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Electromagnetic Waves Test - 34

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Electromagnetic Waves Test - 34
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  • Question 1
    1 / -0
    Choose the correct answer from the alternatives given.
    Assume a bulb of efficiency 2.5% as a point source. The peak values of electric and magnetic fields produced by the radiation coming from a 100 W bulb at a distance of 3 m is respectively 
    Solution
    Here intensity, $$ I = \dfrac{power}{area}$$

    = $$\dfrac{100 \times 2.5 }{4\pi (3)^2 \times 100} = \dfrac{2.5}{36\pi }Wm^{-2}$$

    Half of this intensity belongs to electronic field and half of that to magnetic field.

    $$\therefore \dfrac{I}{2} \,= \, \dfrac{1}{4}\varepsilon_0E^2_0c$$

    or  
    $$E_o = \sqrt{\dfrac{2I}{\epsilon _0c}}\,\\\Rightarrow \, \sqrt{\dfrac{2 \times \dfrac{2.5}{36\pi }}{\dfrac{1}{4\pi \times 9\times 10^9 }}\times 3\times 10^8}\\\Rightarrow 4.08 V m^{-i}$$

    $$\therefore B_o =  \dfrac{E_0}{c} \,=\, \dfrac{4.08}{3\times 10^8}\\ = 1.36 \times 10^{-8}T$$
  • Question 2
    1 / -0
    A plane EM wave travelling alone z-direction is described by $${ \overrightarrow { E } \  =\  { E }_{ 0 } }\sin { (kz\  -\  \omega t)\hat{ i } }$$ and $${\vec B\  =\  { B }_{ 0 } }\sin { (kz\  -\  \omega t)\hat{ j } }$$.
    Solution
    (i) The e.m. wave carries energy which is due to electric field vector and magnetic field vector. In e.m. wave $$E$$ and $$B$$ vary from point to point and from moment to moment. Let $$E$$ and $$B$$ be their time average. The energy density due to the electric field $$E$$ is

    $$u_E = \dfrac{1}{2} \in_0 E^2$$

    The energy density due to magnetic field $$B$$ is $$u B = \dfrac{1}{2}\dfrac{B^2}{\mu_0}$$
    Total average energy density of em wave 
    $$u_{av}=uE+uB=\dfrac{1}{2}\in_0E^2+\dfrac{1}{2}\dfrac{B^2}{\mu_0}$$     ...(i)

    Let the em wave be propagation along z-direction. The electric field vector and magnetic field vectors be represented by
    $$E=E_0\sin (kz-wt)$$
    $$B= B_0\sin (kz-wt)$$

    The time average value of $$E^2$$ over complete cycle $$= E_0^2/2$$

    and time average value of $$B^2$$ over complete cycle $$= B_0^2/2$$

    $$\therefore u_{av} = \dfrac{1}{2} \in_0 \dfrac{E_0^2}{2} + \dfrac{1}{2}\mu_0\left(\dfrac{B_0^2}{2}\right) = \dfrac{1}{4} \in_0 E_0^2 + \dfrac{B_0^2}{4\mu_0}$$

    (ii) we know that $$E_0 = cB_0$$ and $$c = \dfrac{1}{\sqrt{\mu_0\in_0}}$$.

    $$\therefore \dfrac{1}{4} \dfrac{B_0^2}{\mu_0} = \dfrac{1}{4} \dfrac{E_0^2/c^2}{\mu_0} = \dfrac{E_0^2}{4\mu_0} \times \mu_0 \in_0 = \dfrac{1}{4} \in_0 E_0^2$$

    $$\therefore uB = uE$$

    Hence, $$u_{av} = \dfrac{1}{4} \in_0 E^2_0 + \dfrac{1}{4} \dfrac{B_0^2}{\mu_0} = \dfrac{1}{4} \in_0 E_0^2 + \dfrac{1}{4}\in_0 E^2_0=\dfrac{1}{4}\in_0E_0^2=\dfrac{1}{2}\dfrac{B^2_0}{\mu_0}$$

    Time average intensity of the wave

    $$I_{av} = u_{av}c=\dfrac{1}{2} \in E_0^2c=\dfrac{1}{2}\in_0cE_0^2$$
    Hence, the correct option is $$(C)$$
  • Question 3
    1 / -0
    Suppose that the electric field amplitude of an electromagnetic wave propagating along x-direction is $${ E }_{ 0}$$ = 120 N $${ C }^{ -1 }$$ and that its frequency is $$\upsilon$$ = 50.0 MHz.
    Solution
    $$E_0=120\,NC$$

    $$\omega=2\pi f$$
    $$\omega=2\pi\times 50\times 10^{6}=100\pi\times 10^{6}$$

    $$\cfrac{\omega}{k}=c$$
    $$\Rightarrow \cfrac{100\pi\times 10^{6}}{k}=3\times 10^{8}$$
    $$\Rightarrow k=\cfrac{\pi}{3}$$

    The standard equaton for electric field is:
    $$E=E_0\ sin(kx-\omega t)$$
    $$\implies E=120\sin (\cfrac{\pi}{3}x-100\pi\times 10^{6}t)\hat j$$

    The magnetic field intensity is given by:
    $$B_0=\dfrac{E_0}{c}$$

    $$\Rightarrow B_0=\dfrac{120}{3\times10^8}=40\times 10^{-8}\ T$$

    The standard equaton for magnetic field is:
    $$B=B_0\ sin(kx-\omega t)$$
    $$\implies B=40\times 10^{-8}\sin(\cfrac{\pi}{3}x-\pi\times 10^{8}t)\hat k$$

    Option $$(D)$$ is correct.
  • Question 4
    1 / -0
    A plane e.m wave of frequency $$30MHz$$ travels in free space along the x-direction. The electric field component of the wave at a particular point of space and time $$E=6V/m$$ along $$y$$-direction. Its magnetic field component $$B$$ at this point would be
    Solution
    Given data
    frequency$$ = 30 MHz$$
    Electric field $$\varepsilon=\cfrac { 6v }{ m } \hat { J } $$ (along + y axis)
    Now we know that
    $$c=\cfrac { { \varepsilon  }_{ 0 } }{ { B }_{ 0 } } $$
    c = speed of EM wave$$=3\times { 10 }^{ 8 }m/s$$
    $${ \varepsilon  }_{ 0 }=$$peak value of electric field
     $${ B }_{ 0 }=$$peak value of magnetic field
    $$c=\cfrac { \varepsilon }{ B } $$                     
    B = magnetic field
    $$3\times { 10 }^{ 8 }=\cfrac { 6 }{ B } $$           
    $$B=\cfrac { 6 }{ 3\times { 10 }^{ 8 } } $$        $$B=2\times { 10 }^{ -8 }$$ Tesla
    Now we have to find direction of magnetic field
    We know that wave propagates in the direction perpendicular to oscillating electric field and magnetic field.
    $$c=\vec { \varepsilon  } \times \vec { B } $$ (only for direction)
    c = along x axis
    $$\varepsilon =$$along y axis
    So B should be along z axis
    $$B=2\times { 10 }^{ -8 }T$$ along z axis
  • Question 5
    1 / -0
    The electric field part of an electromagnetic wave in vacuum is
    $$E=3.1\cos { \left[ \left( 1.8\dfrac { rad }{ m }  \right) y+\left( 5.4\times { 10 }^{ 8 }\dfrac { rad }{ s }  \right) t \right] \hat { i }  } $$.The frequency corresponding to the given part of the electromagnetic wave is?
    Solution
    Given equation
    $$E=3.1\cos { \left[ \left( 1.8\dfrac { rad }{ m }  \right) y+\left( 5.4\times { 10 }^{ 8 }\dfrac { rad }{ s }  \right) t \right] \hat { i }  } $$...........(i)

    Standard equation at electromagnetic wave in terms of electric field,

    $$E=E_0\cos(ky+wt)$$.........(ii)

    If the wave is moving in $$-y$$ direction

    Wave length, $$\lambda=\dfrac{2\pi}{Coefficient\,of\,y}$$

    $$=\dfrac{2\pi}{1.8}=\dfrac{2\times 22/7}{1.8}$$

    $$\lambda=\dfrac{44}{1.8\times 7}=3.49=3.5m$$

    velocity of wave, $$v=\dfrac{\text{coefficient of l}}{\text{coefficient of y}}$$
     
    $$v=\dfrac{5.4\times 10^8}{1.8}=3\times 10^8$$

    frequency, $$f=\dfrac{v}{\lambda}=\dfrac{3\times 10^8}{3.5}=8.6\times 10^7$$ Hz
    Hence, the correct option is $$(B)$$
  • Question 6
    1 / -0
    In an electromagnetic wave, the amplitude of electric and magnetizing fields are 100 V/m and 0.265 A/m/ The maximum energy flow is -
    Solution

  • Question 7
    1 / -0
    Potential difference across plates of a capacitor $$6\mu F$$ is changing at the rate of $$72V{ s }^{ -1 }$$. Displacement current at that instant will be 
    Solution
    Given, 
    $$C=\dfrac{A\varepsilon_0}{d}=6\mu C$$
    $$\dfrac{dV}{dt}=72V/s$$
    Displacement current, $$I_D=\varepsilon_0 \dfrac{d\phi_E}{dt}$$
    $$I_D=\varepsilon_0\dfrac{d(EA)}{dt}$$

    $$I_D=\varepsilon_0 A\dfrac{d(V/d)}{dt}$$

    $$I_D=\dfrac{\varepsilon_0 A}{d}.\dfrac{dV}{dt}$$

    $$I_D=C\dfrac{dV}{dt}$$

    $$I_D=6\times 10^{-6}\times 72$$

    $$I_D=432\times 10^{-6}A$$

    The correct option is D.
  • Question 8
    1 / -0
    A plane electromagnetic wave with an intensity of $$200 W/m^2$$ is incident normal to a flat plate of radius 30 cm. If the plate absorbs $$60\%$$ and reflects $$40\%$$ of the incident radiation, what is the momentum transferred to it in 5 min?
    Solution

  • Question 9
    1 / -0
    The magnetic field in a plane electromagnetic wave is given by$$B=2.01\times10^{-7} \sin(6.28\times10^2x+2.2\times10^{10}t)T$$. [where x in cm and t in second]. The wavelength of the given wave is 
    Solution

  • Question 10
    1 / -0
    A parallel late condenser consists of two circular plate each of radius $$2cm$$ separated by a distance of $$0.1mm$$. A time varying potential difference of $$5\times 10^{13}v/s$$ is applied across the plated of the condenser: The displacement current is 
    Solution

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