The frequency-domain form of the Terminating Impedance boundary condition is derived from the current flowing through the load impedance, as is shown in
Equation 4-9. The time derivative of
Equation 4-9 reads
To derive the Absorbing Boundary boundary condition, the load impedance in
Equation 4-10 is replaced by the characteristic impedance. This results in the frequency-domain form of the
Absorbing Boundary condition:
Equation 4-17 can be expressed in terms of the propagation constant as
where the propagation constant is
. In order to derive the time-domain form of Equation 4-18, it is required to perform the Taylor series expansion of the propagation constant. The resulting Taylor series of the corresponding products of
γ are given by
In the case when R and
G are very small, the higher-order terms can be neglected and the propagation constant simplifies to
In the The Transmission Line Interface, the
Lumped Port boundary condition (for a Cable lumped port) reads as
Substituting
in Equation 4-24, gives the time-domain form of the
Lumped Port boundary condition:
In the case of current Lumped Port, the time-domain boundary condition can be evaluated from
Equation 4-11 as
For a current type lumped port, Iin is the terminal current and is an input parameter.