How Do We Derive the Transmission Line Equations Using Differential Methods?

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SUMMARY

The discussion focuses on deriving the transmission line equations using differential methods, specifically through the substitution of Equation (2.5) into Equations (2.1) and (2.2). The key equations are: Eqn. (2.1) ∂v/∂z = -L ∂i/∂t, Eqn. (2.2) ∂i/∂z = -C ∂v/∂t, and Eqn. (2.5) v(z,t) = V^+f(t - z/v_p) + V^-f(t + z/v_p). The derivation leads to the current expression i(z,t) = (V^+/Z_0)f(t - z/v_p) + (V^-/Z_0)f(t + z/v_p), confirming that the current and voltage share a similar functional form. The phase velocity is established as v_p = 1/√(LC).

PREREQUISITES
  • Understanding of partial differential equations (PDEs)
  • Familiarity with transmission line theory
  • Knowledge of the concepts of inductance (L) and capacitance (C)
  • Ability to differentiate functions with respect to multiple variables
NEXT STEPS
  • Study the derivation of wave equations from transmission line equations
  • Learn about the physical significance of phase velocity in transmission lines
  • Explore the implications of boundary conditions on transmission line behavior
  • Investigate the applications of transmission line theory in electrical engineering
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Electrical engineers, physics students, and researchers interested in transmission line theory and differential methods in electromagnetism.

yayscience
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Eqn. (2.1)
\frac{\partial v}{\partial z} = -L \frac{\partial i}{\partial t}
Eqn. (2.2)
\frac{\partial i}{\partial z} = -C \frac{\partial v}{\partial t}
Eqn. (2.5)
v(z,t)=V^+f(t-\frac{z}{v_p})+V^-f(t+\frac{z}{v_p})

From the book I'm reading:
"By substituting Equation (2.5) into Equations (2.1) and (2.2), we
determine that the current has the form:"
i(z,t)=\frac{V^+}{Z_0}f(t-\frac{z}{v_p})+\frac{V^-}{Z_0}f(t+\frac{z}{v_p})

So, I've seen this derivation about four different ways, and I know this is the result, but I can't see what moves I need to substitute 2.5 into 2.1 and 2.2 to get 2.5. Can someone please enlighten me? Thanks all!
 
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yayscience said:
Eqn. (2.1)
\frac{\partial v}{\partial z} = -L \frac{\partial i}{\partial t}
Eqn. (2.2)
\frac{\partial i}{\partial z} = -C \frac{\partial v}{\partial t}
Eqn. (2.5)
v(z,t)=V^+f(t-\frac{z}{v_p})+V^-f(t+\frac{z}{v_p})

From the book I'm reading:
"By substituting Equation (2.5) into Equations (2.1) and (2.2), we
determine that the current has the form:"
i(z,t)=\frac{V^+}{Z_0}f(t-\frac{z}{v_p})+\frac{V^-}{Z_0}f(t+\frac{z}{v_p})

So, I've seen this derivation about four different ways, and I know this is the result, but I can't see what moves I need to substitute 2.5 into 2.1 and 2.2 to get 2.5. Can someone please enlighten me? Thanks all!

Just some preliminaries first. If you differentiate 2.1 wrt "t" and 2.2 wrt "z" (and then repeat the other way around) you get the following second order PDE's.

\frac{\partial^2 v}{\partial z^2} = L C \frac{\partial^2 v}{\partial t^2}

\frac{\partial^2 i}{\partial z^2} = L C \frac{\partial^2 i}{\partial t^2}

These separable PDE's give the motivation for the form given in 2.5 and tell us that the phase velocity is:

v_p = \frac{1}{\sqrt{L C}}


Since the above second order PDE's tell us that i(z,t) will be in the same form as v(z,t) we can therefore write:

i(z,t)=I^+ \, f(t-\frac{z}{v_p})+I^- \, f(t+\frac{z}{v_p})

By differentiating the above wrt "t" and differentiating 2.5 wrt "z" and substituting into 2.1 we can equate coefficients to show the following:

I+ = \frac{V^+}{L v_p} = \frac{V^+}{Z_0}

I- = - \frac{V^-}{L v_p} = - \frac{V^-}{Z_0}

Hope that helps.
 

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