Third-order intercept point: Difference between revisions

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[[File:Megger Time-Domain Reflectometer MTDR1.jpg|thumb|Time-domain reflectometer for [[cable]] fault detection]]
[[File:Megger MTDR1 screenshot.jpg|thumb|Display of commercial time-domain reflectometer showing transmitted and reflected pulses]]
[[File:Partial transmittance.gif|thumb|Signal transmitted through and reflected from a discontinuity]]


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A '''time-domain reflectometer''' ('''TDR''') is an electronic instrument that uses [[time-domain reflectometry]] to characterize and locate faults in metallic cables (for example, [[twisted pair|twisted wire pairs]], [[coaxial cable]]s).<ref>{{FS1037C}}</ref> It can also be used to locate discontinuities in a connector, [[printed circuit board]], or any other electrical path. The equivalent device for [[optical fiber]] is an [[optical time-domain reflectometer]].
 
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A TDR transmits a short [[rise time]] [[pulse]] along the conductor. If the conductor is of a uniform [[Electrical impedance|impedance]] and is properly [[Electrical termination|terminated]], the entire transmitted pulse will be absorbed in the far-end termination and no signal will be reflected toward the TDR. Any impedance discontinuities will cause some of the incident signal to be sent back towards the source. This is similar in principle to [[radar]].


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Increases in the impedance create a reflection that reinforces the original pulse whilst decreases in the impedance create a reflection that opposes the original pulse.
 
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The resulting [[signal reflection|reflected pulse]] that is measured at the [[Input/output|output/input]] to the TDR is displayed or plotted as a function of time and, because the speed of signal propagation is almost constant for a given transmission medium, can be read as a function of [[cable]] length.


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Because of this sensitivity to impedance variations, a TDR may be used to verify cable impedance characteristics, [[Fusion splicing|splice]] and [[electrical connector|connector]] locations and associated losses, and estimate cable lengths.
 
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==Example traces==


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These traces were produced by a time-domain reflectometer made from common lab equipment connected to approximately 100 feet of 50 ohm coaxial cable. The propagation velocity of this cable is approximately 66% of the speed of light in a vacuum.
 
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== Michael Kors Tasker  hun var i koma. Ærligt ==
<gallery>
File:Simple Time Domain Reflectometer Diagram.png|Simple TDR made from lab equipment
File:Time Domain Reflectometer made from common lab equipment.JPG|Simple TDR made from lab equipment
File:TDR trace of cable with open termination.JPG|TDR trace of a transmission line with an open termination
File:TDR trace of cable with a short circuit termination.JPG|TDR trace of a transmission line with a short circuit termination
File:TDR trace of cable with a capacitor termination.jpg|TDR trace of a transmission line with a 1nF capacitor termination
File:TDR trace of cable terminationed with its characteristic impedance.jpg|TDR trace of a transmission line with an almost ideal termination
File:TDR trace of cable with cable terminated on an oscilloscope.JPG|TDR trace of a transmission line terminated on an oscilloscope high impedance input. The blue trace is the pulse as seen at the far end. It is offset so that the baseline of each channel is visible
</gallery>


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== Explanation ==
 
Consider the case where the far end of the cable is shorted (that is, it is terminated into zero ohms impedance). When the rising edge of the pulse is launched down the cable, the voltage at the launching point "steps up" to a given value instantly and the pulse begins propagating down the cable towards the short. When the pulse hits the short, no energy is absorbed at the far end. Instead, an opposing pulse reflects back from the short towards the launching end. It is only when this opposing reflection finally reaches the launch point that the voltage at this launching point abruptly drops back to zero, signalling the fact that there is a short at the end of the cable. That is, the TDR had no indication that there is a short at the end of the cable until its emitted pulse can travel down the cable at roughly the speed of light and the echo can return up the cable at the same speed. It is only after this round-trip delay that the short can be perceived by the TDR. Assuming that one knows the [[velocity of propagation|signal propagation speed]] in the particular cable-under-test, then in this way, the distance to the short can be measured.
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A similar effect occurs if the far end of the cable is an open circuit (terminated into an infinite impedance). In this case, though, the reflection from the far end is polarized identically with the original pulse and adds to it rather than cancelling it out. So after a round-trip delay, the voltage at the TDR abruptly jumps to twice the originally-applied voltage.


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Note that a theoretical perfect termination at the far end of the cable would entirely absorb the applied pulse without causing any reflection. In this case, it would be impossible to determine the actual length of the cable. Luckily, perfect terminations are very rare and some small reflection is nearly always caused.
 
 
  <li>[http://51zzjk.com/forum.php?mod=viewthread&tid=248473 http://51zzjk.com/forum.php?mod=viewthread&tid=248473]</li>
The magnitude of the reflection is referred to as the reflection coefficient or ρ. The coefficient ranges from 1 (open circuit) to -1 (short circuit). The value of zero means that there is no reflection. The reflection coefficient is calculated as follows:
 
 
  <li>[http://torncraft.tk/forum/viewtopic.php?f=4&t=306718 http://torncraft.tk/forum/viewtopic.php?f=4&t=306718]</li>
<center><math>\rho = \frac{Z_t - Z_o}{Z_t + Z_o}</math></center>
 
 
  <li>[http://ilubulu.com/forum.php?mod=viewthread&tid=7601&fromuid=4011 http://ilubulu.com/forum.php?mod=viewthread&tid=7601&fromuid=4011]</li>
Where Zo is defined as the characteristic impedance of the transmission medium and Zt is the impedance of the termination at the far end of the [[transmission line]].
 
 
  <li>[http://bbs.zg-gly.com/forum.php?mod=viewthread&tid=443392&fromuid=11558 http://bbs.zg-gly.com/forum.php?mod=viewthread&tid=443392&fromuid=11558]</li>
Any discontinuity can be viewed as a termination impedance and substituted as Zt. This includes abrupt changes in the characteristic impedance. As an example, a trace width on a printed circuit board doubled at its midsection would constitute a discontinuity. Some of the energy will be reflected back to the driving source; the remaining energy will be transmitted. This is also known as a scattering junction.
 
 
  <li>[http://frank1908.com/news/html/?31636.html http://frank1908.com/news/html/?31636.html]</li>
==Usage==
 
Time domain reflectometers are commonly used for in-place testing of very long cable runs, where it is impractical to dig up or remove what may be a kilometers-long cable. They are indispensable for [[preventive maintenance]] of [[telecommunication]] lines, as they can reveal growing resistance levels on joints and [[connectors]] as they [[corrosion|corrode]], and increasing [[Electrical insulation|insulation]] leakage as it degrades and absorbs moisture long before either leads to catastrophic failures. Using a TDR, it is possible to pinpoint a fault to within centimetres.
</ul>
 
TDRs are also very useful tools for [[technical surveillance counter-measures]], where they help determine the existence and location of [[telephone tapping|wire tap]]s. The slight change in line impedance caused by the introduction of a tap or splice will show up on the screen of a TDR when connected to a phone line.
 
TDR equipment is also an essential tool in the [[failure analysis]] of modern high-frequency printed circuit boards whose signal traces are carefully crafted to emulate [[transmission line]]s. By observing reflections, any unsoldered pins of a [[ball grid array]] device can be detected. Additionally, short circuited pins can also be detected in a similar fashion.
 
The TDR principle is used in industrial settings, in situations as diverse as the testing of [[integrated circuit]] packages to measuring liquid levels. In the former, the time domain reflectometer is used to isolate failing sites in the same. The latter is primarily limited to the process industry.
 
===TDR in level measurement===
In a TDR-based level measurement device, the device generates an impulse that propagates down a thin wave guide (also referred to as a probe) – typically a metal rod or a steel cable. When this impulse hits the surface of the medium to be measured, part of the impulse reflects back up the wave guide.  The device determines the fluid level by measuring the time difference between when the impulse was sent and when the reflection returned. The sensors can output the analyzed level as a continuous analog signal or switch output signals. In TDR technology, the impulse velocity is primarily affected by the permittivity of the medium through which the pulse propagates, which can vary greatly by the moisture content and temperature of the medium. In many cases, this effect can be corrected without undue difficulty. In some cases, such as in boiling and/or high temperature environments, the correction can be difficult. In particular, determining the froth (foam) height and the collapsed liquid level in a frothy / boiling medium can be very difficult.
 
===TDR used in anchor cables in dams ===
The Dam Safety Interest Group of CEA Technologies, Inc. (CEATI), a consortium of electrical power organizations, has applied [[Spread-spectrum time-domain reflectometry]] to identify potential faults in concrete dam anchor cables. The key benefit of Time Domain reflectometry over other testing methods is the non-destructive method of these tests.<ref>C. Furse, P. Smith, M. Diamond, “[http://www.ece.utah.edu/~cfurse/Center%20of%20Excellence/wiring_papers/anchors%20R1.pdf Feasibility of Reflectometry for Nondestructive Evaluation of Prestressed Concrete Anchors],” IEEE Journal of Sensors, Vol. 9. No. 11, Nov. 2009, pp. 1322 - 1329</ref>
 
===TDR used in the earth and agricultural sciences===
TDR is used to determine [[moisture content]] in soil and porous media, where over the last two decades substantial advances have been made; including in soils, grains and food stuffs, and in sediments. The key to TDR’s success is its ability to accurately determine the permittivity (dielectric constant) of a material from wave propagation, and the fact that there is a strong relationship between the permittivity of a material and its water content, as demonstrated in the pioneering works of Hoekstra and Delaney (1974) and Topp et al. (1980). Recent reviews and reference work on the subject include, Topp and Reynolds (1998), Noborio (2001), Pettinellia et al. (2002), Topp and Ferre (2002) and Robinson et al. (2003). The TDR method is a transmission line technique, and determines an apparent TDR permittivity (Ka) from the travel time of an electromagnetic wave that propagates along a transmission line, usually two or more parallel metal rods embedded in a soil or sediment. TDR probes are usually between 10 and 30&nbsp;cm in length and connected to the TDR via a coaxial cable.
 
===TDR in geotechnical usage===
Time domain reflectometry has also been utilized to monitor slope movement in a variety of geotechnical settings including highway cuts, rail beds, and open pit mines (Dowding & O'Connor, 1984, 2000a, 2000b; Kane & Beck, 1999). In stability monitoring applications using TDR, a coaxial cable is installed in a vertical borehole passing through the region of concern. The electrical impedance at any point along a coaxial cable changes with deformation of the insulator between the conductors. A brittle grout surrounds the cable to translate earth movement into an abrupt cable deformation that shows up as a detectable peak in the reflectance trace. Until recently, the technique was relatively insensitive to small slope movements and could not be automated because it relied on human detection of changes in the reflectance trace over time. Farrington and Sargand (2004) developed a simple signal processing technique using numerical derivatives to extract reliable indications of slope movement from the TDR data much earlier than by conventional interpretation.
 
Another application of TDRs in geotechnical engineering is to determine the soil moisture content. This can done by placing the TDRs in different soil layers and measurement of the time of start of precipitation and the time that TDR indicate an increase in the soil moisture content. The depth of the TDR (d) is a known factor and the other is the time it takes the drop of water to reach that depth (t); therefore the speed of water [[Infiltration (hydrology)]] (v) can be determined. This is a good method to assess the effectiveness of Best Management Practices (BMPs) in reducing [[stormwater]] [[Surface runoff]].
 
===TDR in semiconductor device analysis===
Time domain reflectometry is used in semiconductor failure analysis as a non-destructive method for the location of defects in semiconductor device packages. The TDR provides an electrical signature of individual conductive traces in the device package, and is useful for determining the location of opens and shorts.
 
===TDR in aviation wiring maintenance===
Time domain reflectometry, specifically [[spread-spectrum time-domain reflectometry]] is used for aviation wiring for both preventative maintenance and intermittent fault location.<ref>Smith, P., C. Furse, and J. Gunther, 2005. "Analysis of spread spectrum time domain [http://livewiretest.com/analysis-of-spread-spectrum-time-domain-reflectometry-for-wire-fault-location/ reflectometry for wire fault location]". IEEE Sensors Journal 5:1469–1478.</ref> The spread spectrum time domain reflectometry has the advantage of precisely locating the fault location within thousands of miles of aviation wiring. Additionally, this technology is worth considering for live aviation monitoring as the spread spectrum reflectometry works on a live wire.
 
This method has been shown to be useful to locating intermittent electrical faults.<ref>Furse, Cynthia, Smith, P.,Safavi, Mehdi, and M. Lo, Chet. "[http://livewiretest.com/feasibility-of-spread-spectrum-sensors-for-location-of-arcs-on-live-wires/ Feasibility of Spread Spectrum Sensors for Location of Arcs on Live Wires]". IEEE Sensors Journal. December 2005.</ref>
 
==See also==
* [[Frequency domain sensor]]
* [[Murray loop bridge]]
* [[Noise-Domain Reflectometry]]
* [[Return loss]]
* [[Standing wave ratio]]
 
== References ==
{{reflist|colwidth=30em}}
 
===Further reading===
*Hoekstra, P. and A. Delaney, 1974. "Dielectric properties of soils at UHF and microwave frequencies". ''Journal of Geophysical Research'' '''79''':1699–1708.
*Smith, P., C. Furse, and J. Gunther, 2005. "[http://ieeexplore.ieee.org/xpl/freeabs_all.jsp?arnumber=1532290 Analysis of spread spectrum time domain reflectometry for wire fault location]". ''IEEE Sensors Journal'' '''5''':1469–1478.
*Waddoups, B., C. Furse and M. Schmidt. "Analysis of Reflectometry for Detection of Chafed Aircraft Wiring Insulation". Department of Electrical and Computer Engineering. Utah State University.
*Noborio K. 2001. "Measurement of soil water content and electrical conductivity by time domain reflectometry: A review". ''Computers and Electronics in Agriculture'' '''31''':213–237.
*Pettinelli E., A. Cereti, A. Galli, and F. Bella, 2002. "Time domain reflectometry: Calibration techniques for accurate measurement of the dielectric properties of various materials". ''Review of Scientific Instruments'' '''73''':3553–3562.
*Robinson D.A., S.B. Jones, J.M. Wraith, D. Or and S.P. Friedman, 2003 "A review of advances in dielectric and electrical conductivity measurements in soils using time domain reflectometry". ''Vadose Zone Journal'' '''2''': 444–475.
* Robinson, D. A., C. S. Campbell, J. W. Hopmans, B. K. Hornbuckle, Scott B. Jones, R. Knight, F. Ogden, J. Selker, and O. Wendroth, 2008. "Soil moisture measurement for ecological and hydrological watershed-scale observatories: A review." ''Vadose Zone Journal'' 7: 358-389.
*Topp G.C., J.L. Davis and A.P. Annan, 1980. "Electromagnetic determination of soil water content: measurements in coaxial transmission lines". ''Water Resources Research'' '''16''':574–582.
*Topp G.C. and W.D. Reynolds, 1998. "Time domain reflectometry: a seminal technique for measuring mass and energy in soil". ''Soil Tillage Research'' '''47''':125–132.
*Topp, G.C. and T.P.A. Ferre, 2002. "Water content", in ''Methods of Soil Analysis. Part 4''. (Ed. J.H. Dane and G.C. Topp), SSSA Book Series No. 5. Soil Science Society of America, Madison WI.
*Dowding, C.H. & O'Connor, K.M. 2000a. "Comparison of TDR and Inclinometers for Slope Monitoring". ''Geotechnical Measurements—Proceedings of Geo-Denver2000'': 80–81. Denver, CO.
*Dowding, C.H. & O'Connor, K.M. 2000b. "Real Time Monitoring of Infrastructure using TDR Technology". ''Structural Materials Technology NDT Conference 2000''
*Kane, W.F. & Beck, T.J. 1999. "Advances in Slope Instrumentation: TDR and Remote Data Acquisition Systems". ''Field Measurements in Geomechanics, 5th International Symposium on Field Measurements in Geomechanics'': 101–105. Singapore.
*Farrington, S.P. and Sargand, S.M., "Advanced Processing of Time Domain Reflectometry for Improved Slope Stability Monitoring", ''Proceedings of the Eleventh Annual Conference on Tailings and Mine Waste'', October, 2004.
*{{cite conference| last=Smolyansky| first=D.| title=Electronic Package Fault Isolation Using TDR | booktitle=Microelectronics Failure Analysis | pages= 289–302 | year=2004 |publisher=ASM International | isbn= 0-87170-804-3 }}
 
== External links ==
*[http://www.radiodetection.com/Document_links.asp?sec_id=2722 Radiodetection Extended Training] - ABC's of TDR's
*[http://news.bbc.co.uk/2/hi/technology/7228315.stm Work begins to repair severed net]
*[http://cp.literature.agilent.com/litweb/pdf/5966-4855E.pdf AN-1304-2: Time Domain Reflectometry Theory] (from Agilent Technologies)
*[http://www.aeatechnology.com/software/application-notes/an201 AN201 Step verses Pulse TDR Technology] (from AEA Technology, Inc.)
 
{{DEFAULTSORT:Time-Domain Reflectometer}}
[[Category:Electronic test equipment]]
[[Category:Soil physics]]
[[Category:Semiconductor analysis]]

Revision as of 17:51, 10 December 2013

Time-domain reflectometer for cable fault detection
Display of commercial time-domain reflectometer showing transmitted and reflected pulses
Signal transmitted through and reflected from a discontinuity

A time-domain reflectometer (TDR) is an electronic instrument that uses time-domain reflectometry to characterize and locate faults in metallic cables (for example, twisted wire pairs, coaxial cables).[1] It can also be used to locate discontinuities in a connector, printed circuit board, or any other electrical path. The equivalent device for optical fiber is an optical time-domain reflectometer.

Description

A TDR transmits a short rise time pulse along the conductor. If the conductor is of a uniform impedance and is properly terminated, the entire transmitted pulse will be absorbed in the far-end termination and no signal will be reflected toward the TDR. Any impedance discontinuities will cause some of the incident signal to be sent back towards the source. This is similar in principle to radar.

Increases in the impedance create a reflection that reinforces the original pulse whilst decreases in the impedance create a reflection that opposes the original pulse.

The resulting reflected pulse that is measured at the output/input to the TDR is displayed or plotted as a function of time and, because the speed of signal propagation is almost constant for a given transmission medium, can be read as a function of cable length.

Because of this sensitivity to impedance variations, a TDR may be used to verify cable impedance characteristics, splice and connector locations and associated losses, and estimate cable lengths.

Example traces

These traces were produced by a time-domain reflectometer made from common lab equipment connected to approximately 100 feet of 50 ohm coaxial cable. The propagation velocity of this cable is approximately 66% of the speed of light in a vacuum.

Explanation

Consider the case where the far end of the cable is shorted (that is, it is terminated into zero ohms impedance). When the rising edge of the pulse is launched down the cable, the voltage at the launching point "steps up" to a given value instantly and the pulse begins propagating down the cable towards the short. When the pulse hits the short, no energy is absorbed at the far end. Instead, an opposing pulse reflects back from the short towards the launching end. It is only when this opposing reflection finally reaches the launch point that the voltage at this launching point abruptly drops back to zero, signalling the fact that there is a short at the end of the cable. That is, the TDR had no indication that there is a short at the end of the cable until its emitted pulse can travel down the cable at roughly the speed of light and the echo can return up the cable at the same speed. It is only after this round-trip delay that the short can be perceived by the TDR. Assuming that one knows the signal propagation speed in the particular cable-under-test, then in this way, the distance to the short can be measured.

A similar effect occurs if the far end of the cable is an open circuit (terminated into an infinite impedance). In this case, though, the reflection from the far end is polarized identically with the original pulse and adds to it rather than cancelling it out. So after a round-trip delay, the voltage at the TDR abruptly jumps to twice the originally-applied voltage.

Note that a theoretical perfect termination at the far end of the cable would entirely absorb the applied pulse without causing any reflection. In this case, it would be impossible to determine the actual length of the cable. Luckily, perfect terminations are very rare and some small reflection is nearly always caused.

The magnitude of the reflection is referred to as the reflection coefficient or ρ. The coefficient ranges from 1 (open circuit) to -1 (short circuit). The value of zero means that there is no reflection. The reflection coefficient is calculated as follows:

Where Zo is defined as the characteristic impedance of the transmission medium and Zt is the impedance of the termination at the far end of the transmission line.

Any discontinuity can be viewed as a termination impedance and substituted as Zt. This includes abrupt changes in the characteristic impedance. As an example, a trace width on a printed circuit board doubled at its midsection would constitute a discontinuity. Some of the energy will be reflected back to the driving source; the remaining energy will be transmitted. This is also known as a scattering junction.

Usage

Time domain reflectometers are commonly used for in-place testing of very long cable runs, where it is impractical to dig up or remove what may be a kilometers-long cable. They are indispensable for preventive maintenance of telecommunication lines, as they can reveal growing resistance levels on joints and connectors as they corrode, and increasing insulation leakage as it degrades and absorbs moisture long before either leads to catastrophic failures. Using a TDR, it is possible to pinpoint a fault to within centimetres.

TDRs are also very useful tools for technical surveillance counter-measures, where they help determine the existence and location of wire taps. The slight change in line impedance caused by the introduction of a tap or splice will show up on the screen of a TDR when connected to a phone line.

TDR equipment is also an essential tool in the failure analysis of modern high-frequency printed circuit boards whose signal traces are carefully crafted to emulate transmission lines. By observing reflections, any unsoldered pins of a ball grid array device can be detected. Additionally, short circuited pins can also be detected in a similar fashion.

The TDR principle is used in industrial settings, in situations as diverse as the testing of integrated circuit packages to measuring liquid levels. In the former, the time domain reflectometer is used to isolate failing sites in the same. The latter is primarily limited to the process industry.

TDR in level measurement

In a TDR-based level measurement device, the device generates an impulse that propagates down a thin wave guide (also referred to as a probe) – typically a metal rod or a steel cable. When this impulse hits the surface of the medium to be measured, part of the impulse reflects back up the wave guide. The device determines the fluid level by measuring the time difference between when the impulse was sent and when the reflection returned. The sensors can output the analyzed level as a continuous analog signal or switch output signals. In TDR technology, the impulse velocity is primarily affected by the permittivity of the medium through which the pulse propagates, which can vary greatly by the moisture content and temperature of the medium. In many cases, this effect can be corrected without undue difficulty. In some cases, such as in boiling and/or high temperature environments, the correction can be difficult. In particular, determining the froth (foam) height and the collapsed liquid level in a frothy / boiling medium can be very difficult.

TDR used in anchor cables in dams

The Dam Safety Interest Group of CEA Technologies, Inc. (CEATI), a consortium of electrical power organizations, has applied Spread-spectrum time-domain reflectometry to identify potential faults in concrete dam anchor cables. The key benefit of Time Domain reflectometry over other testing methods is the non-destructive method of these tests.[2]

TDR used in the earth and agricultural sciences

TDR is used to determine moisture content in soil and porous media, where over the last two decades substantial advances have been made; including in soils, grains and food stuffs, and in sediments. The key to TDR’s success is its ability to accurately determine the permittivity (dielectric constant) of a material from wave propagation, and the fact that there is a strong relationship between the permittivity of a material and its water content, as demonstrated in the pioneering works of Hoekstra and Delaney (1974) and Topp et al. (1980). Recent reviews and reference work on the subject include, Topp and Reynolds (1998), Noborio (2001), Pettinellia et al. (2002), Topp and Ferre (2002) and Robinson et al. (2003). The TDR method is a transmission line technique, and determines an apparent TDR permittivity (Ka) from the travel time of an electromagnetic wave that propagates along a transmission line, usually two or more parallel metal rods embedded in a soil or sediment. TDR probes are usually between 10 and 30 cm in length and connected to the TDR via a coaxial cable.

TDR in geotechnical usage

Time domain reflectometry has also been utilized to monitor slope movement in a variety of geotechnical settings including highway cuts, rail beds, and open pit mines (Dowding & O'Connor, 1984, 2000a, 2000b; Kane & Beck, 1999). In stability monitoring applications using TDR, a coaxial cable is installed in a vertical borehole passing through the region of concern. The electrical impedance at any point along a coaxial cable changes with deformation of the insulator between the conductors. A brittle grout surrounds the cable to translate earth movement into an abrupt cable deformation that shows up as a detectable peak in the reflectance trace. Until recently, the technique was relatively insensitive to small slope movements and could not be automated because it relied on human detection of changes in the reflectance trace over time. Farrington and Sargand (2004) developed a simple signal processing technique using numerical derivatives to extract reliable indications of slope movement from the TDR data much earlier than by conventional interpretation.

Another application of TDRs in geotechnical engineering is to determine the soil moisture content. This can done by placing the TDRs in different soil layers and measurement of the time of start of precipitation and the time that TDR indicate an increase in the soil moisture content. The depth of the TDR (d) is a known factor and the other is the time it takes the drop of water to reach that depth (t); therefore the speed of water Infiltration (hydrology) (v) can be determined. This is a good method to assess the effectiveness of Best Management Practices (BMPs) in reducing stormwater Surface runoff.

TDR in semiconductor device analysis

Time domain reflectometry is used in semiconductor failure analysis as a non-destructive method for the location of defects in semiconductor device packages. The TDR provides an electrical signature of individual conductive traces in the device package, and is useful for determining the location of opens and shorts.

TDR in aviation wiring maintenance

Time domain reflectometry, specifically spread-spectrum time-domain reflectometry is used for aviation wiring for both preventative maintenance and intermittent fault location.[3] The spread spectrum time domain reflectometry has the advantage of precisely locating the fault location within thousands of miles of aviation wiring. Additionally, this technology is worth considering for live aviation monitoring as the spread spectrum reflectometry works on a live wire.

This method has been shown to be useful to locating intermittent electrical faults.[4]

See also

References

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Further reading

  • Hoekstra, P. and A. Delaney, 1974. "Dielectric properties of soils at UHF and microwave frequencies". Journal of Geophysical Research 79:1699–1708.
  • Smith, P., C. Furse, and J. Gunther, 2005. "Analysis of spread spectrum time domain reflectometry for wire fault location". IEEE Sensors Journal 5:1469–1478.
  • Waddoups, B., C. Furse and M. Schmidt. "Analysis of Reflectometry for Detection of Chafed Aircraft Wiring Insulation". Department of Electrical and Computer Engineering. Utah State University.
  • Noborio K. 2001. "Measurement of soil water content and electrical conductivity by time domain reflectometry: A review". Computers and Electronics in Agriculture 31:213–237.
  • Pettinelli E., A. Cereti, A. Galli, and F. Bella, 2002. "Time domain reflectometry: Calibration techniques for accurate measurement of the dielectric properties of various materials". Review of Scientific Instruments 73:3553–3562.
  • Robinson D.A., S.B. Jones, J.M. Wraith, D. Or and S.P. Friedman, 2003 "A review of advances in dielectric and electrical conductivity measurements in soils using time domain reflectometry". Vadose Zone Journal 2: 444–475.
  • Robinson, D. A., C. S. Campbell, J. W. Hopmans, B. K. Hornbuckle, Scott B. Jones, R. Knight, F. Ogden, J. Selker, and O. Wendroth, 2008. "Soil moisture measurement for ecological and hydrological watershed-scale observatories: A review." Vadose Zone Journal 7: 358-389.
  • Topp G.C., J.L. Davis and A.P. Annan, 1980. "Electromagnetic determination of soil water content: measurements in coaxial transmission lines". Water Resources Research 16:574–582.
  • Topp G.C. and W.D. Reynolds, 1998. "Time domain reflectometry: a seminal technique for measuring mass and energy in soil". Soil Tillage Research 47:125–132.
  • Topp, G.C. and T.P.A. Ferre, 2002. "Water content", in Methods of Soil Analysis. Part 4. (Ed. J.H. Dane and G.C. Topp), SSSA Book Series No. 5. Soil Science Society of America, Madison WI.
  • Dowding, C.H. & O'Connor, K.M. 2000a. "Comparison of TDR and Inclinometers for Slope Monitoring". Geotechnical Measurements—Proceedings of Geo-Denver2000: 80–81. Denver, CO.
  • Dowding, C.H. & O'Connor, K.M. 2000b. "Real Time Monitoring of Infrastructure using TDR Technology". Structural Materials Technology NDT Conference 2000
  • Kane, W.F. & Beck, T.J. 1999. "Advances in Slope Instrumentation: TDR and Remote Data Acquisition Systems". Field Measurements in Geomechanics, 5th International Symposium on Field Measurements in Geomechanics: 101–105. Singapore.
  • Farrington, S.P. and Sargand, S.M., "Advanced Processing of Time Domain Reflectometry for Improved Slope Stability Monitoring", Proceedings of the Eleventh Annual Conference on Tailings and Mine Waste, October, 2004.
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External links

  1. Template:FS1037C
  2. C. Furse, P. Smith, M. Diamond, “Feasibility of Reflectometry for Nondestructive Evaluation of Prestressed Concrete Anchors,” IEEE Journal of Sensors, Vol. 9. No. 11, Nov. 2009, pp. 1322 - 1329
  3. Smith, P., C. Furse, and J. Gunther, 2005. "Analysis of spread spectrum time domain reflectometry for wire fault location". IEEE Sensors Journal 5:1469–1478.
  4. Furse, Cynthia, Smith, P.,Safavi, Mehdi, and M. Lo, Chet. "Feasibility of Spread Spectrum Sensors for Location of Arcs on Live Wires". IEEE Sensors Journal. December 2005.