Deck 33: Electromagnetic Waves

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Question
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 the so-called displacement current is

A) Bds\oint \vec { B } \cdot d \vec { s }
B) μ0I\mu _ { 0 } I
C) μ0ε0dΦEdt\mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }
D) No term in this equation is related to the displacement current.
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Question
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

A) Bds\oint \vec { B } \cdot d \vec { s }
B) μ0I\mu _ { 0 } I
C) μ0ε0dΦEdt\mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }
D) No term in this equation is related to the displacement current.
Question
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

A) EdA=Qinside ε0\oint \vec { E } \cdot d \vec { A } = \frac { Q _ { \text {inside } } } { \varepsilon _ { 0 } }
B) BdA=0\oint \vec { B } \cdot d \vec { A } = 0
C) Eds=dΦBdt\oint \vec { E } \cdot d \vec { s } = - \frac { d \Phi _ { B } } { d t }
D) Bds=μ0I+μ0ε0dΦEdt\oint \vec { B } \cdot d \vec { s } = \mu _ { 0 } I + \mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }
Question
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 a changing magnetic flux induces an electric field is

A) EdA=Qinside ε0\oint \vec { E } \cdot d \vec { A } = \frac { Q _ { \text {inside } } } { \varepsilon _ { 0 } }
B) BdA=0\oint \vec { B } \cdot d \vec { A } = 0
C) Eds=dΦBdt\oint \vec { E } \cdot d \vec { s } = - \frac { d \Phi _ { B } } { d t }
D) Bds=μ0I+μ0ε0dΦEdt\oint \vec { B } \cdot d \vec { s } = \mu _ { 0 } I + \mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }
Question
A 4.0-A current is charging a 10.0-mF capacitor. The total displacement current between the capacitor plates is

A) 4.0 A.
B) -4.0 A.
C) 0 A.
D) Not enough information is given to solve this problem.
Question
A current is used to charge a capacitor. After the capacitor has been charged, the magnetic field between the plates is

A) given by B=μ0I2πrB = \frac { \mu _ { 0 } I } { 2 \pi r }
B) given by B=μ0I22πrB = \frac { \mu _ { 0 } I ^ { 2 } } { 2 \pi r }
C) given by B=μ0I2πr2B = \frac { \mu _ { 0 } I } { 2 \pi r ^ { 2 } }
D) zero.
Question
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

A) 1.5×106 J1.5 \times 10 ^ { - 6 } \mathrm {~J}
B) 3.0×106 J3.0 \times 10 ^ { - 6 } \mathrm {~J}
C) 4.5×106 J4.5 \times 10 ^ { - 6 } \mathrm {~J}
D) 6.0×106 J6.0 \times 10 ^ { - 6 } \mathrm {~J}
Question
A parallel-plate capacitor consists of circular plates with a radius of one unit. During the charging process the magnitude of the magnetic field as a function of radius is

A) <strong>A parallel-plate capacitor consists of circular plates with a radius of one unit. During the charging process the magnitude of the magnetic field as a function of radius is</strong> A)   B)   C)   D)   <div style=padding-top: 35px>
B) <strong>A parallel-plate capacitor consists of circular plates with a radius of one unit. During the charging process the magnitude of the magnetic field as a function of radius is</strong> A)   B)   C)   D)   <div style=padding-top: 35px>
C) <strong>A parallel-plate capacitor consists of circular plates with a radius of one unit. During the charging process the magnitude of the magnetic field as a function of radius is</strong> A)   B)   C)   D)   <div style=padding-top: 35px>
D) <strong>A parallel-plate capacitor consists of circular plates with a radius of one unit. During the charging process the magnitude of the magnetic field as a function of radius is</strong> A)   B)   C)   D)   <div style=padding-top: 35px>
Question
A charge undergoes an acceleration. The tangential component of the electric field produced during the acceleration is

A) a maximum in the direction of the acceleration.
B) larger than the radial component.
C) decreasing in a manner that is proportional to 1/r2 from the source.
D) All of the above answers are correct.
E) None of the above answers is correct.
Question
The functional dependence of the transverse component of the radiation field produced by an accelerating charge as a function of distance from the charge is proportional to

A) r.
B) 1/r.
C) r2.
D) 1/r2.
E) none of the above.
Question
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

A) r.
B) 1/r.
C) r2.
D) 1/r2.
E) none of the above.
Question
Given a wave pulse that is traveling in the i^\hat { i } direction while its electric field is in the k^- \hat { k } direction, the magnetic field is in the

A) j^- \hat { j } direction.
B) j^ \hat {j }

direction.
C) k^+i^- \hat { k } + \hat { i } direction.
D) k^i^- \hat { k } - \hat { i } direction.
Question
A wave pulse is traveling in the j^- \hat { j } direction while its magnetic field is in the k^- \hat { k } direction. The electric field is in the

A) i^- \hat { i } direction.
B) j^ \hat {j } direction.
C) k^\hat { k } direction.
D) k^- \hat { k } direction.
Question
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 does not contribute to the theoretical description of the propagation of an electromagnetic wave pulse is

A) Bds\oint \vec { B } \cdot d \vec { s }
B) μ0I\mu _ { 0 } I
C) μ0ε0dΦEdt\mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }
D) No term in this equation is related to the propagation of the electromagnetic wave pulse.
Question
The frequency of an electromagnetic wave is 2.0×1014 Hz2.0 \times 10 ^ { 14 } \mathrm {~Hz} . The wavelength of this wave is

A) 150 nm.
B) 67 mm.
C) 1500 nm.
D) 670 nm.
Question
A gamma ray has a wavelength of 5.0×1014 m5.0 \times 10 ^ { - 14 } \mathrm {~m} . The frequency of this wave is

A) 6.0×1021 Hz6.0 \times 10 ^ { 21 } \mathrm {~Hz}
B) 6.0×1020 Hz6.0 \times 10 ^ { 20 } \mathrm {~Hz}
C) 3.0×1021 Hz3.0 \times 10 ^ { 21 } \mathrm {~Hz}
D) 15×1021 Hz15 \times 10 ^ { 21 } \mathrm {~Hz}
Question
The amplitude of the electric field of an electromagnetic wave is 6.0 ×\times 10 -3 V/m. The amplitude of the magnetic field of this wave is

A) 1.8 ×\times
106 T.
B) 1.8 ×\times
10-11 T.
C) 1.8 ×\times
10-10 T.
D) 2.0 ×\times
10-11 T.
Question
Unpolarized light with an intensity of I0 is traveling in the + x direction. The light is incident on a polarizer whose axis is aligned along the y axis. The light that passes through the polarizer has an intensity that is

A) (1/2)I0 with a polarization along the z axis.
B) (1/2)I0 with a polarization along the y axis.
C) I0 with a polarization along the z axis.
D) I0 with a polarization along the y axis.
Question
Initially polarized light is incident on a polarizer. If the intensity of the light after passing through the polarizer is (3/4) of the initial intensity, the angle between the polarizer axis and the original polarization axis of the light is

A) 41.4°.
B) 30°.
C) 48.6°.
D) 60°.
Question
Unpolarized light of intensity I0 is incident upon the first of two polarizers. The second polarizer has its preferential direction at 50° with respect to the first polarizer. The final transmitted intensity is

A) (0.21) I0.
B) (0.41) I0.
C) (0.044) I0.
D) (0.59) I0.
Question
Unpolarized light of intensity I0 is incident upon the first of two polarizers. The final transmitted intensity is (3/8)I0. With respect to the first polarizer, the second polarizer has its preferential direction at

A) 52°.
B) 41°.
C) 38°.
D) 30°.
Question
The following electromagnetic radiation has a wavelength that is closest to the size of automobile:

A) Radio waves
B) Infrared radiation
C) Visible radiation
D) Ultraviolet radiation
Question
The unit associated with an energy flux is

A) joule.
B) watt/meter.
C) watt/meter2.
D) joule/meter2.
Question
At a given point the electric field is 0.25 V/m. The energy flux at this point is

A) 1.7 ×\times
10-4 W/m2.
B) 2.8 ×\times
10-4 W/m2.
C) 8.2 ×\times
10-4 W/m2.
D) 8.2 ×\times
10-5 W/m2.
Question
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 the wave is traveling in is

A) k^\hat { k }
B) j^\hat { j }
C) - j^\hat { j }

D) i^\hat { i }
Question
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

A) k^\hat { k }
B) j^\hat { j }

C) - j^\hat { j }

D) i^\hat { i }
Question
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

A) 9.42×1015 Hz9.42 \times 10 ^ { 15 } \mathrm {~Hz}
B) 9.42×1015rad/s9.42 \times 10 ^ { 15 } \mathrm { rad } / \mathrm { s }
C) 1.5×1015 Hz1.5 \times 10 ^ { 15 } \mathrm {~Hz}
D) 9.0×105 V/m9.0 \times 10 ^ { 5 } \mathrm {~V} / \mathrm { m }
Question
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 wavelength of the wave is

A) 2.0×107 m2.0 \times 10 ^ { - 7 } \mathrm {~m}
B) 2.0×107 m2.0 \times 10 ^ { 7 } \mathrm {~m}
C) 9.99×106 m9.99 \times 10 ^ { 6 } \mathrm {~m}
D) 3.1×107 m3.1 \times 10 ^ { 7 } \mathrm {~m}
Question
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 wave number of the magnetic field associated with this wave is

A) 3.1×107 m13.1 \times 10 ^ { 7 } \mathrm {~m} ^ { - 1 }
B) 3.0×103 m13.0 \times 10 ^ { - 3 } \mathrm {~m} ^ { - 1 }
C) 3.0×105 m3.0 \times 10 ^ { 5 } \mathrm {~m}
D) 3.1×107 m3.1 \times 10 ^ { 7 } \mathrm {~m}
Question
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

A) 1.0×103 T1.0 \times 10 ^ { - 3 } \mathrm {~T}
B) 2.0×103 T2.0 \times 10 ^ { - 3 } \mathrm {~T}
C) 3.0×103 T3.0 \times 10 ^ { - 3 } \mathrm {~T}
D) 6.0×103 T6.0 \times 10 ^ { - 3 } \mathrm {~T}
Question
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

A) j^\hat { j }

B) k^\hat { k }
C) i^\hat { i }
D) Hold on. The wave is not polarized.
Question
The speed of radio waves traveling in a vacuum depends on

A) the wavelength of the waves.
B) the frequency of the waves.
C) the polarization of the waves.
D) none of the above.
Question
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

A) 1125 W/m2.
B) 2250 W/m2.
C) 4500 W/m2.
D) 9000 W/m2.
Question
A pressure of 15×106 N/m215 \times 10 ^ { - 6 } \mathrm {~N} / \mathrm { m } ^ { 2 } is due to sunlight being absorbed by a surface of a "solar sail." The energy flux incident on the surface is

A) 1125 W/m2.
B) 2250 W/m2.
C) 4500 W/m2.
D) 9000 W/m2.
Question
A wave has double the amplitude of a second wave. The energy density of the second wave is

A) four times that of the first wave.
B) double that of the first wave.
C) equal to that of the first wave.
D) half that of the first wave.
E) one-quarter that of the first wave.
Question
An electromagnetic wave with an electric field amplitude of 0.15 V/m has an intensity of

A) 1.0×105 W/m21.0 \times 10 ^ { - 5 } \mathrm {~W} / \mathrm { m } ^ { 2 }
B) 3.0×106 W/m23.0 \times 10 ^ { - 6 } \mathrm {~W} / \mathrm { m } ^ { 2 }
C) 1.0×105 W/m21.0 \times 10 ^ { - 5 } \mathrm {~W} / \mathrm { m } ^ { 2 } .
D) 3.0×105 W/m23.0 \times 10 ^ { - 5 } \mathrm {~W} / \mathrm { m } ^ { 2 } .
Question
A spherical wave spreads out from a source, and the total power at a distance of R0 is P0. At a distance of 2R0 the power is

A) P0/8.
B) P0/4.
C) P0/2.
D) P0.
Question
A spherical wave spreads out from a source, and the energy flux at a distance of R0 is S0. At a distance of 2R0 the energy flux is

A) S0/8.
B) S0/4.
C) S0/2.
D) S0.
Question
An electromagnetic wave consists of

A) only an electric field.
B) only a magnetic field.
C) an electric field and a magnetic field oriented parallel to each other.
D) an electric field and a magnetic field oriented perpendicular to each other.
Question
The direction of propagation of an electromagnetic wave is given by

A) EB\vec { E } \cdot \vec { B }
B) EB- \vec { E } \cdot \vec { B }
C) E×B\vec { E } \times \vec { B }
D) B×E\vec { B } \times \vec { E }
Question
Stationary charges produce

A) electromagnetic waves.
B) only magnetic fields.
C) only electric fields.
D) both electric and magnetic fields.
Question
Accelerating charges produce

A) electromagnetic standing waves.
B) only magnetic fields.
C) only electric fields.
D) both electric and magnetic fields.
Question
ε0\varepsilon _ { 0 } is related to the speed of light and the permeability of free space through the relation

A) ε0=c2μ0\varepsilon _ { 0 } = c ^ { 2 } \mu _ { 0 }
B) ε0=c2μ0\varepsilon _ { 0 } = \frac { c ^ { 2 } } { \mu _ { 0 } }
C) ε0=1c2μ0\varepsilon _ { 0 } = \frac { 1 } { c ^ { 2 } \mu _ { 0 } }
D) ε0=μ0c2\varepsilon _ { 0 } = \frac { \mu _ { 0 } } { c ^ { 2 } }
Question
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

A) 1 μ\mu s.
B) 10 μ\mu s.
C) 100 μ\mu s.
D) 1 ms.
Question
Consider a 150-W incandescent lightbulb that radiates light in all directions. At a distance of 1.5 m the time-averaged energy flux emitted by the bulb is

A) 7.9 W/m2.
B) 5.3 W/m2.
C) 100 W/m2.
D) 67 W/m2.
Question
Consider a 150-W incandescent lightbulb that radiates light in all directions. At a distance of 1.5 m the amplitude of the oscillating electric field E0 is

A) 77 V/m.
B) 63 V/m.
C) 225 V/m.
D) 39 V/m.
Question
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

A) 2.6×107 T2.6 \times 10 ^ { - 7 } \mathrm {~T}
B) 2.1×107 T2.1 \times 10 ^ { - 7 } \mathrm {~T}
C) 7.5×107 T7.5 \times 10 ^ { - 7 } \mathrm {~T}
D) 1.3×107 T1.3 \times 10 ^ { - 7 } \mathrm {~T}
Question
The electric field component of an electromagnetic wave is 130 V/m. The electric energy density of the wave is

A) 7.5×108 J7.5 \times 10 ^ { - 8 } \mathrm {~J}
B) 7.5×108 J/m7.5 \times 10 ^ { - 8 } \mathrm {~J} / \mathrm { m }
C) 7.5×108 J/m27.5 \times 10 ^ { - 8 } \mathrm {~J} / \mathrm { m } ^ { 2 }
D) 7.5×108 J/m37.5 \times 10 ^ { - 8 } \mathrm {~J} / \mathrm { m } ^ { 3 }
Question
The magnetic field component of an electromagnetic wave is 25 μT\mu \mathrm { T } . The electric energy density of the wave is

A) 2.5×104 J/m32.5 \times 10 ^ { - 4 } \mathrm {~J} / \mathrm { m } ^ { 3 }
B) 2.5×104 J/m22.5 \times 10 ^ { - 4 } \mathrm {~J} / \mathrm { m } ^ { 2 }
C) 2.5×102 J/m32.5 \times 10 ^ { - 2 } \mathrm {~J} / \mathrm { m } ^ { 3 }
D) 2.5×102 J/m22.5 \times 10 ^ { - 2 } \mathrm {~J} / \mathrm { m } ^ { 2 }
Question
Radiation from a source is striking a surface at a rate of 50 W/m2. The peak value of the electric field is

A) 110 V/m.
B) 150 V/m.
C) 190 V/m.
D) 250 V/m.
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Deck 33: Electromagnetic Waves
1
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 the so-called displacement current is

A) Bds\oint \vec { B } \cdot d \vec { s }
B) μ0I\mu _ { 0 } I
C) μ0ε0dΦEdt\mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }
D) No term in this equation is related to the displacement current.
μ0ε0dΦEdt\mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }
2
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

A) Bds\oint \vec { B } \cdot d \vec { s }
B) μ0I\mu _ { 0 } I
C) μ0ε0dΦEdt\mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }
D) No term in this equation is related to the displacement current.
μ0I\mu _ { 0 } I
3
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

A) EdA=Qinside ε0\oint \vec { E } \cdot d \vec { A } = \frac { Q _ { \text {inside } } } { \varepsilon _ { 0 } }
B) BdA=0\oint \vec { B } \cdot d \vec { A } = 0
C) Eds=dΦBdt\oint \vec { E } \cdot d \vec { s } = - \frac { d \Phi _ { B } } { d t }
D) Bds=μ0I+μ0ε0dΦEdt\oint \vec { B } \cdot d \vec { s } = \mu _ { 0 } I + \mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }
BdA=0\oint \vec { B } \cdot d \vec { A } = 0
4
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 a changing magnetic flux induces an electric field is

A) EdA=Qinside ε0\oint \vec { E } \cdot d \vec { A } = \frac { Q _ { \text {inside } } } { \varepsilon _ { 0 } }
B) BdA=0\oint \vec { B } \cdot d \vec { A } = 0
C) Eds=dΦBdt\oint \vec { E } \cdot d \vec { s } = - \frac { d \Phi _ { B } } { d t }
D) Bds=μ0I+μ0ε0dΦEdt\oint \vec { B } \cdot d \vec { s } = \mu _ { 0 } I + \mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }
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5
A 4.0-A current is charging a 10.0-mF capacitor. The total displacement current between the capacitor plates is

A) 4.0 A.
B) -4.0 A.
C) 0 A.
D) Not enough information is given to solve this problem.
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6
A current is used to charge a capacitor. After the capacitor has been charged, the magnetic field between the plates is

A) given by B=μ0I2πrB = \frac { \mu _ { 0 } I } { 2 \pi r }
B) given by B=μ0I22πrB = \frac { \mu _ { 0 } I ^ { 2 } } { 2 \pi r }
C) given by B=μ0I2πr2B = \frac { \mu _ { 0 } I } { 2 \pi r ^ { 2 } }
D) zero.
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7
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

A) 1.5×106 J1.5 \times 10 ^ { - 6 } \mathrm {~J}
B) 3.0×106 J3.0 \times 10 ^ { - 6 } \mathrm {~J}
C) 4.5×106 J4.5 \times 10 ^ { - 6 } \mathrm {~J}
D) 6.0×106 J6.0 \times 10 ^ { - 6 } \mathrm {~J}
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8
A parallel-plate capacitor consists of circular plates with a radius of one unit. During the charging process the magnitude of the magnetic field as a function of radius is

A) <strong>A parallel-plate capacitor consists of circular plates with a radius of one unit. During the charging process the magnitude of the magnetic field as a function of radius is</strong> A)   B)   C)   D)
B) <strong>A parallel-plate capacitor consists of circular plates with a radius of one unit. During the charging process the magnitude of the magnetic field as a function of radius is</strong> A)   B)   C)   D)
C) <strong>A parallel-plate capacitor consists of circular plates with a radius of one unit. During the charging process the magnitude of the magnetic field as a function of radius is</strong> A)   B)   C)   D)
D) <strong>A parallel-plate capacitor consists of circular plates with a radius of one unit. During the charging process the magnitude of the magnetic field as a function of radius is</strong> A)   B)   C)   D)
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9
A charge undergoes an acceleration. The tangential component of the electric field produced during the acceleration is

A) a maximum in the direction of the acceleration.
B) larger than the radial component.
C) decreasing in a manner that is proportional to 1/r2 from the source.
D) All of the above answers are correct.
E) None of the above answers is correct.
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10
The functional dependence of the transverse component of the radiation field produced by an accelerating charge as a function of distance from the charge is proportional to

A) r.
B) 1/r.
C) r2.
D) 1/r2.
E) none of the above.
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11
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

A) r.
B) 1/r.
C) r2.
D) 1/r2.
E) none of the above.
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12
Given a wave pulse that is traveling in the i^\hat { i } direction while its electric field is in the k^- \hat { k } direction, the magnetic field is in the

A) j^- \hat { j } direction.
B) j^ \hat {j }

direction.
C) k^+i^- \hat { k } + \hat { i } direction.
D) k^i^- \hat { k } - \hat { i } direction.
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13
A wave pulse is traveling in the j^- \hat { j } direction while its magnetic field is in the k^- \hat { k } direction. The electric field is in the

A) i^- \hat { i } direction.
B) j^ \hat {j } direction.
C) k^\hat { k } direction.
D) k^- \hat { k } direction.
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14
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 does not contribute to the theoretical description of the propagation of an electromagnetic wave pulse is

A) Bds\oint \vec { B } \cdot d \vec { s }
B) μ0I\mu _ { 0 } I
C) μ0ε0dΦEdt\mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }
D) No term in this equation is related to the propagation of the electromagnetic wave pulse.
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15
The frequency of an electromagnetic wave is 2.0×1014 Hz2.0 \times 10 ^ { 14 } \mathrm {~Hz} . The wavelength of this wave is

A) 150 nm.
B) 67 mm.
C) 1500 nm.
D) 670 nm.
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16
A gamma ray has a wavelength of 5.0×1014 m5.0 \times 10 ^ { - 14 } \mathrm {~m} . The frequency of this wave is

A) 6.0×1021 Hz6.0 \times 10 ^ { 21 } \mathrm {~Hz}
B) 6.0×1020 Hz6.0 \times 10 ^ { 20 } \mathrm {~Hz}
C) 3.0×1021 Hz3.0 \times 10 ^ { 21 } \mathrm {~Hz}
D) 15×1021 Hz15 \times 10 ^ { 21 } \mathrm {~Hz}
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17
The amplitude of the electric field of an electromagnetic wave is 6.0 ×\times 10 -3 V/m. The amplitude of the magnetic field of this wave is

A) 1.8 ×\times
106 T.
B) 1.8 ×\times
10-11 T.
C) 1.8 ×\times
10-10 T.
D) 2.0 ×\times
10-11 T.
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18
Unpolarized light with an intensity of I0 is traveling in the + x direction. The light is incident on a polarizer whose axis is aligned along the y axis. The light that passes through the polarizer has an intensity that is

A) (1/2)I0 with a polarization along the z axis.
B) (1/2)I0 with a polarization along the y axis.
C) I0 with a polarization along the z axis.
D) I0 with a polarization along the y axis.
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19
Initially polarized light is incident on a polarizer. If the intensity of the light after passing through the polarizer is (3/4) of the initial intensity, the angle between the polarizer axis and the original polarization axis of the light is

A) 41.4°.
B) 30°.
C) 48.6°.
D) 60°.
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20
Unpolarized light of intensity I0 is incident upon the first of two polarizers. The second polarizer has its preferential direction at 50° with respect to the first polarizer. The final transmitted intensity is

A) (0.21) I0.
B) (0.41) I0.
C) (0.044) I0.
D) (0.59) I0.
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21
Unpolarized light of intensity I0 is incident upon the first of two polarizers. The final transmitted intensity is (3/8)I0. With respect to the first polarizer, the second polarizer has its preferential direction at

A) 52°.
B) 41°.
C) 38°.
D) 30°.
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22
The following electromagnetic radiation has a wavelength that is closest to the size of automobile:

A) Radio waves
B) Infrared radiation
C) Visible radiation
D) Ultraviolet radiation
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23
The unit associated with an energy flux is

A) joule.
B) watt/meter.
C) watt/meter2.
D) joule/meter2.
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24
At a given point the electric field is 0.25 V/m. The energy flux at this point is

A) 1.7 ×\times
10-4 W/m2.
B) 2.8 ×\times
10-4 W/m2.
C) 8.2 ×\times
10-4 W/m2.
D) 8.2 ×\times
10-5 W/m2.
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25
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 the wave is traveling in is

A) k^\hat { k }
B) j^\hat { j }
C) - j^\hat { j }

D) i^\hat { i }
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26
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

A) k^\hat { k }
B) j^\hat { j }

C) - j^\hat { j }

D) i^\hat { i }
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27
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

A) 9.42×1015 Hz9.42 \times 10 ^ { 15 } \mathrm {~Hz}
B) 9.42×1015rad/s9.42 \times 10 ^ { 15 } \mathrm { rad } / \mathrm { s }
C) 1.5×1015 Hz1.5 \times 10 ^ { 15 } \mathrm {~Hz}
D) 9.0×105 V/m9.0 \times 10 ^ { 5 } \mathrm {~V} / \mathrm { m }
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28
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 wavelength of the wave is

A) 2.0×107 m2.0 \times 10 ^ { - 7 } \mathrm {~m}
B) 2.0×107 m2.0 \times 10 ^ { 7 } \mathrm {~m}
C) 9.99×106 m9.99 \times 10 ^ { 6 } \mathrm {~m}
D) 3.1×107 m3.1 \times 10 ^ { 7 } \mathrm {~m}
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29
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 wave number of the magnetic field associated with this wave is

A) 3.1×107 m13.1 \times 10 ^ { 7 } \mathrm {~m} ^ { - 1 }
B) 3.0×103 m13.0 \times 10 ^ { - 3 } \mathrm {~m} ^ { - 1 }
C) 3.0×105 m3.0 \times 10 ^ { 5 } \mathrm {~m}
D) 3.1×107 m3.1 \times 10 ^ { 7 } \mathrm {~m}
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30
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

A) 1.0×103 T1.0 \times 10 ^ { - 3 } \mathrm {~T}
B) 2.0×103 T2.0 \times 10 ^ { - 3 } \mathrm {~T}
C) 3.0×103 T3.0 \times 10 ^ { - 3 } \mathrm {~T}
D) 6.0×103 T6.0 \times 10 ^ { - 3 } \mathrm {~T}
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31
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

A) j^\hat { j }

B) k^\hat { k }
C) i^\hat { i }
D) Hold on. The wave is not polarized.
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32
The speed of radio waves traveling in a vacuum depends on

A) the wavelength of the waves.
B) the frequency of the waves.
C) the polarization of the waves.
D) none of the above.
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33
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

A) 1125 W/m2.
B) 2250 W/m2.
C) 4500 W/m2.
D) 9000 W/m2.
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34
A pressure of 15×106 N/m215 \times 10 ^ { - 6 } \mathrm {~N} / \mathrm { m } ^ { 2 } is due to sunlight being absorbed by a surface of a "solar sail." The energy flux incident on the surface is

A) 1125 W/m2.
B) 2250 W/m2.
C) 4500 W/m2.
D) 9000 W/m2.
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35
A wave has double the amplitude of a second wave. The energy density of the second wave is

A) four times that of the first wave.
B) double that of the first wave.
C) equal to that of the first wave.
D) half that of the first wave.
E) one-quarter that of the first wave.
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36
An electromagnetic wave with an electric field amplitude of 0.15 V/m has an intensity of

A) 1.0×105 W/m21.0 \times 10 ^ { - 5 } \mathrm {~W} / \mathrm { m } ^ { 2 }
B) 3.0×106 W/m23.0 \times 10 ^ { - 6 } \mathrm {~W} / \mathrm { m } ^ { 2 }
C) 1.0×105 W/m21.0 \times 10 ^ { - 5 } \mathrm {~W} / \mathrm { m } ^ { 2 } .
D) 3.0×105 W/m23.0 \times 10 ^ { - 5 } \mathrm {~W} / \mathrm { m } ^ { 2 } .
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37
A spherical wave spreads out from a source, and the total power at a distance of R0 is P0. At a distance of 2R0 the power is

A) P0/8.
B) P0/4.
C) P0/2.
D) P0.
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38
A spherical wave spreads out from a source, and the energy flux at a distance of R0 is S0. At a distance of 2R0 the energy flux is

A) S0/8.
B) S0/4.
C) S0/2.
D) S0.
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39
An electromagnetic wave consists of

A) only an electric field.
B) only a magnetic field.
C) an electric field and a magnetic field oriented parallel to each other.
D) an electric field and a magnetic field oriented perpendicular to each other.
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40
The direction of propagation of an electromagnetic wave is given by

A) EB\vec { E } \cdot \vec { B }
B) EB- \vec { E } \cdot \vec { B }
C) E×B\vec { E } \times \vec { B }
D) B×E\vec { B } \times \vec { E }
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41
Stationary charges produce

A) electromagnetic waves.
B) only magnetic fields.
C) only electric fields.
D) both electric and magnetic fields.
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42
Accelerating charges produce

A) electromagnetic standing waves.
B) only magnetic fields.
C) only electric fields.
D) both electric and magnetic fields.
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43
ε0\varepsilon _ { 0 } is related to the speed of light and the permeability of free space through the relation

A) ε0=c2μ0\varepsilon _ { 0 } = c ^ { 2 } \mu _ { 0 }
B) ε0=c2μ0\varepsilon _ { 0 } = \frac { c ^ { 2 } } { \mu _ { 0 } }
C) ε0=1c2μ0\varepsilon _ { 0 } = \frac { 1 } { c ^ { 2 } \mu _ { 0 } }
D) ε0=μ0c2\varepsilon _ { 0 } = \frac { \mu _ { 0 } } { c ^ { 2 } }
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44
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

A) 1 μ\mu s.
B) 10 μ\mu s.
C) 100 μ\mu s.
D) 1 ms.
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45
Consider a 150-W incandescent lightbulb that radiates light in all directions. At a distance of 1.5 m the time-averaged energy flux emitted by the bulb is

A) 7.9 W/m2.
B) 5.3 W/m2.
C) 100 W/m2.
D) 67 W/m2.
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46
Consider a 150-W incandescent lightbulb that radiates light in all directions. At a distance of 1.5 m the amplitude of the oscillating electric field E0 is

A) 77 V/m.
B) 63 V/m.
C) 225 V/m.
D) 39 V/m.
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47
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

A) 2.6×107 T2.6 \times 10 ^ { - 7 } \mathrm {~T}
B) 2.1×107 T2.1 \times 10 ^ { - 7 } \mathrm {~T}
C) 7.5×107 T7.5 \times 10 ^ { - 7 } \mathrm {~T}
D) 1.3×107 T1.3 \times 10 ^ { - 7 } \mathrm {~T}
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48
The electric field component of an electromagnetic wave is 130 V/m. The electric energy density of the wave is

A) 7.5×108 J7.5 \times 10 ^ { - 8 } \mathrm {~J}
B) 7.5×108 J/m7.5 \times 10 ^ { - 8 } \mathrm {~J} / \mathrm { m }
C) 7.5×108 J/m27.5 \times 10 ^ { - 8 } \mathrm {~J} / \mathrm { m } ^ { 2 }
D) 7.5×108 J/m37.5 \times 10 ^ { - 8 } \mathrm {~J} / \mathrm { m } ^ { 3 }
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49
The magnetic field component of an electromagnetic wave is 25 μT\mu \mathrm { T } . The electric energy density of the wave is

A) 2.5×104 J/m32.5 \times 10 ^ { - 4 } \mathrm {~J} / \mathrm { m } ^ { 3 }
B) 2.5×104 J/m22.5 \times 10 ^ { - 4 } \mathrm {~J} / \mathrm { m } ^ { 2 }
C) 2.5×102 J/m32.5 \times 10 ^ { - 2 } \mathrm {~J} / \mathrm { m } ^ { 3 }
D) 2.5×102 J/m22.5 \times 10 ^ { - 2 } \mathrm {~J} / \mathrm { m } ^ { 2 }
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50
Radiation from a source is striking a surface at a rate of 50 W/m2. The peak value of the electric field is

A) 110 V/m.
B) 150 V/m.
C) 190 V/m.
D) 250 V/m.
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