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An electromagnetic wave with frequency \(65.0 \mathrm{~Hz}\) travels in an insulating magnetic material that has dielectric constant \(3.64\) and relative permeability \(5.18\) at this frequency. The electric field has amplitude \(7.20 \times 10^{-3} \mathrm{~V} / \mathrm{m}\). (a) What is the speed of propagation of the wave? (b) What is the wavelength of the wave? (c) What is the amplitude of the magnetic field?

Short Answer

Expert verified
The speed of propagation is approximately \(7.80 \times 10^7 \text{ m/s}\). The wavelength is \(1.20 \times 10^6 \text{ m}\). The magnetic field amplitude is \(9.23 \times 10^{-11} \text{ T}\).

Step by step solution

01

Speed of Propagation

The speed of propagation of an electromagnetic wave in a medium is given by \( v = \frac{c}{\sqrt{\varepsilon_r \mu_r}} \), where \( c \) is the speed of light in vacuum \( (c = 3 \times 10^8 \, \text{m/s}) \), \( \varepsilon_r \) is the dielectric constant, and \( \mu_r \) is the relative permeability. Plugging in the given values, we have:\[ v = \frac{3 \times 10^8}{\sqrt{3.64 \times 5.18}} \approx 7.80 \times 10^7 \, \text{m/s} \]
02

Calculate the Wavelength

The wavelength \( \lambda \) of the wave can be calculated using the formula \( \lambda = \frac{v}{f} \), where \( v \) is the speed of propagation we just calculated, and \( f \) is the frequency.\[ \lambda = \frac{7.80 \times 10^7}{65.0} \approx 1.20 \times 10^6 \, \text{m} \]
03

Amplitude of the Magnetic Field

The amplitude of the magnetic field \( B_0 \) can be found using the relationship \( B_0 = \frac{E_0}{v} \), where \( E_0 \) is the amplitude of the electric field and \( v \) is the speed of propagation.\[ B_0 = \frac{7.20 \times 10^{-3}}{7.80 \times 10^7} \approx 9.23 \times 10^{-11} \, \text{T} \]

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Key Concepts

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

Dielectric Constant
The dielectric constant is an important property of materials when discussing electromagnetic waves. It tells us how much a material can store electrical energy in an electric field compared to a vacuum. It's like how a sponge can hold water better than a plain surface. The greater the dielectric constant, the more energy it can store. For instance, the material in the given problem has a dielectric constant of 3.64. This value indicates its capacity to reduce the speed of the electromagnetic wave compared to its speed in a vacuum.

The dielectric constant is represented as \( \varepsilon_r \). Its influence on wave speed is seen through the equation \( v = \frac{c}{\sqrt{\varepsilon_r \mu_r}} \), where \( c \) is the speed of light in a vacuum. Larger values of \( \varepsilon_r \) lead to a smaller wave speed. Understanding this concept helps in figuring out how electromagnetic waves interact with different materials.
Relative Permeability
Relative permeability is similar to the dielectric constant but deals with magnetic fields. It measures how easily a material can become magnetized, or in simpler terms, how well it supports the formation of a magnetic field. The relative permeability is denoted as \( \mu_r \).

When electromagnetic waves pass through a magnetic material, \( \mu_r \) affects the wave's speed. In the exercise, \( \mu_r = 5.18 \), which means this material supports magnetic fields much more than a standard non-magnetic material would. This value, along with the dielectric constant, determines how much the electromagnetic wave slows down in the material compared to its speed in a vacuum. It's crucial because recognizing how materials magnetize helps us understand and manipulate electromagnetic fields in various applications.
Wave Speed
The speed at which an electromagnetic wave travels through a medium is a fundamental concept in physics. In a vacuum, electromagnetic waves travel at the speed of light, \( c \), which is approximately \(3 \times 10^8 \text{ m/s} \). However, in every other medium, the speed is slower due to the material’s properties, specifically the dielectric constant \(\varepsilon_r\) and relative permeability \(\mu_r\).

To calculate the wave speed \( v \), the formula \( v = \frac{c}{\sqrt{\varepsilon_r \mu_r}} \) is used. In the example problem, plugging in \(\varepsilon_r = 3.64\) and \(\mu_r = 5.18\) results in a calculated wave speed of about \(7.80 \times 10^7 \text{ m/s}\). Understanding wave speed is important for predicting how waves behave in different environments.
Wavelength Calculation
Wavelength describes the distance between consecutive peaks of the wave, and it's a crucial property when examining waves. It is often represented by the symbol \(\lambda\). Knowing the wavelength helps in determining how waves interact with objects and the energy they carry.

To find the wavelength, use the equation \( \lambda = \frac{v}{f} \), where \( f \) is the frequency of the wave, and \( v \) is the wave speed. In the problem provided, the wave speed is \(7.80 \times 10^7 \text{ m/s}\) and the frequency is \(65.0 \text{ Hz}\). By substitution, you get a wavelength of approximately \(1.20 \times 10^6 \text{ m}\). Calculating wavelength is essential for applications such as signal broadcast, communication technologies, and radar systems.
Magnetic Field Amplitude
The magnetic field amplitude is a measure of the maximum strength of the magnetic field component in an electromagnetic wave. It's usually denoted as \( B_0 \). Understanding the amplitude is important because it relates to the energy carried by the wave, affecting how it interacts with its surroundings.

To find the amplitude of the magnetic field, use the relationship \( B_0 = \frac{E_0}{v} \), where \( E_0 \) is the electric field amplitude and \( v \) is the wave speed. From the given problem, with \( E_0 = 7.20 \times 10^{-3} \text{ V/m}\) and \( v = 7.80 \times 10^7 \text{ m/s}\), the computation results in a magnetic field amplitude \( B_0 \) of about \(9.23 \times 10^{-11} \text{ T}\). Knowing the magnetic field amplitude is crucial for predicting how waves will affect electronic and magnetic devices.

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Most popular questions from this chapter

Testing a Space Radio Transmitter. You are a NASA mission specialist on your first flight aboard the space shuttle. Thanks to your extensive training in physics, you have been assigned to evaluate the performance of a new radio transmitter on board the International Space Station (ISS). Perched on the shuttle's movable arm, you aim a sensitive detector at the ISS, which is \(2.5 \mathrm{~km}\) away. You find that the electric-field amplitude of the radio waves coming from the ISS transmitter is \(0.090 \mathrm{~V} / \mathrm{m}\) and that the frequency of the waves is \(244 \mathrm{MHz}\). Find the following: (a) the intensity of the radio wave at your location; (b) the magnetic-field amplitude of the wave at your location; (c) the total power output of the ISS radio transmitter. (d) What assumptions, if any, did you make in your calculations?

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 \(\vec{B}(y, t)\)

The electric field of a sinusoidal electromagnetic wave obeys the equation \(E=(375 \mathrm{~V} / \mathrm{m}) \cos \left[\left(1.99 \times 10^{7} \mathrm{rad} / \mathrm{m}\right) x+\right.\) \(\left.\left(5.97 \times 10^{15} \mathrm{rad} / \mathrm{s}\right) t\right] .\) (a) What are the amplitudes of the electric and magnetic fields of this wave? (b) What are the frequency, wavelength, and period of the wave? Is this light visible to humans? (c) What is the speed of the wave?

Consider each of the following electric-and magnetic-field orientations. In each case, what is the direction of propagation of the wave? (a) \(\vec{E}=E \hat{i}, \overrightarrow{\boldsymbol{B}}=-B \hat{j} ;\) (b) \(\overrightarrow{\boldsymbol{E}}=E \hat{\boldsymbol{J}}, \overrightarrow{\boldsymbol{B}}=B \hat{\boldsymbol{i}} ;\) (c) \(\vec{E}=\) \(-E \hat{k}, \vec{B}=-B \hat{i} ;(\) d) \(\vec{E}=E \hat{i}, \vec{B}=-B \hat{k}\).

You want to support a sheet of fireproof paper horizontally, using only a vertical upward beam of light spread uniformly over the sheet. There is no other light on this paper. The sheet measures \(22.0 \mathrm{~cm}\) by \(28.0 \mathrm{~cm}\) and has a mass of \(1.50 \mathrm{~g}\). (a) If the paper is black and hence absorbs all the light that hits it, what must be the intensity of the light beam? (b) For the light in part (a), what are the amplitudes of its electric and magnetic fields? (c) If the paper is white and hence reflects all the light that hits it, what intensity of light beam is needed to support it? (d) To see if it is physically reasonable to expect to support a sheet of paper this way, calculate the intensity in a typical \(0.500-\mathrm{mW}\) laser beam that is \(1.00 \mathrm{~mm}\) in diameter, and compare this value with your answer in part (a).

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