physicsElectromagnetic waves propagate much differently in conductors than they do in dielectrics or in vacuum. If the resistivity of the conductor is sufficiently low (that is, if it is a sufficiently good conductor), the oscillating electric field of the wave gives rise to an oscillating conduction current that is much larger than the displacement current. In this case, the wave equation for an electric field $\vec{E}(x, t)=E_{y}(x, t) \hat{\jmath}$ propagating in the +x-direction within a conductor is
$$
\frac{\partial^{2} E_{y}(x, t)}{\partial x^{2}}=\frac{\mu}{\rho} \frac{\partial E_{y}(x, t)}{\partial t}
$$
where m is the permeability of the conductor and r is its resistivity. (a) A solution to this wave equation is $E_{y}(x, t)=E_{\max } e^{-k C x} \cos \left(k_{C} x-\omega t)\right.$, where $k_{\mathrm{C}}=\sqrt{\omega \mu / 2 \rho}$. Verify this by substituting $E_{y}(x, t)$ into the above wave equation. (b) The exponential term shows that the electric field decreases in amplitude as it propagates. Explain why this happens. (c) Show that the electric-field amplitude decreases by a factor of 1/e in a distance $1 / k_{\mathrm{C}}=\sqrt{2 \rho / \omega \mu}$ and calculate this distance for a radio wave with frequency f = 1.0 MHz in copper (resistivity $1.72 \times 10^{-8} \Omega \cdot \mathrm{m}$; permeability $\mu=\mu_{0}$). Since this distance is so short, electromagnetic waves of this frequency can hardly propagate at all into copper. Instead, they are reflected at the surface of the metal. This is why radio waves cannot penetrate through copper or other metals, and why radio reception is poor inside a metal structure. 9th Edition•ISBN: 9781285530284C Thomas Olivo, Thomas P Olivo609 solutions
9th Edition•ISBN: 9781133010838C Thomas Olivo, Thomas P Olivo609 solutions
5th Edition•ISBN: 9780471406464J.L. Meriam, L.G. Kraige363 solutions
9th Edition•ISBN: 9781435483781 (1 more)C Thomas Olivo, Thomas P Olivo609 solutions
