Chapter 17: Problem 27
The displacement current flows in the dielectric of a capacitor (A) becomes zero. (B) has assumed a constant value. (C) is increasing with time. (D) is decreasing with time.
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Chapter 17: Problem 27
The displacement current flows in the dielectric of a capacitor (A) becomes zero. (B) has assumed a constant value. (C) is increasing with time. (D) is decreasing with time.
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The rms value of the electric field of the light coming from the sun is \(720 \mathrm{~N} / \mathrm{C}\). The average total energy density of the electromagnetic wave is [2006] (A) \(3.3 \times 10^{-3} \mathrm{~J} / \mathrm{m}^{3}\) (B) \(4.58 \times 10^{-6} \mathrm{~J} / \mathrm{m}^{3}\) (C) \(6.37 \times 10^{-9} \mathrm{~J} / \mathrm{m}^{3}\) (D) \(81.35 \times 10^{-12} \mathrm{~J} / \mathrm{m}^{3}\)
The Maxwell's four equations are written as (i) \(\oint \vec{E} \cdot \overrightarrow{d s}=\frac{q_{0}}{\varepsilon_{0}}\) (ii) \(\oint \vec{B} \cdot \overrightarrow{d s}=0\) (iii) \(\oint \vec{E} \cdot \overrightarrow{d l}=\frac{d}{d t} \oint \vec{B} \cdot \overrightarrow{d s}\) (iv) \(\oint \vec{B} \cdot \overrightarrow{d s}=\mu_{0} \varepsilon_{0} \frac{d}{d t} \oint \vec{E} \cdot \overrightarrow{d s}\) The equations which have sources of \(\vec{E}\) and \(\vec{B}\) (A) (i), (ii) and (iii) (B) (i) and (ii) (C) (i) and (iii) (D) (i) and (iv)
Match List-I (Electromagnetic wave type) with List-II (Its association/application)and select the correct option from the choices given below the lists. [2014] $$ \begin{array}{ll} \text { List-I } & \text { List-II } \\ \hline \text { (P) Infrared wave } & \text { (i) To treat muscular strain } \\\ \text { (Q) Radio waves } & \text { (ii) For broadcasting } \\ \text { (R) X-rays } & \text { (iii) To detect fracture of bones } \\ \text { (S) Ultraviolet } & \text { (iv) Absorbed by the ozone } \\ \text { rays } & \text { layer of the atmosphere } \end{array} $$ $$ \begin{array}{c|c|c|c|c} & \text { P } & \text { Q } & \text { R } & \text { S } \\ \hline \text { A } & \text { (i) } & \text { (ii) } & \text { (iii) } & \text { (iv) } \\ \hline \text { B } & \text { (iv) } & \text { (iii) } & \text { (ii) } & \text { (i) } \\ \hline \text { C } & \text { (i) } & \text { (ii) } & \text { (iv) } & \text { (iii) } \\ \hline \text { D } & \text { (iii) } & \text { (ii) } & \text { (i) } & \text { (iv) } \\ \hline \end{array} $$
The magnetic field between the plates of a capacitor when \(r>R\) is given by (A) \(\frac{\mu_{0} I_{D} r}{2 \pi R^{2}}\) (B) \(\frac{\mu_{0} I_{D}}{2 \pi R}\) (C) \(\frac{\mu_{0} I_{D}}{2 \pi r}\) (D) \(\mathrm{kWU}\)
Electromagnetic waves are transverse in nature is evident by \([\mathbf{2 0 0 2}]\) (A) Polarization (B) Interference (C) Reflection (D) Diffraction
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