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USOO8917818B2
(12) United States Patent (10) Patent N0.: US 8,917,818 B2
Rozendaal (45) Date of Patent: Dec. 23, 2014
(54) METHOD AND SYSTEM FOR DETERMINING USPC .......................................... 379/1.01, 1.04, 24
A NUMBER OF LOAD COILS IN A See application ?le for complete search history.
TRANSMISSION LINE
56 References Cited
(71) Applicant: JDS Uniphase Corporation, Milpitas, ( )
CA (US) US. PATENT DOCUMENTS
(72) Inventor: Evert H. Rozendaal, Roanoke, VA (US) 4,087,657 A 5/1978 Peoples ....................... .. 324/615
5,404,388 A 4/1995 Eu . . . . . . . . . . . . . . .. 379/24
(73) Assignee: JDS Uniphase Corporation, Milpitas, 5,881,130 A * 3/1999 Zhang ~~~~~~~' 3790708
CA (Us) 6,263,047 B1 7/2001 Randle et a1. . . . . . . . . . .. 379/31
6,631,178 B1 10/2003 Blackwell et a1. . .. 379/104
. . . . . 6,668,041 B2 12/2003 K 31' tal. .. 379/104
( * ) Not1ce: Subject to any disclaimer, the term ofthis 7,395,162 B2 * 7/2008 F321; :t 31‘ u 702/57
patent is extended or adjusted under 35 7,436,935 132* 10/2008 Faulkner H 379/104
U.S.C. 154(b) by 0 days. 7,778,317 B2 8/2010 Jin ............... .. 375/224
7,844,436 B2 11/2010 Lindqvist et a1. 703/13
(21) App1_NO_; 14/157,291 2002/0067802 A1* 6/2002 Smith et a1. .. 379/104
2004/0230390 A1* 11/2004 Galliet a1. .. 702/66
- _ 2004/0267678 A1* 12/2004 Gao et a1. . . . . . . . . . . . . .. 706/2
(22) Flled' Jan'16’ 2014 2005/0285935 A1 * 12/2005 Hodges @181. 348/1408
_ _ _ 2007/0206668 A1* 9/2007 Jin ................... .. 375/224
(65) Prlor Publlcatlon Data 2009/0024340 A1* 1/2009 Borjesson etal. . 702/65
Us 2014/0198902 A1 Jul 17 2014 2010/0156553 A1* 6/2010 Lindqvist et a1. ............. .. 333/32
Related US. Application Data * Cited by exammer
(60) Provisional application No. 61/753,633, ?led on Jan. Primary Examiner i Quoc D Tran
17’ 2013' (74) Attorney, Agent, or Firm * JDS Uniphase Corporation
51 Int. Cl.
( ) H04M 1/24 (2006.01) (57) ABSTRACT
H04M 3/08 (2006.01) A method and system for determining a number ofload coils
H04M 3/22 (2006-01) in a transmission line are provided. An impulse response of
H04M 3/30 (2006-01) the transmission line is calculated from a characteristic
(52) US. Cl. impedance of the transmission line. A number of complex
................................... .. conjugate pole pairs of a transfer ?lnetion of the impulse
USPC ............................................ 379/24, 379/101 response is then determined' Thereby, the number of load
(58) Field of Classi?cation Search coils in the transmission line, Which is equal to the number of
CPC H04M 3/306; H04M 3/2209; H04M 3/30; complex conjugate pole pairs, is determined.
H04M 3/305; H04M 3/304; H04M 3/301;
H04M 3/308; H04M 1/24 18 Claims, 11 Drawing Sheets
1 1 | 1 ' 4
1000 2000 3000 42300 5000 6000 7000 8000
Frequency
4000 8000
Frequency
D 1 000 2000 3000 4000 5000 6000 7000 8000
Frequency
US. Patent Dec. 23, 2014 Sheet 1 0111 US 8,917,818 B2
100
 111 111
101
110 V I, 110
101 FM
111 111
FIG. 1
PRIOR ART
240
FIG. 2A
US. Patent Dec. 23, 2014 Sheet 2 0f 11
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US 8,917,818 B2
FIG. 2B
US. Patent Dec. 23, 2014 Sheet 3 0f 11 US 8,917,818 B2
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US. Patent
hnpedance
Ampiitude
Dec. 23, 2014 Sheet 4 0f 11
Frequensy Responsa
US 8,917,818 B2
~2
500
300
200
. . _ . _ . . . - . . . . . . _ . . _ . . _ . . _ . . . . . . . . . v _ . . _ . . _ . ‘ v . . .
3609 1:000 5000
Frequency {82}
i G00 2000
FIG. 4A
6060
Impulse Response
400
0.4 0:6 0.8
Time {uSec}
0.2
FIG. 4B
US. Patent Dec. 23, 2014 Sheet 5 0f 11 US 8,917,818 B2
Pmies
Q: ~95 :3 (15 1Reai?art
FIG. 4C
X i 04 Frequency Respun‘se
s
impedance
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Frequency {Hz}
FIG. 5A
US. Patent Dec. 23, 2014 Sheet 6 0f 11 US 8,917,818 B2
§mpulse Response
FIG. 5C
US. Patent
impedance
Ampiitucie
Dec. 23, 2014 Sheet 7 0f 11 US 8,917,818 B2
X 1 04 Frequency Response
2 , . , 0
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Frequency {Hz}
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US. Patent
impedance
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Dec. 23, 2014
Paiies
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Vaiid Paias
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FIG. 6C
Frequency Response
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Frequency 1H2}
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FIG. 7A
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US. Patent Dec. 23, 2014 Sheet 9 0f 11 US 8,917,818 B2
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Dec. 23, 2014 Sheet 10 0f 11 US 8,917,818 B2
¢ Frequency Rgspmnse
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Frequency {Hz}
FIG. 8A
impulse Response
0,4 0.6 0.8 1
Time {uSec}
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FIG. 8B
US. Patent Dec. 23, 2014 Sheet 11 0111 US 8,917,818 B2
Fates
$5
“1 .q ' ~ l : ~
A 5 :1 43.5 {1 0.5 1 15
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FIG. 8C
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US 8,917,818 B2
1
METHOD AND SYSTEM FOR DETERMINING
A NUMBER OF LOAD COILS IN A
TRANSMISSION LINE
CROSS-REFERENCE TO RELATED
APPLICATIONS
This application claims priority from US. Provisional
PatentApplicationNo. 61/753,633 to Rozendaal, ?led on Jan.
17, 2013, which is incorporated herein by reference.
TECHNICAL FIELD OF THE INVENTION
The present invention relates to detecting load coils in a
transmission line. More particularly, the present invention
relates to determining the number of load coils in a transmis
sion line by using the characteristic impedance of the trans
mission line.
BACKGROUND OF THE INVENTION
A load coil is an inductor that is inserted into a circuit to
increase its inductance. Load coils are often inserted into a
transmission line, e.g., a loop, to reduce amplitude and phase
distortions of signals transmitted over the transmission line.
As a result of their relatively high inductance, load coils
generate poles in the transfer function representing the char
acteristic impedance ofthe transmission line.
With reference to FIG. 1, in the past, load coils 110 were
inserted periodically, e.g., at a spacing on the order of kilo
meters, into a twisted-pair transmission line 100 used for
plain old telephone service (POTS) to improve the quality of
voice signals transmitted over the transmission line 100.
Typically, each load coil 110 includes two windings 111, each
connected in series with one wire 101 of the twisted-pair
transmission line 100.
However, the insertion of load coils into the transmission
line leads to a rapid increase in attenuation above a cut-off
frequency that depends on the spacing ofthe load coils. Typi
cally, transmission lines including load coils at a spacing
suitable for POTS have a cut-off frequency just above the
upper voice frequency limit of3 .4 kHZ. Therefore, in order to
use these loaded transmission lines for services, e.g., digital
subscriber line (DSL) services, operating at higher frequen
cies, e.g., above 10 kHZ, the load coils must be detected and
removed.
One prior-art technique fordetermining the number ofload
coils in a transmission line involves ?nding, e.g., by taking a
derivative, and counting local maxima in the characteristic
impedance of the transmission line. Variations of this tech
nique are disclosed in US. Pat. No. 7,778,317 to Jin, issued
onAug. 17, 2010, in US. Pat. No. 7,395,162 to Fertner et al.,
issued on Jul. 1, 2008, in US. Pat. No. 5,881,130 to Zhang,
issued on Mar. 9, 1999, in US. Pat. No. 5,404,388 to Eu,
issued on Apr. 4, 1995, and in US. Pat. No. 4,087,657 to
Peoples, issued on May 2, 1978, for example. Unfortunately,
when the local maxima are close to one another or overlap
ping, it is often di?icult to correctly determine the number of
local maxima.
SUMMARY OF THE INVENTION
Accordingly, one aspect ofthe present invention relates to
a method of determining a number of load coils in a trans
mission line having a characteristic impedance, the method
comprising: calculating an impulse response ofthe transmis
sion line from the characteristic impedance of the transmis
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60
65
2
sion line; and determining a number of complex conjugate
pole pairs of a transfer function of the impulse response to
thereby determine the number of load coils in the transmis
sion line, wherein the number of complex conjugate pole
pairs is equal to the number of load coils.
Another aspect ofthe present invention relates to a system
for determining a number of load coils in a transmission line
having a characteristic impedance, the system comprising: a
processing unit for calculating an impulse response of the
transmission line from the characteristic impedance of the
transmission line; and for determining a number of complex
conjugate pole pairs of a transfer function of the impulse
response to thereby determine the number ofload coils in the
transmission line, wherein the number ofcomplex conjugate
pole pairs is equal to the number of load coils.
BRIEF DESCRIPTION OF THE DRAWINGS
The present invention will be described in greater detail
with reference to the accompanying drawings, wherein:
FIG. 1 is a schematic illustration of a twisted-pair trans
mission line including two load coils;
FIG. 2A is a circuit diagram of an exemplary embodiment
of a measurement circuit;
FIG. 2B is a simpli?ed circuit diagram ofthe measurement
circuit of FIG. 2A;
FIG. 3 is a plot ofthe characteristic impedances measured
using the measurement circuit of FIG. 2A and calculated
according to a mathematical model for a transmission line
including four load coils;
FIG. 4A is a plot ofthe characteristic impedance measured
for a transmission line not including any load coils;
FIG. 4B is a plot of the impulse response calculated from
the characteristic impedance of FIG. 4A;
FIG. 4C is a plot ofthe poles ofthe transfer function ofthe
impulse response of FIG. 4B;
FIG. 5A is a plot ofthe characteristic impedance measured
for a transmission line including one load coil;
FIG. 5B is a plot of the impulse response calculated from
the characteristic impedance of FIG. 5A;
FIG. 5C is a plot ofthe poles ofthe transfer function ofthe
impulse response of FIG. 5B;
FIG. 6A is a plot ofthe characteristic impedance measured
for a transmission line including two load coils;
FIG. 6B is a plot of the impulse response calculated from
the characteristic impedance of FIG. 6A;
FIG. 6C is a plot ofthe poles ofthe transfer function ofthe
impulse response of FIG. 6B;
FIG. 7A is a plot ofthe characteristic impedance measured
for a transmission line including three load coils;
FIG. 7B is a plot of the impulse response calculated from
the characteristic impedance of FIG. 7A;
FIG. 7C is a plot ofthe poles ofthe transfer function ofthe
impulse response of FIG. 7B;
FIG. 8A is a plot ofthe characteristic impedance measured
for a transmission line including four load coils;
FIG. 8B is a plot of the impulse response calculated from
the characteristic impedance of FIG. 8A;
FIG. 8C is a plot ofthe poles ofthe transfer function ofthe
impulse response of FIG. 8B; and
FIG. 9 is a block diagram of an exemplary embodiment of
a system for determining the number of load coils in a trans
mission line.
DETAILED DESCRIPTION OF THE INVENTION
The present invention provides a method and system for
determining the number of load coils in a transmission line.
US 8,917,818 B2
3
Advantageously, the present invention allows the number of
load coils in the transmission line to be determined in a simple
and straightforward manner by using the characteristic
impedance of the transmission line.
The characteristic impedance ofthe transmission line is the
impedance ofthe transmission line as a function offrequency,
i.e., the frequency response of the transmission line. The
characteristic impedance is a property ofthe transmission line
and is independent ofthe method and apparatus used to mea
sure the characteristic impedance. Several suitable measure
ment methods and apparatus are available, any ofwhich may
be used by the present invention.
With reference to FIG. 2A, an exemplary measurement
circuit 200 for measuring the characteristic impedance of a
transmission line includes a digital-to-analog converter
(DAC) 210, resistors 220-225, capacitors 230-232, and an
analog-to-digital converter (ADC) 240. The DAC 210 is used
to generate sine waves of different frequencies, e.g., 64 dif
ferent frequencies up to about 6 kHz. The different frequen
cies are, preferably, evenly spacedto facilitate the subsequent
calculation of an inverse Fourier transform.
The sine waves are sent to the ADC 240 via the resistors
220-225 and capacitors 230-232 as illustrated in FIG. 2A. The
measurement circuit 200 is connectedto the tip andring ofthe
loop, i.e., the two wires of the transmission line. The imped
ance ofthe transmission line at the different frequencies will
change the voltage Vin at the input of the ADC 240. These
changes in voltage at the different frequencies are used to
determine the characteristic impedance ZO of the transmis
sion line.
The output impedance of the DAC 210 and the input
impedance of the ADC 240 are very close to zero, so the
measurement circuit 200 may simpli?ed as illustrated in FIG.
2B, where Zl-Z4 are impedances ofthe measurement circuit
200. Since the output impedance ofthe DAC 210 is very close
to zero, the output voltage V01” is substantially the same
whether or not the transmission line is connected. Therefore,
the input voltageVin is measured at different frequencies and
is stored in memory as calibration data, e.g., in a calibration
?le. This calibration data is used to calculate the output volt
age V according to Equation (1):out
To calculate the characteristic impedance ZO of the trans
mission line, we notice that the voltageVAB between points A
and B may be expressed according to Equation (2):
v- (2)
vAB = %(Z2 + 23) = vow
3
where the symbol means “parallel to”. Using Equation (1)
and renaming Vin to VinCal, Equation (3) is obtained:
Vin(ZZ +Zs) : (3)
in which the characteristic impedance Z0 is the only
unknown. By solving for Z0, Equation (4) is obtained:
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4
((Vout — Vin)Z3 — VinZZ — VinZl)Z4 —
Vinzlzs — VinZlZZ
(Vow — Vin)Z3 — vinZZ — VinZl
(4)
20:
To simplify, two variables T1 and T2 are assigned according
to Equations (5) and (6):
TIIVZ-nZi; (5)
Using these variables, Equation (4) reduces to Equation
(7):
_ Tzzt - Tiz3 - T122 (7)
Therefore, by measuring the input voltage Vin at different
frequencies, the characteristic impedance ZO ofthe transmis
sion line may be determined by applying Equation (7). With
reference to FIG. 3, the characteristic impedance 310 mea
sured according to this method for a standard transmission
line including four load coils is in good agreement with the
characteristic impedance 320 calculated according to a math
ematical model for the same transmission line. The large
capacitors at the input are responsible for the angle mismatch
at low frequencies.
In general, the characteristic impedance of a transmission
line may be represented as a transfer function H(z) in poly
nomial form, having Q coef?cients bl- and P coef?cients a],
according to Equation (8):
Q _ (8)
Equation (8) may be rewritten in factored form to give Equa
tion (9):
H =b i.
(Z) 0(1— plruu — P2171) (1 — pm)
As shown by Equation (9), the numerator of the transfer
function H(z) has Q roots qi, which correspond to the zeros of
the transfer function H(z). At the zeros, the transfer function
H(z), representingthe characteristic impedance Z0, is equal to
zero. As also shown by Equation (9), the denominator ofthe
transfer function H(z) has P roots pi, which correspond to the
poles ofthe transfer function H(z). At the poles, the transfer
function H(z), representing the characteristic impedance Z0,
is in?nite. Typically, the zeros and poles occur as complex
conjugate pairs, i.e., as complex numbers z:a+bi and z:a—bi
having real parts a that are equal in magnitude and sign, and
imaginary parts b that are equal in magnitude but opposite in
sign.
For load coil detection, we are interested in the poles ofthe
transfer function H(z) in factored form of Equation (9),
because the number ofcomplex conjugate pole pairs is equal
to the number of load coils in the transmission line. Rather
than attempting to ?nd local maxima in the characteristic
US 8,917,818 B2
5
impedance, the present invention calculates the impulse
response, i.e., the time response, ofthe transmission line from
the characteristic impedance and determines the number of
complex conjugate poles pairs from the impulse response.
As is commonly known, the impulse response of a system
is the output signal when the input signal is an impulse. The
transfer function of the impulse response describes the rela
tion between the input and output signals.
Accordingto thepresent invention, the impulse response of
the transmission line is, typically, calculated by performing
an inverse Fourier transform, e.g., an inverse fast Fourier
transform (FFT), on the characteristic impedance. The num
ber ofcomplex conjugate pole pairs ofthe transferfunction of
the impulse response is then determined.
Typically, the transfer function of the impulse response is
found by applying a parametric modeling technique to the
impulse response.As is commonly known, a parametric mod
eling technique ?nds the parameters for a mathematical
model describing a system, by using known information
about the system. Several suitable parametric modeling tech
niques are available for use in the present invention, such as
the Prony method, the Levinson-Durbin method, the Yule
Walker method, etc. The Prony method is presently preferred
as the parametric modeling technique.
In general, the parametric modeling technique ?nds the
coef?cients bl- and aj ofthe transfer function H(z) in polyno
mial form of Equation (8) by using the impulse response.
Once the transfer function has been found, a root-?nding
algorithm ?nds the poles and the zeros, i.e., the roots pl- and q,
ofthe transfer function H(z) in factored form ofEquation (9).
Typically, the parametric modeling technique requires ini
tial guess values for the number ofpoles P and the number of
zeros Q, i.e., the number of coef?cients, ofthe transfer func
tion H(z). The guess values for the numbers ofpoles and zeros
are selected to be greater than the expected numbers ofpoles
and zeros. Typically, the guess values forthe numbers ofpoles
and zeros are the same and are greater than the expected
number ofpoles, which is two times the expected number of
load coils in the transmission line. The expected number of
load coils in the transmission line, in turn, may be determined
from the length ofthe transmission line, by considering stan
dard spacings ofload coils, e.g., a spacing of 6000 ft between
load coils, and a spacing of 3000 ft before and after the ?rst
and last load coils.
Typically, the guess values for the numbers of poles and
zeros are selected to be at least two times greater than the
expected numbers of poles and zeros, i.e., at least four times
greater than the expected number of load coils. For example,
if the expected number of load coils in a transmission line is
three, the expected number ofpoles is six, i.e., three complex
conjugate pole pairs, and the guess values for the numbers of
poles and zeros are each selected to be at least 12.
The transfer function found by the parametric modeling
technique has poles equal in number to the guess value for the
number ofpoles. Once the poles ofthe transfer function have
been found by the root-?nding algorithm, it is necessary to
determine which of the poles are valid. Valid poles occur as
complex conjugate pole pairs. Therefore, the number ofcom
plex conjugate pairs indicates the number ofload coils in the
transmission line.
Accordingly, complex conjugate pole pairs are identi?ed
among the poles found by the root-?nding algorithm. Poles
having an imaginary part b with an absolute magnitude ofless
than a ?rst threshold, e.g., |b|<0.08, are not considered fur
ther. The remaining poles are identi?ed as complex poles.
Complex conjugate pole pairs are then identi?ed among the
complex poles by calculating distances between the complex
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poles and conjugates of the complex poles. If the absolute
distance between a ?rst complex pole Z1 and the conjugate E2
ofa second complex pole is less than a second threshold, e.g.,
lzl—z2<0.15, the ?rst complex pole Z1 and the second com
plex pole z2 are identi?ed as a complex conjugate pole pair.
Ideally, the absolute distance should be zero, but in practice it
is usually small because ofnoise and limited hardware accu
racy.
The ?rst and second thresholds are selected by taking prac
tical limitations into consideration. Typically, the ?rst and
secondthresholds are determined empirically through experi
mentation.
The complex conjugate pole pairs identi?ed in this manner
are considered to be valid poles. The complex conjugate pole
pairs are then counted to determine the number of load coils
in the transmission line, which is equal to the number of
complex conjugate pole pairs.
Several examples are provided hereafter to further illus
trate the present invention. With reference to FIG. 4, in a ?rst
example, the present invention was applied to a 15 000 ft
transmission line not including any load coils. The character
istic impedance, i.e., the frequency response, ofthe transmis
sion line, which is plotted in FIG. 4A, was measured by using
the measurement circuit 200 ofFIG. 2. The impulse response
of the transmission line, which is plotted in FIG. 4B, was
calculated by applying an inverse Fourier transform to the
characteristic impedance. The transfer function of the
impulse response was found by applying the Prony method to
the impulse response. 10 poles ofthe transfer function, which
are plotted in FIG. 4C, were found by using a root-?nding
algorithm. However, all of the poles were determined to be
invalid because they did not belong to valid complex conju
gate pole pairs. Therefore, the number of load coils in the
transmission line was correctly determined to be zero. It
should be noted that the direct current (DC) and very low
frequency response could not be detected by the alternating
current (AC) coupled hardware and was approximated by
extrapolation. Consequently, one pair of poles is close to a
valid complex conjugate pole pair, but the absolute distance
lzl—zzl is greater than the second threshold.
With reference to FIG. 5, in a second example, the present
invention was applied to a transmission line including one
load coil (LC) at the following spacing: 3000 ft, LC, 3000 ft.
The characteristic impedance, i.e., the frequency response, of
the transmission line, which is plotted in FIG. 5A, was mea
sured by using the measurement circuit 200 of FIG. 2. The
impulse response ofthe transmission line, which is plotted in
FIG. 5B, was calculated by applying an inverse Fourier trans
form to the characteristic impedance. The transfer function of
the impulse response was found by applying the Prony
method to the impulse response. 10 poles of the transfer
function, which are plotted in FIG. 5C, were found by using
a root-?nding algorithm. Of these, one pair of poles was
determined to be a valid complex conjugate pole pair. There
fore, the number of load coils in the transmission line was
correctly determined to be one.
With reference to FIG. 6, in a third example, the present
invention was applied to a transmission line including two
loadcoils (LCs) atthe following spacing: 3000 ft, LC, 6000 ft,
LC, 3000 ft. The characteristic impedance, i.e., the frequency
response, of the transmission line, which is plotted in FIG.
6A, was measured by using the measurement circuit 200 of
FIG. 2. The impulse response ofthe transmission line, which
is plotted in FIG. 6B, was calculated by applying an inverse
Fourier transform to the characteristic impedance. The trans
fer function of the impulse response was found by applying
the Prony method to the impulse response. 14 poles of the
US 8,917,818 B2
7
transfer function, which are plotted in FIG. 6C, were found by
using a root-?nding algorithm. Of these, two pairs of poles
were determined to be valid complex conjugate pole pairs.
Therefore, the number of load coils in the transmission line
was correctly determined to be two.
With reference to FIG. 7, in a fourth example, the present
invention was applied to a transmission line including three
load coils (LCs) at the following spacing: 3000 ft, LC, 15 000
ft, LC, 6000 ft, LC, 3000 ft. The characteristic impedance,
i.e., the frequency response, ofthe transmission line, which is
plotted in FIG. 7A, was measured by using the measurement
circuit 200 of FIG. 2. The impulse response of the transmis
sion line, which is plotted in FIG. 7B, was calculated by
applying an inverse Fourier transform to the characteristic
impedance. The transfer function ofthe impulse response was
foundby applying the Prony method to the impulse response.
14 poles ofthe transfer function, which are plotted in FIG. 7C,
were found by using a root-?nding algorithm. Ofthese, three
pairs ofpoles were determined to be valid complex conjugate
pole pairs. Therefore, the number of load coils in the trans
mission line was correctly determined to be three.
With reference to FIG. 8, in a ?fth example, the present
invention was applied to a transmission line including four
loadcoils (LCs) atthe following spacing: 3000 ft, LC, 6000 ft,
LC, 6000 ft, LC, 6000 ft, LC, 3000 ft. The characteristic
impedance, i.e., the frequency response, ofthe transmission
line, which is plotted in FIG. 8A, was measured by using the
measurement circuit 200 of FIG. 2. The impulse response of
the transmission line, which is plotted in FIG. 8B, was calcu
lated by applying an inverse Fourier transform to the charac
teristic impedance. The transfer function of the impulse
response was found by applying the Prony method to the
impulse response. 14 poles ofthe transfer function, which are
plotted in FIG. 8C, were found by using a root-?nding algo
rithm. Of these, four pairs of poles were determined to be
valid complex conjugate pole pairs. Therefore, the number of
load coils in the transmission line was correctly determined to
be four.
The present invention may be implemented in hardware,
software, or a combination thereof. When implemented in
software, instructions for carrying out the actions described
heretofore are stored in a non-transitory computer-readable
storage medium, e.g., memory, and are executed by a proces
sor of a hardware device, e.g., a general purpose computer or
a test device.
With reference to FIG. 9, an exemplary system 900 for
determining the number of load coils in a transmission line
includes a measurement unit 910 and a processing unit 920. In
a preferred embodiment, the system 900 is embodied as a test
device, e.g., a portable or ?xed test device, in which the
measurement unit 910 and the processing unit 920 are sup
ported by a common housing. In other embodiments, the
measurement unit 910 may be embodied as a test device, e.g.,
a portable or ?xed test device, and the processing unit 920
may be embodied as a separate hardware device or as soft
ware stored and executed by a separate hardware device, e.g.,
a general purpose computer.
The measurement unit 910 measures the characteristic
impedance of the transmission line, typically, by means of a
measurement circuit, such as the measurement circuit 200 of
FIG. 2 described heretofore. The processing unit 920 calcu
lates the impulse response of the transmission line from the
characteristic impedance and determines the number ofcom
plex conjugate pole pairs of the transfer function of the
impulse response, as described heretofore. Thereby, the pro
cessing unit 920 determines the number of load coils in the
transmission line, which is equal to the number of complex
20
25
30
35
40
45
50
55
60
65
8
conjugate pole pairs. Typically, the number of load coils is
reported by the system 900, e.g., on a display.
It should be noted that other embodiments of the system
may omit the measurement unit, which is optional. Embodi
ments omitting the measurement unit are suitably con?gured
to receive the characteristic impedance, i.e., frequency-de
pendent impedance data, as input.
Ofcourse, numerous other embodiments may be envisaged
without departing from the spirit and scope of the invention.
1 claim:
1. A method of determining a number of load coils in a
transmission line having a characteristic impedance, the
method comprising:
calculating, using a processing unit, animpulseresponse of
the transmission line from the characteristic impedance
of the transmission line; and
determining, using a processing unit, a number ofcomplex
conjugate pole pairs ofa transferfunction ofthe impulse
response to thereby determine the number of load coils
in the transmission line, wherein the number ofcomplex
conjugate pole pairs is equal to the number ofload coils,
by:
?nding the transfer function by applying a parametric
modeling technique to the impulse response; and
?nding poles of the transfer function by using a root
?nding algorithm, wherein the poles of the transfer
function are greater in number than two times an
expected number of load coils in the transmission
line.
2. The method of claim 1, further comprising:
measuring the characteristic impedance of the transmis
sion line.
3. The method ofclaim 1, wherein calculating the impulse
response includes performing an inverse Fourier transform on
the characteristic impedance.
4. The method ofclaim 1, whereinthe parametric modeling
technique is the Prony method.
5. A method of determining a number of load coils in a
transmission line having a characteristic impedance, the
method comprising:
calculating, using a processing unit, animpulseresponse of
the transmission line from the characteristic impedance
of the transmission line; and
determining, using a processing unit, a number ofcomplex
conjugate pole pairs ofa transferfunction ofthe impulse
response to thereby determine the number of load coils
in the transmission line, wherein the number ofcomplex
conjugate pole pairs is equal to the number ofload coils,
?nding the transfer function by applying a parametric
modeling technique to the impulse response;
?nding poles of the transfer function by using a root
?nding algorithm;
identifying complex poles among the poles ofthe trans
fer function;
identifying complex conjugate pole pairs among the
complex poles; and
counting the complex conjugate pole pairs.
6. The method of claim 5, further comprising:
measuring the characteristic impedance of the transmis
sion line.
7. The method ofclaim 5, wherein calculating the impulse
response includes performing an inverse Fourier transform on
the characteristic impedance.
8. The method ofclaim 5, whereinthe parametric modeling
technique is the Prony method.
US 8,917,818 B2
9. A system for determining a number of load coils in a
transmission line having a characteristic impedance, the sys
tem comprising:
a processing unit for calculating an impulse response ofthe
transmission line from the characteristic impedance of
the transmission line; and for determining a number of
complex conjugate pole pairs of a transfer function of
the impulse response to thereby determine the number of
load coils in the transmission line, Wherein the number
of complex conjugate pole pairs is equal to the number
ofload coils, by:
?nding the transfer function by applying a parametric
modeling technique to the impulse response; and
?nding poles of the transfer function by using a root
?nding algorithm, Wherein the poles of the transfer
function are greater in number than two times an
expected number of load coils in the transmission
line.
10. The system of claim 9, further comprising:
a measurement unit for measuring the characteristic
impedance of the transmission line.
11. The system of claim 10, Wherein the system is a por
table test device.
12. The system ofclaim 9, Wherein calculating the impulse
response includes performing an inverse Fourier transform on
the characteristic impedance.
13. The system of claim 9, Wherein the parametric model
ing technique is the Prony method.
14. A system for determining a number of load coils in a
transmission line having a characteristic impedance, the sys
tem comprising:
25
10
a processing unit for calculating an impulse response ofthe
transmission line from the characteristic impedance of
the transmission line; and for determining a number of
complex conjugate pole pairs of a transfer function of
the impulse response to thereby determine the number of
load coils in the transmission line, Wherein the number
of complex conjugate pole pairs is equal to the number
of load coils, by:
?nding the transfer function by applying a parametric
modeling technique to the impulse response;
?nding poles of the transfer function by using a root
?nding algorithm;
identifying complex poles among the poles ofthe trans
fer function;
identifying complex conjugate pole pairs among the
complex poles; and
counting the complex conjugate pole pairs.
15. The system of claim 14, further comprising:
a measurement unit for measuring the characteristic
impedance of the transmission line.
16. The system of claim 15, Wherein the system is a por
table test device.
17. The system of claim 14, Wherein calculating the
impulse response includes performing an inverse Fourier
transform on the characteristic impedance.
18. The system of claim 14, Wherein the parametric mod
eling technique is the Prony method.
* * * * *

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US8917818B2

  • 1. USOO8917818B2 (12) United States Patent (10) Patent N0.: US 8,917,818 B2 Rozendaal (45) Date of Patent: Dec. 23, 2014 (54) METHOD AND SYSTEM FOR DETERMINING USPC .......................................... 379/1.01, 1.04, 24 A NUMBER OF LOAD COILS IN A See application ?le for complete search history. TRANSMISSION LINE 56 References Cited (71) Applicant: JDS Uniphase Corporation, Milpitas, ( ) CA (US) US. PATENT DOCUMENTS (72) Inventor: Evert H. Rozendaal, Roanoke, VA (US) 4,087,657 A 5/1978 Peoples ....................... .. 324/615 5,404,388 A 4/1995 Eu . . . . . . . . . . . . . . .. 379/24 (73) Assignee: JDS Uniphase Corporation, Milpitas, 5,881,130 A * 3/1999 Zhang ~~~~~~~' 3790708 CA (Us) 6,263,047 B1 7/2001 Randle et a1. . . . . . . . . . .. 379/31 6,631,178 B1 10/2003 Blackwell et a1. . .. 379/104 . . . . . 6,668,041 B2 12/2003 K 31' tal. .. 379/104 ( * ) Not1ce: Subject to any disclaimer, the term ofthis 7,395,162 B2 * 7/2008 F321; :t 31‘ u 702/57 patent is extended or adjusted under 35 7,436,935 132* 10/2008 Faulkner H 379/104 U.S.C. 154(b) by 0 days. 7,778,317 B2 8/2010 Jin ............... .. 375/224 7,844,436 B2 11/2010 Lindqvist et a1. 703/13 (21) App1_NO_; 14/157,291 2002/0067802 A1* 6/2002 Smith et a1. .. 379/104 2004/0230390 A1* 11/2004 Galliet a1. .. 702/66 - _ 2004/0267678 A1* 12/2004 Gao et a1. . . . . . . . . . . . . .. 706/2 (22) Flled' Jan'16’ 2014 2005/0285935 A1 * 12/2005 Hodges @181. 348/1408 _ _ _ 2007/0206668 A1* 9/2007 Jin ................... .. 375/224 (65) Prlor Publlcatlon Data 2009/0024340 A1* 1/2009 Borjesson etal. . 702/65 Us 2014/0198902 A1 Jul 17 2014 2010/0156553 A1* 6/2010 Lindqvist et a1. ............. .. 333/32 Related US. Application Data * Cited by exammer (60) Provisional application No. 61/753,633, ?led on Jan. Primary Examiner i Quoc D Tran 17’ 2013' (74) Attorney, Agent, or Firm * JDS Uniphase Corporation 51 Int. Cl. ( ) H04M 1/24 (2006.01) (57) ABSTRACT H04M 3/08 (2006.01) A method and system for determining a number ofload coils H04M 3/22 (2006-01) in a transmission line are provided. An impulse response of H04M 3/30 (2006-01) the transmission line is calculated from a characteristic (52) US. Cl. impedance of the transmission line. A number of complex ................................... .. conjugate pole pairs of a transfer ?lnetion of the impulse USPC ............................................ 379/24, 379/101 response is then determined' Thereby, the number of load (58) Field of Classi?cation Search coils in the transmission line, Which is equal to the number of CPC H04M 3/306; H04M 3/2209; H04M 3/30; complex conjugate pole pairs, is determined. H04M 3/305; H04M 3/304; H04M 3/301; H04M 3/308; H04M 1/24 18 Claims, 11 Drawing Sheets 1 1 | 1 ' 4 1000 2000 3000 42300 5000 6000 7000 8000 Frequency 4000 8000 Frequency D 1 000 2000 3000 4000 5000 6000 7000 8000 Frequency
  • 2. US. Patent Dec. 23, 2014 Sheet 1 0111 US 8,917,818 B2 100 111 111 101 110 V I, 110 101 FM 111 111 FIG. 1 PRIOR ART 240 FIG. 2A
  • 3. US. Patent Dec. 23, 2014 Sheet 2 0f 11 "H. US 8,917,818 B2 FIG. 2B
  • 4. US. Patent Dec. 23, 2014 Sheet 3 0f 11 US 8,917,818 B2 Re§Zc} a: ReiZm} g irm‘Zc} E- im(2m} ' < .~4000 * = 1 i x z 5 0 H380 2000 3000 4630 5000 6090 7000 800G Frequency 5000 x - 1 ! x z i ‘ ' 310 ‘ ‘ ------------- -- Cale.(G 3g p . v . ‘ . . ‘ . . m 0 t I l l z i O 1080 2000 3608 4-808 5000 6080 "$080 8006 Frequency 2 : f 1 i ,_ > 4 . ‘ . > . . . is gm 0 _ 8 8 . . a <2 J; M '_‘ ~ . . . v > _ 8 , , . . _ . . .7 ._ l m“ “2 i l ! ¥ 1 U 1 000 2060 3088 4880 50% 60538 T900 8069 Frequency FIG. 3
  • 5. US. Patent hnpedance Ampiitude Dec. 23, 2014 Sheet 4 0f 11 Frequensy Responsa US 8,917,818 B2 ~2 500 300 200 . . _ . _ . . . - . . . . . . _ . . _ . . _ . . _ . . . . . . . . . v _ . . _ . . _ . ‘ v . . . 3609 1:000 5000 Frequency {82} i G00 2000 FIG. 4A 6060 Impulse Response 400 0.4 0:6 0.8 Time {uSec} 0.2 FIG. 4B
  • 6. US. Patent Dec. 23, 2014 Sheet 5 0f 11 US 8,917,818 B2 Pmies Q: ~95 :3 (15 1Reai?art FIG. 4C X i 04 Frequency Respun‘se s impedance O 1 690 20GB 3600 4600 5800 6000 Frequency {Hz} FIG. 5A
  • 7. US. Patent Dec. 23, 2014 Sheet 6 0f 11 US 8,917,818 B2 §mpulse Response FIG. 5C
  • 8. US. Patent impedance Ampiitucie Dec. 23, 2014 Sheet 7 0f 11 US 8,917,818 B2 X 1 04 Frequency Response 2 , . , 0 ' m Reai ,5 _ ~~~~~~~~~~ Imag “ 0 1000 3000 4000 5000 0000 Frequency {Hz} 2809 FIG. 6A ¥mpuise Response 1000 800...... ..1......H.... ......8..H.H.. l..... U. 400- ' 200 ~200 “800. .........H.... ...... ..H.I.. .....I ‘0“.H... “8000 0.2 0}: 0.6 0.8 1 Time [0800] FIG. 6B
  • 9. US. Patent impedance ~05 imaginaryPM Dec. 23, 2014 Paiies Sheet80f11 lnvaiid Poies Vaiid Paias x10 Heat Part FIG. 6C Frequency Response US 8,917,818 B2 VVVVVVVVVVVVVVVVVVVV 1 3080 7 Frequency 1H2} 2000 FIG. 7A 4800 50100 6000
  • 10. US. Patent Dec. 23, 2014 Sheet 9 0f 11 US 8,917,818 B2 imputse Response 12% ~ - 1899 ‘ 880 - 8GB " 4GB ' a 289 Ampiizude ass-E M489 , . . v . . . . . . . . . . . v . . v . . . r . . . . ..j . . . . v v . . ..j . . . . . . . .. 4569» I FIG. 7B hwaiid Poies Vaiid Poias irragmmyPM a oin //' // //,~ ‘5 // ’0 p “‘"45/"¢ 1 93m I “1:35 A 0 {is *=‘ 15> Heat Part FIG. 7C
  • 11. US. Patent x10 Dec. 23, 2014 Sheet 10 0f 11 US 8,917,818 B2 ¢ Frequency Rgspmnse 1.5 impedance l QM“ Real ~~~~~~~~~~ imag ~~~~~~~~“Abs . i200 1000- - 800' 200Ampiitude ~200' -600 0 Frequency {Hz} FIG. 8A impulse Response 0,4 0.6 0.8 1 Time {uSec} 0.2 FIG. 8B
  • 12. US. Patent Dec. 23, 2014 Sheet 11 0111 US 8,917,818 B2 Fates $5 “1 .q ' ~ l : ~ A 5 :1 43.5 {1 0.5 1 15 Real Part FIG. 8C 900 Processing [920 unit Zo Measurement /910 unit FIG. 9
  • 13. US 8,917,818 B2 1 METHOD AND SYSTEM FOR DETERMINING A NUMBER OF LOAD COILS IN A TRANSMISSION LINE CROSS-REFERENCE TO RELATED APPLICATIONS This application claims priority from US. Provisional PatentApplicationNo. 61/753,633 to Rozendaal, ?led on Jan. 17, 2013, which is incorporated herein by reference. TECHNICAL FIELD OF THE INVENTION The present invention relates to detecting load coils in a transmission line. More particularly, the present invention relates to determining the number of load coils in a transmis sion line by using the characteristic impedance of the trans mission line. BACKGROUND OF THE INVENTION A load coil is an inductor that is inserted into a circuit to increase its inductance. Load coils are often inserted into a transmission line, e.g., a loop, to reduce amplitude and phase distortions of signals transmitted over the transmission line. As a result of their relatively high inductance, load coils generate poles in the transfer function representing the char acteristic impedance ofthe transmission line. With reference to FIG. 1, in the past, load coils 110 were inserted periodically, e.g., at a spacing on the order of kilo meters, into a twisted-pair transmission line 100 used for plain old telephone service (POTS) to improve the quality of voice signals transmitted over the transmission line 100. Typically, each load coil 110 includes two windings 111, each connected in series with one wire 101 of the twisted-pair transmission line 100. However, the insertion of load coils into the transmission line leads to a rapid increase in attenuation above a cut-off frequency that depends on the spacing ofthe load coils. Typi cally, transmission lines including load coils at a spacing suitable for POTS have a cut-off frequency just above the upper voice frequency limit of3 .4 kHZ. Therefore, in order to use these loaded transmission lines for services, e.g., digital subscriber line (DSL) services, operating at higher frequen cies, e.g., above 10 kHZ, the load coils must be detected and removed. One prior-art technique fordetermining the number ofload coils in a transmission line involves ?nding, e.g., by taking a derivative, and counting local maxima in the characteristic impedance of the transmission line. Variations of this tech nique are disclosed in US. Pat. No. 7,778,317 to Jin, issued onAug. 17, 2010, in US. Pat. No. 7,395,162 to Fertner et al., issued on Jul. 1, 2008, in US. Pat. No. 5,881,130 to Zhang, issued on Mar. 9, 1999, in US. Pat. No. 5,404,388 to Eu, issued on Apr. 4, 1995, and in US. Pat. No. 4,087,657 to Peoples, issued on May 2, 1978, for example. Unfortunately, when the local maxima are close to one another or overlap ping, it is often di?icult to correctly determine the number of local maxima. SUMMARY OF THE INVENTION Accordingly, one aspect ofthe present invention relates to a method of determining a number of load coils in a trans mission line having a characteristic impedance, the method comprising: calculating an impulse response ofthe transmis sion line from the characteristic impedance of the transmis 20 25 30 35 40 45 50 55 60 65 2 sion line; and determining a number of complex conjugate pole pairs of a transfer function of the impulse response to thereby determine the number of load coils in the transmis sion line, wherein the number of complex conjugate pole pairs is equal to the number of load coils. Another aspect ofthe present invention relates to a system for determining a number of load coils in a transmission line having a characteristic impedance, the system comprising: a processing unit for calculating an impulse response of the transmission line from the characteristic impedance of the transmission line; and for determining a number of complex conjugate pole pairs of a transfer function of the impulse response to thereby determine the number ofload coils in the transmission line, wherein the number ofcomplex conjugate pole pairs is equal to the number of load coils. BRIEF DESCRIPTION OF THE DRAWINGS The present invention will be described in greater detail with reference to the accompanying drawings, wherein: FIG. 1 is a schematic illustration of a twisted-pair trans mission line including two load coils; FIG. 2A is a circuit diagram of an exemplary embodiment of a measurement circuit; FIG. 2B is a simpli?ed circuit diagram ofthe measurement circuit of FIG. 2A; FIG. 3 is a plot ofthe characteristic impedances measured using the measurement circuit of FIG. 2A and calculated according to a mathematical model for a transmission line including four load coils; FIG. 4A is a plot ofthe characteristic impedance measured for a transmission line not including any load coils; FIG. 4B is a plot of the impulse response calculated from the characteristic impedance of FIG. 4A; FIG. 4C is a plot ofthe poles ofthe transfer function ofthe impulse response of FIG. 4B; FIG. 5A is a plot ofthe characteristic impedance measured for a transmission line including one load coil; FIG. 5B is a plot of the impulse response calculated from the characteristic impedance of FIG. 5A; FIG. 5C is a plot ofthe poles ofthe transfer function ofthe impulse response of FIG. 5B; FIG. 6A is a plot ofthe characteristic impedance measured for a transmission line including two load coils; FIG. 6B is a plot of the impulse response calculated from the characteristic impedance of FIG. 6A; FIG. 6C is a plot ofthe poles ofthe transfer function ofthe impulse response of FIG. 6B; FIG. 7A is a plot ofthe characteristic impedance measured for a transmission line including three load coils; FIG. 7B is a plot of the impulse response calculated from the characteristic impedance of FIG. 7A; FIG. 7C is a plot ofthe poles ofthe transfer function ofthe impulse response of FIG. 7B; FIG. 8A is a plot ofthe characteristic impedance measured for a transmission line including four load coils; FIG. 8B is a plot of the impulse response calculated from the characteristic impedance of FIG. 8A; FIG. 8C is a plot ofthe poles ofthe transfer function ofthe impulse response of FIG. 8B; and FIG. 9 is a block diagram of an exemplary embodiment of a system for determining the number of load coils in a trans mission line. DETAILED DESCRIPTION OF THE INVENTION The present invention provides a method and system for determining the number of load coils in a transmission line.
  • 14. US 8,917,818 B2 3 Advantageously, the present invention allows the number of load coils in the transmission line to be determined in a simple and straightforward manner by using the characteristic impedance of the transmission line. The characteristic impedance ofthe transmission line is the impedance ofthe transmission line as a function offrequency, i.e., the frequency response of the transmission line. The characteristic impedance is a property ofthe transmission line and is independent ofthe method and apparatus used to mea sure the characteristic impedance. Several suitable measure ment methods and apparatus are available, any ofwhich may be used by the present invention. With reference to FIG. 2A, an exemplary measurement circuit 200 for measuring the characteristic impedance of a transmission line includes a digital-to-analog converter (DAC) 210, resistors 220-225, capacitors 230-232, and an analog-to-digital converter (ADC) 240. The DAC 210 is used to generate sine waves of different frequencies, e.g., 64 dif ferent frequencies up to about 6 kHz. The different frequen cies are, preferably, evenly spacedto facilitate the subsequent calculation of an inverse Fourier transform. The sine waves are sent to the ADC 240 via the resistors 220-225 and capacitors 230-232 as illustrated in FIG. 2A. The measurement circuit 200 is connectedto the tip andring ofthe loop, i.e., the two wires of the transmission line. The imped ance ofthe transmission line at the different frequencies will change the voltage Vin at the input of the ADC 240. These changes in voltage at the different frequencies are used to determine the characteristic impedance ZO of the transmis sion line. The output impedance of the DAC 210 and the input impedance of the ADC 240 are very close to zero, so the measurement circuit 200 may simpli?ed as illustrated in FIG. 2B, where Zl-Z4 are impedances ofthe measurement circuit 200. Since the output impedance ofthe DAC 210 is very close to zero, the output voltage V01” is substantially the same whether or not the transmission line is connected. Therefore, the input voltageVin is measured at different frequencies and is stored in memory as calibration data, e.g., in a calibration ?le. This calibration data is used to calculate the output volt age V according to Equation (1):out To calculate the characteristic impedance ZO of the trans mission line, we notice that the voltageVAB between points A and B may be expressed according to Equation (2): v- (2) vAB = %(Z2 + 23) = vow 3 where the symbol means “parallel to”. Using Equation (1) and renaming Vin to VinCal, Equation (3) is obtained: Vin(ZZ +Zs) : (3) in which the characteristic impedance Z0 is the only unknown. By solving for Z0, Equation (4) is obtained: 20 25 30 35 40 45 50 55 60 65 4 ((Vout — Vin)Z3 — VinZZ — VinZl)Z4 — Vinzlzs — VinZlZZ (Vow — Vin)Z3 — vinZZ — VinZl (4) 20: To simplify, two variables T1 and T2 are assigned according to Equations (5) and (6): TIIVZ-nZi; (5) Using these variables, Equation (4) reduces to Equation (7): _ Tzzt - Tiz3 - T122 (7) Therefore, by measuring the input voltage Vin at different frequencies, the characteristic impedance ZO ofthe transmis sion line may be determined by applying Equation (7). With reference to FIG. 3, the characteristic impedance 310 mea sured according to this method for a standard transmission line including four load coils is in good agreement with the characteristic impedance 320 calculated according to a math ematical model for the same transmission line. The large capacitors at the input are responsible for the angle mismatch at low frequencies. In general, the characteristic impedance of a transmission line may be represented as a transfer function H(z) in poly nomial form, having Q coef?cients bl- and P coef?cients a], according to Equation (8): Q _ (8) Equation (8) may be rewritten in factored form to give Equa tion (9): H =b i. (Z) 0(1— plruu — P2171) (1 — pm) As shown by Equation (9), the numerator of the transfer function H(z) has Q roots qi, which correspond to the zeros of the transfer function H(z). At the zeros, the transfer function H(z), representingthe characteristic impedance Z0, is equal to zero. As also shown by Equation (9), the denominator ofthe transfer function H(z) has P roots pi, which correspond to the poles ofthe transfer function H(z). At the poles, the transfer function H(z), representing the characteristic impedance Z0, is in?nite. Typically, the zeros and poles occur as complex conjugate pairs, i.e., as complex numbers z:a+bi and z:a—bi having real parts a that are equal in magnitude and sign, and imaginary parts b that are equal in magnitude but opposite in sign. For load coil detection, we are interested in the poles ofthe transfer function H(z) in factored form of Equation (9), because the number ofcomplex conjugate pole pairs is equal to the number of load coils in the transmission line. Rather than attempting to ?nd local maxima in the characteristic
  • 15. US 8,917,818 B2 5 impedance, the present invention calculates the impulse response, i.e., the time response, ofthe transmission line from the characteristic impedance and determines the number of complex conjugate poles pairs from the impulse response. As is commonly known, the impulse response of a system is the output signal when the input signal is an impulse. The transfer function of the impulse response describes the rela tion between the input and output signals. Accordingto thepresent invention, the impulse response of the transmission line is, typically, calculated by performing an inverse Fourier transform, e.g., an inverse fast Fourier transform (FFT), on the characteristic impedance. The num ber ofcomplex conjugate pole pairs ofthe transferfunction of the impulse response is then determined. Typically, the transfer function of the impulse response is found by applying a parametric modeling technique to the impulse response.As is commonly known, a parametric mod eling technique ?nds the parameters for a mathematical model describing a system, by using known information about the system. Several suitable parametric modeling tech niques are available for use in the present invention, such as the Prony method, the Levinson-Durbin method, the Yule Walker method, etc. The Prony method is presently preferred as the parametric modeling technique. In general, the parametric modeling technique ?nds the coef?cients bl- and aj ofthe transfer function H(z) in polyno mial form of Equation (8) by using the impulse response. Once the transfer function has been found, a root-?nding algorithm ?nds the poles and the zeros, i.e., the roots pl- and q, ofthe transfer function H(z) in factored form ofEquation (9). Typically, the parametric modeling technique requires ini tial guess values for the number ofpoles P and the number of zeros Q, i.e., the number of coef?cients, ofthe transfer func tion H(z). The guess values for the numbers ofpoles and zeros are selected to be greater than the expected numbers ofpoles and zeros. Typically, the guess values forthe numbers ofpoles and zeros are the same and are greater than the expected number ofpoles, which is two times the expected number of load coils in the transmission line. The expected number of load coils in the transmission line, in turn, may be determined from the length ofthe transmission line, by considering stan dard spacings ofload coils, e.g., a spacing of 6000 ft between load coils, and a spacing of 3000 ft before and after the ?rst and last load coils. Typically, the guess values for the numbers of poles and zeros are selected to be at least two times greater than the expected numbers of poles and zeros, i.e., at least four times greater than the expected number of load coils. For example, if the expected number of load coils in a transmission line is three, the expected number ofpoles is six, i.e., three complex conjugate pole pairs, and the guess values for the numbers of poles and zeros are each selected to be at least 12. The transfer function found by the parametric modeling technique has poles equal in number to the guess value for the number ofpoles. Once the poles ofthe transfer function have been found by the root-?nding algorithm, it is necessary to determine which of the poles are valid. Valid poles occur as complex conjugate pole pairs. Therefore, the number ofcom plex conjugate pairs indicates the number ofload coils in the transmission line. Accordingly, complex conjugate pole pairs are identi?ed among the poles found by the root-?nding algorithm. Poles having an imaginary part b with an absolute magnitude ofless than a ?rst threshold, e.g., |b|<0.08, are not considered fur ther. The remaining poles are identi?ed as complex poles. Complex conjugate pole pairs are then identi?ed among the complex poles by calculating distances between the complex 10 20 25 30 35 40 45 50 55 60 65 6 poles and conjugates of the complex poles. If the absolute distance between a ?rst complex pole Z1 and the conjugate E2 ofa second complex pole is less than a second threshold, e.g., lzl—z2<0.15, the ?rst complex pole Z1 and the second com plex pole z2 are identi?ed as a complex conjugate pole pair. Ideally, the absolute distance should be zero, but in practice it is usually small because ofnoise and limited hardware accu racy. The ?rst and second thresholds are selected by taking prac tical limitations into consideration. Typically, the ?rst and secondthresholds are determined empirically through experi mentation. The complex conjugate pole pairs identi?ed in this manner are considered to be valid poles. The complex conjugate pole pairs are then counted to determine the number of load coils in the transmission line, which is equal to the number of complex conjugate pole pairs. Several examples are provided hereafter to further illus trate the present invention. With reference to FIG. 4, in a ?rst example, the present invention was applied to a 15 000 ft transmission line not including any load coils. The character istic impedance, i.e., the frequency response, ofthe transmis sion line, which is plotted in FIG. 4A, was measured by using the measurement circuit 200 ofFIG. 2. The impulse response of the transmission line, which is plotted in FIG. 4B, was calculated by applying an inverse Fourier transform to the characteristic impedance. The transfer function of the impulse response was found by applying the Prony method to the impulse response. 10 poles ofthe transfer function, which are plotted in FIG. 4C, were found by using a root-?nding algorithm. However, all of the poles were determined to be invalid because they did not belong to valid complex conju gate pole pairs. Therefore, the number of load coils in the transmission line was correctly determined to be zero. It should be noted that the direct current (DC) and very low frequency response could not be detected by the alternating current (AC) coupled hardware and was approximated by extrapolation. Consequently, one pair of poles is close to a valid complex conjugate pole pair, but the absolute distance lzl—zzl is greater than the second threshold. With reference to FIG. 5, in a second example, the present invention was applied to a transmission line including one load coil (LC) at the following spacing: 3000 ft, LC, 3000 ft. The characteristic impedance, i.e., the frequency response, of the transmission line, which is plotted in FIG. 5A, was mea sured by using the measurement circuit 200 of FIG. 2. The impulse response ofthe transmission line, which is plotted in FIG. 5B, was calculated by applying an inverse Fourier trans form to the characteristic impedance. The transfer function of the impulse response was found by applying the Prony method to the impulse response. 10 poles of the transfer function, which are plotted in FIG. 5C, were found by using a root-?nding algorithm. Of these, one pair of poles was determined to be a valid complex conjugate pole pair. There fore, the number of load coils in the transmission line was correctly determined to be one. With reference to FIG. 6, in a third example, the present invention was applied to a transmission line including two loadcoils (LCs) atthe following spacing: 3000 ft, LC, 6000 ft, LC, 3000 ft. The characteristic impedance, i.e., the frequency response, of the transmission line, which is plotted in FIG. 6A, was measured by using the measurement circuit 200 of FIG. 2. The impulse response ofthe transmission line, which is plotted in FIG. 6B, was calculated by applying an inverse Fourier transform to the characteristic impedance. The trans fer function of the impulse response was found by applying the Prony method to the impulse response. 14 poles of the
  • 16. US 8,917,818 B2 7 transfer function, which are plotted in FIG. 6C, were found by using a root-?nding algorithm. Of these, two pairs of poles were determined to be valid complex conjugate pole pairs. Therefore, the number of load coils in the transmission line was correctly determined to be two. With reference to FIG. 7, in a fourth example, the present invention was applied to a transmission line including three load coils (LCs) at the following spacing: 3000 ft, LC, 15 000 ft, LC, 6000 ft, LC, 3000 ft. The characteristic impedance, i.e., the frequency response, ofthe transmission line, which is plotted in FIG. 7A, was measured by using the measurement circuit 200 of FIG. 2. The impulse response of the transmis sion line, which is plotted in FIG. 7B, was calculated by applying an inverse Fourier transform to the characteristic impedance. The transfer function ofthe impulse response was foundby applying the Prony method to the impulse response. 14 poles ofthe transfer function, which are plotted in FIG. 7C, were found by using a root-?nding algorithm. Ofthese, three pairs ofpoles were determined to be valid complex conjugate pole pairs. Therefore, the number of load coils in the trans mission line was correctly determined to be three. With reference to FIG. 8, in a ?fth example, the present invention was applied to a transmission line including four loadcoils (LCs) atthe following spacing: 3000 ft, LC, 6000 ft, LC, 6000 ft, LC, 6000 ft, LC, 3000 ft. The characteristic impedance, i.e., the frequency response, ofthe transmission line, which is plotted in FIG. 8A, was measured by using the measurement circuit 200 of FIG. 2. The impulse response of the transmission line, which is plotted in FIG. 8B, was calcu lated by applying an inverse Fourier transform to the charac teristic impedance. The transfer function of the impulse response was found by applying the Prony method to the impulse response. 14 poles ofthe transfer function, which are plotted in FIG. 8C, were found by using a root-?nding algo rithm. Of these, four pairs of poles were determined to be valid complex conjugate pole pairs. Therefore, the number of load coils in the transmission line was correctly determined to be four. The present invention may be implemented in hardware, software, or a combination thereof. When implemented in software, instructions for carrying out the actions described heretofore are stored in a non-transitory computer-readable storage medium, e.g., memory, and are executed by a proces sor of a hardware device, e.g., a general purpose computer or a test device. With reference to FIG. 9, an exemplary system 900 for determining the number of load coils in a transmission line includes a measurement unit 910 and a processing unit 920. In a preferred embodiment, the system 900 is embodied as a test device, e.g., a portable or ?xed test device, in which the measurement unit 910 and the processing unit 920 are sup ported by a common housing. In other embodiments, the measurement unit 910 may be embodied as a test device, e.g., a portable or ?xed test device, and the processing unit 920 may be embodied as a separate hardware device or as soft ware stored and executed by a separate hardware device, e.g., a general purpose computer. The measurement unit 910 measures the characteristic impedance of the transmission line, typically, by means of a measurement circuit, such as the measurement circuit 200 of FIG. 2 described heretofore. The processing unit 920 calcu lates the impulse response of the transmission line from the characteristic impedance and determines the number ofcom plex conjugate pole pairs of the transfer function of the impulse response, as described heretofore. Thereby, the pro cessing unit 920 determines the number of load coils in the transmission line, which is equal to the number of complex 20 25 30 35 40 45 50 55 60 65 8 conjugate pole pairs. Typically, the number of load coils is reported by the system 900, e.g., on a display. It should be noted that other embodiments of the system may omit the measurement unit, which is optional. Embodi ments omitting the measurement unit are suitably con?gured to receive the characteristic impedance, i.e., frequency-de pendent impedance data, as input. Ofcourse, numerous other embodiments may be envisaged without departing from the spirit and scope of the invention. 1 claim: 1. A method of determining a number of load coils in a transmission line having a characteristic impedance, the method comprising: calculating, using a processing unit, animpulseresponse of the transmission line from the characteristic impedance of the transmission line; and determining, using a processing unit, a number ofcomplex conjugate pole pairs ofa transferfunction ofthe impulse response to thereby determine the number of load coils in the transmission line, wherein the number ofcomplex conjugate pole pairs is equal to the number ofload coils, by: ?nding the transfer function by applying a parametric modeling technique to the impulse response; and ?nding poles of the transfer function by using a root ?nding algorithm, wherein the poles of the transfer function are greater in number than two times an expected number of load coils in the transmission line. 2. The method of claim 1, further comprising: measuring the characteristic impedance of the transmis sion line. 3. The method ofclaim 1, wherein calculating the impulse response includes performing an inverse Fourier transform on the characteristic impedance. 4. The method ofclaim 1, whereinthe parametric modeling technique is the Prony method. 5. A method of determining a number of load coils in a transmission line having a characteristic impedance, the method comprising: calculating, using a processing unit, animpulseresponse of the transmission line from the characteristic impedance of the transmission line; and determining, using a processing unit, a number ofcomplex conjugate pole pairs ofa transferfunction ofthe impulse response to thereby determine the number of load coils in the transmission line, wherein the number ofcomplex conjugate pole pairs is equal to the number ofload coils, ?nding the transfer function by applying a parametric modeling technique to the impulse response; ?nding poles of the transfer function by using a root ?nding algorithm; identifying complex poles among the poles ofthe trans fer function; identifying complex conjugate pole pairs among the complex poles; and counting the complex conjugate pole pairs. 6. The method of claim 5, further comprising: measuring the characteristic impedance of the transmis sion line. 7. The method ofclaim 5, wherein calculating the impulse response includes performing an inverse Fourier transform on the characteristic impedance. 8. The method ofclaim 5, whereinthe parametric modeling technique is the Prony method.
  • 17. US 8,917,818 B2 9. A system for determining a number of load coils in a transmission line having a characteristic impedance, the sys tem comprising: a processing unit for calculating an impulse response ofthe transmission line from the characteristic impedance of the transmission line; and for determining a number of complex conjugate pole pairs of a transfer function of the impulse response to thereby determine the number of load coils in the transmission line, Wherein the number of complex conjugate pole pairs is equal to the number ofload coils, by: ?nding the transfer function by applying a parametric modeling technique to the impulse response; and ?nding poles of the transfer function by using a root ?nding algorithm, Wherein the poles of the transfer function are greater in number than two times an expected number of load coils in the transmission line. 10. The system of claim 9, further comprising: a measurement unit for measuring the characteristic impedance of the transmission line. 11. The system of claim 10, Wherein the system is a por table test device. 12. The system ofclaim 9, Wherein calculating the impulse response includes performing an inverse Fourier transform on the characteristic impedance. 13. The system of claim 9, Wherein the parametric model ing technique is the Prony method. 14. A system for determining a number of load coils in a transmission line having a characteristic impedance, the sys tem comprising: 25 10 a processing unit for calculating an impulse response ofthe transmission line from the characteristic impedance of the transmission line; and for determining a number of complex conjugate pole pairs of a transfer function of the impulse response to thereby determine the number of load coils in the transmission line, Wherein the number of complex conjugate pole pairs is equal to the number of load coils, by: ?nding the transfer function by applying a parametric modeling technique to the impulse response; ?nding poles of the transfer function by using a root ?nding algorithm; identifying complex poles among the poles ofthe trans fer function; identifying complex conjugate pole pairs among the complex poles; and counting the complex conjugate pole pairs. 15. The system of claim 14, further comprising: a measurement unit for measuring the characteristic impedance of the transmission line. 16. The system of claim 15, Wherein the system is a por table test device. 17. The system of claim 14, Wherein calculating the impulse response includes performing an inverse Fourier transform on the characteristic impedance. 18. The system of claim 14, Wherein the parametric mod eling technique is the Prony method. * * * * *