shows the magneto-optic sensor assembly mounted on a circular cable. 
     
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS  
       [0048]    With reference to FIG. 1 through FIG. 9, the device in accordance with a preferred embodiment is a transmissive magneto-optical sensor that can be operated in either non-reciprocal mode or in reciprocal mode. In non-reciprocal mode, light only travels in one direction through the current sensor assembly  20 , whereas in reciprocal mode light travels simultaneously in opposing directions through the sensor assembly  20 . Non-reciprocal mode can be used to simplify signal processing and to reduce system cost, whereas reciprocal mode is used where higher measurement resolution or vibration immunity is the governing goals. In either mode, optical operation of the device is the same.  
         [0049]    The operation of the device in non-reciprocal mode is preferably as follows. An optical wavefront of light energy, such as that from a semiconductor laser, enters the current sensor assembly  20  through furcation tube  1   a  containing an internal optical fiber  5   a . The optical fiber  5   a  may be held in place via capillary tubing  4   a , and the capillary tubing  4   a /optical fiber  5   a  may be optically bonded to a quarter-pitch graded index lens  6   a , which serves to expand and collimate the input light beam. The capillary tubing  5   a  and graded index lens  6   a  may be held secure in the assembly by a hollow-core tube  3   a  and non-ferrous collimator outer housing  2   a . The light is then projected through polarizer  7   a , which can be held securely in place by retainer/adjuster  8   a . This polarizer  7   a  establishes an arbitrary but fixed state of polarization for the incident optical wavefront.  
         [0050]    The Faraday rotator material  10  can be held in a preferred orientation within the sensor assembly by the Faraday rotator material carrier  11  and locking pin  12 . The Faraday rotator material carrier  11  is preferably hollow and is aligned with the propagating light wavefront from polarizer  7   a . Situated between, and axially aligned with retainer/adjuster  8   a  and Faraday rotator material carrier  11  is a spacer  9   a , which is used to slightly offset the polarizer  7   a  from the Faraday rotator material  10 . The propagating light wavefront from polarizer  7   a  travels through spacer  9   a , is incident upon the Faraday rotator material  10 , and exits through the Faraday rotator material carrier  11 . In the presence of a magnetic field this lightwave will undergo a rotation of the polarization state established by polarizer  7   a . This rotation is proportional to the strength of the magnetic field intersecting the Faraday rotator material  10  in the same direction as the direction of the propagating lightwave.  
         [0051]    The propagating light now passes through another spacer  9   b , which may be positioned axially between the Faraday rotator material carrier  11  and another retainer/adjuster  8   b . This retainer/adjuster  8   b  holds another polarizer  7   b  whose transmission axis is in the same plane as polarizer  7   a  but is rotationally offset by an amount that is established by the system configuration. This polarizer  7   b  serves to separate the polarization rotation induced by the Faraday rotator material  10  into a polarization component that varies the intensity of the propagating wavefront as a function of the applied magnetic field. The remaining components of the sensor  20  are preferably a mirror image of the assembly previously described. The collimated optical wavefront from polarizer  7   b  is incident upon the graded-index lens  6   b  and is refocused upon the optical fiber  5   b . From here the light is sent down the optical fiber  5   b  and furcation tube  1   b  where it is eventually converted to an electric current by a photodiode  24  and then is processed by a semiconductor driver and electronics signal processing circuit  21 . A second hollow-core tube  3   b  and second capillary tube  4   b  are preferably provided.  
         [0052]    A sensor housing  13  may be provided, and preferably includes tensioning screws  14   a ,  14   b  and a through bore such that the inner diameter of the housing matches the outer diameter of the collimator outer housings  2   a ,  2   b.    
         [0053]    [0053]FIG. 3 shows an example of a small-signal linearity of the transducer  20  with a 60-Hz sinusoidal excitation. As can be seen, the response of the transducer  20  is extremely linear for small variations in signal response, with a 0.99943 coefficient of correlation between the transducer output and a linear curve fit.  
         [0054]    [0054]FIG. 4 shows an example of a large-signal linearity of the transducer  20  with a 60-Hz sinusoidal excitation., As can be sent the response of the transducer  20  is linear, but as the magnitude of the excitation increases, a slight hysteresis develops. This is purely a function of the materials that comprise the Faraday rotator material  10  and in no way limit the usefulness of the transducer  20 . The coefficient of correlation between the transducer output and a linear curve fit is 0.9936 for the representative data shown.  
         [0055]    [0055]FIG. 5 shows a non-reciprocal transmissive electro-optical system capable of measuring the polarization rotation of a magneto-optic sensor assembly  20 . Light energy is generated by a semiconductor light source  22  and is transmitted via optical fiber to the transducer assembly  20 . In the presence of a magnetic field that has a field component oriented with the direction of the propagation of the optical wavefront, the intensity output will vary in proportion to the intensity of the magnetic field component and will be detected by photodetector  24 . The output of photodetector  24  is then processed by analog or digital signal processing electronics  21 .  
         [0056]    [0056]FIG. 6. shows a non-reciprocal transmissive electro-optical system capable of measuring the polarization rotation of magneto-optical sensor assembly  20 . Light energy is generated by a semiconductor light source  22  and is transmitted via optical fiber to the transducer assembly  20 . In the presence of a magnetic field that has a field component oriented with the direction of the propagation of the optical wavefront, the intensity output of the transducer  20  will vary in proportion to the intensity of the magnetic field component. Polarizing beamsplitter  28  serves the purpose of separating the incident optical wavefront into two orthogonal components. The separated outputs of polarizing beamsplitter are then incident upon two independent photodiodes  24  and  25 , which are then processed by analog or digital signal processing electronics  21 .  
         [0057]    In the system configuration of FIG. 6. if the incident optical wavefront is connected to the input fiber  5   a , it is not necessary to utilize polarizer  7   b  in transducer assembly  20  as this polarization analyzing function is accomplished in polarization beamsplitter  28 .  
         [0058]    [0058]FIG. 7. shows a non-reciprocal transmissive electro-optical system capable of simultaneously measuring the polarization rotation of magneto-optical sensor assembly  20  due to the influence of magnetic fields and variations in temperature. Light energy is alternately generated by semiconductor light sources  22  and  23  and is coupled into the same transmission path is transmitted via an optical coupler  30 . The optical coupler  30  is connected via optical fiber to the transducer assembly  20 . In the presence of a magnetic field that has a field component oriented with the direction of the propagation of the optical wavefront, or in the presence of a temperature fluctuation affecting the Faraday rotator material  10 , the intensity output of the transducer  20  will vary in proportion to the intensity of the magnetic field component or change in temperature of the Faraday rotator material  10 . Polarizing beamsplitter  28  serves the purpose of separating the incident optical wavefront into two orthogonal components. The separated outputs of polarizing beamsplitter are then incident upon two independent photodiodes  24  and  25 , which are then processed by analog or digital signal processing electronics  21 .  
         [0059]    In the system configuration of FIG. 7. if the incident optical wavefront is connected to the input fiber  5   a , it is not necessary to utilize polarizer  7   b  in transducer assembly  20  as this polarization analyzing function is accomplished in polarization beamsplitter  28 . Furthermore, the dual-source configuration of FIG. 7 can be used with single photodetector configuration shown in FIG. 5 without any loss of generality.  
         [0060]    [0060]FIG. 8 shows a reciprocal transmissive electro-optical system capable of simultaneously measuring the polarization rotation of magneto-optical sensor assembly  20  due to the influence of magnetic fields and variations in temperature. Light energy is alternately generated by semiconductor light sources  22  and  23  and is coupled into the same transmission path is transmitted via an optical coupler  30 . The optical coupler  30  is connected via optical fiber two additional couplers  31  and  32  that serve to establish the counter-propagating reciprocal structure through transducer assembly  20 . In the presence of a magnetic field that has a field component oriented with the direction of the propagation of the optical wavefront, or in the presence of a temperature fluctuation affecting the Faraday rotator material  10 , the intensity output of the transducer  20  will vary in proportion to the intensity of the magnetic field component or change in temperature of the Faraday rotator material  10 . The output of transducer  20  is then sent back through optical couplers  31  and  32 , where the optical energy is transmitted to polarizing beamsplitters  28  and  29  as appropriate. Polarizing beamsplitters  28  and  29  serve the purpose of separating the incident optical wavefront into two orthogonal components. The separated outputs of polarizing beamsplitter are then incident upon four independent photodiodes  24  through  27 , which are then processed by analog or digital signal processing electronics  21 .  
         [0061]    The dual magnetic field and temperature analyzing function taught in FIGS. 7 and 8 can be separated as follows. Typically, Faraday rotators materials  10  are both temperature sensitive and wavelength sensitive. If Faraday rotator materials  10  that have a non-zero temperature coefficient are utilized in the transducer  20 , then the Faraday rotation detected by a single photodiode  24  or by a pair of photodiodes  24  and  25  become a function of both temperature and magnetic field. The basic relationships governing this interaction are given by:  
         Θ(λ 1 )= C   1   ·dB+C   2   ·dT    EQN(1)  
         Θ(λ 2 )= C   3   ·dB+C   4   ·dT    EQN(2)  
         [0062]    where  
         [0063]    Θ(λ 1 ) is the total rotation measured by the photodetectors  24 / 25  in single or combination at one particular wavelength λ1;  
         [0064]    Θ(λ 2 ) is the total rotation measured by the photodetectors  24 / 25  in single or combination at another particular wavelength λ2;  
         [0065]    dB is the desired change in magnetic flux component that contributed to the rotation Θ(λ1) and Θ(λ2);  
         [0066]    dT is the desired change in temperature component that contributed to the rotation Θ(λ1) and Θ(λ2);  
         [0067]    C 1  and C 2  are coefficients determined a priori that correspond to λ1; and  
         [0068]    C 3  and C 4  are coefficients determined a priori that correspond to λ2.  
         [0069]    Once C 1  through C 4  have been characterized and the total rotation Θ(λ1, λ2) has been measured, the desired quantities dB and dT can be determined in real-time from:  
             dB   =           C   4          Θ        (     λ   1     )         -       C   2          Θ        (     λ   2     )                 C   1          C   4       -       C   2          C   3                   EQN   .                (   3   )                 dT   =           C   1          Θ        (     λ   2     )         -       C   3          Θ        (     λ   1     )                 C   1          C   4       -       C   2          C   3                   EQN   .                (   4   )                                 
 
         [0070]    This dual-functionality has tremendous utility in applications requiring both information concerning the local conductor temperature as well as the magnitude of the load current through the conductor being monitored.  
         [0071]    [0071]FIG. 9 shows the optical current sensor assembly  20  mounted in a magneto-optical current sensor assembly holder  41  that is made to fit a given size of conductor, specifically the size of the outer insulting jacket  43  and inner metallic conductor  44 . The holder  41  serves the purpose of specifically orienting the magneto-optic sensor assembly  20  such that the internal Faraday rotator material  10  of the sensor assembly  20  is located a fixed distance from the current carrying conductor  43 / 44  so that the magnetic field induced by the current carrying conductor  43 / 44  is exactly parallel to the propagating optical wavefront traveling through the Faraday rotator material  10 . An additional purpose of holder  41  is to position the sensor assembly  20  in such a manner as not to cause the internal Faraday rotator material of  20  to not saturate. Another purpose of holder  41  is to provide a method so that the optical current sensor assembly  20  can be connected and disconnected from the current carrying conductor  43 / 44  easily, without disconnecting the conductor from the system and disrupting the current flow to the electrical load.  
         [0072]    Fiber optic cable retainer  42  serves the purpose of dressing the furcation tubing  1   a / 1   b  that extends to and from the magneto-optical sensor assembly  20  so that the tubing  1   a / 1   b  containing optical fiber  5   a / 5   b  is somewhat protected and the effects of optical birefringence are lessened.  
         [0073]    Further details of sensors which can be used in accordance with the principles taught herein are set forth in U.S. patent application Ser. No. 09/421,399 entitled “Methods and Apparatus for Optically Measuring Polarization Rotation of Optical Wavefronts Using Rare Earth Iron Garnets,” and U.S. patent application Ser. No. 09/783,390 entitled Fiber Optic Sensors And Methods Therefor,” the entire disclosures of which are incorporated herein by reference. The sensor devices taught herein can be used in systems and methods such as those described in U.S. patent application Ser. No. 09/841,164 entitled “System and Method for Distributed Monitoring Using Remote Sensors,” the entire disclosure of which is incorporated herein by reference. The sensor devices taught herein may be used, e.g., to monitor current and temperature, and/or to sense faults, in high-voltage power transmission and distribution lines, shipboard zonal power systems for monitoring load current and temperature, such as temperature of conductor and/or power panel, as well as load current through conductor and/or power panel. The sensors may also be used, e.g., in power inversion systems to provide intrinsic isolation between high-power and low-power control electronics, and may offer greater safety in such applications.  
         [0074]    While the invention has been particularly shown and described with reference to a preferred embodiment thereof, it will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the rit and scope of the invention.