| TDR
Tutorial - Introduction to Time Domain Reflectometry
An Introduction
to Time Domain Reflectometers
Time Domain Reflectometers
have been around for many years and remain the fastest, most
accurate way to pinpoint cabling problems.
Historically,
the TDR has been reserved for only large companies and high
level engineers. This was due to the complexity of operation
and high cost of the instruments. The TDR has been greatly
under utilized.
Riser-Bond Instruments
recognized these shortcomings and developed the first "little
TDR" in the early 1980s. The simplified digital TDR has now
become a standard tool for the first level technician. Riser-Bond
Instruments' complete product line has been permeated by the
concept that test equipment should be simple, accurate, user-friendly,
rugged, and high value for the cost.
Due to advances
in today's technology, the operation and interpretation of
a TDR have been greatly simplified. Because of its ability
to identify cable problems, the TDR is now rapidly regaining
popularity throughout communications industries.
If a cable is
metal and it has at least two conductors, it can be tested
by a TDR. TDRs will troubleshoot and measure all types of
twisted pair and coaxial cables, both aerial and underground.
TDRs are used
to locate and identify faults in all types of metallic paired
cable. TDRs can locate major or minor cabling problems including;
sheath faults, broken conductors, water damage, loose connectors,
crimps, cuts, smashed cables, shorted conductors, system components,
and a variety of other fault conditions. In addition, TDRs
can be used to test reels of cable for shipping damage, cable
shortages, cable usage, and inventory management.
The speed and
accuracy of the time domain reflectometer makes it today's
preferred method of cable fault location. Although today's
instruments are more user friendly, a good understanding of
the basic principles and applications of a TDR is essential
to successful troubleshooting. Like all new equipment, getting
to know the instrument and its operation makes the TDR a more
valuable tool.
Principles
of Operation
The TDR works
on the same principle as radar. A pulse of energy is transmitted
down a cable. When that pulse reaches the end of the cable,
or a fault along the cable, part or all of the pulse energy
is reflected back to the instrument.
The TDR measures
the time it takes for the signal to travel down the cable,
see the problem, and reflect back. The TDR then converts this
time to distance and displays the information as a waveform
and/or distance reading.
TYPES OF TDRs
There are two
ways a TDR can display the information it receives. The first
and more traditional method is to display the actual waveform
or "signature" of the cable. The display, which is either
a CRT or an LCD, will display the outgoing (transmitted) pulse
generated by the TDR and any reflections which are caused
by impedance discontinuities along the length of the cable.
The second type
of display is simply a numeric readout which supplies the
distance indication in feet or meters to the first major reflection
caused by an impedance change or discontinuity. Some instruments
also display if the fault is an OPEN or SHORT indicating a
HIGH IMPEDANCE change or a LOW IMPEDANCE change respectively.
Traditional Waveform
TDRs supply more information than do the digital numeric versions.
However, the simplified digital models are less expensive
and easier to operate. Costing only a fraction of a traditional
TDR, many simplified digital TDRs are just as accurate and
can locate most major cable faults.
IMPEDANCE
Any time two metallic
conductors are placed close together, they form a cable impedance.
A TDR looks for a change in impedance which can be caused
by a variety of circumstances, including cable damage, water
ingress, change in cable type, improper installation, and
even manufacturing flaws.
The insulating
material that keeps the conductors separated is called the
cable dielectric. The impedance of the cable is determined
by the spacing of the conductors from each other and the type
of dielectric used.
If the conductors
are manufactured with exact spacing and the dielectric is
exactly constant, then the cable will be constant. If the
conductors are randomly spaced or the dielectric changes along
the cable, then the impedance will also vary along the cable.
A TDR sends electrical
pulses down the cable and samples the reflected energy. Any
impedance change will cause some energy to reflect back toward
the TDR and will be displayed. How much the impedance changes
determines the amplitude of the reflection.
PULSE WIDTHS
Many TDRs have
selectable pulse width settings. The larger the pulse width,
the more energy is transmitted and therefore the further the
signal will travel down the cable. Pulse widths may include
2 nsec, 10 nsec, 100 nsec, 1000 nsec, 2000 nsec, and 4000
nsec. A TDR may contain only one or all of the pulse width
settings.
NOTE: Even when
testing very long lengths of cable, always start the fault
finding procedure in the shortest pulse width available, as
the fault may be only a short distance away. If the fault
is not located, switch to the next larger pulse width and
retest. Keep switching to the next larger pulse until the
fault is located.
Sometimes larger
pulse widths are helpful even for locating faults that are
relatively dose. If the fault is very small, the signal strength
of a small pulse may not be enough to travel down the cable,
" see" the fault, and travel back. The attenuation of the
cable combined with the small reflection of the partial fault
can make it difficult to detect. A larger pulse width would
transmit more energy down the cable, making it easier to see
the small fault.
BLIND SPOTS
The pulse generated
by the TDR takes a certain amount of time and thus distance
to launch. This distance is known as the blind spot. The length
of the blind spot varies with the pulse width. The larger
the pulse width, the larger the blind spot.
It is more difficult
to locate a fault contained within the blind spot. If a fault
is suspected within the first few feet of cable, it is advisable
to add a length of cable between the TDR and the cable being
tested. Any faults that may have been hidden in the blind
spot can now easily be located. When adding a length of cable
to eliminate the blind spot, remember the TDR is also reading
the length of this jumper cable. The length of the jumper
must be subtracted from the cable when measuring from the
point of connection.
It is best if
the jumper cable is the same impedance as the cable under
test. The quality of the connection is an important factor
regardless of the type of connection or jumper being used.
VELOCITY OF
PROPAGATION (VOP)
The TDR is an
extremely accurate instrument. However, variables in the cable
itself sometimes cause errors in distance measurements. One
way to minimize error is to use the correct Velocity of Propagation
(VOP) of the cable under test. The VOP is a specification
of the cable indicating the speed at which a signal travels
down the cable. Different cables have different VOPs. In order
to assure the most accurate distance measurements, the cable
VOP must be determined.
VOP Defined: The
speed of light in a vacuum is 186,400 miles per second. This
speed is represented by the number 1 (100%). All other signals
are slower. A cable with a VOP of .85 would transmit a signal
at 85% of the speed of light. A twisted pair cable, which
typically has a lower VOP (such as .65), can transmit a signal
at 65% of the speed of light.
The VOP number
of a cable is determined by the dielectric material that separates
the two conductors . In a coaxial cable, the foam separating
the center conductor and the outer sheath is the material
determining the VOP. In twisted pair, the VOP number is determined
by the spacing between the plastic.
Knowing the VOP
of a cable is the most important factor when using a TDR for
fault finding. By entering the correct VOP, the instrument
is calibrated to the particular cable. Typically, the VOP
of the cable under test will be listed in the cable manufacturer's
catalog or specification sheet. If not, simply measure a length
of good cable (no faults) and change the TDR's VOP setting
until the display shows the same distance reading as the measured
length. The VOP of a cable can change with temperature and
age. It can also vary from one manufacturing run to another.
Even new cable can vary as much as +/- 3%.
One might think
the variations in VOP would make it almost impossible to locate
a fault accurately. Fortunately, there are ways to minimize
the error in the VOP when testing a faulted cable, resulting
in very accurate distance measurements. These techniques do
not work when testing or measuring good (no fault) cable.
The most common
technique used to reduce VOP error is to test the faulty cable
from both ends. The procedure is as follows:
Determine the
path of the cable. With a Measuring wheel or tape, measure
the exact length of the cable being tested. Set the VOP according
to the manufacturers specifications, test the cable from one
end, and record the distance reading. Next, using the same
VOP setting, test from the opposite end of the cable and record.
If the sum of the readings is the exact length of the cable
that was measured, the VOP is correct and the fault has been
located.
If the sum of
the two readings is more than the measured distance, reduce
the VOP setting and re-test. If the sum of the two readings
is less than the measured distance, increase the VOP setting.
In this case, the operator must also consider the possibility
of two faults.
The same result
can be obtained mathematically. Take the actual cable length
and divide by the sum of the two TDR readings obtained by
the tests from each end . This gives the adjustment factor.
Then multiply each of the TDR readings by the adjustment factor.
This result will be the corrected length readings.
A partial listing
of cable types and their Velocity of Propagation.
| CABLE TYPE |
TYPE |
VOP |
|
| |
| TELEPHONE |
| 19 AWG |
Gel-Filled |
68 |
| 22 AWG |
Gel-Filled |
66 |
| 24 AWG |
Gel-Filled |
62 |
| 26 AWG |
Gel-Filled |
60 |
| |
| 19 AWG |
AIR |
72 |
| 22 AWG |
AIR |
67 |
| 24 AWG |
AIR |
66 |
| 26 AWG |
AIR |
64 |
| |
|
Polyethylene |
66 |
|
Polypropylene |
66 |
|
Teflon |
69 |
|
PIC |
67 |
|
Pulp |
72 |
|
| CATV |
|
| Belden |
Foam |
78S-82 |
| |
Solid |
66 |
| |
| Comm/Scope
|
(F) |
82 |
| PARA I |
|
82 |
| PARA III
|
|
87 |
| QR |
|
88 |
| |
| Times
Fiber |
RG-59 |
93 |
| T4,6,10,TR+
|
|
87 |
| TX, TX10
|
|
89 |
| Dynafoam
|
|
90 |
| Trilogy
|
(F) |
83 |
| 7 SERIES
|
|
88 |
| |
| CapScan
|
FOAM |
S2 |
| CC SS |
|
88 |
| |
| CZ
Labs |
FOAM |
82 |
| |
| General
Cable |
RG-59 |
82 |
| MC2 |
|
93 |
| |
| Scientific
Atlanta |
RG-59 |
81 |
| Trunk |
|
87 |
| |
| LAN |
|
| UTP 26 |
|
64 |
| Thinnet
|
|
66-70 |
| Ethernet
|
|
77 |
| Token Ring
|
|
78 |
| Arcnet |
|
84 |
| Twinaxial
|
AIR |
80 |
| Twinaxial
|
|
71 |
| Appletalk
|
|
68 |
| |
| IBM |
|
| Type 1 |
|
64 |
| Type 2 |
|
66 |
| Type 3 |
|
70 |
| Type 4 |
|
72 |
| Type 5 |
|
76 |
| Type 6 |
|
78 |
| Type 7 |
|
82 |
| Type 8 |
|
84 |
| Type 9 |
|
82 |
| |
| LAND/MOBILE |
|
| ANDREW |
|
| RADIAX |
All |
79 |
| |
| HELIAX |
|
| FHJI-50
|
1/4" |
79 |
| FSJI-50
|
1/4" |
78 |
| FSJ4-50B
|
1/2" |
81 |
| LDF2-50
|
3/8" |
88 |
| LDF4-50A
|
1/2" |
80 |
| LDF4-75
|
1/2" |
88 |
| LDF5-50A
|
7/8" |
89 |
| LDF7-50
|
1 5/8" |
88 |
| FT4-50 |
1/2" |
85 |
| FT5-50 |
7/8" |
89 |
| HJ4-50 |
1/2" |
91 |
| HJ5-50 |
7/8" |
92 |
| HJ5-75 |
7/8" |
90 |
| HJ7-50A
|
1 5/8" |
92 |
| HJS-50B
|
3" |
93 |
| HJ11-50
|
4" |
92 |
| HJ9-50 |
5" |
93 |
| |
| CABLEWAVE |
|
| FLC12-50J
|
1/2" |
88 |
| FLC78-50J
|
7/8" |
88 |
| |
| CABLEFLEX
FOAMFCC + FLC |
|
| FCC 38-50J
|
3/8" |
81 |
| FLC 12-50J
|
1/2" |
88 |
| FLC 78-50J
|
7/8" |
88 |
| FLC 158-50J
|
1 5/8" |
88 |
| |
| CABLEWAVE |
ALL |
88 |
| |
| COAX
TRANSMISSION LINE |
|
| 920213 |
7/8" |
99 |
| 920214 |
1 5/8" |
99 |
| |
| FLEXWELL
HCC |
|
| HCC12-50J
|
1/2" |
91 |
| HCC7S-50J
|
7/8" |
91 |
| HCC15S-50J
|
1 5/8" |
95 |
| HCC300-50J
|
3" |
96 |
| HCC312-50J
|
3 1/2" |
96 |
| HF41/2CU24
|
4 1/2" |
97 |
|