Accelerating Charges & Light: Massless Particles

In summary, massless particles can still accelerate even though they travel at the speed of light. This can be seen with the example of photons bending around a star due to gravitational lensing. However, chargeless particles cannot emit light without decaying, and it is unlikely for electrically charged particles to be massless according to the standard model.
  • #1
cragar
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If accelerating charges emit light. Then would this imply that mass less particle could not emit light because they cannot accelerate?
 
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  • #2
Actually, massless particles must always travel at the speed of light, but they can still accelerate. Acceleration is speed plus direction. Thus if their speed can't change, their direction can still change, meaning they can still accelerate. Think of the massless photon bending around a star as it experiences gravitational lensing.

The more correct statement is that chargeless particles don't emit light without decaying and massless particles tend to be chargeless.
 
  • #3
Interesting, forgot about that part of acceleration. but if a massless particle had charge it could emit light.
 
  • #4
In fact, there are good reasons to assume that electrically charged particles cannot be massless. At least in the standard model, there aren't any.
 
  • #5


The concept of massless particles emitting light is a complex and ongoing topic of research in the field of physics. While it is true that according to classical mechanics, massless particles cannot accelerate, the theory of relativity introduces the concept of mass-energy equivalence, where even massless particles can have energy and momentum. This means that although they may not have a rest mass, they can still have a non-zero energy and therefore can interact with other particles and emit light.

In fact, photons, which are the particles that make up light, are considered to be massless according to the standard model of particle physics. Yet, they can still be accelerated by electric and magnetic fields, and as a result, they can emit light. This is known as the electromagnetic radiation produced by accelerating charges.

Therefore, the idea that massless particles cannot emit light is not accurate. However, it is important to note that the behavior of massless particles, such as photons, is governed by the laws of quantum mechanics rather than classical mechanics. This means that their behavior may not always follow our intuitive understanding of how particles with mass behave.

In conclusion, the relationship between accelerating charges and light emission is a complex and fascinating area of study, and the existence of massless particles does not prevent them from emitting light. Further research and experiments are needed to fully understand the behavior of these particles and their role in the emission of light.
 

FAQ: Accelerating Charges & Light: Massless Particles

1. What is an accelerating charge?

An accelerating charge is a charged particle that is changing its velocity, either by speeding up or slowing down. This change in velocity produces an electric field and electromagnetic radiation, including light.

2. How do accelerating charges produce light?

When an accelerating charge changes its velocity, it creates an oscillating electric field. This oscillating electric field then produces an oscillating magnetic field, which in turn creates an electromagnetic wave, or light.

3. Why are massless particles associated with light?

Massless particles, such as photons, have no rest mass and travel at the speed of light. This is why they are associated with light, as they are the carriers of electromagnetic radiation.

4. Can accelerating charges produce other types of radiation besides light?

Yes, accelerating charges can produce other types of electromagnetic radiation, such as radio waves, microwaves, and x-rays. The type of radiation produced depends on the frequency and energy of the oscillations.

5. How does the energy of a photon relate to the frequency of light?

The energy of a photon is directly proportional to the frequency of light. This relationship is described by the equation E=hf, where E is the energy of the photon, h is Planck's constant, and f is the frequency of the light wave.

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