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    832.

    A plane electromagnetic wave travelling along the XX-direction has a wavelength of 3  mm3\;mm. The variation in the electric field occurs in the YY-direction with an amplitude 66  Vm166\;V{m^{ - 1}}. The equations for the electric and magnetic fields as a function of x  and  tx\;and\;t are respectively

    A

    Ey=33cosπimes1011(txc){E_y} = 33\cos \pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    Bz=1.1imes107cosπimes1011(txc){B_z} = 1.1 imes {10^{ - 7}}\cos \pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    B

    Ey=11cos2πimes1011(txc){E_y} = 11\cos 2\pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    By=11imes107cos2πimes1011(txc){B_y} = 11 imes {10^{ - 7}}\cos 2\pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    C

    Ex=33cosπimes1011(txc){E_x} = 33\cos \pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    Bx=11imes107cosπimes1011(txc){B_x} = 11 imes {10^{ - 7}}\cos \pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    D

    Ey=66cos2πimes1011(txc){E_y} = 66\cos 2\pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    Bz=2.2imes107cos2πimes1011(txc){B_z} = 2.2 imes {10^{ - 7}}\cos 2\pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    Question Tags

    833.

    A plane electromagnetic wave travelling along the XX-direction has a wavelength of 3  mm3\;mm. The variation in the electric field occurs in the YY-direction with an amplitude 66  Vm166\;V{m^{ - 1}}. The equations for the electric and magnetic fields as a function of x  and  tx\;and\;t are respectively

    A

    Ey=33cosπimes1011(txc){E_y} = 33\cos \pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    Bz=1.1imes107cosπimes1011(txc){B_z} = 1.1 imes {10^{ - 7}}\cos \pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    B

    Ey=11cos2πimes1011(txc){E_y} = 11\cos 2\pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    By=11imes107cos2πimes1011(txc){B_y} = 11 imes {10^{ - 7}}\cos 2\pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    C

    Ex=33cosπimes1011(txc){E_x} = 33\cos \pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    Bx=11imes107cosπimes1011(txc){B_x} = 11 imes {10^{ - 7}}\cos \pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    D

    Ey=66cos2πimes1011(txc){E_y} = 66\cos 2\pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

    Bz=2.2imes107cos2πimes1011(txc){B_z} = 2.2 imes {10^{ - 7}}\cos 2\pi imes {10^{11}}\left( {t - \frac{x}{c}} \right)

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    834.

    If ε0{\varepsilon _0} and μ0{\mu _0} are respectively, the electric permittivity and the magnetic permeability of free space, ε\varepsilon and μ\mu the corresponding quantities in a medium, the refractive index of the medium is

    A

    μεμ0ε0\sqrt {\frac{{\mu \,\varepsilon }}{{{\mu _0}\,{\varepsilon _0}}}}

    B

    μεμ0ε0\frac{{\mu \,\varepsilon }}{{{\mu _0}\,{\varepsilon _0}}}

    C

    μ0ε0με\sqrt {\frac{{{\mu _0}\,{\varepsilon _0}}}{{\mu \,\varepsilon }}}

    D

    μμ0εε0\sqrt {\frac{{\mu \,{\mu _0}}}{{\varepsilon \,{\varepsilon _0}}}}

    Question Tags

    835.

    If ε0{\varepsilon _0} and μ0{\mu _0} are respectively, the electric permittivity and the magnetic permeability of free space, ε\varepsilon and μ\mu the corresponding quantities in a medium, the refractive index of the medium is

    A

    μεμ0ε0\sqrt {\frac{{\mu \,\varepsilon }}{{{\mu _0}\,{\varepsilon _0}}}}

    B

    μεμ0ε0\frac{{\mu \,\varepsilon }}{{{\mu _0}\,{\varepsilon _0}}}

    C

    μ0ε0με\sqrt {\frac{{{\mu _0}\,{\varepsilon _0}}}{{\mu \,\varepsilon }}}

    D

    μμ0εε0\sqrt {\frac{{\mu \,{\mu _0}}}{{\varepsilon \,{\varepsilon _0}}}}

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