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Magnetic Component Two The magnetic component of a polarized wave of light is $$ B_{x}=\left(4.0 \times 10^{-6} \mathrm{~T}\right) \sin \left[\left(1.57 \times 10^{7} \mathrm{~m}^{-1}\right) y+\omega t\right] $$ (a) Parallel to which axis is the light polarized? What are the (b) frequency and (c) intensity of the light?

Short Answer

Expert verified
The light is polarized parallel to the z-axis. The frequency is approximately \(7.5 \times 10^{14} \mathrm{~Hz}\), and the intensity is approximately \(1.4 \times 10^3 \mathrm{~W/m^2}\).

Step by step solution

01

- Identify axis of polarization

The magnetic component of the wave is given as \(B_x\). Since \(B_x\) is along the x-axis, and considering that the magnetic field in an electromagnetic wave is perpendicular to the direction of propagation, the light must be polarized parallel to the z-axis.
02

- Determine the frequency

The wave number (k) is given as \(1.57 \times 10^7 \mathrm{~m}^{-1}\). The relationship between the wave number (k) and the wavelength (λ) is \(k = \frac{2\pi}{\lambda}\). Therefore, \[\lambda = \frac{2\pi}{k} = \frac{2\pi}{1.57 \times 10^7 \mathrm{~m}^{-1}} \approx 4.0 \times 10^{-7} \mathrm{~m}\]. The speed of light (c) is approximately \(3 \times 10^8 \mathrm{~m/s}\). The frequency (f) can be found using the relationship \(c = f\lambda\). Thus, \[ f = \frac{c}{\lambda} = \frac{3 \times 10^8 \mathrm{~m/s}}{4.0 \times 10^{-7} \mathrm{~m}} = 7.5 \times 10^{14} \mathrm{~Hz}\].
03

- Calculate the intensity

The intensity (I) of an electromagnetic wave can be calculated using the formula \[ I = \frac{c}{2\mu_0}E_0^2 \], where \(E_0\) is the amplitude of the electric field. First, find the amplitude of the electric field (\(E_0\)) using the relationship between the magnetic field and the electric field in a polarized electromagnetic wave: \(E_0 = cB_0\). Here, \(B_0 = 4.0 \times 10^{-6} \mathrm{~T}\) and \(c = 3 \times 10^8 \mathrm{~m/s}\). Thus, \[ E_0 = 3 \times 10^8 \mathrm{~m/s} \times 4.0 \times 10^{-6} \mathrm{~T} = 1200 \mathrm{~V/m} \]. Next, use this to find the intensity:\[ I = \frac{(3 \times 10^8 \mathrm{~m/s})(1200 \mathrm{~V/m})^2}{2(4\pi \times 10^{-7} \mathrm{~T} \cdot \mathrm{m/A})} \approx 1.4 \times 10^3 \mathrm{~W/m^2} \].

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Key Concepts

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

Polarization of Light
Polarization refers to the orientation of the oscillations of the electromagnetic waves. Light waves oscillate in different directions perpendicular to the direction of the wave's travel. In the given problem, the magnetic component of the light wave, denoted as \(B_x\), is oriented along the x-axis. This tells us that the electric field component Must be oscillating in a direction perpendicular to both the magnetic field and the direction of light propagation. Since the light propagates along the y-axis, and considering the perpendicular nature of electric and magnetic fields in electromagnetic waves, the light is polarized along the z-axis.
Frequency Calculation
Frequency is the number of oscillations of a wave that pass a particular point per second. The wave number \(k\) given is \(1.57 \times 10^7 \mathrm{~m^{-1}}\). The wave number is related to the wavelength \(\lambda\) as follows: \[ \lambda = \frac{2 \pi}{k} = \frac{2 \pi}{1.57 \times 10^7 \mathrm{~m^{-1}}} \approx 4.0 \times 10^{-7} \m \] Using the speed of light \(c\) which is approximately \(3 \times 10^8 \mathrm{~m/s}\), we can find the frequency \(f\) using the relationship \[ f = \frac{c}{\lambda} = \frac{3 \times 10^8 \mathrm{~m/s}}{4.0 \times 10^{-7} \m} \approx 7.5 \times 10^{14} \mathrm{~Hz} \] So the frequency of the light is \(7.5 \times 10^{14} \mathrm{~Hz}\).
Intensity of Light
Intensity of light describes the amount of energy a wave carries per unit area per unit of time. To calculate the intensity, we use \( I = \frac{c}{2 \mu_0} E_0^2 \). Here \( E_0\) is the maximum amplitude of the electric field, which can be determined by the relationship between the electric and magnetic fields in light waves: \(E_0 = c B_0 \). Given \( B_0 = 4.0 \times 10^{-6} \mathrm{~T}\) and \( c = 3 \times 10^8 \mathrm{~m/s}\), we get: \[ E_0 = 3 \times 10^8 \mathrm{~m/s} \times 4.0 \times 10^{-6} \,\r{~T} = 1200 \mathrm{~V/m} \] Now substitute \( E_0 \) into the intensity formula: \[ I = \frac{(3 \times 10^8 \mathrm{~m/s})(1200 \mathrm{~V/m})^2}{2 (4\pi \times 10^{-7} \mathrm{~T \cdot m/A})} \approx 1.4 \times 10^3 \mathrm{~W/m^2} \] Therefore, the intensity of the light is approximately \( 1.4 \times 10^{3} \mathrm{~W/m^{2}}\).
Wave Number
Wave number represents the number of wavelengths per unit of distance and is denoted by \(k\). It quantifies the spatial frequency of the wave and is calculated as the reciprocal of the wavelength multiplied by \(2 \pi\): \[ k = \frac{2 \pi}{\lambda} \] In our problem, it is given directly as \( 1.57 \times 10^7 \mathrm{~m^{-1}}\). Understanding the wave number helps in determining various other properties of the wave, such as wavelength and frequency. It is a critical value in analyzing wave interaction with materials and various medium characteristics.
Speed of Light
The speed of light in a vacuum is a fundamental constant denoted by \(c\) and is approximately \(3 \times 10^{8} \mathrm{~m/s}\). This value is essential for calculating other properties of electromagnetic waves, including frequency and wavelength, using the relationship \( c = f \lambda \). The speed of light remains constant in a vacuum, but when light travels through different mediums, its speed can change, affecting other properties like refraction.

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Most popular questions from this chapter

At a beach the light is generally partially polarized due to reflections off sand and water. At a particular beach on a particular day near sundown, the horizontal component of the electric field vector is \(2.3\) times the vertical component. A standing sunbather puts on polarizing sunglasses; the glasses eliminate the horizontal field component. (a) What fraction of the light intensity received before the glasses were put on now reaches the sunbather's eyes? (b) The sunbather, still wearing the glasses, lies on his side. What fraction of the light intensity received before the glasses were put on now reaches his eyes?

What is the radiation pressure \(1.5 \mathrm{~m}\) away from a \(500 \mathrm{~W}\) lightbulb? Assume that the surface on which the pressure is exerted faces the bulb and is perfectly absorbing and that the bulb radiates uniformly in all directions.

Some neodymium-glass lasers can provide 100 terawatts of power in \(1.0 \mathrm{~ns}\) pulses at a wavelength of \(0.26 \mu \mathrm{m}\). How much energy is contained in a single pulse?

An unpolarized beam of light is sent through a stack of four polarizing sheets, oriented so that the angle between the polarizing directions of adjacent sheets is \(30^{\circ} .\) What fraction of the incident intensity is transmitted by the system?

Although light appears to travel at a speed that is for all practical purposes infinite, for some modern purposes the time delay due to light travel time is of great importance. The Global Positioning System (GPS) allows you to determine your position from comparison of the time delays between radio signals from 4 satellites at a height of \(20,000 \mathrm{~km}\) above the surface of the earth. (There are actually 24 of these satellites. Your GPS picks out the closest 4 to your current position.) In order to get some idea of how important the speed of light is in establishing your position with one of these gadgets, make some simple assumptions. Assume that a satellite is almost directly overhead. Then figure out how far the satellite will move in the time it takes light (the radio signal) to get from the satellite to your GPS receiver. This estimates how far off the reading of your position would be if your device didn't include the speed of light in its calculations. To do this: (a) Figure out what speed the satellite must be traveling to be in a circular orbit. (b) Estimate the time it would take for a radio signal to get from the satellite to your receiver. (c) Estimate how far the satellite would move in that time. If you ignore light travel time, this tells about how wrong you would get the satellite's position (and therefore how wrong you would get your position).

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