Article View: sci.electronics
Article #9806Re: Telephone Lines
From: Larry Lippman
Date: Tue, 29 Jan 1991 05:09
Date: Tue, 29 Jan 1991 05:09
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In article <1991Jan26.163014.1986@athena.cs.uga.edu>, mcovingt@athena.cs.uga.edu (Michael A. Covington) writes:
> >While in a meeting, one technical "guru" declared that my statement was wrong
> >when I said that a telephone was a form of transmission line. The "guru"
> >declared that, not only was I totally wrong, but that he and a senior
> >engineer in the company had "proven" that a telephone line was not a
> >transmission line nor could it be modelled as such. So, is a telephone line
> > a form of transmission line or am I totally wrong as this "guru" declared?
With respect to the original author's article, this alleged "guru"
doesn't seem to know much about the definition of a "transmission line"!
> It certainly is a transmission line; in fact, long phone lines have
> 88-mH inductors inserted into them periodically to keep the transmission
> line impedance closer to 600 ohms (which is the source impedance of a
> telephone set).
A non-loaded transmission line of sufficient length does a nice job
of establishing a characteristic impedance (Zo) at a given frequency *without*
the use of series inductors (loading coils). The purpose of loading coils
is to "counteract" the effect of distributed capacitance and reduce the
insertion loss at frequencies below 3,000 Hz. A loaded transmission line
has a comparatively flat curve of insertion loss -vs- frequency up to a
cutoff frequency determined by the loading design and cable characteristcs.
Such a cutoff frequency is usually between 3,000 and 3,500 Hz.
It is important to understand that Zo of a telephone transmission
varies with the frequency. The impedance specification commonly used in
communication apparatus generally refers to a frequency of 1 kHz.
It is also important to realize that Zo from an equipment design
standpoint is merely a *compromise*, represents an engineering guideline,
and is not some magic absolute figure.
Non-loaded telephone transmission lines are generally considered
to have a Zo of 600 ohms @ 1 kHz. More specifcally, 22 AWG cable has a
Zo of around 560 ohms, and 24 AWG cable has a Zo of around 760 ohms. The
finer the gauge, the higher the Zo (which should suprise no one).
Loaded telephone transmission lines for voice frequency service
are generally considered to have a Zo of 900 ohms @ 1 kHz with H-88 loading
which uses 88 mH loading coils space every 6,000 feet. More specifcally,
22 AWG cable with H-88 loading has a Zo of around 1,050 ohms, and 24 AWG
cable with H-88 loading has a Zo of around 1,080 ohms. Note the small
difference in Zo between the same wire gauges loaded versus the larger
difference unloaded. 26 AWG cable with H-88 loading has a Zo of around
1,170 ohms, which is why some subscriber loop apparatus, such as 2W/4W
terminating sets, is also available in a 1,200 ohm impedance.
Larry Lippman @ Recognition Research Corp. "Have you hugged your cat today?"
VOICE: 716/688-1231 {boulder, rutgers, watmath}!ub!kitty!larry
FAX: 716/741-9635 [note: ub=acsu.buffalo.edu] uunet!/ \aerion!larry
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Path: arc1-ca.pugleaf.net!utzoo!utgpu!news-server.csri.toronto.edu!cs.utexas.edu!swrinde!zaphod.mps.ohio-state.edu!ub!kitty!larry From: larry@kitty.UUCP (Larry Lippman) Newsgroups: sci.electronics Subject: Re: Telephone Lines Summary: Characteristic impedance of telephone lines Message-ID: <4651@kitty.UUCP> Date: 29 Jan 91 05:09:31 GMT References: <4574@mindlink.UUCP> <1991Jan26.163014.1986@athena.cs.uga.edu> Organization: Recognition Research Corp., Clarence, NY Lines: 51