Standing wave ratio

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In telecommunications, standing wave ratio (SWR) is the ratio of the amplitude of a partial standing wave at an antinode (maximum) to the amplitude at an adjacent node (minimum), in an electrical transmission line.

The SWR is usually defined as a voltage ratio called the VSWR, (sometimes pronounced "viswar"[1] [2]), for voltage standing wave ratio. For example, the VSWR value 1.2:1 denotes a maximum standing wave amplitude that is 1.2 times greater than the minimum standing wave value. It is also possible to define the SWR in terms of current, resulting in the ISWR, which has the same numerical value. The power standing wave ratio (PSWR) is defined as the square of the VSWR. To avoid confusion, wherever SWR is used without modification in this article, assume it is referring to the VSWR.

SWR is used as an efficiency measure for transmission lines, electrical cables that conduct radio frequency signals, used for purposes such as connecting radio transmitters and receivers with their antennas, and distributing cable television signals. A problem with transmission lines is that impedance mismatches in the cable tend to reflect the radio waves back toward the source end of the cable, preventing all the power from reaching the destination end. SWR measures the relative size of these reflections. An ideal transmission line would have an SWR of 1:1, with all the power reaching the destination and none of the power reflected back. An infinite SWR represents complete reflection, with all the power reflected back down the cable. The SWR of a transmission line can be measured with an instrument called an SWR meter, and checking the SWR is a standard part of installing and maintaining transmission lines.

Relationship to the reflection coefficient[edit]

The voltage component of a standing wave in a uniform transmission line consists of the forward wave (with amplitude V_f) superimposed on the reflected wave (with amplitude V_r).

Reflections occur as a result of discontinuities, such as an imperfection in an otherwise uniform transmission line, or when a transmission line is terminated with other than its characteristic impedance. The reflection coefficient \Gamma is defined thus:

\Gamma = {V_r \over V_f}.

\Gamma is a complex number that describes both the magnitude and the phase shift of the reflection. The simplest cases, when the imaginary part of \Gamma is zero, are:

For the calculation of SWR, only the magnitude of \Gamma, denoted by \rho, is of interest. Therefore, we define

\rho =  | \Gamma | .

At some points along the line the two waves interfere constructively, and the resulting amplitude V_\max is the sum of their amplitudes:

V_\max = V_f + V_r = V_f + \rho V_f = V_f (1 + \rho).\,

At other points, the waves interfere destructively, and the resulting amplitude V_\min is the difference between their amplitudes:

V_\min = V_f - V_r = V_f - \rho V_f = V_f ( 1 - \rho).\,

The voltage standing wave ratio is then equal to:

VSWR = {V_\max \over V_\min} = {{1 + \rho} \over {1 - \rho}}.

As \rho, the magnitude of \Gamma, always falls in the range [0,1], the SWR is always ≥ +1.

The SWR can also be defined as the ratio of the maximum amplitude of the electric field strength to its minimum amplitude, E_\max/E_\min.

Since power is proportional to V2, VSWR can be expressed in terms of forward and reflected power as follows:

 \frac {P_r}{P_f} = \left ( \frac {VSWR - 1}{VSWR + 1} \right )^2

Further analysis[edit]

If the standing waves are only the result of a mismatch between the characteristic impedance and load impedance of the line, the VSWR can be expressed as one of the two equations below (pick the one that gives a value greater than 1):

VSWR = \frac{Z_\text{0}}{R_\text{L}}       or       VSWR = \frac{R_\text{L}}{Z_\text{0}}

To understand the standing wave ratio in detail, we need to calculate the voltage (or, equivalently, the electrical field strength) at any point along the transmission line at any moment in time. We can begin with the forward wave, whose voltage as a function of time t and of distance x along the transmission line is:

V_f(x,t) = A \sin (\omega t - kx),\,

where A is the amplitude of the forward wave, ω is its angular frequency and k is the wave number (equal to ω divided by the speed of the wave). The voltage of the reflected wave is a similar function, but spatially reversed (the sign of x is inverted) and attenuated by the reflection coefficient ρ:

V_r(x,t) = \rho A \sin (\omega t + kx).\,

The total voltage V_t on the transmission line is given by the superposition principle, which is just a matter of adding the two waves:

V_t(x,t) = A \sin (\omega t - kx) + \rho A \sin (\omega t + kx).\,

Using standard trigonometric identities, this equation can be converted to the following form:

V_t(x,t) = A \sqrt {4\rho\cos^2 kx+(1-\rho)^2} \cos(\omega t + \phi),\,

where {\tan \phi}={{(1+\rho)}\over{(1-\rho)}}\cot(kx).

This form of the equation shows, if we ignore some of the details, that the maximum voltage over time Vmot at a distance x from the transmitter is the periodic function

V_\mathrm{mot} = A \sqrt {4\rho\cos^2 kx+(1-\rho)^2}.

This varies with x from a minimum of A(1-\rho) to a maximum of A(1+\rho), as we saw in the earlier, simplified discussion. A graph of V_\mathrm{mot} against kx, for a range of ρ, is shown below. The maximum and minimum of Vmot in a period are V_\min and V_\max and are the values used to calculate the SWR.

Standing wave ratio for a range of ρ. In this graph, A and k are set to unity.

Note that this graph does not show the instantaneous voltage profile, Vt(x,t), along the transmission line. It only shows Vt(x) or the voltage amplitude as a function of space at a single point in time. The instantaneous voltage is a function of both time and distance, so could only be shown fully by a three-dimensional or animated graph.

Practical implications of SWR[edit]

The most common case for measuring and examining SWR is when installing and tuning transmitting antennas. When a transmitter is connected to an antenna by a feed line, the impedance of the antenna and feed line must match exactly for maximum energy transfer from the feed line to the antenna to be possible. The impedance of the antenna varies based on many factors including: the antenna's natural resonance at the frequency being transmitted, the antenna's height above the ground, and the size of the conductors used to construct the antenna.[3]

When an antenna and feedline do not have matching impedances, some of the electrical energy cannot be transferred from the feedline to the antenna.[4] Energy not transferred to the antenna is reflected back towards the transmitter.[5] It is the interaction of these reflected waves with forward waves which causes standing wave patterns.[4] Reflected power has three main implications in radio transmitters: Radio Frequency (RF) energy losses increase, distortion on transmitter due to reflected power from load[4] and damage to the transmitter can occur.[6]

Matching the impedance of the antenna to the impedance of the feed line is typically done using an antenna tuner. The tuner can be installed between the transmitter and the feed line, or between the feed line and the antenna. Both installation methods will allow the transmitter to operate at a low SWR, however if the tuner is installed at the transmitter, the feed line between the tuner and the antenna will still operate with a high SWR, causing additional RF energy to be lost through the feedline.

Feed line loss typically increases with frequency. For example, a dipole antenna tuned to operate at 3.75 MHz—the center of the 80 meter amateur radio band—will exhibit an SWR of about 6:1 at the edges of the band. If the antenna is fed with 250 feet of RG-8A coax, the loss due to standing waves is 2.2dB. The same 6:1 mismatch to 250 feet of RG-8A coax would incur 10.8dB of loss at 146 MHz.[4] Thus, a better match of the antenna to the feedline, that is, a lower SWR, becomes increasingly important with increasing frequency.

Implications of SWR on medical applications[edit]

SWR can also have a detrimental impact upon the performance of microwave based medical applications. In microwave electrosurgery an antenna that is placed directly into tissue may not always have an optimal match with the feedline resulting in an SWR. The presence of SWR can affect monitoring components used to measure power levels impacting the reliability of such measurements.[7]

See also[edit]


  1. ^ Knott, Eugene F.; Shaeffer, John F.; Tuley, Michael T. (2004). Radar cross section. SciTech Radar and Defense Series (2nd ed.). SciTech Publishing. p. 374. ISBN 978-1-891121-25-8. 
  2. ^ Schaub, Keith B.; Kelly, Joe (2004). Production testing of RF and system-on-a-chip devices for wireless communications. Artech House microwave library. Artech House. p. 93. ISBN 978-1-58053-692-9. 
  3. ^ Hutchinson, Chuck, ed. (2000). The ARRL Handbook for Radio Amateurs 2001. Newington, CT: ARRL—the national association for Amateur Radio. p. 20.2. ISBN 0-87259-186-7. 
  4. ^ a b c d Hutchinson, Chuck, ed. (2000). The ARRL Handbook for Radio Amateurs 2001. Newington, CT: ARRL—the national association for Amateur Radio. pp. 19.4–19.6. ISBN 0-87259-186-7. 
  5. ^ Ford, Steve (April 1997). "The SWR Obsession" (PDF). QST (Newington, CT: ARRL—The national association for Amateur Radio) 78 (4): 70–72. Retrieved 2008-09-26. 
  6. ^ Hutchinson, Chuck, ed. (2000). The ARRL Handbook for Radio Amateurs 2001. Newington, CT: ARRL—the national association for Amateur Radio. p. 19.13. ISBN 0-87259-186-7. 
  7. ^ "Problems with VSWR in medical applications". 

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