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Electromagnetic Waves Test - 18

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Electromagnetic Waves Test - 18
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  • Question 1
    1 / -0
    The charge on a parallel plate capacitor is varying as $$q={ q }_{ 0 }\sin { \left( 2\pi nt \right)  } $$. The plates are very large and close together. neglecting the edge effects, the displacement current through the capacitor is:
    Solution
    Displacement current through a surface is $$\epsilon_0$$ times the rate of change of flux through the surface.
    Since $$E=\dfrac{q}{A\epsilon_0}$$.
    Therefore electric flux through the surface is $$\phi = EA=\dfrac{q}{\epsilon_0}$$
    So real current though the capacitor $$i = \dfrac{d\phi}{dt} = \epsilon_0 \dfrac{d}{dt}(\dfrac{q}{\epsilon_0})=\dfrac{dq}{dt}=i$$
    Thus displacement current is $$\dfrac{dq}{dt}=2\pi n q_0\cos2\pi ft$$
  • Question 2
    1 / -0

    Directions For Questions

    A plane electromagnetic wave frequency $$40MHz$$ travels in free space in the X-direction. At some point and at some distant, the electric field has its maximum value of $$750N/C$$ in Y-direction.

    ...view full instructions

    The period of the wave will be
    Solution
    Time period,  $$T= \dfrac{1}{\nu}$$
    $$T= \dfrac{1}{40 \times 10^6}$$
    $$\implies T= .025   \mu s$$
  • Question 3
    1 / -0

    Directions For Questions

    A parallel plate capacitor made of circular plates each of radius $$R=6\ cm$$ has capacitance $$C=100\ pF$$. The capacitor is connected to a $$230\ V$$ AC supply with an angular frequency of $$300\ rad/s$$.

    ...view full instructions

    The $$rms$$ value of conduction current will be:
    Solution
     Rms value of conduction current, $$I=V/X_c$$
    Where,
    $$X_c$$ = Capacitive reactance
    $$=1/ωC$$
    ∴ $$ I = V × ωC $$
    = $$230\times 300\times 100\times 10^{-12}$$
    = $$6.9\times 10^{-6} $$ A
    = $$6.9$$  μA
  • Question 4
    1 / -0
    Maxwell's four equations are written as
    (i) $$\oint { \overrightarrow { E } .\overrightarrow { d } s } =\cfrac { { q }_{ 0 } }{ { \varepsilon  }_{ 0 } } \quad $$
    (ii)$$\oint { \overrightarrow { B } .\overrightarrow { d } s } =0$$
    (iii)$$\oint { \overrightarrow { E } .\overrightarrow { d } l } =\cfrac { d }{ dt } \quad \oint { \overrightarrow { B } .\overrightarrow { d } s } $$
    (iv)$$\oint { \overrightarrow { B } .\overrightarrow { d } s } ={ \mu  }_{ 0 }{ \varepsilon  }_{ 0 }\cfrac { d }{ dt } \quad \oint { \overrightarrow { E } .\overrightarrow { d } s }  $$
    Which of the above Maxwell's equations shows that electric field lines do not form closed loops?
    Solution
    $$\oint  \vec{E}.\vec{d}s   $$ represents electric flux which is equal to the number of electric field lines crossing through an area.
    Now for $$q_o \neq 0$$,  implies  $$\oint  \vec{E}.\vec{d}s  \neq 0 $$ which indicates Electric field lines do not form closed loops. 
  • Question 5
    1 / -0

    Directions For Questions

    A plane electromagnetic wave frequency $$40MHz$$ travels in free space in the X-direction. At some point and at some distant, the electric field has its maximum value of $$750N/C$$ in Y-direction.

    ...view full instructions

    The wavelength of the wave is
    Solution
    Using $$v=\nu \lambda$$   where $$v$$ is the speed of EM wave.
    As  $$v= c= 3 \times 10^8   m/s                                  $$
    $$\implies 3 \times 10^8 = 40 \times 10^6    \lambda$$
    $$\implies \lambda = 7.5   m$$
  • Question 6
    1 / -0

    Directions For Questions

    A plane electromagnetic wave frequency $$40MHz$$ travels in free space in the X-direction. At some point and at some distant, the electric field has its maximum value of $$750N/C$$ in Y-direction.

    ...view full instructions

    The angular frequency of emf wave will be (in rad/s)
    Solution
    Frequency of wave  $$f = 40\times 10^6 \ Hz$$
    Angular frequency,  $$\omega = 2\pi \nu$$
    $$\omega = 2\pi \times 40 \times 10^6$$
    $$\implies   \omega = 8 \pi \times 10^7  \   rad/s$$
  • Question 7
    1 / -0
    Maxwell's four equations are written as
    (i) $$\oint { \overrightarrow { E } .\overrightarrow { d } s } =\cfrac { { q }_{ 0 } }{ { \varepsilon  }_{ 0 } } \quad $$
    (ii)$$\oint { \overrightarrow { B } .\overrightarrow { d } s } =0$$
    (iii)$$\oint { \overrightarrow { E } .\overrightarrow { d } l } =\cfrac { d }{ dt } \quad \oint { \overrightarrow { B } .\overrightarrow { d } s } $$
    (iv)$$\oint { \overrightarrow { B } .\overrightarrow { d } s } ={ \mu  }_{ 0 }{ \varepsilon  }_{ 0 }\cfrac { d }{ dt } \quad \oint { \overrightarrow { E } .\overrightarrow { d } s }  $$
    Out of the four Maxwell's equation above, which one shows the non-existence of monopoles?
    Solution
    Had there been a monopole, the integral of $$\vec{B}.\vec{ds}$$ on a closed surface enclosing the monopole would have been non-zero.
    Thus the second equation shows the non-existence of monopole.
  • Question 8
    1 / -0
    The Sun delivers $${{10}^{3}}W/{{m}^{2}}$$ of electromagnetic flux to the Earth's surface. The radiation force on the roof of dimensions $$8m\times 20m$$ will be:
    Solution
    Poynting vector, $$S={10}^3 W/m^2$$
    Pressure, $$P=\dfrac{S}{c}=$$$$\dfrac{1000}{3\times 10^8}$$
                         $$=3.33\times {10}^{-6} N/m^2$$
    Radiation force on the roof is given by:
    $$F=P\times 8\times 20 = 5.33 \times {10}^{-4}N$$
  • Question 9
    1 / -0

    Directions For Questions

    A plane electromagnetic wave frequency $$40MHz$$ travels in free space in the X-direction. At some point and at some distant, the electric field has its maximum value of $$750N/C$$ in Y-direction.

    ...view full instructions

    The propagation constant of the wave will be
    Solution
    Using $$v=\nu \lambda$$   where $$v$$ is the speed of EM wave.
    As  $$v= c= 3 \times 10^8   m/s                                  $$
    $$\implies 3 \times 10^8 = 40 \times 10^6    \lambda$$
    $$\implies \lambda = 7.5   m$$
    Propagation constant,   $$K= \dfrac{2\pi}{\lambda}= \dfrac{2\pi}{7.5}$$
    $$\implies K= 0.838   m^{-1}$$
  • Question 10
    1 / -0
    An electromagnetic wave, going through vacuum is described by $$E=E_0\sin{(kx-\omega t)}$$. Which of the following is independent of wavelength?
    Solution
    $$k=\dfrac{2\pi}{\lambda}$$

    $$\omega = \dfrac{2\pi c}{\lambda}, $$where $$c$$ is the velocity of light 

    Hence, $$\dfrac{k}{2\pi} = \dfrac{\omega}{2\pi c} \implies \dfrac{k}{\omega}$$ is independent of the wavelength.
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