reflection coefficient
coefficient of reflection

The reflection coefficient is often thought of as a correction factor.

Note that if the reflection coefficient is zero, the process becomes much easier.

For common glass, the reflection coefficient is about 4%.

The reflection coefficient may also be established using other field or circuit quantities.

They also relate the transmission and reflection coefficients for the interaction.

Note: should not be confused with albedo or reflection coefficient.

In this energy range the transmission and reflection coefficient differ from the classical case.

This assumes a limited number of reflection coefficients, with larger amplitude.

The reflection coefficient is displayed graphically using a Smith chart.

Reflection coefficient is used in feeder testing for reliability of medium.

That is, return loss with a negative sign is more properly called reflection coefficient.

However, to completely characterise the reflection coefficient, the phase of ρ must also be found.

Reflection coefficients can be read directly from the chart as they are unitless parameters.

The degrees scale represents the angle of the voltage reflection coefficient at that point.

The reflection coefficient is closely related to the transmission coefficient.

Note that as the reflection coefficient approaches zero, power to the load is maximized.

Now the reflection coefficients are very large and more power is reaching the load than was injected in the input port.

This is correct for reflection coefficients with a magnitude no greater than unity, which is usually the case.

Real coatings do not reach perfect performance, though they are capable of reducing a surface's reflection coefficient to less than 0.1%.

In optics, intensity and amplitude reflection coefficients are used.

Here it is the corollary of reflection coefficient.

The low reflection coefficient means better measurement accuracy.

The Fresnel reflection coefficient between layer n and n+1 is then given by:

Mathematically this means that the Fresnel reflection coefficient becomes a complex rather than a real number.

Voltage reflection coefficients on opposite sides of the boundary have opposite signs.