A transmission line consists of two parallel wires, of radius \(a\) and separation \(b,\) carrying uniform linear charge densities \(\pm \lambda\), respectively. With \(a \ll b\), their electric field is the superposition of the fields from two long straight lines of charge. Find the capacitance per unit length for this transmission line.

Short Answer

Expert verified
The capacitance of the transmission line per unit length is \(\pi\epsilon_0\).

Step by step solution

01

Compute the Electric Field

Recognize that the electric field \(E\) for a long line of uniform charge is given by \(E = \frac{\lambda}{2\pi\epsilon_0r}\), where \(r\) is the distance from the charge, \(\lambda\) is the linear charge density, and \(\epsilon_0\) is the permittivity of free space. Here, since there are two wires with charges \(\pm\lambda\) respectively, the electric field between the wires is the superposition of their individual electric fields. Since the charges are opposite and the field lines are in opposite directions, the resultant electric field in between the wires becomes \(E = \frac{\lambda}{\pi\epsilon_0 b}\).
02

Compute Potential Difference

The electric field \(E\) between the plates relates to the potential difference \(V\) between them by the equation \(E = \frac{V}{d}\), where \(d\) represents the separation between the charge distributions, which is \(b\) here. Solving for \(V\) gives \(V = E*b = \frac{\lambda b}{\pi\epsilon_0 b}\), the \(b\) cancels out and we get \(V= \frac{\lambda }{\pi\epsilon_0} \).
03

Compute the Capacitance

Capacitance \(C\) relates to charge \(Q\) and potential difference \(V\) by \(C = \frac{Q}{V}\). Here, \(Q = \lambda * l\), where \(l\) is the length of the transmission line per unit length. Hence substituting \(Q\) and \(V\) into the capacitance formula gives \(C = \frac{\lambda l}{\frac{\lambda }{\pi\epsilon_0}}\), with cancelling terms this simplifies to \(C= \pi\epsilon_0 \) per unit length.

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