The Plane Electromagnetic Wave in Vacuum

In summary, the conversation discusses the representation of a plane electromagnetic wave in vacuum, the wave velocity and Lorentz transformations, and the formulas for relativistic Doppler Effect. It is argued that the value of {\frac{\omega}{k}} should not change after transformation, but it is also noted that mistakes in math may cause changes. The conversation concludes with the acknowledgement that understanding how to derive the formulas is important.
  • #1
Anamitra
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A plane electromagnetic wave[traveling in the x-direction in an inertial frame]in vacuum is usually represented by an equation of the form:

[tex]{E}{=}{E_{0}}{exp{[}{i}{(}{k}{x}{-}{\omega}{t}{)}{]}}[/tex]

The wave velocity[phase velocity] is given by:

[tex]{c}{=}{\frac{\omega}{k}}[/tex]

We can perform Lorentz transformation on t and x[and y,z] to some other inertial frame moving in the x-x' direction.

The value [tex]{\frac{\omega}{k}}[/tex] changes after transformation.But the value of c [wave velocity=phase velocity]should not change.
How does one explain this?
[If one considers a wave packet in vacuum each component should have the same speed=c]
 
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  • #2
Anamitra said:
The value [tex]{\frac{\omega}{k}}[/tex] changes after transformation.
No it doesn't. You must have made a mistake in your math.
 
  • #3
[tex]{t}{=}{\gamma}{(}{t^{'}}{+}{\frac{vx^{'}}{c^{2}}{)}[/tex]
[tex]{x}{=}{\gamma}{(}{x^{'}}{+}{vt^{'}}{)}[/tex]

[tex]{{k}{x}{-}{\omega}{t}}{=}{x^{'}}{\gamma}{(}{k}{-}{v}{/}{c^{2}}{)}{-}{{t}^{'}}{\gamma}{(}{\omega}{-}{kv}{)}[/tex]

[tex]{\frac{{\omega}^{'}}{k^{'}}}{=}{\frac{{\omega}{-}{kv}}{{k}{-}{{v}{\omega}{/}{c^{2}}}[/tex]
 
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  • #4
Yes, you almost have it. Now just make the substitution:
[tex]\omega=ck[/tex]
And simplify.
 
  • #5
Dalespam is of course correct. Thanks for that.

In fact we can get the formulas for relativistic Doppler Effect from the transformations of "omega" and "k" in the formulas of thread #3, without any reference to the position/location of the source[there is a small typing error in the second last formula of thread #3]
 
  • #6
Anamitra said:
In fact we can get the formulas for relativistic Doppler Effect from the transformations of "omega" and "k" in the formulas of thread #3, without any reference to the position/location of the source
Yes, that is a very useful formula. I am glad you know how to derive it. I think that is a deeper level of understanding than just using the formula.
 

1. What is a plane electromagnetic wave in vacuum?

A plane electromagnetic wave in vacuum is a type of electromagnetic radiation that travels in a straight line and does not require a medium to propagate. It consists of perpendicular electric and magnetic fields that oscillate at right angles to each other and to the direction of wave propagation.

2. How is the speed of a plane electromagnetic wave in vacuum determined?

The speed of a plane electromagnetic wave in vacuum is determined by the properties of the medium it is traveling through. In a vacuum, the speed of light is approximately 299,792,458 meters per second, which is the maximum speed at which any object or information can travel in the universe.

3. What is the relationship between the wavelength and frequency of a plane electromagnetic wave in vacuum?

The wavelength and frequency of a plane electromagnetic wave in vacuum are inversely proportional. This means that as the frequency increases, the wavelength decreases, and vice versa. This relationship is described by the equation: c = λν, where c is the speed of light, λ is the wavelength, and ν is the frequency.

4. How do plane electromagnetic waves behave when they encounter obstacles or boundaries?

When plane electromagnetic waves encounter obstacles or boundaries, they can be reflected, refracted, or diffracted. The behavior of the waves depends on the properties of the obstacle or boundary and the angle at which the wave hits it. For example, a plane wave hitting a smooth surface at a right angle will be reflected back in the opposite direction.

5. What are some real-world applications of plane electromagnetic waves in vacuum?

Plane electromagnetic waves in vacuum have a wide range of applications, including communication technologies such as radio, television, and cellular networks. They are also used in medical imaging, remote sensing, and astronomy. Additionally, many modern technologies such as Wi-Fi and Bluetooth rely on the use of plane electromagnetic waves in vacuum to transmit data wirelessly.

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