The source of an electromagnetic wave can be a charge

  • A
    moving with a constant velocity
  • B
    moving in a circular orbit
  • C
    at rest
  • D
    moving parallel to the magnetic field

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Similar Questions

An insulator plate is passed between the plates of a capacitor. Then the displacement current

$A$ parallel plate capacitor is completely immersed in a liquid of resistivity $\rho = 0.25 \, \Omega m$ and relative permittivity $\epsilon_r = 80$. If the plates of the capacitor are connected to an alternating voltage source of $V = V_0 \sin(\omega t)$ at a frequency of $f = 0.4 \, GHz$,then the ratio of the amplitudes of the displacement current $(I_d)$ and conduction current $(I_c)$ is:

If the rate of change in electric flux between the plates of a capacitor is $9 \pi \times 10^3 \text{ Vm s}^{-1}$,then the displacement current inside the capacitor is (in $\mu \text{A}$)

Inside a parallel plate capacitor,the electric field $E$ varies with time as $t^2$. The variation of the induced magnetic field with time is given by

Match the following Maxwell’s equations: (The symbols used here have their usual meanings)
List-$I$List-$II$
$(a)$ Gauss’ law for electrostatics$(i)$ $\oint \vec{E} \cdot d\vec{A} = \frac{Q}{\epsilon_0}$
$(b)$ Gauss’ law for magnetism(ii) $\oint \vec{B} \cdot d\vec{l} = \mu_0 [i_c + \epsilon_0 \frac{d\phi_E}{dt}]$
$(c)$ Faraday’s law(iii) $\oint \vec{B} \cdot d\vec{A} = 0$
$(d)$ Ampere-Maxwell’s law(iv) $\oint \vec{E} \cdot d\vec{l} = -\frac{d\phi_B}{dt}$

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