The **propagation constant** of an electromagnetic wave is a measure of the change undergone by the amplitude of the wave as it propagates in a given direction. The quantity being measured can be the voltage or current in a circuit or a field vector such as electric field strength or flux density. The propagation constant itself measures change per metre but is otherwise dimensionless.

The propagation constant is expressed logarithmically, almost universally to the base e, rather than the more usual base 10 used in telecommunications in other situations. The quantity measured, such as voltage, is expressed as a sinusiodal phasor. The phase of the sinusoid varies with distance which results in the propagation constant being a complex number, the imaginary part being caused by the phase change.

### Alternative namesEdit

The term propagation constant is somewhat of a misnomer as it usually varies strongly with *ω*. It is probably the most widely used term but there are a large variety of alternative names used by various authors for this quantity. These include, **transmission parameter**, **transmission function**, **propagation parameter**, **propagation coefficient** and **transmission constant**. In plural, it is usually implied that *α* and *β* are being referenced separately but collectively as in **transmission parameters**, **propagation parameters**, **propagation coefficients**, **transmission constants** and **secondary coefficients**. This last occurs in transmission line theory, the term *secondary* being used to contrast to the *primary line coefficients*. The primary coefficients being the physical properties of the line; R,C,L and G, from which the secondary coefficients may be derived using the telegrapher's equation. Note that, at least in the field of transmission lines, the term transmission coefficient has a different meaning despite the similarity of name. Here it is the corollary of reflection coefficient.

### DefinitionEdit

The propagation constant, symbol γ, for a given system is defined by the ratio of the amplitude at the source of the wave to the amplitude at some distance *x*, such that,

- $ \frac{A_0}{A_x}=e^{\gamma x} $

Since the propagation constant, is a complex quantity we can write;

- $ \gamma = \alpha +i \beta \, $

where

- α, the real part, is called the attenuation constant
- β, the imaginary part, is called the phase constant

That β does indeed represent phase can be seen from Euler's formula;

- $ e^{i\theta}=\cos{\theta}+i\sin{\theta}\,\! $

which is a sinusoid which varies in phase as θ varies but does not vary in amplitude because;

- $ \left|e^{i\theta}\right|=\sqrt{\cos^2{\theta}+\sin^2{\theta}}=1 $

The reason for the use of base e is also now made clear. The imaginary phase constant, iβ, can be added directly to the attenuation constant, α, to form a single complex number that can be handled in one mathematical operation provided they are to the same base. Angles measured in radians require base e, so the attenuation is likewise in base e.

For a copper transmission line, the propagation constant can be calcualted from the primary line coefficients by means of the relationship;

- $ \gamma=\sqrt{ZY} $

where;

- $ Z=R+i\omega L\,\! $, the series impedance of the line per metre and,

- $ Y=G+i\omega C\,\! $, the shunt admittance of the line per metre.

## Attenuation constantEdit

In telecommunications, the term **attenuation constant**, also called **attenuation parameter** or **coefficient**, is the attenuation of an electromagnetic wave propagating through a medium per unit distance from the source. It is the real part of the propagation constant and is measured in nepers per metre. A neper is approximately 8.7dB. Attenuation constant can be defined by the amplitude ratio;

- $ \left|\frac{A_0}{A_x}\right|=e^{\alpha} $

### Copper linesEdit

The attenuation constant can be calculated from the primary line coefficients as shown above. For a line meeting the distortionless condition, the attenuation constant is given by;

- $ \alpha=\sqrt{RG}\,\! $

however, a real line is unlikely to meet this condition without the addition of loading coils and, furthermore, there are some decidedly non-linear effects operation on the primary "constants" which cause a frequency dependence of the loss. There are two main components to these losses, the metal loss and the dielectric loss.

The loss of most transmission lines are dominated by the metal loss, which causes a frequency dependency due to finite conductivity of metals, and the skin effect. The skin effect causes R to be approximately dependent on frequency according to;

- $ R \propto \sqrt{\omega} $

Losses in the dielectric depend on the loss tangent ($ {tan \delta} $) of the material, which depends inversely on the wavelength of the signal and is directly proportional to the frequency.

- $ \alpha_d={{\pi}\sqrt{\varepsilon_r}\over{\lambda}}{\tan \delta} $

### Optical fibreEdit

The attenuation constant for a particular propagation mode in an optical fiber, the real part of the axial propagation constant.

## Phase constantEdit

In electromagnetic theory, the **phase constant**, also called **phase change constant**, **parameter** or **coefficient** is the imaginary component of the propagation constant for a plane wave. It represents the change in phase per metre along the path travelled by the wave at any instant and is equal to the angular wavenumber (often incorrectly abbreviated to wavenumber) of the wave. It is represented by the symbol β and is measured in units of radians per metre.

From the definition of angular wavenumber;

- $ k = \frac{2\pi}{\lambda} = \beta $

For a transmission line, the Heaviside condition of the telegrapher's equation tells us that the wavenumber must be proportional to frequency for the transmission of the wave to be undistorted in the time domain. This includes, but is not limited to, the ideal case of a lossless line. The reason for this condition can be seen by considering that a useful signal is composed of many different wavelengths in the frequency domain. For there to be no distortion of the waveform, all these waves must travel at the same velocity so that they arrive at the far end of the line at the same time as a group. Since wave phase velocity is given by;

- $ v_p=\frac{\lambda}{T}=\frac{f}{\tilde{\nu}}=\frac{\omega}{\beta} $

it is proved that β is required to be proportional to ω. In terms of primary coefficients of the line, this yields from the telegrapher's equation for a distortionless line the condition;

- $ \beta = \omega \sqrt{LC} $

However, practical lines can only be expected to approximately meet this condition over a limited frequency band.

## FiltersEdit

The term propagation constant or propagation function is applied to filters and other two-port networks used for signal processing. In these cases, however, the attenuation and phase coefficients are expressed in terms of nepers and radians per network section rather than per metre. Some authors^{[1]} make a distinction between per metre measures (for which "constant" is used) and per section measures (for which "function" is used).

The propagation constant is a useful concept in filter design which invariably uses a cascaded section topology. In a cascaded topology, the propagation constant, attenuation constant and phase constant of individual sections may be simply added to find the total propagation constant etc.

## Cascaded networksEdit

As input and output impedences are equal under z_{o} termination
ie, z_{o} termination = V_{1}/I_{1} = V_{2}/(-I_{2})

V_{1}/V_{2}= I_{1}/I_{2}= e^{γ}

For 'n' number of sections cascaded' with all of them having the same z_{o} value' the ratio of currents can be written as

(I _{1}/ -I _{2}) × (-I _{2} / -I _{3}) × ..... × (-I _{n-1} / -I _{n}) = (I _{1} / -I _{n})

=> e^{γ1} × e^{γ2} × ... × = e^{γ}

The over all propagation constant
γ = γ_{1}+γ_{2}+....+γ_{n}

## NotesEdit

## ReferencesEdit

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