THE WHATIS.COM WORD-OF-THE-DAY   
September 24, 2002

standing-wave ratio 
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TODAY'S WORD: standing-wave ratio 

See our definition with hyperlinks at 
http://whatis.techtarget.com/definition/0,,sid9_gci852555,00.html 

Standing-wave ratio (SWR) is a mathematical expression of the
non-uniformity of an electromagnetic field (EM field) on a
transmission line such as coaxial cable. Usually, SWR is defined as
the ratio of the maximum radio-frequency (RF) voltage to the minimum
RF voltage along the line. This is also known as the voltage
standing-wave ratio (VSWR). The SWR can also be defined as the ratio
of the maximum RF current to the minimum RF current on the line
(current standing-wave ratio or ISWR). For most practical purposes,
ISWR is the same as VSWR. 

Under ideal conditions, the RF voltage on a signal transmission line
is the same at all points on the line, neglecting power losses caused
by electrical resistance in the line wires and imperfections in the
dielectric material separating the line conductors. The ideal VSWR is
therefore 1:1. (Often the SWR value is written simply in terms of the
first number, or numerator, of the ratio because the second number,
or denominator, is always 1.) When the VSWR is 1, the ISWR is also 1.
This optimum condition can exist only when the load (such as an
antenna or a wireless receiver), into which RF power is delivered,
has an impedance identical to the impedance of the transmission line.
This means that the load resistance must be the same as the
characteristic impedance of the transmission line, and the load must
contain no reactance (that is, the load must be free of inductance or
capacitance). In any other situation, the voltage and current
fluctuate at various points along the line, and the SWR is not 1. 

When the line and load impedances are identical and the SWR is 1, all
of the RF power that reaches a load from a transmission line is
utilized by that load. When the load is an antenna, the utilization
takes the form of EM-field radiation. If the load is a communications
receiver or terminal, the signal power is converted into some other
form, such as an audio-visual display. If the impedance of the load
is not identical to the impedance of the transmission line, the load
does not absorb all the RF power (called forward power) that reaches
it. Instead, some of the RF power is sent back toward the signal
source when the signal reaches the point where the line is connected
to the load. This is known as reflected power or reverse power. 

The presence of reflected power, along with the forward power, sets
up a pattern of voltage maxima (loops) and minima (nodes) on the
transmission line. The same thing happens with the distribution of
current. The SWR is the ratio of the RF voltage at a loop to the RF
voltage at a node, or the ratio of the RF current at a loop to the RF
current at a node. In theory, there is no limit to how high this
ratio can get. The worst cases (highest SWR values) occur when there
is no load connected to the end of the line. This condition, known as
an unterminated transmission line, is manifested when the end of the
line is either short-circuited or left open. In theory, the SWR is
infinite in either of these cases; in practice, it is limited by line
losses, but can exceed 100. This can give rise to extreme voltages
and currents at certain points on the line. 

The SWR on a transmission line is mathematically related to (but not
the same as) the ratio of reflected power to forward power. In
general, the higher the ratio of reflected power to forward power,
the greater is the SWR. The converse is also true. When the SWR on a
transmission line is high, the power loss in the line is greater than
the loss that occurs when the SWR is 1. This exaggerated loss, known
as SWR loss, can be significant, especially when the SWR exceeds 2
and the transmission line has significant loss to begin with. For
this reason, RF engineers strive to minimize the SWR on
communications transmission lines. A high SWR can have other
undesirable effects, too, such as transmission-line overheating or
breakdown of the dielectric material separating the line conductors. 
In some situations, such as those encountered at relatively low RF
frequencies, low RF power levels, and short lengths of low-loss
transmission line

RELATED TERMS:

electromagnetic field 
http://whatis.techtarget.com/definition/0,,sid9_gci212055,00.html 

radio frequency
http://searchnetworking.techtarget.com/sDefinition/0,,sid7_gci214263,00.html

voltage
http://whatis.techtarget.com/definition/0,,sid9_gci213320,00.html

current
http://whatis.techtarget.com/definition/0,,sid9_gci211871,00.html

resistance
http://whatis.techtarget.com/definition/0,,sid9_gci212894,00.html

dielectric material
http://whatis.techtarget.com/definition/0,,sid9_gci211945,00.html 

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SELECTED LINKS:

Allen D. Kass provides an online program for calculating SWR in terms
of forward and reflected power. 
http://www.tl.infi.net/~allenk/vswr.html 

______________________
THIS DAY IN IT HISTORY | September 24, 1990 

SONY announces it will begin selling digital audio tape (DAT)
players. 
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