Maxwell's Equations β€” Question 4

Section 32-4 Β· Physics pages 5238–5239

Question 4 A longitudinal electric traveling pattern requires sources A proposed field is E = E0 cos(kx βˆ’Ο‰t)Λ†x and B = 0. Treat it as a local prescribed pattern in vacuum. x Ex Schematic; labels, not drawing lengths, specify the data. (a) Find the charge and current densities required by Maxwell equations. (b) Check continuity and decide whether the pattern can be a source-free vacuum wave.
Show solutionHide solution
Question 4 - Solution A longitudinal electric traveling pattern requires sources x Ex (a) Method and calculation ρ = Ο΅0βˆ‡Β· E = βˆ’Ο΅0kE0 sin(kx βˆ’Ο‰t). Jx = βˆ’Ο΅0βˆ‚tEx = βˆ’Ο΅0Ο‰E0 sin(kx βˆ’Ο‰t) . (b) Interpretation and further calculation βˆ‚tρ = Ο΅0kΟ‰E0 cos(kx βˆ’Ο‰t), βˆ‚xJx = βˆ’Ο΅0kΟ‰E0 cos(kx βˆ’Ο‰t). ˙ρ + βˆ‡Β· J = 0; ρ, JΜΈ = 0 in general . Physical check Mathematical time dependence alone does not make a field a source-free electromagnetic wave.

Question 4

A longitudinal electric traveling pattern requires sources

A proposed field is 𝑬=E0cos⁡(kxβˆ’Ο‰t)xΜ‚\mathbf E=E_0\cos(kx-\omega t)\hat x and 𝑩=0\mathbf B=0. Treat it as a local prescribed pattern in vacuum.

Diagram shown in the original SVG worksheet.

  1. Find the charge and current densities required by Maxwell equations.

  2. Check continuity and decide whether the pattern can be a source-free vacuum wave.

Question 4 - Solution

A longitudinal electric traveling pattern requires sources

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ρ=Ο΅0βˆ‡β‹…π‘¬=βˆ’Ο΅0kE0sin⁡(kxβˆ’Ο‰t).\rho=\epsilon_0\nabla\cdot\mathbf E=-\epsilon_0kE_0\sin(kx-\omega t).Jx=βˆ’Ο΅0βˆ‚tEx=βˆ’Ο΅0Ο‰E0sin⁡(kxβˆ’Ο‰t).\boxed{J_x=-\epsilon_0\partial_tE_x=-\epsilon_0\omega E_0\sin(kx-\omega t)}.

(b) Interpretation and further calculation

βˆ‚tρ=Ο΅0kΟ‰E0cos⁡(kxβˆ’Ο‰t),βˆ‚xJx=βˆ’Ο΅0kΟ‰E0cos⁡(kxβˆ’Ο‰t).\partial_t\rho=\epsilon_0k\omega E_0\cos(kx-\omega t),\quad\partial_xJ_x=-\epsilon_0k\omega E_0\cos(kx-\omega t).ρ̇+βˆ‡β‹…π‘±=0;ρ,𝑱≠0in general.\boxed{\dot\rho+\nabla\cdot\mathbf J=0;\quad\rho,\mathbf J\ne0\ \text{in general}}.

Physical check

Mathematical time dependence alone does not make a field a source-free electromagnetic wave.