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Ch. 31 - Maxwell's Equations and Electromagnetic Waves
Giancoli Douglas - Physics for Scientists and Engineers 5th edition
Giancoli Douglas5th editionPhysics for Scientists and EngineersISBN: 9780137488179Not the one you use?Change textbook
Chapter 30, Problem 78b

Suppose that a right-moving EM wave overlaps with a left-moving EM wave so that, in a certain region of space, the total electric field in the y direction and magnetic field in the z direction are given by Eᵧ = E₀ sin(kx - ωt) + E₀ sin(kx + ωt) and Bz = B₀ sin(kx - ωt) - B₀ sin(kx + ωt). Determine the Poynting vector and find the x locations at which it is zero at all times.

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Step 1: Recall the formula for the Poynting vector, which represents the energy flux of an electromagnetic wave. It is given by **S = E × B / μ₀**, where E is the electric field, B is the magnetic field, and μ₀ is the permeability of free space. Here, we are tasked with finding the Poynting vector using the given expressions for Eᵧ and Bz.
Step 2: Substitute the given expressions for Eᵧ and Bz into the formula for the Poynting vector. The electric field is **Eᵧ = E₀ sin(kx - ωt) + E₀ sin(kx + ωt)**, and the magnetic field is **Bz = B₀ sin(kx - ωt) - B₀ sin(kx + ωt)**. The cross product of these fields will give the Poynting vector.
Step 3: Simplify the expressions for the electric and magnetic fields using trigonometric identities. For the electric field, use the identity **sin(A) + sin(B) = 2 sin((A + B)/2) cos((A - B)/2)**. Similarly, for the magnetic field, use **sin(A) - sin(B) = 2 cos((A + B)/2) sin((A - B)/2)**. This will help express the fields in terms of simpler trigonometric functions.
Step 4: Compute the cross product **E × B**. Since the electric field is in the y-direction and the magnetic field is in the z-direction, the resulting Poynting vector will point in the x-direction. After simplifying, determine the conditions under which the Poynting vector is zero. This occurs when the product of the electric and magnetic field components is zero.
Step 5: Analyze the resulting expression for the Poynting vector to find the x-locations where it is zero at all times. This will involve solving for the positions where the trigonometric terms in the simplified expression cancel out. Specifically, identify the values of x that satisfy the condition for zero energy flux.

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Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Electromagnetic Waves

Electromagnetic (EM) waves are oscillations of electric and magnetic fields that propagate through space. They are characterized by their wavelength, frequency, and speed, which is the speed of light in a vacuum. The electric field (E) and magnetic field (B) are perpendicular to each other and to the direction of wave propagation, following Maxwell's equations. Understanding the behavior of these waves is crucial for analyzing their interactions and superpositions.
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Superposition Principle

The superposition principle states that when two or more waves overlap in space, the resultant wave is the sum of the individual waves. This principle applies to all types of waves, including EM waves, and allows for the analysis of complex wave patterns. In the given problem, the total electric and magnetic fields are derived from the superposition of two EM waves moving in opposite directions, leading to interference patterns that can be analyzed mathematically.
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Poynting Vector

The Poynting vector represents the directional energy flux (the rate of energy transfer per unit area) of an electromagnetic field. It is calculated using the formula S = (1/μ₀)(E × B), where E is the electric field, B is the magnetic field, and μ₀ is the permeability of free space. The Poynting vector is essential for understanding how energy is transported by EM waves, and finding locations where it is zero indicates points of destructive interference in the wave patterns.
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