2.) Electric current in a long, insulated cable: Suppose we have an insulated wire with current i = i(x, t) and voltage E = E(x, t). Let R be the resistance, L be the inductance, C be the capacitance...


2.) Electric current in a long, insulated cable: Suppose we have an insulated wire with current i =<br>i(x, t) and voltage E = E(x, t). Let R be the resistance, L be the inductance, C be the<br>capacitance and G be the conductance (or leakage), all per unit length and all constant, of the<br>wire. It can be shown that both i and E satisfy the telegraph equation:<br>Ux = LCu + (RC + LG)u, + RGu.<br>If we may neglect L and G, we see that i and E can be simplified to:<br>Ux = RCu,<br>Derive the simple implicit finite difference parabolic equation for the simplified telegraph<br>equation and explain the derivation steps.<br>

Extracted text: 2.) Electric current in a long, insulated cable: Suppose we have an insulated wire with current i = i(x, t) and voltage E = E(x, t). Let R be the resistance, L be the inductance, C be the capacitance and G be the conductance (or leakage), all per unit length and all constant, of the wire. It can be shown that both i and E satisfy the telegraph equation: Ux = LCu + (RC + LG)u, + RGu. If we may neglect L and G, we see that i and E can be simplified to: Ux = RCu, Derive the simple implicit finite difference parabolic equation for the simplified telegraph equation and explain the derivation steps.

Jun 11, 2022
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