Talk:Travelling Wave Line Model

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Footnotes

Derivation of Voltage Equation

The general solution to the transmission line wave equations are:

Where is the velocity of propagation (m/s).

and are arbitrary current functions of time.
and are arbitrary voltage functions of time.

The Laplace Transform of the above equations are:

... Equ. (1)
... Equ. (2)

Recall the Telegrapher's equation for current:

Taking the Laplace Transform of this equation, we get:

... Equ. (3)

Substituting Equations (1) and (2) into Equ. (3):

We can differentiate the left-hand side:

Equating the and terms on both sides, we get the following pair of equations:

Solving for voltage yields the following:

... Equ. (4)
... Equ. (5)

Where is the characteristic impedance (Ohms)

We can use the above equations to re-write the voltage equation of Equ. (2) in terms of current as follows:

Finally, taking the inverse Laplace Transform of the equation above, we get: