Exploring Wave Equation Solutions for E-fields

In summary, the conversation discusses the relationship between Electric and Magnetic fields, and how they are perpendicular to each other and to the direction of propagation. It also mentions the solution to the wave equation for E-fields and how it leads to E being a constant. The conversation ends with a question about why Ex and Ey are not also constant. The response explains that this is because they vary along the direction of propagation, making them a plane wave.
  • #1
dyn
773
61
Hi.
I'm following the "derivation" in some lecture notes which shows that the Electric and Magnetic fields are perpendicular to each other and to the direction of propagation. There are 2 points I don't understand

A solution to the wave equation for E-fields is given as E = E0 exp i(ωt-kz).
It then states that if the propagation is along z only then ∂/∂x and ∂/∂y of any property is zero. Why is this so ?

Using Gauss's law this then leads to ∂Ez/∂z = 0 which implies Ez is a constant which is set to zero. But we also have ∂Ex/∂x = 0 and ∂Ey/∂y = 0 so why aren't Ex and Ey equal to a constant which can be set to zero ? I realize this would give no wave.
Thanks
 
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  • #2
dyn said:
It then states that if the propagation is along z only then ∂/∂x and ∂/∂y of any property is zero. Why is this so ?
That is what defines a plane wave. They vary only along the direction of propagation, and they are uniform in the plane normal to that direction. Not all waves behave this way, but those that do are called plane waves.
 

1. What is the wave equation for E-fields?

The wave equation for E-fields is a mathematical representation of how electric fields propagate through space. It is given by d2E/dt2 = c22E, where E is the electric field, t is time, c is the speed of light, and is the gradient operator.

2. How is the wave equation solved for E-fields?

The wave equation for E-fields can be solved by using various mathematical techniques, such as separation of variables, Fourier transforms, or Green's functions. These methods allow us to find the general solution to the wave equation, which can then be applied to specific boundary conditions to obtain a particular solution.

3. What are the applications of exploring wave equation solutions for E-fields?

Exploring wave equation solutions for E-fields has a wide range of applications in various fields of science and engineering. It is used to understand the behavior of electromagnetic waves, design and analyze electrical circuits, and develop technologies such as antennas, radar, and wireless communication systems.

4. What are some challenges in solving the wave equation for E-fields?

One of the main challenges in solving the wave equation for E-fields is dealing with complex boundary conditions and geometries. This requires advanced mathematical techniques and numerical methods to obtain accurate solutions. Additionally, the wave equation is a second-order partial differential equation, which can be difficult to solve analytically.

5. How does the solution to the wave equation for E-fields relate to Maxwell's equations?

The wave equation for E-fields is derived from Maxwell's equations, which describe the fundamental laws of electromagnetism. Specifically, the wave equation is a combination of two of Maxwell's equations: Gauss's law for electric fields and Faraday's law of induction. Therefore, the solution to the wave equation is a manifestation of the principles described by Maxwell's equations.

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