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A sinusoidal electromagnetic wave emitted by a cellular phone has a wavelength of \(35.4 \mathrm{~cm}\) and an electric-field amplitude of \(5.40 \times 10^{-2} \mathrm{~V} / \mathrm{m}\) at a distance of \(250 \mathrm{~m}\) from the phone. \(\mathrm{Cal}-\) culate (a) the frequency of the wave; (b) the magnetic-field amplitude; (c) the intensity of the wave.

Short Answer

Expert verified
Frequency: ~8.47 x 10^8 Hz; Magnetic field: ~1.80 x 10^-10 T; Intensity: ~3.88 x 10^-3 W/m^2.

Step by step solution

01

Convert Wavelength to Meters

The given wavelength is 35.4 cm. To convert this to meters, divide by 100: \[\lambda = \frac{35.4}{100} = 0.354 \text{ meters}\]
02

Calculate the Speed of Light

The speed of light in a vacuum is a constant: \[ c = 3 \times 10^8 \text{ meters/second} \]
03

Calculate the Frequency of the Wave

The frequency \( f \) of a wave is calculated by the formula: \[ f = \frac{c}{\lambda} \]Substitute the values:\[ f = \frac{3 \times 10^8}{0.354} \approx 8.47 \times 10^8 \text{ Hz} \]
04

Calculate the Magnetic-field Amplitude

The relation between the electric field \( E \), magnetic field \( B \), and speed of light \( c \) is given by:\[ c = \frac{E}{B} \] Rearranging gives the magnetic field amplitude: \[ B = \frac{E}{c} \] Substitute the given electric field and speed of light:\[ B = \frac{5.40 \times 10^{-2}}{3 \times 10^8} \approx 1.80 \times 10^{-10} \text{ T} \]
05

Calculate the Intensity of the Wave

The intensity \( I \) of a wave can be calculated using the formula:\[ I = \frac{1}{2} \epsilon_0 c E^2 \]where \( \epsilon_0 = 8.85 \times 10^{-12} \text{ F/m} \).Substitute the values:\[ I = \frac{1}{2} (8.85 \times 10^{-12}) (3 \times 10^8) (5.40 \times 10^{-2})^2 \approx 3.88 \times 10^{-3} \text{ W/m}^2 \]

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Frequency Calculation
Electromagnetic waves, such as the ones emitted by a cellular phone, are characterized by their frequency. The frequency of a wave is the number of complete wave cycles that pass a given point per second. It's denoted by the symbol \( f \) and is measured in Hertz (Hz).
Calculating the frequency involves knowing the wavelength, which is the distance between successive crests of a wave. In our exercise, the wavelength \( \lambda \) is given as 35.4 cm. To work with it in equations, it must be converted to meters: \( \lambda = 0.354 \text{ m} \).
Since the speed of light \( c \) is a constant \( 3 \times 10^8 \text{ m/s} \) for all electromagnetic waves in a vacuum, the frequency can be determined using the formula:
  • \( f = \frac{c}{\lambda} \)
By plugging in the values, we find the frequency to be approximately \( 8.47 \times 10^8 \text{ Hz} \). This value tells us how rapidly the wave oscillates in space, an important characteristic of electromagnetic waves.
Magnetic Field Amplitude
The magnetic field amplitude \( B \) describes the strength of the magnetic field in the electromagnetic wave. Electromagnetic waves have both electric and magnetic fields. These fields oscillate perpendicular to each other and to the direction of wave propagation.
Electric field amplitude \( E \) can help calculate the magnetic field amplitude using the wave speed. The speed of light \( c \) sets the relationship between these amplitudes, given by the equation:
  • \( c = \frac{E}{B} \)
Rearranging this formula allows us to solve for \( B \):
  • \( B = \frac{E}{c} \)
By substituting the given value for the electric field amplitude \( E = 5.40 \times 10^{-2} \text{ V/m} \) and the speed of light, we find that \( B \approx 1.80 \times 10^{-10} \text{ T} \). This shows how weak the magnetic field component is compared to the electric field in such electromagnetic waves.
Intensity of Waves
The intensity of an electromagnetic wave indicates how much energy the wave conveys per unit time per unit area. It is a crucial factor in understanding the power of a wave.
The expression for intensity \( I \) of an electromagnetic wave is:
  • \( I = \frac{1}{2} \epsilon_0 c E^2 \)
Here \( \epsilon_0 \), the vacuum permittivity, is a constant \( 8.85 \times 10^{-12} \text{ F/m} \). By inserting the known values for \( E \), \( c \), and \( \epsilon_0 \) into the equation, we can compute the intensity:
\[ I = \frac{1}{2} (8.85 \times 10^{-12}) (3 \times 10^8) (5.40 \times 10^{-2})^2 \]
Leading to an intensity of approximately \( 3.88 \times 10^{-3} \text{ W/m}^2 \).
This value gives us a measure of how much electromagnetic energy is passing through a square meter of area in one second.

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Most popular questions from this chapter

An electromagnetic wave has an electric field given by \(\overrightarrow{\boldsymbol{E}}(y, t)=\left(3.10 \times 10^{5} \mathrm{~V} / \mathrm{m}\right) \hat{k} \cos \left[\mathrm{ky}-\left(12.65 \times 10^{12} \mathrm{rad} / \mathrm{s}\right) t\right]\) (a) In which direction is the wave traveling? (b) What is the wavelength of the wave? (c) Write the vector equation for \(\vec{B}(y, t)\)

An electromagnetic standing wave in a certain material has frequency \(1.20 \times 10^{10} \mathrm{~Hz}\) and speed of propagation \(2.10 \times\) \(10^{8} \mathrm{~m} / \mathrm{s}\). (a) What is the distance between a nodal plane of \(\overrightarrow{\boldsymbol{B}}\) and the closest antinodal plane of \(\overrightarrow{\boldsymbol{B}}\) ? (b) What is the distance between an antinodal plane of \(\overrightarrow{\boldsymbol{E}}\) and the closest antinodal plane of \(\overrightarrow{\boldsymbol{B}}\) ? (c) What is the distance between a nodal plane of \(\overrightarrow{\boldsymbol{E}}\) and the closest nodal plane of \(\overrightarrow{\boldsymbol{B}}\) ?

Very short pulses of high-intensity laser beams are used to repair detached portions of the retina of the eye. The brief pulses of energy absorbed by the retina weld the detached portions back into place. In one such procedure, a laser beam has a wavelength of \(810 \mathrm{~nm}\) and delivers \(250 \mathrm{~mW}\) of power spread over a circular spot \(510 \mu \mathrm{m}\) in diameter. The vitreous humor (the transparent fluid that fills most of the eye) has an index of refraction of \(1.34\). (a) If the laser pulses are each \(1.50 \mathrm{~ms}\) long. how much energy is delivered to the retina with each pulse? (b) What average pressure does the pulse of the laser beam exert on the retina as it is fully absorbed by the circular spot? (c) What are the wavelength and frequency of the laser light inside the vitreous humor of the eye? (d) What are the maximum values of the electric and magnetic fields in the laser beam? ?

If the eye receives an average intensity greater than \(1.0 \times 10^{2} \mathrm{~W} / \mathrm{m}^{2}\), damage to the retina can occur. This quantity is called the damage threshold of the retina. (a) What is the largest average power (in \(\mathrm{mW}\) ) that a laser beam \(1.5 \mathrm{~mm}\) in diameter can have and still be considered safe to view head-on? (b) What are the maximum values of the electric and magnetic fields for the beam in part (a)? (c) How much energy would the beam in part (a) deliver per second to the retina? (d) Express the damage threshold in \(\mathrm{W} / \mathrm{cm}^{2} .\)

Radio station WCCO in Minneapolis broadcasts at a frequency of \(830 \mathrm{kHz}\). At a point some distance from the transmitter, the magnetic- field amplitude of the electromagnetic wave from WCCO is \(4.82 \times 10^{-11} \mathrm{~T}\). Calculate (a) the wavelength; (b) the wave number; (c) the angular frequency; (d) the electric-field amplitude.

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