US20050203711A1  Method and apparatus for transmission line and waveguide testing  Google Patents
Method and apparatus for transmission line and waveguide testing Download PDFInfo
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 US20050203711A1 US20050203711A1 US11/034,592 US3459205A US2005203711A1 US 20050203711 A1 US20050203711 A1 US 20050203711A1 US 3459205 A US3459205 A US 3459205A US 2005203711 A1 US2005203711 A1 US 2005203711A1
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 G—PHYSICS
 G01—MEASURING; TESTING
 G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
 G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
 G01R31/28—Testing of electronic circuits, e.g. by signal tracer
 G01R31/317—Testing of digital circuits
 G01R31/31712—Input or output aspects
 G01R31/31717—Interconnect testing

 G—PHYSICS
 G01—MEASURING; TESTING
 G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
 G01R27/00—Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom
 G01R27/02—Measuring real or complex resistance, reactance, impedance, or other twopole characteristics derived therefrom, e.g. time constant
 G01R27/04—Measuring real or complex resistance, reactance, impedance, or other twopole characteristics derived therefrom, e.g. time constant in circuits having distributed constants, e.g. having very long conductors or involving high frequencies

 G—PHYSICS
 G01—MEASURING; TESTING
 G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
 G01R27/00—Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom
 G01R27/28—Measuring attenuation, gain, phase shift or derived characteristics of electric four pole networks, i.e. twoport networks using network analysers Measuring transient response
 G01R27/32—Measuring attenuation, gain, phase shift or derived characteristics of electric four pole networks, i.e. twoport networks using network analysers Measuring transient response in circuits having distributed constants, e.g. having very long conductors or involving high frequencies

 G—PHYSICS
 G01—MEASURING; TESTING
 G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
 G01R35/00—Testing or calibrating of apparatus covered by the preceding groups
 G01R35/005—Calibrating; Standards or reference devices, e.g. voltage or resistance standards, "golden" references

 H—ELECTRICITY
 H04—ELECTRIC COMMUNICATION TECHNIQUE
 H04B—TRANSMISSION
 H04B3/00—Line transmission systems
 H04B3/02—Details
 H04B3/46—Monitoring; Testing

 H—ELECTRICITY
 H04—ELECTRIC COMMUNICATION TECHNIQUE
 H04B—TRANSMISSION
 H04B3/00—Line transmission systems
 H04B3/02—Details
 H04B3/46—Monitoring; Testing
 H04B3/493—Testing echo effects or singing

 H—ELECTRICITY
 H04—ELECTRIC COMMUNICATION TECHNIQUE
 H04B—TRANSMISSION
 H04B3/00—Line transmission systems
 H04B3/54—Systems for transmission via power distribution lines
 H04B3/56—Circuits for coupling, blocking, or bypassing of signals

 G—PHYSICS
 G01—MEASURING; TESTING
 G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
 G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
 G01R31/08—Locating faults in cables, transmission lines, or networks
 G01R31/11—Locating faults in cables, transmission lines, or networks using pulse reflection methods

 H—ELECTRICITY
 H04—ELECTRIC COMMUNICATION TECHNIQUE
 H04B—TRANSMISSION
 H04B2203/00—Indexing scheme relating to line transmission systems
 H04B2203/54—Aspects of powerline communications not already covered by H04B3/54 and its subgroups
 H04B2203/5404—Methods of transmitting or receiving signals via power distribution lines
 H04B2203/5425—Methods of transmitting or receiving signals via power distribution lines improving S/N by matching impedance, noise reduction, gain control

 H—ELECTRICITY
 H04—ELECTRIC COMMUNICATION TECHNIQUE
 H04B—TRANSMISSION
 H04B2203/00—Indexing scheme relating to line transmission systems
 H04B2203/54—Aspects of powerline communications not already covered by H04B3/54 and its subgroups
 H04B2203/5462—Systems for power line communications
 H04B2203/5483—Systems for power line communications using coupling circuits

 H—ELECTRICITY
 H04—ELECTRIC COMMUNICATION TECHNIQUE
 H04B—TRANSMISSION
 H04B2203/00—Indexing scheme relating to line transmission systems
 H04B2203/54—Aspects of powerline communications not already covered by H04B3/54 and its subgroups
 H04B2203/5462—Systems for power line communications
 H04B2203/5491—Systems for power line communications using filtering and bypassing

 H—ELECTRICITY
 H04—ELECTRIC COMMUNICATION TECHNIQUE
 H04B—TRANSMISSION
 H04B2203/00—Indexing scheme relating to line transmission systems
 H04B2203/54—Aspects of powerline communications not already covered by H04B3/54 and its subgroups
 H04B2203/5462—Systems for power line communications
 H04B2203/5495—Systems for power line communications having measurements and testing channel
Abstract
A multiport junction is used in combination with an Inverse Fourier Transform to detect distance to fault in an RF transmission line or waveguide without the use of heterodyne downconversion circuits. To provide an ultrawide bandwidth frequency domain reflectometer the output ports of the multiport junction are used to calculate distance to fault and return loss. The Inverse Fourier Transform algorithm is modified to take into account both phase shift per unit length of the transmission line and attenuation per unit of length in the transmission line, with the output of the modified Inverse Fourier Transform being applied to a module that subtracts out the effect of previous faults by solving for the distances ahead of time before knowing amplitudes and for solving for amplitude at each prior fault starting with the first fault. The output of this module is then used thresholded to remove the effects of noise, secondary reflections and inconsequential peaks. The result is a time domain waveform in which peak positions indicate the distance to real faults and in which return loss or percent reflection is calculated for each of the faults. Moreover, internal calibration loads and specialized processing are used to effortlessly calibrate the reflectometer in the field.
Description
 This Application claims rights under 35 USC § 119(e) from U.S. Application Ser. No. 60/536,886 filed Jan. 15, 2004, and U.S. Patent Application Ser. No. 60/536,977 filed Jan. 15, 2004, the contents of which are incorporated herein by reference.
 This invention relates to frequency domain reflectometers and more particularly to a downconversionless system employing the use of a multiport junction in combination with an Inverse Fourier Transform.
 It will be appreciated that faults in RF transmission lines and waveguides require detection so that the distance to the fault may be calculated. Moreover, the ability to detect and locate multiple faults that oftentimes result in ghosts that resemble faults requires sophisticated techniques to eliminate the need for skilled technicians.
 Nowhere are reflectometers more desirable than in aircraft applications in which long lengths of cable or waveguides are used, both for the control of the aircraft and for the electronics devices such as radar or communication systems carried by the aircraft. Additionally, civilian use of reflectometers finds application in cable systems in which faults are detected based on the distance from a cable plant.
 Likewise, for satellite and terrestrialbased communications, RF transmissions lines and waveguides can become faulty, especially at the interface between two cables as at a connection, and the ability to identify and locate the fault is a paramount concern.
 A fault is anything that causes a change of impedance in the material properties of the cable or waveguide that causes some of the energy that is being transmitted through the transmission line to be reflected. Typically the faults occur at the interface between two cables, for instance, if a connection is not torqued properly or the connectors are old. If there is no good interface there will be a difference in material properties at the interface so that when one is sending a signal down the transmission line, at the interface some of the energy will be reflected. Thus, cable discontinuities or faults can be the result of interface problems between the cables or when a cable is bent and tweaked enough, the material properties will change at the bend that cause a reflection. Also, if the shielding to the cable is damaged in any way, part of the cable may couple to, for instance, the body of an aircraft, causing an impedance mismatch.
 Thus, in the past, whether it be for military applications so that one does not have to tear into a large amount of cabling in an aircraft in order to locate a fault, or whether one is testing cell tower base stations to locate faults in transmission lines for the cell towers, or if one is using a distancetofault (DTF) detector for satellite ground terminals, there is a need to be able to automatically and accurately identify the fault, to find its severity and to obtain the distance to the fault, especially in a multifault environment.
 There are two primary methods of determining faults in any transmission line. The first is based on time domain reflectometry and the other is based on frequency domain reflectometry. In time domain reflectometry one can simply place a pulse on a transmission line and measure the time it takes for a return pulse to be received. Propagation time within the cables therefore determines the distance of the fault to a measuring plane. Thus, by knowing the velocity of propagation of the specific cable, one can convert the time that the reflected pulse comes back to a distance to know how far away the fault is.
 It is noted that time domain reflectometry is particularly well adapted for low frequency applications because one can easily create a system that produces short duration pulses that are narrow enough to resolve fault locations with acceptable accuracy. However, when one starts to get into high frequency applications exceeding for example 1 GHz, obtaining a physical system to produce an impulse that is of short enough duration is very difficult to realize in hardware. Moreover, even if one can create such a short pulse, the shape of the pulse is hard to control.
 It is noted that those employing time domain reflectometry do not obtain information on spectral characteristics. With frequency domain reflectometry one has full control of the spectral characteristics. Thus, the other technique for reflectometry, which has proved to be quite useful, involves frequency domain reflectometry in which a couple of very different approaches have been used.
 As illustrated in U.S. Pat. No. 4,630,228, what is described is a frequency difference method in which a swept source is applied to a device under test (DUT) and the reflected wave is mixed down and measured. Then the distance to the fault is determined by the difference frequency.
 Another approach is illustrated in U.S. Pat. No. 5,068,614, which is the automation of a manual distance to fault or DTF technique that uses a spectrum analyzer and an offset tracking generator to find the distance to a fault. The output of the tracking generator is mixed with the return from the device under test. The tracking generator offset frequency is then adjusted to maximize the power displayed on the spectrum analyzer, with the distance to the fault calculated from the offset frequency. Note that this system also employs a frequency difference method.
 As illustrated in U.S. Pat. Nos. 5,949,236 and 5,994,905, the systems employed are not frequency difference systems. Rather they measure the reflection coefficient of the device under test as a function of frequency. The reflection coefficient varies as a function of frequency. This variation is based on the location of each fault and the percent of energy reflected from each fault. If a device under test contains a single fault the reflection coefficient will vary as an exponentially decaying sinusoid across frequency. The method employed is to use an Inverse Fourier Transform or IFT to obtain an impulse or time domain response that is then used to determine the distance to the fault.
 The problem with the methods described in these two patents is that they only measure the amplitude of the reflection coefficient, not the phase. This introduces nonlinearities that generate harmonics and intermodulation products in the impulse response. These undesirable responses do not occur if there is only one fault. However, the number of spurious responses increases exponentially with multiple faults. These spurious responses are sometimes called ghosts.
 In short, there are an extremely large number of spurious responses when a device under test contains several faults and removing them all becomes both cumbersome and, in some cases, impossible, at least by visual inspection of the results of an Inverse Fourier Transform (IFT).
 To make matters somewhat worse, when one seeks to measure distance to fault over a wide operating frequency range, typically in the past the measured signals are downconverted to a single frequency range from which Inverse Fourier Transform measurements are obtained. Downconversion adds its own set of problems and involves many local oscillators and mixers.
 Additionally, when multiple faults are involved, the energy transmitted through the first fault will be of considerably lower amplitude when it reaches a subsequent fault. Thus, the apparent reflection from a subsequent fault, which may be more highly reflective than the first, oftentimes has a magnitude much less than the amplitude of the peak associated with the first fault due to the attenuation of the signal that gets by the first fault, and also due to line attenuation. The result is that one may fail to recognize a subsequent stronger fault. Thus, those systems that do not adjust for prior faults are incapable of distinguishing, in subsequent faults, the severity of the fault.
 The result is that it takes an extremely skilled technician to be able to recognize that a certain peak is the result of a fault, especially when the peaks start to fall into the noise level due to the amplitude attenuation associated with the line itself. Secondly, those systems that use an inverse amplitude attenuation function to compensate for attenuation tend to mask the faults at greater and greater distances.
 There are some frequency domain reflectometers that rely on phase shifts to determine the distance to a fault. However, those systems that measure phase shift only which are based on real phase shifts, have no attenuation information. While they do take into account phase shifts per unit length of transmission line, they fail to take into account attenuation per unit length of transmission line.
 Finally, those systems that use an Inverse Fourier Transform without further processing are incapable of subtracting out the effect of previous faults when trying to identify or locate peaks useful in determining distance to a fault; or in determining the severity of a fault.
 By way of further background, in order for some of the prior systems to be able to obtain a wide operational frequency bandwidth, some prior systems use a stepped frequency approach and downconversion, in which one transmits a sine wave at a set number of frequency points within the defined bandwidth. At each frequency point one is radiating a sine wave and one seeks to be able to measure the amplitude and phase of the returned sine wave. In so doing, one obtains a discrete frequency response of the cable or waveguide. If one then performs an Inverse Fourier transform one obtains a temporal response, at which point one can obtain the same results as time domain reflectometers.
 The trouble is that for a wide bandwidth, the prior art systems use downconvert, downmix or heterodyning circuits, employing a local oscillator to downmix to a signal that one can sample. One then needs to sample at one frequency range and then step through the remainder of the frequency ranges to obtain the wide bandwidth. For a wide bandwidth system it would be desirable to eliminate oscillators and downconverters and to eliminate a great many stepping functions.
 More particularly, when one utilizes downconversion, one wants to measure a vector voltage. In other words, one wants to measure the phase and amplitude. This is a relatively easy task at a single frequency, but the problem is, as soon as one starts trying to do it over a wide range of frequencies, devices become nonideal and they are hard to calibrate. Thus, measuring a device over a wide frequency range is very difficult. In order to be able to do so, one downconverts to a single frequency and makes the measurements at this frequency.
 As mentioned above, in multifault scenarios, prior frequency domain reflectometers suffer from ambiguities or ghosts, with ghost faults appearing at distances that are multiples of the actual distance between each fault. Ghosts can also appear if the reflectometer measures only the magnitude of the reflection coefficient. In the first case if one has a cable with multiple faults, one is going to get some energy reflected at the first fault, which is passed back to the receiver. Some energy propagates through the first fault and then is reflected from the second fault, with that energy passing all the way back to the receiver through the first fault. It is noted that there are also an infinite number of bounces between the two faults and each time some of the energy leaks back to the receiver. What one sees, therefore, are these delayed versions of the fault so that when one looks at the display one sees all of the ghost faults. In the second case, if one has a cable with multiple faults one will see faults at the sum and difference distances of those true fault locations. This occurs because the magnitude of the reflection coefficient does not contain enough information to resolve the actual locations therefore ghosts appear.
 In the past, the processing philosophy was to first address the biggest fault, which was assumed to be the closest fault, and the fix it. Thereafter, one would test the cable or waveguide for the rest of the faults.
 In short, both types of ghosts exist primarily by not measuring the amplitude and phase of the complex reflection coefficient at each frequency and or by not compensating for multiple reflections when determining fault locations. This results in false alarms that do not reflect where the fault is or even whether or not there is a fault.
 There is therefore a requirement to provide a system that can measure the amplitude and phase of the reflection coefficient at each frequency for the transmission line under test and can identify the main peak for the first fault, the main peak for the second fault, et cetera. One could then see, identify and ignore reduced peaks at the sum and difference frequencies from which the actual peaks can be distinguished.
 What is therefore required is a wideband frequency domain reflectometer that has easily configurable frequency coverage, that has automatic fault location for multiple faults, that discriminates against ghosts, that has accurate Fault Return Loss estimation and employs a quick initial calibration process. The reflectometer should also have the ability to test multiple different interconnected cables.
 Rather than having to design hardware that is complicated with oscillators, mixers downconverters and even fairly highspeed analogtodigital converters, in the subject system one uses a downconversionless frequency domain reflectometer involving a multiport junction, power detectors and a digital signal processor that employs an Inverse Fourier Transform.
 The subject system improves on the operation of prior frequency domain reflectometers by utilizing a complex value of the reflection coefficient rather than its absolute magnitude to be able to detect and remove one source of ghosts and uses a means for estimating multiple faults to remove the second source of ghosts as described hereinabove.
 Moreover, a modified Inverse Fourier Transform is used that takes into account not only the phase shift per unit length of transmission line but also the attenuation per unit length of transmission line to accurately measure the magnitude of each fault in a multifault environment.
 In a further embodiment, in order to reduce computational complexity, a simple Inverse Fast Fourier Transform is performed first, followed by a process that refines fault locations derived from the Inverse Fast Fourier Transform. The refinement process utilizes the modified Inverse Fourier Transform, which operates on many fewer data points than those associated with the Inverse Fast Fourier Transform. Moreover, the refinement process compensates for granularity by calculating the modified Inverse Fourier Transform distances for not only a candidate fault distance but also for a set of distances to either side of each detected peak.
 Additionally, the system compensates for the effect of prior faults and filters out faults below a predetermined threshold to filter out noise, secondary reflections and small, insignificant faults.
 Moreover, in order to make using a multiport junction easy, the reflectometer utilizes internal calibration which uses factory measured scattering parameters and a number of internal calibration loads. Since the characteristics of the passive multiport junction do not vary after manufacture, the transfer function of the multiport junction is measured at the factory. Thereafter, in a second step, the subject system uses one of two calibration procedures to characterize both the variability in the RF source output power and the variability in the detection circuitry characteristics across frequency whose response can drift after factory calibration. The first calibration procedure involves using a number of calibration loads internal to the reflectometer in conjunction with signal processing for computing gain and offset for each frequency and each port, while the other calibration procedure involves a matched load and a bank of switchable attenuators in conjunction with an alternative signal processing system for computing gain and offset for each frequency and each port. Regardless of which calibration procedure is used, new offsets and gains are generated to be substituted for the gains and offsets in the process that estimates the complex reflection coefficient used in the reflectometer.
 As a result of the above techniques, an accurate estimate of the complex reflection coefficient frequency profile can be measured. Also, because the Inverse Fourier Transform operates on a complex value of the reflection coefficient after calibration, ghosts due to the multiple faults, nonlinearities are eliminated. This is unlike prior Inverse Fourier Transform systems, which operate on the absolute magnitude of the reflection coefficient that does not take into account that the reflection coefficient is complex. Since it is, one can take advantage of this fact to correctly model the transmission line and therefore eliminate one source of ghosts.
 Secondly, because the modified Inverse Fourier Transform takes into account line attenuation, the modified Inverse Fourier Transform accurately calculates the amplitudes of the reflection coefficients, thus to permit reliable detection and location of faults in a multifault environment. Calculation of the associated return losses or percent reflection is also made possible through the use of the modified Inverse Fourier Transform. Moreover, in one embodiment computational complexity is greatly reduced by first doing a simple and fast Inverse Fast Fourier Transform and then processing only a subset of the data points operated on by the first transform with the modified Inverse Fourier Transform.
 As noted above, the multiport junction eliminates the necessity for downconversion and results in an ultrawide bandwidth reflectometer.
 Finally, a calibration technique makes it convenient to use the multiport junction in the field, with the calibration involving generating revised offset and gain parameters across frequency that account for the variability in the RF source power and variability in the detector circuitry. These estimated gains and offsets are then used in conjunction with detection circuitry output power measurements for estimating the complex reflection coefficient of the transmission line under test. This complex reflection coefficient frequency profile is then used by the rest of the signal processing chain to estimate the location and return loss of each fault in the transmission line.
 As a result, a field calibratable frequency domain reflectometer in one embodiment has a wide operating frequency from 10 MHz to 18 GHz that is the result of a downconversionless system having a high dynamic range, greater than 70 dB. This means that faults can be detected at longer ranges, with the ability to detect, classify and locate multiple faults in a single transmission line. The use of the sixport junction in combination with a modified Inverse Fourier Transform is capable of handling a single series of connected transmission lines with multiple different propagation characteristics. Moreover, the system uses both phase and attenuation, thus eliminating the necessity for compensating for transmission line attenuation with an inverse attenuation characteristic that is ineffective. Thus, in the modified Inverse Fourier Transform, attenuation per unit length is part of the equation such that the use of phase shift alone is avoided.
 In summary, a multiport junction is used in combination with an Inverse Fourier Transform to detect distance to fault in an RF transmission line or waveguide without the use of heterodyne downconversion circuits. To provide an ultrawide bandwidth frequency domain reflectometer the output ports of the multiport junction are used to calculate distance to fault and return loss. The Inverse Fourier Transform algorithm is modified to take into account both phase shift per unit length of the transmission line and attenuation per unit of length in the transmission line, with the output of the modified Inverse Fourier Transform being applied to a module that subtracts out the effect of previous faults by solving for the distances ahead of time before knowing amplitudes and for solving for amplitude at each prior fault starting with the first fault. The output of this module is then used thresholded to remove the effects of noise, secondary reflections and inconsequential peaks. The result is a time domain waveform in which peak positions indicate the distance to real faults and in which return loss or percent reflection is calculated for each of the faults. Moreover, internal calibration loads and specialized processing are used to effortlessly calibrate the reflectometer in the field.
 These and other features of the subject invention will be better understood in connection with a Detailed Description, in conjunction with the Drawings, of which:

FIG. 1 is a block diagram illustrating a frequency domain reflectometer utilizing a multiport junction in combination with an Inverse Fourier Transform to calculate distance to a fault, to calculate the return loss of the fault and to display the results; 
FIG. 2 is a diagrammatic illustration of the utilization of a sixport junction coupled to a frequency source and a cable under test to determine the distance to a fault and estimate the magnitude of the fault by detecting the power at four of the output ports of the sixport junction, also illustrating the utilization of a modified Inverse Fourier Transform; 
FIG. 3A is a block diagram illustrating the multiport junction ofFIGS. 1 and 2 coupled to a module for estimating the complex reflection coefficient based on output power from four ports of the junction, and applying a modified Inverse Fourier Transform to take into account attenuation per unit length of transmission line, also showing a system for filtering out faults below a predetermined threshold so as to present on a display real faults and the magnitude of the faults; 
FIG. 3B is a diagrammatic representation of the utilization of a complex value of the reflection coefficient to reduce ghosts, and the utilization of an expression to which e is raised which takes into account attenuation per unit length; 
FIG. 4A is a block diagram illustrating the calibration of the reflectometer by setting gain and offset in the reflection coefficient estimator, also utilizing the measured multiport scattering matrix, and performing a modified Inverse Fourier Transform to generate one complex reflection coefficient for each distance, followed by identifying candidate faults, calculating fault magnitudes compensating for prior faults, and filtering out faults below a given magnitude; 
FIG. 4B is a block diagram illustrating first performing an Inverse Fourier Transform on each complex reflection coefficient for each frequency, identifying candidate faults and refining fault locations using a modified Inverse Fourier Transform, thus to reduce computational complexity; 
FIG. 5 is a block diagram of the module inFIGS. 4A and 4B that takes measurements, illustrating detection circuitry for detecting output power on four output ports of a sixport junction, thus to output four voltages for each frequency; 
FIG. 6 is a block diagram of the estimation of the reflection coefficient associated with the four voltages generated inFIG. 5 in which the calibration ofFIGS. 4A and 4B is accomplished in two stages, the first to recalculate offset and gain based on measurements in the field, and the second to apply a sixport calibration involving a premeasured scattering matrix for the sixport junction; 
FIG. 7 is a diagrammatic illustration of the module inFIG. 4A that performs a modified Inverse Fourier Transform on complex reflection coefficients; 
FIG. 8 is a diagrammatic illustration of the identification of candidate faults inFIGS. 4A and 4B in which candidate faults are identified utilizing peak detection algorithms; 
FIG. 9 is a diagrammatic illustration of the module inFIGS. 4A and 4B which calculates fault magnitudes compensating for prior faults, illustrating the algorithm used therefor; 
FIG. 10 is a diagrammatic illustration of the module inFIGS. 4A and 4B that filters out faults below a predetermined magnitude using a thresholding circuit, utilizing the magnitude of candidate faults from the unit that calculates magnitudes compensating for prior faults; 
FIG. 11 is an algebraic expression relating to the operation of a sixport junction, defining sixport network parameters and the associated reflection coefficients; 
FIG. 12 is an algebraic expression illustrating that in a reflection coefficient equation certain components thereof are related to attenuation per unit length of transmission line, with other components relating to rotation; 
FIG. 13 is a block diagram illustrating the utilization of calibration standards switched to the cable test port of a multiport circuit having the power output thereof as an input to a digital signal processor for determining offset and gain; 
FIG. 14 is a block diagram of a calibration circuit utilizing calibration loads in the form of attenuators switched between an RF source and a multiport circuit, with a digital signal processor providing offset and gain parameters; 
FIG. 15 is a flow chart for the calibration of the frequency domain reflectometer ofFIG. 13 in which two calibration loads are sequentially coupled to the test port of the reflectometer and in which measured responses are compared with model circuit responses, thus to permit the calculation of gain and offset using a least square estimate; 
FIG. 16 is a flow chart illustrating the calibration procedure for the reflectometer ofFIG. 14 utilizing calibration loads in the form of attenuator in which offset and gain are calculated by a comparison of measured data with model data and in which a least squared estimate is used to provide gain; 
FIG. 17 is a diagrammatic illustration of an RLC circuit which can be switched as a calibration load to the test port of the reflectometer ofFIG. 14 ; and, 
FIG. 18 is a schematic diagram of loads configured in accordance withFIG. 17 that can be switched to the test port of the reflectometer prior to switching the test port to the cable under test.  Prior to describing the subject system in detail, a theoretical discussion of the subject system is presented.
 It is a feature of the subject invention that since the output measurements from the sixport junction involves scaled versions of an RF source plus the returned signal from the cable under test, one can use these measurements to generate a complex reflection coefficient Γ(f) of the entire transmission line, be it a cable or waveguide. This complex reflection coefficient is then used to derive the scattering parameters of the individual faults themselves. Once one has derived the scattering parameters, the distance and severity of a fault can be ascertained.
 As the frequency is stepped or swept, the complex reflection coefficient of the cable is modified by the fault. If it is a perfect cable, then the cable has an impedance that is matched to the measuring circuit. Therefore, all of the energy propagates through the cable to ground and nothing gets reflected. In this case the Γ(f) would be 0 across the entire test frequency range for a perfect cable.
 However, if one has a fault, at every frequency that fault imparts an attenuation and phase shift to the signal. If one mathematically models the physics of the cable, one can derive what the amplitude and the phase profile looks like. Thus, in an imperfect cable, one will have a nonzero complex Γ at every frequency. The Γ is complex in that it is the result of an amplitude and phase shift of the outgoing signal. Using a number of power measurements from the multiport junction, one is able to derive or estimate Γ(f) for each frequency in the test range.
 From microwave circuit theory, the complete transfer function between each combination of ports of a multiport junction can be defined by the circuit's complex scattering parameters (Sparameters), also referred to as a scattering matrix (Smatrix), across the circuits entire operating frequency. In general, there is a complex scattering parameter denoted S_{nm}(f) for each frequency “f” and each combination of ports “nm”. Each scattering parameter describes the attenuation and phase shift imparted on a sinusoid of frequency “f” that is sent into port “m” and out of port “n”. In the subject invention one is concerned with two junctions. One is the transmission line under test, which is a single port junction, and the other is the multiport junction that is used to measure the transfer function of the transmission line under test. Because the transmission line is actually a single port junction it can be completely describe by its S_{11}(f) parameter. This is known as the complex reflection coefficient of the transmission line across frequency and is denoted as Γ(f). In the subject invention one uses the multiport junction in conjunction with an RF signal source, power detector and a digital signal processor to measure the reflection coefficient of the transmission line. Therefore, one must know the entire N×N scattering matrix defined across the entire operating frequency of the multiport junction to correctly measure Γ(f) of the transmission line, where N is the number of ports in the multiport junction. As described in the calibration section hereinafter, the scattering parameters of the multiport junction are measured in the factory using a network analyzer and are stored in the digital signal processor memory to be used when calculating the reflection coefficient profile Γ(f) for a device under test.
 More particularly, in order to characterize a coupler, passive device, splitter or some other piece of hardware, one can characterize the device using what are called scattering parameters. Thus, the transfer function of the device is characterized by the scattering parameters. In general, scattering parameters are denoted by the letter S so that S_{11 }is the transfer function from when one sends a wave into port 1 and obtains a wave reflected from the same port. In general, S_{11 }will be the reflected wave divided by the incident wave and it is a complex number, meaning that it has both phase and amplitude. Determining the scattering parameters determines the transfer function of the fault, with the scattering parameters defining what happened at the fault. It has been found that, in a sixport junction in which one measures power at four different ports, one can use the four measured powers to solve equations that will yield the complex reflection coefficient frequency profile of the transmission line. Using this complex reflection coefficient frequency profile one can detect faults and determine their location and severity.
 Multiport junctions in general and the sixport junction specifically are described in an IEEE Transaction on Microwave Theory and Techniques, Vol. 45, No. 12, December 1997, in an article entitled “A Historical” Review of the SixPort Measurement Technique” by Glenn F. Engen. It is noted that multiport junctions are not and have not priorly been used to determine distance to a fault.
 In this paper Engen describes a quantity Γ_{1 }that is determined by q_{3}, D_{2}/A_{2}, and P3/P4. It is therefore desirable to measure P3 and P4 and one knows q_{3}. D and A are the result of calibration so that one can solve for the reflection coefficient Γ. From Γ derived from the multiport junction as a function of frequency, one performs in an Inverse Fourier Transform and uses the result to determine the distance to fault and the magnitude of the fault.
 Heretofore, sixport junctions have not been used to determine distance to fault, primarily because the calibration techniques required were exceptionally cumbersome. They involved carting around as many as six or eight heavy calibration cables and to calibrate the device at each of the frequencies to be used. Thus, while the sixport junction could be used in a laboratory for measuring the transfer function of various devices, it was not suitable for use in characterizing transmission lines, cables or waveguides in a nonlaboratory setting.
 It is noted that the transfer functions are critically dependent upon the calibration procedures used. This means that the quantities D and A in the sixport equation described in Engen were not easy to ascertain. Nor was it easy to ascertain q_{3}, which is defined as −B/A. Note that A, B and D are sixport network parameters, with C being set to 0.
 Having ascertained that one can actually do a legitimate distance to fault determination using a sixport junction because one can sufficiently calibrate it with a relative degree of ease using an internal calibration scheme, it is important that when one performs the Inverse Fourier Transform on the complex reflection coefficient frequency profile Γ(f) one takes into account both phase shift per unit length of transmission line and attenuation per unit length of transmission line.
 More specifically, it is important to be able to accurately locate peaks without errors related to the amplitudes of prior faults. As mentioned hereinabove, prior art techniques have sought to compensate for transmission line attenuation by an approach involving multiplying the output of the Inverse Fourier Transform with an inverse attenuation function. All this does is to mask the peaks because, as mentioned before, as the distance to the fault increases, the amplitude of the effect can be lost in the noise. Thus one cannot apply an inverse attenuation without amplifying the effects of the noise in the measurements.
 The reason that the inverse attenuation function does not work is that, first of all, existing frequency domain reflectometers utilize an inappropriate transform, mainly a simple Inverse Fourier Transform. The simple Inverse Fourier Transform does take into account the phase shift per unit length of the transmission line, but does not take into account the attenuation per unit length of the transmission line. To make up for this lack, the prior art systems apply a gain that attempts to compensate for the transmission line attenuation. This is applied after the transform and does not correctly take out the line attenuation, as it is an approximation.
 In the subject invention, in order to take into account the transmission line attenuation, one modifies the transform itself so that it takes attenuation into account in the body of the transform. The result is that one obtains a more accurate distance to fault determination and a more accurate fault reflection coefficient magnitude.
 By using the modified Inverse Fourier Transform one can obtain the magnitude of the reflection of the fault commonly referred to as the return loss at the fault in the multifault environment that usually exists.
 Note that the usual Inverse IFT has a term e^{−jθ}, namely the phase shift, which is different for every frequency.
 However, the power to which e is raised must be complex in order to not only take into account phase shift but also attenuation. Note that while phase shift is real, the addition of attenuation makes the reflection coefficient a complex number.
 The practical effect is that knowledge of the attenuation of the cable is subsumed in the transform. This is shown in the following equations. Note that Equation 0.1 shows the mathematical node under test and refers to the reflection coefficient of the cable, referenced to the DTF tester test port:
$\begin{array}{cc}{\Gamma}_{k}=\sum _{m=1}^{M}{e}^{2{\gamma}_{k}{d}_{m}}{S}_{11,m}\prod _{p=1}^{m1}{S}_{12,p}{S}_{21,p}\text{}\mathrm{where}\text{}{\gamma}_{k}\equiv \alpha \sqrt{{f}_{k}}+j\frac{2\pi \text{\hspace{1em}}{f}_{k}}{v}& \left(0.1\right)\end{array}$  Note that in Equation 0.1, α{square root}f_{k }is the attenuation per unit length. Here both ν (speed of light in transmission line) and α are normalized by the frequency.
 In the above equation, M is the number of faults. Γ_{k }is the measured quantity, so it is known. γ_{κ} is known, since it depends only on the type of cable and the frequency. m is the index of the current fault. p is the index of the prior faults. M, d_{m}, S_{11,m}, S_{12,m}, and S_{21,m }are unknown. To solve for d_{m }and S_{11,m},
$\begin{array}{cc}\mathrm{Let}\text{\hspace{1em}}{S}_{m}={S}_{11,m}\prod _{p=1}^{m1}{S}_{12,p}{S}_{21,p}& \left(0.2\right)\end{array}$  One assumes that the faults are wide band (to simplify the equations). This means that their S parameters do not vary over the swept frequency range. Substituting in
$\begin{array}{cc}{\Gamma}_{k}=\sum _{m=1}^{M}{e}^{2{\gamma}_{k}{d}_{m}}{S}_{m}& \left(0.3\right)\end{array}$  Next, one processes this Γ(f) data with something similar to an Inverse Fourier Transform. This is the subject modified IFT, herein called the “Taylor transform.”. It differs from an IFT in that the exponent in the summation is complex, and therefore takes into account the loss of the cable, in addition to the phase shift. Note that h_{m }is the complex reflection coefficient for the distance m.
$\begin{array}{cc}{h}_{m}=\frac{1}{K}\sum _{k=1}^{K}\sum _{n=1}^{M}{e}^{2{\gamma}_{k}\left({d}_{n}{d}_{m}\right)}{S}_{n}& \left(0.4\right)\\ {h}_{m}=\frac{1}{K}\sum _{k=1}^{K}{\Gamma}_{k}{e}^{2{\gamma}_{k}{d}_{m}}& \left(0.5\right)\end{array}$  Realize that if there is no fault at location d_{n}, then S_{n}=0, so that the only locations that have an impact on h_{m }are locations d_{m }where actual faults exist.
 Given h(d_{m}), one solves for S_{m }
S_{m}≈h_{m} (0.6)
since the only term that doesn't approximately integrate out in the equation above is when d_{n}=d_{m}. One then needs to solve for S_{11,m}. Previously it was noted that:$\begin{array}{cc}{S}_{m}={S}_{11,m}\prod _{p=1}^{m1}{S}_{12,p}{S}_{21,p}\approx {h}_{m}& \left(0.7\right)\end{array}$ $\begin{array}{cc}{S}_{11,m}\approx \frac{{h}_{m}}{\prod _{p=1}^{m1}{S}_{12,p}{S}_{21,p}}& \left(0.8\right)\end{array}$
but one does not know S_{12,p }and S_{21,p}. If one assumes a reciprocal junction, then S_{12,p}=S_{21,p}, and therefore$\begin{array}{cc}{S}_{11,m}\approx \frac{{h}_{m}}{\prod _{p=1}^{m1}{\left({S}_{12,p}\right)}^{2}}& \left(0.9\right)\end{array}$  Since one only cares about finding the magnitude of S_{11,m},
$\begin{array}{cc}\text{\hspace{1em}}\uf603{S}_{11,m}\uf604\approx \frac{\uf603{h}_{m}\uf604}{\prod _{p=1}^{m1}{\uf603{S}_{12,p}\uf604}^{2}}& \left(0.10\right)\end{array}$  More particularly, after the inverse transform has been applied to the complex reflection coefficient representing the power outputs of the sixport junction, one nonetheless needs to find a way to subtract out the effect of the previous faults so that the amplitude of those faults does not corrupt the measurement of the fault in question. This corruption is usually in the form of noise and inconsequential faults.
 Note that if one just applies a simple inverse attenuation curve, one really is reading the fault return loss magnitude off of the graph, which is incorrect. The reading has an error that is related to the amplitude of the prior faults and one therefore needs a way to subtract out the effect of the prior faults.
 Note that if one has a reflection ahead of a second reflection, the first reflection is going to take off a certain amount of amplitude because one is not going to have that much of a signal going past the first reflection to the second reflection.
 In order to take out the effect of prior reflections, one has to do a twostep process in which one first ascertains the distances of the faults before knowing their amplitudes. In order to do so, one solves for the magnitudes by making an approximating assumption. The assumption is that the fault behaves as a twoport device and that the device is lossless. This means that the power going out is the same as the power going in. In most cases, this is close to reality. One then makes some assumptions about phase. First of all, the phase of the output of that fault with respect to the input is assumed to be zero. Making that assumption, one can solve for the transfer function of the first fault. Once one solves for the transfer function of the first fault, then one has enough knowns to be able to solve for the transfer functions of the subsequent faults.
 Normally, what one receives is a mixture of the losses from the first fault, the second fault, the third fault, et cetera. Thus, one receives a relatively complicated set of data. By following the twostep process, what one is doing is making enough measurements so that one can form simultaneous equations and solve for the unknowns.
 The net result is that one can correctly report the amplitude of a fault, meaning the magnitude of the reflection coefficient of each fault, even if it is preceded by another fault. Thereafter one can use simple amplitude thresholding to filter out low amplitude noise and inconsequential faults.
 The presentation below describes this process as can be seen from Equations 0.60.10.
 If one looks at Equation 0.10, one sees that the magnitude of fault m is shown as S_{11,m}. S_{11,m }is derived from the microwave scattering parameters, meaning that it is the transfer function out of Port 1 and back to Port 1 of the particular prior fault in question. One in essence injects the signal into Port 1 and measures the reflected signal back, with the result being a complex quantity. Thus the magnitude of that particular fault is approximately equal to a quotient, with the top portion of the quotient being the magnitude of h_{m}.
 The bottom of the quotient is a product, and it is a product of all of the magnitudes of prior faults from p=1 to m−1. p is an index of the prior faults, namely the faults to prior to the fault m that one is monitoring. If one looks at the magnitude squared, inside the magnitude is S_{12,p}. What this is saying is that it is the product of the forward transfer functions S_{12 }of all the faults prior to fault m. This procedure removes the effect of prior faults from the measurement of the magnitude of fault m. As a result, what is transpiring in the twostep process is that one takes each of the faults, determines its magnitude and corrects the value of the reflection coefficient of the fault in question by taking into account the magnitudes of all prior faults.
 In the subject invention one can easily use the subject multiport junction because of the use of a unique calibration technique that can be applied in the field. The calibration technique uses a twostage calibration process. The first stage is a factory calibration, in which the transfer function of the multiport junction is characterized. This yields the scattering matrix as a function of frequency for the multiport junction. This matrix is stored in the memory of the digital signal processor and is used in the process for generating the complex reflection coefficient Γ(f). The multiport junction contains microwave components whose transfer functions are not expected to vary much over time or temperature. Thus, a onetime characterization is sufficient.
 The second stage is done in the field, immediately prior to taking measurements, and it characterizes both the detection portion of the circuit and the RF signal source whose output power varies slightly with frequency. The detection portion of the circuit contains semiconductor components whose transfer characteristics vary over time and temperature. The RF source output power varies slightly across frequency due to imperfections in the device and also may drift over time. These variations can be modeled as gain and offset terms that affect the output power measurement of each multiport junction output port as measured by the detection circuitry.
 Therefore, to accurately estimate the complex reflection coefficient Γ(f) of the transmission line under test, the transfer function of the multiport junction and the gains and offsets due to the RF source and detector circuitry variability must be accounted for.
 In general the field calibration method involves applying at least two different calibration loads to the multiport circuit. These two loads produce two data points for each frequency from which the gain and offset parameters of each port can be calculated for each test frequency.
 In operation, regarding the field calibration process, the RF source is swept across a frequency band and measurements are obtained from each detector output at each test frequency for each calibration load. Prior to this, the multiport junction complex scattering parameters are measured at the factory and are used in conjunction with the calibration circuit transfer functions, the switch transfer functions and standard electric component models for the detector circuitry. This allows one to produce a model of the signals measured by the analogtodigital converter at each output port of the detection circuit for each calibration load. Note that the signal model includes the unknown offsets and gains for each port and each frequency. What these offsets and gains are comprised of depends on the type of power detectors used in the detection circuitry.
 If square law power detectors are employed the gain term for each port accounts for the variation in the RF source power across frequency and accounts for the gains in the detector circuitry that map the output power from each port of the multiport RF circuit, from watts to bits. The offset term in this configuration does not vary with frequency; instead it is a constant across frequency for each port. The offset value for each port is a function of the offsets in the detector circuitry.
 If log based power detectors are employed, the gain term for each port accounts only for the gains in the detector circuitry that map the output power from each port of the multiport RF circuit, from dBm to bits. Therefore, in this configuration there is a unique gain that is constant across frequency for each port. The offset term in this configuration does vary across frequency per port. This is because when log detectors are employed the variation in the RF source and the offsets inherent in the detection circuitry per port vary the offset of each signal across frequency as measured at the A/D outputs.
 In the next step the gains and offsets in the system model are varied until one minimizes the square error between the measured A/D output signals for each calibration load and the corresponding model of those measurements. The system gains and offsets which result in minimum square error between the measured signals and the model are then used in conjunction with the factory measured scattering parameters of the multiport RF circuit in the process for generating the complex reflection coefficient Γ(f).
 Note that the number of calibration loads is greater than one and equal to or greater than the number of unknown calibration parameters. Note further that the accuracy of the offset and gain is proportional to the number of loads. The more loads used, the more accurately the offsets and gains can be estimated.
 More particularly, the first stage of calibration uses a commercially available microwave laboratory network analyzer to measure the scattering parameters of the multiport device. The second stage uses one of two calibration methods, one involving the use of attenuators between the signal source and the multiport junction in conjunction with a matched load; and the other involving two or more RLC calibration standards to characterize the transfer functions of the detection circuits and the variability in the RF source power across frequency.
 In the RLC method, the calibration can be done automatically by switching in the RLC calibration standards in a fashion transparent to the operator. In contrast, published sixport calibration methods use 5 to 12 external heavy calibration cables.
 More particularly, it is the ability to precalibrate and rapidly recalibrate in the field, which leads to the attractiveness of using a multiport junction either for reflectometry or for other purposes where the multiport junction is employed.
 However, there are two issues with respect to frequency domain reflectometers using a multiport junction. The first is the frequency source itself, the output of which as a function of frequency may vary over time. The second is the change over time of the power measurement diodes or log amplifiers and other semiconductor devices in the detection circuitry.
 It is noted that the complex scattering parameters of the multiport junction as a function of frequency can be ascertained at the factory using a standard network analyzer.
 In a real system the source power is not exactly constant with frequency. Thus its variation must be accounted for in the calibration. Since the calibration incorporates the nominal source power, the variation with frequency is accounted for in offsets or gains applied to the detection circuit output signals depending on whether log or square law power detectors are used as described above. The detection circuitry contains components whose gains and offsets vary with time and are also accounted for in offsets and gains applied to the detection circuit output signals.
 In order to be able to characterize the detectors and RF source power variation in the field two calibration methods are presented. The first involves sequentially switching the cable under test port to two or more known loads that are each comprised of a different RLC network. Each load has a complex reflection coefficient profile Γ_{c}(f) across frequency that is measured by a network analyzer in the factory. Note c denotes the calibration load index. The complex reflection coefficient profiles for each calibration load are stored in system memory and used during field calibration to determine the gains and offsets.
 It is important to note that since the source varies only slowly with frequency, one need not measure every frequency. Instead, the calibration measurement can take a thinned set of data and can be interpolated to reduce calibration time.
 It is also important to note that one can construct an RLC microwave circuit that does not vary much with temperature. However, this invention does include the ability to measure and store the complex reflection coefficient profiles for each calibration standard taken at multiple different temperatures. Then, when they are used during field calibration a temperature sensor in the device can measure the current temperature of the system and perform the field calibration using the complex reflection coefficient profiles Γ_{c}(f) that were measured at the closest temperature.
 Note for the RLC load method, the value of each RLC element can be any practical valuable that results in the complex reflection coefficient profile of each load to be dissimilar across frequency. In one embodiment one uses a bond ribbon and either a 0.5Ohm resistor or a 150Ohm resistor depending on the calibration load used. The resistor is coupled to a 0.2 nH pedestal inductor, in turn coupled to a 100 pF chip capacitor to ground. By so doing one switches in one of two different calibration loads at the test port, from which not only can the characteristics of each of the diode detectors be measured, but also the power variation of the signal source with frequency. Thus with two internal RLC calibration loads, the characteristics of which are determined at the factory, one can quickly calibrate the reflectometer in the field without the use of multiple calibrated lengths of transmission line.
 For each RLC calibration load the RF source is swept across frequency and the outputs of the each port of the detection circuit is measured with an A/D converter for each test frequency. In so doing one obtains a measured signal out of each detector across frequency for each calibration load denoted b_{cn}(f). For each calibration load a signal model for the A/D measured detector outputs is generated denoted {circumflex over (b)}_{cn}(f,g_{n},a_{n}). This model is based on the scattering parameters of each calibration load and the multiport RF circuit as measured during the factory calibration process. It is also based on the nominal RF source power, standard component models for the detector circuitry and the gains and offsets due to RF source power and detector circuitry variation.
 It is therefore the purpose of this calibration procedure to determine the gains and offsets for each port that minimize the square error between the measured signals b_{cn}(f) for each calibration load Γ_{c}(f) and their respective signal model {circumflex over (b)}_{cn}(f,g_{n},a_{n}). Because the signal model can take on one of two forms depending on whether square law or log detectors are used, the calibration solution also has two respective forms. If log detectors are used then the gain term for each port remains constant while the offset varies with frequency. On the other hand, if square law detectors are used, then the gain term for each port varies with frequency and the offset remains constant. The calibration process, which involves selecting the gains and offsets that minimize the square error between the signal models and the measurements, is described mathematically for each detector type below.
 Square Law Detectors Solution:
$\begin{array}{cc}\left\{{g}_{n}\left(f\right),{a}_{n}\right\}=\mathrm{arg}\text{\hspace{1em}}\mathrm{min}\sum _{c=1}^{C}{\uf605{b}_{\mathrm{cn}}\left(f\right){\hat{b}}_{\mathrm{cn}}\left(f,{g}_{n}\left(f\right),{a}_{n}\right)\uf606}^{2}.& \left(0.11\right)\end{array}$  Log Detectors Solution:
$\begin{array}{cc}\left\{{g}_{n},{a}_{n}\left(f\right)\right\}=\mathrm{arg}\text{\hspace{1em}}\mathrm{min}\sum _{c=1}^{C}{\uf605{b}_{\mathrm{cn}}\left(f\right){\hat{b}}_{\mathrm{cn}}\left(f,{g}_{n},{a}_{n}\left(f\right)\right)\uf606}^{2}& \left(0.12\right)\end{array}$
where the signal model when Square Law Detectors are used is defined as:
{circumflex over (b)} _{cn}(f,g _{n}(f),a _{n})=g _{n}(f)·(α_{n}(f)Γ_{c}cf)^{2}+β_{n}(f)Re{Γ _{c}(f)}+γ_{n}(f)Im{Γ _{c}(f)}+δ_{n}(f))+a _{n} (0.13)
and the signal model when Log Detectors are used is defined as:
{circumflex over (b)} _{cn}(f,g _{n} ,a _{n}(f))=g _{n}·LOG_{10}(α_{n}(f)Γ_{c}(f)^{2}+β_{n}(f)Re{Γ _{c}(f)}+γ_{n}(f)Im{Γ _{c}(f)}+δ_{n}(f))+a _{n}(f) (0.14)  In both models α_{n}(f), β_{n}(f), γ_{n}(f) and δ_{n}(f) are known parameters that are functions of the complex scattering parameters s_{nm}(f) of the multiport circuit and are also functions of the nominal RF source power P_{s}. These relationships are defined in equations 0.150.18 below.
α_{n}(f)=P _{s} ·s _{21}(f)s _{n2}(f)^{2} (0.15)
β_{n}(f)=P _{s}·2[Re{s _{21}(f)s _{n2}(f)}Re{s _{n1}(f)}+Im{s _{21}(f)s _{n2}(f)}Im{s _{n1}(f)}] (0.16)
γ_{n}(f)=P _{s}·2[Re{s _{21}(f)s _{n2}(f)}Im{s _{n1}(f)}−Im{s _{21}(f)s _{n2}(f)}Re{s _{n1}(f)}] (0.17)
δ_{n}(f)=P _{s} ·s _{n1}(f)^{2} (0.18)  Notice that after substitution of the variables of Equations 0.150.18 into equations 0.13 and 0.14 one can see that both signal models are functions of the complex scattering parameters s_{nm}(f) of the multiport circuit as measured during factory calibration, the nominal source power P_{s}, and the complex reflection coefficient profile for each calibration standard Γ_{c}(f) as measured in the factory. Note that in these equations n denotes the detector output port index and c denotes the calibration standard index. C denotes the total number of calibration standards.
 It is important to note the gains and offsets are different for each port. Therefore the optimization described in equation 0.11 and 0.12 is performed independently for each detector port n.
 On a port by port basis, taking the measurements from each port and each calibration standard and subtracting the model, yields an error for every trial of gain and offset (g_{n}(f),a_{n }or g_{n},a_{n}(f)), which when squared and summed over each calibration standard c, yields the total square error for every trial of gains and offsets. One then uses the gains and offsets that result in the minimum square error.
 System models shown in Equations 0.13 and 0.14 are both linear equations in terms of the unknown gains and offsets (g_{n}(f),a_{n }or g_{n},a_{n}(f)). Therefore one can employ linear least squares optimization techniques to determine the values for those gains and offsets that best minimize the square error between the measurements and the model. It is known that one way to solve this type of linear least squares problem is to stack each measurement taken for each calibration load into a vector and define the known portions of the signal model in a matrix. Then using that vector and matrix, one directly computes the unknown gains and offsets.
 In the calibration method involving attenuators, a 50ohm, or matched load is switched to the cable under test port of the device. This has the effect of reducing the reflection from that port to a negligible value (i.e. Γ(f)≈0). Now the A/D measurements at each detector circuitry output port is a function of the RF source, the scattering parameters of the multiport RF circuit and the internals of the detection circuitry. As stated before, if log power detectors are used such as Dynamic Log Video Amplifiers, DLVAs, then the gain is a constant value and the offset changes with frequency for each detector output port. If square law power detectors are uses such as diode detectors, then the gain changes over frequency and the offset is constant. These gains and offsets can be determined by varying the RF source power and at each power setting, sweeping the RF source across frequency, taking detector circuit output measurements using the A/D, and comparing the A/D measurement to a signal model for those measurements that is a function of the unknown gains and offsets. One then selects the gains and offsets that best minimize the error between the measurements and the model.
 This can be accomplished by switching several attenuators between the probe and the RF source and taking power measurements over the region of interest. In place of the switchable attenuators one could also directly vary the RF source output power.
 By varying the power, the set of power measurements at the detectors gives a full characterization of the variability of the RF source, and the gain and offset as determined by the detectors and the conversion from an A/D converter reading to a real power value. Once these power measurements are taken, the gain and the offset values can be determined using a variety of estimation algorithms.
 Similar to the calibration method using RLC loads, the objective of the calibration method using attenuators is to select the values for the gains and offsets for each port that minimize the square error between the detector output measurement and the signal model for those measurements. This optimization is defined in equations 0.11 and 0.12 above. The only difference is that the signal model is slightly different for this calibration technique. In this calibration method the signal model for both square law and log power detectors are defined as follows.
 Signal Model Using Square Law Detectors:
{circumflex over (b)} _{cn}(f,g _{n}(f),a _{n})=g _{n}(f)·(P _{in} [c]s _{n1}(f)^{2})+a _{n} (0.19)  Signal Model Using Log Detectors:
{circumflex over (b)} _{cn}(f,g _{n} ,a _{n}(f))=g _{n}·LOG_{10}(P _{in} [c]s _{n1}(f)^{2})+a _{n}(f) (0.20)
where s_{n1}(f) is the measured scattering parameters of the multiport RF circuit between port 1 and port n and P_{in}[c] is the known power incident on port (1) of the multiport RF circuit when attenuator “c” is connected between the RF signal source and port (1) of the multiport RF circuit. Note that alternatively, P_{in}[c] can be defined as the RF signal source output power when no attenuator is used. In this case this power would differ for each calibration standard “c” by directly changing the RF source output power instead of using a bank of attenuators.  Similar to the calibration approach using RLC loads, on a port by port basis, taking the measurements from each port and each calibration standard and subtracting the model, yields an error for every trial of gain and offset (g_{n}(f),a_{n }or g_{n},a_{n}(f)), which when squared and summed over each calibration standard c, yields the total square error for every trial of gains and offsets. One then uses the gains and offsets that result in the minimum square error.
 System models shown in Equations 0.19 and 0.20 are both linear equations in terms of the unknown gains and offsets (g_{n}(f),a_{n }or g_{n},a_{n}(f)). Therefore one can employ linear least squares optimization techniques to determine the values for those gains and offsets that best minimize the square error between the measurements and the model. It is known that one way to solve this type of linear least squares problem is to stack each measurement taken for each calibration load into a vector and define the known portions of the signal model in a matrix. Then using that vector and matrix, one directly computes the unknown gains and offsets.
 Alternatively one can employ a two step process for estimating the gains and offsets. When log power detectors are employed, one can estimate the gains first using the equation below.
$\begin{array}{cc}{g}_{n}=\left[\begin{array}{cc}1& 0\end{array}\right]\xb7{\left(\begin{array}{cc}{\underset{\_}{\underset{\_}{R}}}_{n}^{T}& {\underset{\_}{\underset{\_}{R}}}_{n}^{T}\end{array}\right)}^{1}{\underset{\_}{\underset{\_}{R}}}_{n}^{T}{\underset{\_}{b}}_{n}\text{\hspace{1em}}\mathrm{where}& \left(0.21\right)\\ {\underset{\_}{\underset{\_}{R}}}_{n}=\left[\begin{array}{cc}\underset{\_}{1}\xb7{\mathrm{log}}_{10}\left({P}_{\mathrm{in}}\left[1\right]\right)& \underset{\_}{1}\\ \vdots & \vdots \\ \underset{\_}{1}\xb7{\mathrm{log}}_{10}\left({P}_{\mathrm{in}}\left[C\right]\right)& \underset{\_}{1}\end{array}\right]& \left(0.22\right)\\ {\underset{\_}{b}}_{n}={\left[\begin{array}{ccccccc}{b}_{1n}\left(1\right)& \dots & {b}_{1n}\left(F\right)& \dots & {b}_{\mathrm{Cn}}\left(1\right)& \dots & {b}_{\mathrm{Cn}}\left(F\right)\end{array}\right]}^{T}& \left(0.23\right)\end{array}$
In the above equations b_{cn}(f) denotes the measured signal out of port n at frequency f for attenuation (calibration standard) c as measured by the A/D converter, F denotes the total number of frequency measurements, C denotes the total number of attenuation values (calibration standards) used and 1 denotes an F×1 vector of ones.  Once the gain for each port is calculated the offsets are determined as follows.
$\begin{array}{cc}\left[\begin{array}{c}{a}_{n}\left(1\right)\\ \vdots \\ {a}_{n}\left(F\right)\end{array}\right]={\left(\begin{array}{cc}{\underset{\_}{\underset{\_}{\Phi}}}^{T}& \underset{\_}{\underset{\_}{\Phi}}\end{array}\right)}^{1}{\underset{\_}{\underset{\_}{\Phi}}}^{T}\xb7\left[{\underset{\_}{b}}_{n}{g}_{n}{\underset{\_}{e}}_{n}\right]\text{\hspace{1em}}\mathrm{where}& \left(0.24\right)\\ {\underset{\_}{e}}_{n}={\left[\begin{array}{c}\begin{array}{cccc}{\mathrm{LOG}}_{10}\left({P}_{\mathrm{in}}\left[1\right]{\uf603{s}_{\mathrm{n1}}\left(1\right)\uf604}^{2}\right)& \dots & {\mathrm{LOG}}_{10}\left({P}_{\mathrm{in}}\left[1\right]{\uf603{s}_{\mathrm{n1}}\left(F\right)\uf604}^{2}\right)& \dots \end{array}\\ \begin{array}{ccc}{\mathrm{LOG}}_{10}\left({P}_{\mathrm{in}}\left[C\right]{\uf603{s}_{\mathrm{n1}}\left(1\right)\uf604}^{2}\right)& \dots & {\mathrm{LOG}}_{10}\left({P}_{\mathrm{in}}\left[C\right]{\uf603{s}_{\mathrm{n1}}\left(F\right)\uf604}^{2}\right)\end{array}\end{array}\right]}^{T}& \left(0.25\right)\\ \underset{\_}{\underset{\_}{\Phi}}=\left[\begin{array}{c}\underset{\_}{\underset{\_}{I}}\\ \vdots \\ \underset{\_}{\underset{\_}{I}}\end{array}\right].& \left(0.26\right)\end{array}$
Note that in equation 0.26, the matrix Φ contains C stacked identity matrices, where each identity matrix I is of dimension F×F.  This two step process is slightly different when square law power detectors are employed. In this case one first estimates the offset for each port using the following equations.
$\begin{array}{cc}{a}_{n}=\left[\begin{array}{cc}1& 0\end{array}\right]\xb7{\left(\begin{array}{cc}{Q}_{n}^{T}& {\underset{\_}{\underset{\_}{Q}}}_{n}\end{array}\right)}^{1}{\underset{\_}{\underset{\_}{Q}}}_{n}^{T}{\underset{\_}{b}}_{n}\text{\hspace{1em}}\mathrm{where}& \left(0.27\right)\\ {\underset{\_}{\underset{\_}{Q}}}_{n}=\left[\begin{array}{cc}\underset{\_}{1}\xb7{P}_{\mathrm{in}}\left[1\right]& \underset{\_}{1}\\ \vdots & \vdots \\ \underset{\_}{1}\xb7{P}_{\mathrm{in}}\left[C\right]& \underset{\_}{1}\end{array}\right]& \left(0.28\right)\end{array}$  Once the offset for each port is calculated the gains are determined as follows.
$\begin{array}{cc}\left[\begin{array}{c}{g}_{n}\left(1\right)\\ \vdots \\ {g}_{n}\left(F\right)\end{array}\right]={\left(\begin{array}{cc}{\underset{\_}{\underset{\_}{\Omega}}}^{T}& \underset{\_}{\underset{\_}{\Omega}}\end{array}\right)}^{1}{\underset{\_}{\underset{\_}{\Omega}}}^{T}\xb7\left[\begin{array}{cc}{\underset{\_}{b}}_{n}& \underset{\_}{1}\xb7{a}_{n}\end{array}\right]\text{\hspace{1em}}\mathrm{where}& \left(0.29\right)\\ \underset{\_}{\underset{\_}{\Omega}}=\left[\begin{array}{c}{\underset{\_}{\underset{\_}{D}}}_{1}\\ \vdots \\ {\underset{\_}{\underset{\_}{D}}}_{C}\end{array}\right].& \left(0.30\right)\\ {\underset{\_}{\underset{\_}{D}}}_{c}=\mathrm{diag}\left(\lfloor \begin{array}{ccc}{P}_{\mathrm{in}}\left[c\right]{\uf603{s}_{\mathrm{n1}}\left(1\right)\uf604}^{2}& \dots & {P}_{\mathrm{in}}\left[c\right]{\uf603{s}_{\mathrm{n1}}\left(F\right)\uf604}^{2}\end{array}\rfloor \right)& \left(0.31\right)\end{array}$
Note that diag(.) is the expression for creating a diagonal matrix from each element of the input vector. Therefore D _{c }is an F×F diagonal matrix.  Referring now to
FIG. 1 , it has been found that one can use the power outputs of a multiport junction to form the basis for an Inverse Fourier Transform to obtain distance to faults in a transmission line or waveguide. Thus, in one embodiment a frequency domain reflectometer includes a multiport junction 10 coupled to a module 11, which estimates the reflection coefficient based on multiport junction outputs. The estimated reflection coefficient is coupled to an Inverse Fourier Transform 12. In the illustrated embodiment the multiport junction is a conventional sixport junction. One port, port 14, of the multiport junction is connected to a transmission line under test 16. The transmission line may be either a cable or a waveguide. In one embodiment the transmission line may be terminated with a 50Ohm resistor 18, nothing noting that the system will work equally well with an unterminated cable or transmission line. Port 20 of junction 10 is provided with a signal source 22, which in one embodiment sweeps through a number of frequency bands, with the output of signal source coupled to the cable under test through the sixport junction.  The power outputs of the multiport junction are converted to a reflection coefficient or Γ(f), which is coupled to the Inverse Fourier Transform to convert the frequency domain representation of the reflection coefficient into a time domain representation. The time domain representation exhibits peaks that when graphed against time indicate the distance to a fault in the transmission line under test. For this purpose a module 24 that calculates distance to a fault is coupled to a display 26 so as to identify faults, as well as the distance thereto.
 The output of the Inverse Fourier Transform is also applied to a module 28, which calculates the return loss at each of the detected peaks. Return loss is a measurement of the severity of the fault or the percent of energy reflected at the fault back to the source.
 Referring now to
FIG. 2 , while numbers of different multiport junctions can be used, in one embodiment the sixport junction is discussed in which the multiport junction 10 includes test port 14 and the signal source port 20.  As will be seen, the output power from the sixport junction is available at ports 30, 32, 34 and 36, respectively P1, P2, P3 and P4.
 The sixport junction includes 90° quadrature hybrids 40, 42, 44 and 46, with an output 48 of hybrid 40 being coupled to a 0° power divider 50 having outputs 52 and 54 respectively coupled to ports 56 and 58 of hybrids 42 and 44.
 Hybrid 42 at port 60 is provided with a signal from hybrid 40 at its port 62, with port 64 of hybrid 42 providing the P3 power output as detected by a diode detector 67.
 Output ports 68 and 70 of hybrid 46 are coupled to respective diode detectors 72 and 74 so that the power P1 and P2 available at ports 68 and 70 can be measured.
 For hybrid 44, output port 72 is connected by a 50Ohm resistor 73 to ground, and output port 74 is coupled through diode 78 so that P4 can be measured.
 The detected output power from the sixport junction available at P1, P2, P3 and P4 is coupled to a unit 80, which estimates the reflection coefficient Γ as a function of frequency. As will be seen, this unit or module utilizes an offset parameter and a gain parameter, the importance of which will become evident.
 These estimates are coupled to a modified Inverse Fourier Transform module 82, the output of which is coupled to a module 84 that calculates the distance to the faults. Having found the distance to the faults, a module 86 is used to estimate the fault magnitude for each of the faults.
 As will be appreciated, the functions of modules 80, 82, 84 and 86 can be carried out in a Digital Signal Processor illustrated by dotted line 87, such that the outputs of DSP 87 can include estimated fault locations, estimated percent reflections from each detected fault, the complex frequency response of the device under test and the γ(d) output of the modified IFT. Please also delete the δ(d) from the bottom of
FIG. 2 , and just make it say “output of modified IFT”.  In general, and referring now to
FIG. 3A , the P1, P2, P3 and P4 outputs of the sixport junction are applied, in one embodiment, to module 80 that estimates the reflection coefficient as a function of frequency. In this embodiment the result is a complex reflection coefficient, as opposed to the absolute magnitude coefficient of the prior art. The complex reflection coefficient is a function of frequency coupled to modified Inverse Fourier Transform module 80 to produce a time domain reflection coefficient as a function of distance that takes into account not only the phase shift per unit length of transmission line as illustrated at 88, but importantly takes into account attenuation per unit length of transmission line as illustrated at 90.  Taking into account attenuation per unit length of transmission line eliminates the necessity for compensating for transmission line attenuation after the IFT, as indicated by dotted box 92, which is not used in the subject system. Since attenuation per unit length of transmission line is a factor in obtaining appropriate results of the IFT, it is of great advantage to take into account the attenuation per unit length of transmission line in the Inverse Fourier Transform itself.
 Referring to
FIG. 3B , while e^{−jφ} ^{ k }was that on which Inverse Fourier Transforms operated in the past, this only measures phase shift as opposed to phase shift plus attenuation.  On the other hand, the portion of the reflection coefficient of Equation 0.1 indicates that e is raised to a complex value, namely e^{−2γ} _{k} ^{d} _{m }where γ_{k }is defined as α{square root}fk+j2πfk/v. As can be seen, γ_{k }takes into account α and v, where α{square root}f_{k }refers to attenuation per unit length and j2πfk/v to phase shift per unit length of transmission line. Thus, the term e^{−γ(dn−dm) }incorporates both phase information and attenuation information directly in the Inverse Fourier Transform, with the equation in
FIG. 3B being derived from Equation 0.4.  Thus the reflection coefficient Γ(f) is a complex reflection coefficient of the entire cable or waveguide, which can be used to derive the scattering parameters of the individual faults themselves.
 It is important to note that, if one does not use the modified Inverse Fourier Transform, herein called the Taylor Transform, one generates peaks with errors related to the amplitudes of prior faults. Any attempt to apply a gain that tries to compensate for the transmission line attenuation causes one to detect peaks with incorrect amplitudes.
 While the above discussion of
FIG. 3B relates to the accuracy of measuring fault amplitude in a multifault environment, elimination of ghosts is accomplished in the subject invention by measuring Γ_{k }as a complex value. In the past, frequency domain reflectometers measured only the absolute value of Γ_{k}, i.e., Γ_{k}. By using a complex value for Γ_{k }one can eliminate the nonlinear absolute value operation, thereby eliminating a source of ghosts, for instance, from the sum and difference values created by multiple reflections.  Having taken into account line attenuation, there is nonetheless the problem of eliminating noise, secondary reflections and inconsequential peaks that are due to prior faults to the one that has been identified. Thus, in order to eliminate the noise, secondary reflections and inconsequential peaks, one essentially has to threshold out the effect of previous faults. In order to do this, in one embodiment one first solves for distances ahead of time before knowing amplitudes, as illustrated at 96. In this twostep process, once knowing where the faults are, one then solves for amplitude of each fault as illustrated at 98. With each fault now having an amplitude or magnitude, one can threshold out those magnitudes below some predetermined threshold as illustrated at 100.
 The output of thresholding circuit 100 is coupled to a display 101 that displays amplitude peaks 102 along a timeline corresponding to distance to a fault as illustrated in 104. The particular faults are indicated by #1, #2, #3 and #4. The severity of the faults is indicated at 100 to be either percent reflection or return loss, with the higher the percent reflection the lower the return loss.
 It will be appreciated that the amplitude of the faults alone does not necessarily correlate to the percent reflection at each of the faults. However, as illustrated at 106, the percent reflection for each of the numbered faults is calculated and displayed so that an operator can ascertain not only the distance to each of the faults but also their severity.
 More particularly and referring now to
FIG. 4A , in one embodiment of the subject invention, as illustrated at 120, one obtains measurements of the powers from the multiport junction and in one embodiment outputs four voltages over line 122 to a module 124 that estimates a complex reflection coefficient Γ(f) for each frequency. The estimation of the complex reflection coefficient is given by$\begin{array}{cc}\Gamma \left(f\right)=\mathrm{arg}\text{\hspace{1em}}\mathrm{min}\sum _{n=3}^{6}{\uf605{b}_{n}\left(f\right){\hat{b}}_{n}\left(f,\Gamma \left(f\right)\right)\uf606}^{2}& \left(0.32\right)\end{array}$
for a sixport circuit. Note that n denotes the output port index of the sixport circuit, b_{n}(f) denotes the measurements out of the n^{th }A/D port and refers to the power out of the n^{th }port of the sixport circuit as measured by the detection circuit. Finally, {circumflex over (b)}_{n}(f,Γ(f)) is the model of each A/D output signal as a function of the unknown complex reflection coefficient Γ(f).  Therefore, from this equation one can see that to estimate the complex reflection coefficient of the transmission line one must select the value of Γ(f) for each frequency that minimizes the square error between the measured signals and the model. There are many techniques known to people skilled in the art, that can be applied to efficiently perform this optimization. However the specific optimization techniques that can be applied are dependant on the structure of the signal model.
 In the case of the a multiport circuit connected to detection circuitry which includes power detectors and A/D converters, as described in this invention, the signal model can take one of two forms. These two forms depend on whether square law or log power detectors are employed in the detection circuitry. These two signal models are defined below for both square law and log detector configurations respectively.
 Square Law Detector
{circumflex over (b)} _{n}(f,Γ(f))=g _{n}(f)·(α_{n}(f)Γ(f)^{2}+β_{n}(f)Re{Γ(f)}+γ_{n}(f)Im{Γ(f)}+δ_{n}(f))+a _{n}(f) (0.33)  Log Detector
{circumflex over (b)} _{n}(f,Γ(f))=g _{n}(f)·LOG_{10}(α_{n}(f)Γ(f)^{2}+β_{n}(f)Re{Γ(f)}+γ_{n}(f)Im{Γ(f)}+δ_{n}(f))+a _{n}(f) (0.34)
Here α_{n}(f), β_{n}(f), γ_{n}(f) and δ_{n}(f) are known parameters that are functions of the complex scattering parameters s_{nm}(f) of the multiport circuit and are also functions of the nominal RF source power P_{s}. These relationships are defined in equations 0.150.18 above.  Notice that after substitution of the variables of Equations 0.150.18 into equations 0.33 and 0.34 one can see that both signal models are functions of the complex scattering parameters s_{nm}(f) of the sixport circuit as measured during factory calibration and are also functions of the gains and offsets, g_{n}(f) and a_{n}(f) that are estimated during the field calibration process.
 Taking the measurements from each port and subtracting the model for each port yields an error for every trial of Γ(f), which when squared and summed over each port yields the total square error for every trial of Γ(f). One then uses the Γ(f) that results in the minimum error. Based on the system models shown in Equations 0.33 and 0.34 one can employ non linear least squares optimization techniques to determine the values of Γ(f) that best minimize the square error between the measurements and the model. One method in particular that can be employed is the Newton search algorithm. This is an algorithm that can optimize Equation 0.32 by employing a computationally efficient searching technique.
 It is noted that when log detectors are employed one may choose to first preprocess the measured data to remove the effects of the gains and offsets and logarithm. This process is equivalent to solving the following optimization problem in place of the one defined in equation 0.32.
$\begin{array}{cc}\Gamma \left(f\right)=\mathrm{arg}\text{\hspace{1em}}\mathrm{min}\sum _{n=3}^{6}{\uf605{10}^{\left(\frac{{b}_{n}\left(f\right){a}_{n}\left(f\right)}{10{g}_{n}\left(f\right)}3\right)}{10}^{\left(\frac{{\hat{b}}_{n}\left(f,\Gamma \left(f\right)\right){a}_{n}\left(f\right)}{{g}_{n}\left(f\right)}\right)}\uf606}^{2}& \left(0.35\right)\end{array}$
Notice that on the left side of the subtraction the gains offsets and affects of the logarithm are removed from the measured signals. Also notice that the model denoted by the right hand side of the subtraction also has the gains offsets and logarithm effects removed. This approach is valid as long as the amount of noise riding on the measured signals is low compared to the signals themselves. This is the case in most applications. Thus using this technique will also produce favorable results.  In estimating the complex reflection coefficient Γ(f), module 124 takes into account gains, offsets and a scattering matrix from a calibration step 125. The scattering matrix is derived from a factory calibration process using a network analyzer. The gains and offsets are derived in the field from using one of two internal calibration techniques, one with RLC loads, and the other involving attenuators that are switched in ahead of the multiport circuit.
 In equation 0.35 the gains offsets and the affects of the logarithm are removed from the measured signals b_{n}(f) prior to minimizing the square error between the signal and the model. As equation 0.35 shows the model on the right side of the subtraction also has the effects of the gains, offsets and logarithm removed. Therefore, it incorporates the measured scattering parameters of the multiport circuit and the known RF source power level. Thus both the factory measurements and the field measurements constitute the calibration as can be seen in
FIG. 6 . This applies to both calibration techniques when log detectors are employed.  For a fourport circuit the estimation of the complex reflection coefficient Γ(f) is given by
$\begin{array}{cc}\hat{\Gamma}\left(f\right)=\frac{H\left\{y\left(f\right)\right\}}{D\left(f\right)}& \left(0.36\right)\end{array}$
where H{ } denotes the Hilbert transform and is applied once given y(f) for all measured frequencies “f”. In this equation y(f) is generated by altering the output measurements for each port as follows.  For Log Detectors
$\begin{array}{cc}y\left(f\right)=\frac{{10}^{\left(\left(\frac{{b}_{3}\left(f\right){a}_{3}\left(f\right)}{10{g}_{3}\left(f\right)}\right)3\right)}{\delta}_{3}\left(f\right)}{{\alpha}_{3}\left(f\right)}\frac{{10}^{\left(\left(\frac{{b}_{4}\left(f\right){a}_{4}\left(f\right)}{10{g}_{4}\left(f\right)}\right)3\right)}{\delta}_{4}\left(f\right)}{{\alpha}_{4}\left(f\right)}& \left(0.37\right)\end{array}$  For Square Law Detectors
$\begin{array}{cc}y\left(f\right)=\frac{{b}_{3}\left(f\right)\left({g}_{3}\left(f\right)\xb7{\delta}_{3}\left(f\right)+{a}_{3}\right)}{{g}_{3}\left(f\right){\alpha}_{3}\left(f\right)}\frac{{b}_{4}\left(f\right)\left({g}_{4}\left(f\right)\xb7{\delta}_{4}\left(f\right)+{a}_{4}\right)}{{g}_{4}\left(f\right){\alpha}_{4}\left(f\right)}& \left(0.38\right)\end{array}$
D(f) is a function of the scattering parameters of the multiport circuit and the RF source power and is defined as follows$\begin{array}{cc}D\left(f\right)=\left(\frac{{\beta}_{3}\left(f\right)}{{\alpha}_{3}\left(f\right)}\frac{{\beta}_{4}\left(f\right)}{{\alpha}_{4}\left(f\right)}\right)j\left(\frac{{\gamma}_{3}\left(f\right)}{{\alpha}_{3}\left(f\right)}\frac{{\gamma}_{4}\left(f\right)}{{\alpha}_{4}\left(f\right)}\right)& \left(0.39\right)\end{array}$
In these equations g_{n}(f) and a_{n}(f) denote the gains and offsets respectively, estimated during field calibration. α_{n}(f), β_{n}(f), γ_{n}(f) and δ_{n}(f) are known parameters that are functions of the complex scattering parameters s_{nm}(f) of the multiport circuit and are also functions of the nominal RF source power P_{s}. These relationships are defined in equations 0.150.18 above.  It is important to note that this approach differs significantly from conventional approaches for estimating the complex reflection coefficient when, for example a sixport RF circuit is employed. When using a sixport circuit one has four output power measurements for each frequency that can be used to unambiguously determine the complex reflection coefficient. In this approach the complex reflection coefficient is calculated independently for each frequency. The solution given in equation 0.36 for use with a fourport circuit on the other hand, uses the Hilbert transform to compute the complex reflection coefficient across all frequencies in one step. This is necessary when using a fourport circuit because at each frequency the value for the complex reflection coefficient could be one of two values. To remove this ambiguity the Hilbert transform is used to apply a constraint that across frequency the real and imaginary component of the complex reflection coefficient profile have the same profile with a ninety degree phase shift between them. This constraint is valid because the components that make up the transmission line under test and the fourport circuit also follow the same physical principle. Therefore, by applying this technique one removes the ambiguity at each frequency and can correctly estimate the complex reflection coefficient profile.
 For clarification of the steps performed in 0.360.39, by using the signal models in equations 0.33 and 0.34 in place of the measurements b_{n}(f) one can define a model for y(f) denoted ŷ(f).
$\begin{array}{cc}\hat{y}\left(f\right)=\mathrm{Re}\left\{\left(\left(\frac{{\beta}_{3}\left(f\right)}{{\alpha}_{3}\left(f\right)}\frac{{\beta}_{4}\left(f\right)}{{\alpha}_{4}\left(f\right)}\right)j\text{\hspace{1em}}\left(\frac{{\gamma}_{3}\left(f\right)}{{\alpha}_{3}\left(f\right)}\frac{{\gamma}_{4}\left(f\right)}{{\alpha}_{4}\left(f\right)}\right)\right)\Gamma \left(f\right)\right\}& \left(0.40\right)\end{array}$
Substituting equation 0.39 into 0.40 yields
ŷ(f)=Re{D(f)Γ(f)} (0.41)
Thus by applying the Hilbert transform to y(f) and then dividing by D(f) as shown in equation (0.36) one obtains an estimate for the complex reflection coefficient Γ(f) for the transmission line under test at each frequency.  It is the purpose of the Γ estimation module to provide one complex reflection coefficient (Γ_{k}) for each frequency. As illustrated at 128, one performs the aforementioned modified IFT, the output of which on line 130 is applied to a unit 132, which identifies the candidate faults and more particularly identifies the distances to the candidate faults without, for instance, calculating the magnitude or amplitude of the fault. The results of the outputs of unit 132 are the distances to the candidate faults, which are outputted on line 134 and are applied to a unit 136 that calculates the fault magnitudes, compensating for prior faults. It is noted that the complex reflection coefficient for each distance is inputted over line 140 so that the fault magnitude calculation can proceed.
 The output of module 136 over line 142 is the magnitude of the candidate faults. These magnitudes are input to a thresholding filter 144, which filters out faults below a given magnitude.
 The results, as illustrated on line 146, are the distances to the faults that are above the threshold and the magnitudes of the faults, with faults under a predetermined magnitude being removed.
 Because the system of
FIG. 4A may be computationally intense and referring now toFIG. 4B , a traditional Inverse Fast Fourier Transform 128′ is substituted for the modified IFT 128 ofFIG. 4A to speed up the initial processing. Secondly, a module 148 is interposed in line 134 to refine fault locations from unit 132. It is module 148 that now employs the modified IFT using the Taylor algorithm. However, it operates on a muchreduced number of data points.  As to the operation of the unit that identifies candidate faults, the algorithm looks at the plot of the complex reflection coefficient versus distance. This plot will have a large number of peaks, most of them due merely to noise. A “peak” is mathematically defined as a location where the plot's slope changes from positive to negative. Thus, the algorithm identifies all of those peaks, the vast majority of them bogus.
 The module that refines fault locations uses the modified Inverse Fourier Transform. However, there is an additional feature of this modified IFT algorithm. The problem is that the complex reflection coefficient vs. distance has some granularity. It is only calculated every “x” inches, for example, perhaps every 6 inches. But the actual fault may lie between two data points (i.e. at the 3″ point). So if one were to calculate the fault magnitude based on the granular distance, then one would have some error due to that granularity. The refinement part of the modified Taylor Inverse Fourier Transform algorithm employed in
FIG. 4B is that one calculates the modified IFT for not only the candidate fault distance given, but also one adjusts the distance slightly in each direction around the candidate fault distance, and picks the distance that gives the largest modified inverse Fourier transform output. Then one goes on to the next candidate fault and does the same thing again for every candidate fault.  The motivation for using a traditional IFFT first to identify candidate faults is as follows:
 The
FIG. 4A embodiment used the modified IFT on the whole complex reflection coefficient vector, which can involve 4096 data points. This was found to be computationally intensive, so that the operator would have to wait a long time for the results. To work around this problem, in one embodiment a traditional IFFT is employed, which is very fast. The traditional IFFT can adequately identify the fault locations. However, the regular IFFT cannot accurately determine the magnitudes of the peaks.  To solve this problem the subject system takes the output of the IFFT and identifies the candidate faults, so that one ends up with some number of candidates that is much smaller than 4096. The modified IFT is then performed on that much smaller number of candidate faults, and it does not take nearly as long as when using the modified IFT of
FIG. 4A . It has been found that theFIG. 4B reflectometer is of very reasonable computational complexity resulting in reasonable operator wait time.  Referring to
FIG. 5 and theFIG. 4A embodiment, with respect to the taking of measurements as illustrated at 120 inFIG. 4A , a signal source 150 is applied in one embodiment to a sixport junction 152, which has the test port thereof 154 coupled to a cable under test 156. The outputs of the sixport junction are four sixport output powers for each frequency, here labeled P_{1}, P_{2}, P_{3 }and P_{4}. These power outputs are applied to a detection unit 158, which converts the powers into four voltages, R_{1}, R_{2}, R_{3 }and R_{4}.  Prior to performing the modified IFT, as illustrated at 124, the four voltages for each frequency generated by detection circuit 158 are applied to a detection calibration module 160 within the complex reflection coefficient estimation unit 124. Detection circuit 158 takes into account offset and gain coefficients to provide an estimate of the sixport output powers, again here illustrated at P_{1}, P_{2}, P_{3 }and P_{4}. These powers are then applied to a sixport calibration module 162, which adjusts the complex reflection coefficient estimation in accordance with the factory testing that is done by a network analyzer. In other words, one takes into account the scattering matrix for the multiport junction measured at the factory. The result, as illustrated on line 126, is one complex cable return loss or reflection coefficient for each frequency.
 Referring to
FIG. 7 , module 128 performs the modified IFT so that, with one complex reflection coefficient for each frequency, one derives one complex reflection coefficient for each distance.  As illustrated in
FIG. 8 , module 132 identifies the candidate faults by taking one complex reflection coefficient for each distance, namely one complex cable return loss for each distance, and applies it to a peak detector 164 to obtain distances to candidate faults that are outputted over line 134.  As illustrated in
FIG. 9 , module 136 for calculating fault magnitudes compensating for prior faults includes inputs over lines 134 and 140, and through use of the transform illustrated, and computes the magnitudes of candidate faults as illustrated on line 142.  As illustrated in
FIG. 10 , thresholding circuit 144 includes a thresholding circuit 170, which for each of the faults has an input of the magnitude of the candidate faults over line 142 and distances to the candidate faults available over line 140.  The output of thresholder 170 is a series of faults with associated distances that magnitudes above the threshold.
 In this manner, not only is noise eliminated and not only are ghosts eliminated, attenuation per unit length of transmission line is taken into account. Moreover, those faults that are insignificant or due to secondary reflection are eliminated.
 Referring now to
FIG. 11 , what is provided for sixport operation is an equation in which there are several sixport network parameters, namely A, B and D, which determine the operation of the sixport junction. Here it will be noted that, in the factory, one can measure A, B and D and therefore measure g_{3}. It is these network parameters that do not change after factory characterization and which are plugged into module 162 ofFIG. 6 .  Referring to
FIG. 12 , the equation for the reflection coefficient is provided in which it can be seen that a certain portion of this equation incorporates attenuation, whereas another portion of this equation incorporates frequency or rotation. Frequency or rotation is equivalent to phase shift such that, as can be seen from the equation ofFIG. 12 , both attenuation and phase shift are accounted for.  Because attenuation and phase shift are accounted for in the modified IFT that is the subject matter of this invention, the accuracy of the measurement of the faults in a multifault environment is assured, since faults due to secondary reflections can be discriminated against.
 As mentioned hereinbefore, internal calibration makes possible the use of the multiport junction without an undue burden on the part of the technicians making the cable measurements. Note that calibration will first be discussed when diode detectors are used. Thereafter the changes necessary when using log amplifiers will be discussed. The calibration can be accomplished in one of two ways, one by switchable loads at the cable under test port and the other by switchable attenuators interposed between the RF source and the multiport junction. Both techniques yield the offset and gain used in the Γ estimation module 124 of
FIG. 4 .  As can be seen in
FIG. 13 , an RF source 200 is coupled to a multiport circuit or junction 202, which has the output powers thereof converted to voltages by power detectors 204 and 206. These voltages are measure by an analogtodigital converter 208, which are then read by a digital signal processor 210.  Digital signal processor 210, as will be seen, takes measurements across a frequency range of interest for each calibration load. It does so at switch 212 by switching between a cable under test 214 and a first calibration standard 216 and a second calibration standard 218.
 As will be described, these two calibration standards in one embodiment can be RLC circuits, such as shown in
FIGS. 17 and 18 .  While the use of two RLC circuits is one way to perform the internal calibration, as illustrated in
FIG. 14 , one can substitute a 50 ohm load onto the switch at the cableundertest port and put attenuators between the RF Source and the RF Input port as inFIG. 13 . The result is still the same in that one can obtain offsets in gains to calibrate the frequency domain reflectometer. Here an RF source 220 is attached to a switch 222 that switches in attenuators 224, 226, or 228, with the larger number of attenuators the better the calibration accuracy. Switch 230 completes the switching in of the various attenuators to the multiport circuit 232. Again, the outputs of the multiport circuit are provided to diode detectors 234 and 236, which are converted by an analogtodigital converter 238 and are processed by digital signal processor 240. The outputs of the calibration procedure are the offsets and gains used by the complex reflection coefficient profile (Γ(f)) estimation module ofFIGS. 4A and 4B .  Also provided is a switch 242 that switches between a cable under test 244 and a 50Ohm load 246.
 In operation and referring now to
FIG. 15 , a flow chart is illustrated for the calibration procedure made possible by the use of two or more RLC calibration loads.  Here it can be seen at 250 that one switches to a first calibration load and then at 252 collects measurements of the output powers over all frequencies. The result of the collection of the measurements for the first calibration load is stored as illustrated at 252, at which point, as illustrated at 254, one switches to collect measurements of a second calibration load at 256. These output power measurements are taken over all test frequencies, with the collected measurements being stored as illustrated at 258.
 As illustrated at 260, one then loads the multiport S parameters and RLC load S parameters from a file, with the parameters being illustrated and stored as illustrated at 262. One then, as illustrated at 264, formulates the model of the output signals measured from each port given the multiport S parameters and calibration load S parameters from the file. This model is a function of the gains and offsets that need to be estimated as illustrated at 266. As illustrated at 270, gains and offsets selected for the model at 266 that minimize the square error between this model and the measurements stored at 252 and 258 for each port respectively. The gains and offsets that minimize this square error are outputs of the calibration procedure as illustrated in 274.
 On the other hand, when one is using attenuators rather than switching in cal standards as is the case in
FIG. 13 , referring now toFIG. 16 , one first switches in attenuators as illustrated at 280, with two attenuators being sufficient, but more than two giving better accuracy. One then collects measurements of the outputs over all frequencies of the multiport junction as illustrated at 282, and stores the results as illustrated at 284. If all of the measurements are completed as illustrated at 286, one proceeds as illustrated at 288 to load attenuator and multiport S parameters from a file such as illustrated at 290. If all of the measurements are not collected, then one switches in more attenuators as illustrated by line 292.  Having loaded in the attenuator and multiport S parameters, as illustrated at 294, formulates the model of the output signals measured from each port as a function of the unknown gains and offsets. As illustrated in 296, gains and offsets are selected for the model that minimize the square error between this model and the measurements for each port stored at 284. The gains and offsets that minimize this square error are outputs of the calibration procedure as illustrated in 302.
 Referring now to
FIG. 17 , one implementation of the RLC circuit described hereinbefore is accomplished by attaching to an RF connector pin 310 a bond ribbon 312, which couples the connector pin to an inductor 314 having a 5Ohm resistor 316. The output of the inductor is coupled to a capacitor 320, which in one embodiment is a 100PF chip capacitor that has one plate connected to the inductor and the other plate grounded.  Referring to
FIG. 18 , as can be seen, test port 310 is connected via switch 322 to either a cable under test 324, a first RLC circuit 326 or second RLC circuit 328.  There are three factors that require the distance to fault, DTF, probe to be calibrated in order to obtain accurate fault detection and distance estimation. The DTF probe contains either dynamic log video amplifiers, DLVAs, or diode detectors or a combination of both, which have varying characteristics over temperature. The power measurements from the multiport circuit are read from an A/D converter, so measured digital values need to be mapped to the real power values. All RF sources have power fluctuation over frequency, which needs to be accounted for. Also any power losses between the RF Source and the circuit need to be compensated for. Calibration methods for network analyzers, which use similar circuit technology, require several calibration measurements with several connections to different calibration standards. These measurements are typically used to determine the S Parameters of the network analyzer circuit. It is desirable to minimize the number of calibration measurements and to put any sort of equipment or standards required by calibration inside the final probe design.
 While the present invention has been described in connection with the preferred embodiments of the various figures, it is to be understood that other similar embodiments may be used or modifications or additions may be made to the described embodiment for performing the same function of the present invention without deviating therefrom. Therefore, the present invention should not be limited to any single embodiment, but rather construed in breadth and scope in accordance with the recitation of the appended claims.
Claims (20)
1. A frequency domain reflectometer, comprising:
an RF signal source for providing an RF signal at a predetermined frequency;
a multiport junction having at least a transmission line under test port, a signal source port coupled to said RF signal source and a number of output power ports;
a module coupled to said output power ports for generating an estimated reflection coefficient as a function of the frequency of said signal source; and,
an Inverse Fourier Transform having an input coupled to said reflection coefficient for transforming the frequency domain input signal to a time domain signal, thus to permit ascertaining by the position of a time domain signal peak the distance to a fault in a transmission line under test.
2. The reflectometer of claim 1 , and further including a peak detector coupled to said time domain signal for ascertaining by the position of a detected peak the distance to a fault for a transmission line under test.
3. The reflectometer of claim 1 , wherein said multiport junction includes a sixport junction.
4. The reflectometer of claim 1 , wherein said Inverse Fourier Transform is modified to take into account the attenuation per unit length of said transmission line.
5. The reflectometer of claim 4 , wherein said modified Inverse Fourier Transform takes the form of
6. The reflectometer of claim 1 , and further including a module for removing from the output of said Inverse Fourier Transform the effects of faults prior to a predetermined fault.
7. The reflectometer of claim 6 , wherein said module or removing from the output of said Inverse Fourier Transform the effects of faults prior to a predetermined fault includes a module for identifying candidate faults without calculating the amplitude thereof.
8. The reflectometer of claim 7 , and further including a module coupled to said module for identifying candidate faults and to the output of said Inverse Fourier Transform for calculating fault magnitudes compensating for prior faults.
9. The reflectometer of claim 8 , wherein the module for calculating fault magnitudes takes the form of
10. The reflectometer of claim 8 , and further including a filter coupled to the output of said Inverse Fourier Transform and the calculated fault magnitude for filtering out faults below a predetermined magnitude, a signal indicating remaining faults, fault amplitude and distances to the remaining faults.
11. The reflectometer of claim 10 , and further including a display coupled to the output of said filter for displaying fault magnitude and distance to the fault.
12. The reflectometer of claim 1 , wherein said estimated reflection coefficient as a function of frequency is complex, thus to permit elimination of certain types of ghosts.
13. The reflectometer of claim 1 , wherein said RF source includes a variable frequency signal source.
14. The reflectometer of claim 1 , wherein said module for generating an estimated reflection coefficient includes a module utilizes an offset and gain from an onsite calibration procedure.
15. The reflectometer of claim 1 , wherein said module for generating an estimated reflection coefficient utilizes a prior measurement of the scattering parameters of said multiport junction.
16. In a frequency domain reflectometer in which a multiport junction is coupled to an RF signal source and in which selected output ports of said multiport junction are used to generate a complex reflection coefficient for each frequency, a system for obtaining the distance to a fault in a transmission line and the severity thereof, comprising:
an Inverse Fourier Transform coupled to said complex reflection coefficient for providing as an output one complex reflection coefficient for each distance;
a module for identifying candidate faults and the distances thereto by peak detection; and,
a module having as inputs said candidate faults and said complex reflection coefficient for each frequency for refining fault locations using a modified Inverse Fourier Transform in which the attenuation per unit length of transmission line is taken into consideration such that said fault refining module only operates on candidate faults whereby the output of said fault refining module indicates the magnitude and distance to said candidate faults.
17. The system of claim 16 , and further including a unit coupled to the output of said fault refining module for calculating fault magnitudes compensating for prior faults, thus to output the magnitude of the candidates having refined fault locations.
18. The system of claim 17 , and further including a thresholding circuit for filtering out those candidate faults having refined fault magnitudes below a predetermined threshold, thereby to output distances and magnitudes of faults having magnitudes above said predetermined threshold, whereby noise, ghosts and secondary reflections are removed.
19. The system of claim 16 , wherein said module that refines fault locations compensates for granularity by calculating modified Inverse Fourier Transforms for distances not only for a candidate fault distance but for distances to either side of said candidate fault distance.
20. The system of claim 18 , wherein said module that refines fault locations selects for an output for a candidate fault, the fault having a distance that give the largest modified Inverse Fourier Transform output.
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US53688604P true  20040115  20040115  
US53697704P true  20040115  20040115  
US11/034,592 US20050203711A1 (en)  20040115  20050113  Method and apparatus for transmission line and waveguide testing 
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US11/034,592 US20050203711A1 (en)  20040115  20050113  Method and apparatus for transmission line and waveguide testing 
US11/110,263 US7061251B2 (en)  20040115  20050420  Method and apparatus for transmission line and waveguide testing 
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US11/034,605 Abandoned US20050256651A1 (en)  20040115  20050113  Algorithm for estimation of multiple faults on a transmission line or waveguide 
US11/035,311 Expired  Fee Related US7061221B2 (en)  20040115  20050113  Reduced complexity transmission line and waveguide fault tester 
US11/034,676 Abandoned US20050228604A1 (en)  20040115  20050113  Method and apparatus for calibrating a frequency domain reflectometer 
US11/034,592 Abandoned US20050203711A1 (en)  20040115  20050113  Method and apparatus for transmission line and waveguide testing 
US11/110,394 Expired  Fee Related US7171322B2 (en)  20040115  20050420  Algorithm for estimation of multiple faults on a transmission line or waveguide 
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US20050256651A1 (en)  20051117 
US7061221B2 (en)  20060613 
US7171322B2 (en)  20070130 
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WO2005069943A2 (en)  20050804 
US20050234661A1 (en)  20051020 
WO2005069943A3 (en)  20060526 
WO2005069883A3 (en)  20060601 
US20050156585A1 (en)  20050721 
WO2005086630A3 (en)  20060601 
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US20050228604A1 (en)  20051013 
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