Exam 33: Electromagnetic Waves

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A charge undergoes an acceleration. The tangential component of the electric field produced during the acceleration is

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E

The following electromagnetic radiation has a wavelength that is closest to the size of automobile:

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An electromagnetic wave has an electric field given by E=(9.0×105 V/m)j^cos[(9.42×1015rad/s)tkz]\vec { E } = - \left( 9.0 \times 10 ^ { 5 } \mathrm {~V} / \mathrm { m } \right) \hat { j } \cos \left[ \left( 9.42 \times 10 ^ { 15 } \mathrm { rad } / \mathrm { s } \right) t - k z \right] . The axis of polarization of the wave is

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An electromagnetic wave has an electric field given by E=(9.0×105 V/m)j^cos[(9.42×1015rad/s)tkz]\vec { E } = - \left( 9.0 \times 10 ^ { 5 } \mathrm {~V} / \mathrm { m } \right) \hat { j } \cos \left[ \left( 9.42 \times 10 ^ { 15 } \mathrm { rad } / \mathrm { s } \right) t - k z \right] . The magnitude of the magnetic field associated with this wave is

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A satellite 300 km above the surface of the Earth emits a radio wave pulse ( λ\lambda = 25m). The transit time for the wave to reach the surface of the Earth is

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A 4.0-A current is charging a 10.0-mF capacitor. The total displacement current between the capacitor plates is

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A pressure of 15×106 N/m215 \times 10 ^ { - 6 } \mathrm {~N} / \mathrm { m } ^ { 2 } is due to sunlight being reflected from a surface of a "solar sail." The energy flux incident on the surface is

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Consider a 150-W incandescent lightbulb that radiates light in all directions. At a distance of 1.5 m the amplitude of the oscillating magnetic field B0 is

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Given that the sun's intensity at the Earth's surface is 1350 W/m2, the amount of electrical energy in a cubic meter at the Earth's surface is

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The speed of radio waves traveling in a vacuum depends on

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The direction of propagation of an electromagnetic wave is given by

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An electromagnetic wave has an electric field given by E=(9.0×105 V/m)j^cos[(9.42×1015rad/s)tkz]\vec { E } = - \left( 9.0 \times 10 ^ { 5 } \mathrm {~V} / \mathrm { m } \right) \hat { j } \cos \left[ \left( 9.42 \times 10 ^ { 15 } \mathrm { rad } / \mathrm { s } \right) t - k z \right] . The direction of the polarization of the magnetic field associated with this wave is

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Maxwell's equations are a compilation of the fundamental laws needed for a complete mathematical description of the behavior of electric and magnetic fields. The equation that mathematically reflects that there are no isolated magnetic poles is

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An electromagnetic wave has an electric field given by E=(9.0×105 V/m)j^cos[(9.42×1015rad/s)tkz]\vec { E } = - \left( 9.0 \times 10 ^ { 5 } \mathrm {~V} / \mathrm { m } \right) \hat { j } \cos \left[ \left( 9.42 \times 10 ^ { 15 } \mathrm { rad } / \mathrm { s } \right) t - k z \right] . The frequency of the wave is

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The functional dependence of the radial component of the field produced by an accelerating charge as a function of distance from the charge is proportional to

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The Maxwell-Ampere Law can be written as; Bds=μ0I+μ0ε0dΦEdt\oint \vec { B } \cdot d \vec { s } = \mu _ { 0 } I + \mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t } . The term in the equation that relates to the magnetic field produced by an electric current is

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At a given point the electric field is 0.25 V/m. The energy flux at this point is

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The magnetic field component of an electromagnetic wave is 25 μT\mu \mathrm { T } . The electric energy density of the wave is

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Radiation from a source is striking a surface at a rate of 50 W/m2. The peak value of the electric field is

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The frequency of an electromagnetic wave is 2.0×1014 Hz2.0 \times 10 ^ { 14 } \mathrm {~Hz} . The wavelength of this wave is

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