Direction of a photon created by bremsstrahlung radiation?

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SUMMARY

The discussion centers on the directionality of radiation emitted during the bremsstrahlung process, specifically addressing the angular distribution of emitted electromagnetic waves when electrons decelerate. The key formula discussed is $$ \frac { \sin^2 \theta } {(1 - \beta \cos \theta)^5} $$, where ## \theta ## represents the angle between the electron's motion and the observation direction, and ## \beta = v/c ## indicates the velocity ratio to the speed of light. The consensus is that bremsstrahlung radiation is not emitted uniformly in all directions but has a specific angular distribution, with maximum emission occurring at angles dependent on the initial velocity of the electrons.

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  • Understanding of bremsstrahlung radiation principles
  • Familiarity with angular distribution in electromagnetic radiation
  • Knowledge of the relationship between velocity and the speed of light (v/c)
  • Basic grasp of trigonometric functions and their application in physics
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  • Study the mathematical derivation of the bremsstrahlung angular distribution formula
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Physicists, electrical engineers, and students studying electromagnetism or radiation physics who seek to understand the nuances of bremsstrahlung radiation and its directional properties.

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basically any time i have an arc, i have electrons flowing in the opposite direction to the field gradient. so when the electrons reach the other side, they will be stopped, which will then produce an EM wave. In, class, my professor drew the direction of radiation in a particular direction, but the electrons deccelarating should produce a wave radially in all directions shouldn't it? with the max amplitude being in the plane normal to the velocity? ie, the charge carrier's direction of travel?
so why would it the bremsstrahlung process emit radiation in only one particular direction?
 
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Wikipedia has a page on bremsstrahlung, which describes the angular distribution.
 
i ddn't understand any of the math behind angular distribution, but i assume the existence of the 'distribution' implies that radiation is indeed emitted radially?
 
I am not sure what "radially" means here. In the initial description, electrons collide with "the other side", presumable the anode, so their motion at that time is mostly linear. In that case, the second formula in the section on angular distribution applies. The most important part of that formula is $$ \frac { \sin^2 \theta } {(1 - \beta \cos \theta)^5} $$

where ## \theta ## is the angle between the direction of motion and the direction of observation, and ## \beta = v/c ##, the ratio of the velocity with the speed of light. It can be seen immediately that there is no emission along the line of motion, and that there is a maximum, the direction of which depends on the initial velocity.
 

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