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279 lines
16 KiB
Text
279 lines
16 KiB
Text
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==Phrack Inc.==
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Volume Three, Issue 29, File #8 of 12
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...........................................
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||||||!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!||||||
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|||!!! !!!|||
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||| The Myth and Reality About |||
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||| Eavesdropping |||
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||| by Phone Phanatic |||
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|||... October 8, 1989 ...|||
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||||||...............................||||||
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!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
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Most Central Office (CO) eavesdropping intercepts in a Bell Operating Company
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(BOC) CO are today performed using a modified Metallic Facility Termination
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(MFT) circuit pack which places about a 100,000 ohm isolated bridging impedance
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across the subscriber line. Supervisory signaling is detected on the
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subscriber loop using a high-impedance electronic circuit, and the signaling is
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repeated in an isolated fashion using the A and B leads of the repeating coil
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in the MFT to "reconstruct" a CO line for the benefit of monitoring apparatus.
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The entire purpose of the above effort is to prevent any trouble or noise on
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the intercept line or monitoring apparatus from causing any trouble, noise or
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transmission impairment on the subject line.
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Some BOCs may elect to use service observing apparatus to provide the necessary
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isolation and repeated loop supervisory signaling. Less common are locally
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engineered variations which merely use an isolation amplifier from an MFT or
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other 4-wire repeater, and which provide no repeated supervisory signaling
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(which is not all that necessary, since voice-activated recorders and DTMF
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signaling detectors can be used, and since dial pulses can be counted by
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playing a tape at slow speed).
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Today, the use of a "bridge lifter" retardation coil for the purpose of
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connecting an eavesdropping intercept line is virtually non-existent since they
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do not provide sufficient isolation and since they provide a fair amount of
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insertion loss without loop current on the "observing" side. Bridge lifter
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coils are primarily intended for answering service intercept lines, and consist
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of a dual-winding inductor which passes 20 Hz ringing and whose windings easily
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saturate when DC current flows. Bridge lifter coils are used to minimize the
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loading effect (and consequent transmission impairment) of two subscriber loops
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on one CO line. Bridge lifter coils provide a significant insertion loss at
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voice frequencies toward the idle loop; i.e., the loop in use will have DC
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current flow, saturating the inductor, and reducing its insertion loss to
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1.0 dB or less.
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Despite gadget advertised in magazines like The Sharper Image, the simple truth
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of the matter is that there is NO WAY for any person using ANY type of
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apparatus at the telephone set location to ascertain whether there is a
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properly installed eavesdropping device connected across their line in the CO.
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The only way such a determination can be made is through the cooperation of the
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telephone company.
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For that matter, there is virtually no way for any person using any type of
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apparatus in their premises to ascertain if there is ANY type of eavesdropping
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apparatus installed ANYWHERE on their telephone line outside their premises,
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unless the eavesdropping apparatus was designed or installed in an
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exceptionally crude manner (not likely today). Some types of eavesdropping
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apparatus may be located, but only with the full cooperation of the telephone
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company.
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The sole capability of these nonsense gadgets is to ascertain if an extension
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telephone is picked up during a telephone call, which is hardly a likely
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scenario for serious eavesdropping!
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These screw-in-the-handset gadgets work by sensing the voltage across the
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carbon transmitter circuit, and using a control to null this voltage using a
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comparator circuit. When a person makes a telephone call, the control is
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adjusted until the light just goes out. If an extension telephone at the
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user's end is picked up during the call, the increased current drain of a
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second telephone set will decrease the voltage across the carbon transmitter
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circuit, unbalancing the voltage comparator circuit, and thereby causing the
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LED to light.
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These voltage comparator "tap detectors" cannot even be left with their
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setpoint control in the same position, because the effective voltage across a
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subscriber loop will vary depending upon the nature of the call (except in the
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case of an all digital CO), and upon other conditions in the CO.
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Electromechanical and analog ESS CO's may present different characteristics to
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the telephone line, depending upon whether it is used at the time of: An
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originated intraoffice call (calling side of intraoffice trunk), an answered
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intraoffice call (called side of intraoffice trunk), an originated tandem call
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(interoffice tandem trunk), an originated toll call (toll trunk), or an
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answered tandem/toll call (incoming tandem or toll trunk). There is usually
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enough variation in battery feed resistance due to design and component
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tolerance changes on these different trunks to cause a variation of up to
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several volts measured at the subscriber end for a given loop and given
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telephone instrument.
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Even more significant are variations in CO battery voltage, which can vary
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(within "normal limits") from 48 volts to slightly over 52 volts, depending
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upon CO load conditions. 50 to 51 volts in most CO's is a typical daily
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variation. If anyone is curious, connect an isolated voltage recorder or data
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logger to a CO loop and watch the on-hook voltage variations; in many CO's the
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resultant voltage vs 24-hour time curve will look just like the inverse of a
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busy-hour graph from a telephone traffic engineering text!
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In some all-digital CO apparatus, the subscriber loop signaling is performed by
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a solid-state circuit which functions as a constant-current (or
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current-limiting) device. With such a solid-state circuit controlling loop
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current, there is no longer ANY meaningful reference to CO battery voltage;
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i.e., one cannot even use short-circuit loop current at the subscriber location
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to even estimate outside cable plant resistance.
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To explode this myth even further, let's do a little Ohm's Law:
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1. Assume a CO loop with battery fed from a dual-winding A-relay (or
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line relay, ESS ferrod line scanner element, or whatever) having 200
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ohms to CO battery and 200 ohms to ground.
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2. Assume a CO loop of 500 ohms (a pretty typical loop).
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3. Assume an eavesdropping device with a DC resistance of 100,000 ohms
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(this is still pretty crude, but I'm being generous with my example).
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4. Using some simple Ohm's law, the presence or absence of this
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hypothetical eavesdropping device at the SUBSCRIBER PREMISES will
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result in a voltage change of less than 0.5 volt when measured in the
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on-hook state. This voltage change is much less than normal
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variations of CO battery voltage.
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5. Using some simple Ohm's law, the presence or absence of this
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hypothetical eavesdropping device at the CENTRAL OFFICE LOCATION will
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result in a voltage change of less than 0.2 volt when measured in the
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on-hook state. This voltage change is an order of magnitude less than
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the expected normal variation of CO battery voltage!
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Measuring voltage variations on a subscriber loop in an effort to detect a
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state-of-the-art eavesdropping device is meaningless, regardless of resolution
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of a voltage measuring device, since the "signal" is in effect buried in the
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"noise".
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Moving on to the subject of subscriber line impedance...
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There is simply no way for any device located on the subscriber's premises to
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obtain any MEANINGFUL information concerning the impedance characteristics of
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the subscriber loop and whether or not anything "unusual" is connected at the
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CO (or for that matter, anywhere else on the subscriber loop). There are a
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number of reasons why this is the case, which include but are not limited to:
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1. The impedance of a typical telephone cable pair results from
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distributed impedance elements, and not lumped elements. Non-loaded
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exchange area cable (22 to 26 AWG @ 0.083 uF/mile capacitance) is
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generally considered to have a characteristic impedance of 600 ohms
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(it actually varies, but this is a good compromise figure). Loaded
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exchange area cable, such as H88 loading which are 88 mH coils spaced
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at 6 kft intervals, is generally considered to have a a characteristic
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impedance of 900 ohms (it actually varies between 800 and 1,200 ohms,
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but 900 ohms is generally regarded as a good compromise figure for the
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voice frequency range of 300 to 3,000 Hz). What this means is that a
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bridged impedance of 100,000 ohms located in the CO on a typical
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subscriber loop will result in an impedance change measured at the
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SUBSCRIBER LOCATION of 0.1% or less. That's IF you could measure the
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impedance change at the subscriber location.
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2. As a general rule of thumb, the impedance of an exchange area
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telephone cable pair changes ONE PERCENT for every TEN DEGREES
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Fahrenheit temperature change. Actual impedance changes are a
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function of the frequency at which the impedance is measured, but the
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above rule is pretty close for the purposes of this discussion.
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3. Moisture in the telephone cable causes dramatic changes in its
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impedance characteristics. While this may appear obvious in the case
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of pulp (i.e., paper) insulated conductors, it is also characteristic
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of polyethylene (PIC) insulated conductors. Only gel-filled cable
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(icky-PIC), which still represents only a small percentage of
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installed cable plant, is relatively immune from the effects of
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moisture.
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4. From a practical standpoint, it is extremely difficult to measure
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impedance in the presence of the DC potential which is ALWAYS found on
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a telephone line. The subscriber has no means to remove the telephone
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pair from the switching apparatus in the CO to eliminate this
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potential.
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Therefore, any attempt at impedance measurement will be subject to DC
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current saturation error of any inductive elements found in an
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impedance bridge. The telephone company can, of course, isolate the
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subscriber cable pair from the switching apparatus for the purpose of
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taking a measurement -- but the subscriber cannot. In addition to the
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DC current problem, there is also the problem of impulse and other
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types of noise pickup on a connected loop which will impress errors in
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the impedance bridge detector circuit. Such noise primarily results
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from the on-hook battery feed, and is present even in ESS offices,
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with ferrod scanner pulses being a good source of such noise. While
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one could possibly dial a telephone company "balance termination" test
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line to get a quieter battery feed, this still leaves something to be
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desired for any actual impedance measurements.
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5. Devices which connect to a telephone pair and use a 2-wire/4-wire
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hybrid with either a white noise source or a swept oscillator on one
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side and a frequency-selective voltmeter on the other side to make a
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frequency vs return loss plot provide impressive, but meaningless
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data. Such a plot may be alleged to show "changes" in telephone line
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impedance characteristics. There is actual test equipment used by
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telephone companies which functions in this manner to measure 2-wire
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Echo Return Loss (ERL), but the ERL measurement is meaningless for
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localization of eavesdropping devices.
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6. It is not uncommon for the routing of a subscriber line cable pair to
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change one or more times during its lifetime due to construction and
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modification of outside cable plant. Outside cable plant bridge taps
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(not of the eavesdropping variety) can come and go, along with back
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taps in the CO to provide uninterrupted service during new cable plant
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additions. Not only can the "active" length of an existing cable pair
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change by several percent due to construction, but lumped elements of
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impedance can come and go due to temporary or permanent bridge taps.
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The bottom line of the above is that one cannot accurately measure the
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impedance of a telephone pair while it is connected to the CO switching
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apparatus, and even if one could, the impedance changes caused by the
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installation of an eavesdropping device will be dwarfed by changes in cable
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pair impedance caused by temperature, moisture, and cable plant construction
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unknown to the subscriber.
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About a year ago on a bulletin board I remember some discussions in which there
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was mention of the use of a time domain reflectometer (TDR) for localization of
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bridge taps and other anomalies. While a TDR will provide a rather detailed
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"signature" of a cable pair, it has serious limitations which include, but are
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not limited to:
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1. A TDR, in general, cannot be operated on a cable pair upon which there
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is a foreign potential; i.e., a TDR cannot be used on a subscriber
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cable pair which is connected to the CO switching apparatus.
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2. A TDR contains some rather sensitive circuitry used to detect the
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reflected pulse energy, and such circuitry is extremely susceptible to
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noise found in twisted pair telephone cable. A TDR is works well with
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coaxial cable and waveguide, which are in effect shielded transmission
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lines. The use of a TDR with a twisted cable pair is a reasonable
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compromise provided it is a _single_ cable pair within one shield.
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The use of a TDR with a twisted cable pair sharing a common shield
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with working cable pairs is an invitation to interference by virtue of
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inductive and capacitive coupling of noise from the working pairs.
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3. Noise susceptibility issues notwithstanding, most TDR's cannot be used
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beyond the first loading coil on a subscriber loop since the loading
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coil inductance presents far too much reactance to the short pulses
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transmitted by the TDR. There are one or two TDR's on the market
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which claim to function to beyond ONE loading coil, but their
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sensitivity is poor.
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There is simply no device available to a telephone subscriber that without the
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cooperation of the telephone company which can confirm or deny the presence of
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any eavesdropping device at any point beyond the immediate premises of the
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subscriber. I say "immediate premises of the subscriber" because one presumes
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that the subscriber has the ability to isolate the premises wiring from the
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outside cable plant, and therefore has complete inspection control over the
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premises wiring.
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I have used the phrase "without the cooperation of the telephone company"
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several times in this article. No voltage, impedance or TDR data is meaningful
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without knowing the actual circuit layout of the subscriber loop in question.
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Circuit layout information includes such data as exact length and guages of
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loop sections, detailed description of loading (if present), presence and
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location of multiples and bridge taps, calculated and measured resistance of
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the loop, loop transmission loss, etc. There is NO way that a telephone
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company is going to furnish that information to a subscriber! Sometimes it's
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even difficult for a government agency to get this information without judicial
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intervention.
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Despite what I have stated in this article, you will see claims made by third
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parties as to the existence of devices which will detect the presence of
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telephone line eavesdropping beyond the subscriber's immediate premises. With
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the exception of the trivial cases of serious DC current draw by an extension
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telephone or the detection of RF energy emitted by a transmitter, this just
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ain't so. Companies like Communication Control Corporation (which advertises
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in various "executive" business publications) get rich by selling devices which
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claim to measure minute voltage and impedance changes on a telephone line --
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but consider those claims in view of the voltage changes due to CO battery
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variations and due to temperature changes in outside cable plant -- and you
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should get the true picture.
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>--------=====END=====--------<
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