Since D = KE and B = μH, we have

_i_A_v_(κE_y_) = -_ci_A(H_{_z_} + _u_KE_{_y_}) (1·22)

_i_A_v_(μH_{_z_}) = -_ci_A(E_{_y_} + _u_μH_{_z_}) (2·22)

or _v_(K - _u_)E_{_y_} = _c_H_{_z_} (1·23)

μ(_v_ - _u_)H_{_z_} = _c_E_{_y_} (2·23)

The Principle of Relativity · 第 188 / 203 题