What Angle Does a Light Beam Make in Different Reference Frames?

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SUMMARY

The discussion centers on the calculation of the angle a light beam makes with respect to different reference frames in the context of special relativity. The correct formula for the angle \(\theta\) in frame S, given an angle \(\theta_o\) in frame S', is established as \( \cos\theta = \frac{(cos\theta_o + \frac{v}{c})}{(1 + \frac{v}{c} cos\theta_o)} \). Participants clarify the derivation using velocity transformations and confirm the accuracy of the formula after addressing a typographical error in the original homework statement. The discussion emphasizes the importance of precise mathematical representation in physics problems.

PREREQUISITES
  • Understanding of special relativity concepts, specifically Lorentz transformations.
  • Familiarity with trigonometric functions and their applications in physics.
  • Knowledge of the speed of light (c) and its significance in relativistic equations.
  • Ability to manipulate algebraic expressions involving square roots and trigonometric identities.
NEXT STEPS
  • Study the derivation of Lorentz transformations in special relativity.
  • Learn about the implications of velocity transformations on light propagation.
  • Explore the relationship between angles and velocities in different inertial frames.
  • Investigate the role of gamma (\(\gamma\)) factor in relativistic physics.
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Students of physics, particularly those studying special relativity, as well as educators and anyone involved in teaching or learning about the behavior of light in different reference frames.

csnsc14320
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Homework Statement


A light beam is emitted at an angle [tex]\theta_o[/tex] with respect to the x' axis in S'

a) Find the angle [tex]\theta[/tex] the beam makes with respect to the x-axis in S.
- Ans. : [tex]cos\theta = (cos\theta_o + \frac{v}{c})(1 + \frac{v}{c} cos\theta_o)[/tex]

The Attempt at a Solution


From an example problem in our book, we know that with a ruler at an angle in the same situation has angle in laboratory frame:

[tex]\theta = arctan(tan(\theta_o)\gamma)[/tex], where [tex]\gamma = \frac{1}{\sqrt{1-frac{v^2}{c^2}}}[/tex]

if you just take cos of both sides, then you have

[tex]cos\theta = cos(arctan((tan(\theta_o)\gamma)))[/tex]

Drawing a triangle with the right leg as [tex]tan(\theta_o)[/tex] and the bottom leg as [tex]\frac{1}{\gamma}[/tex] you get a hypotenuse of [tex]\sqrt{(\frac{1}{\gamma})^2 + tan(\theta_o)^2}[/tex]

from this i narrowed it down to

[tex]cos\theta = \frac{\frac{1}{\gamma}}{\sqrt{(\frac{1}{\gamma})^2 + tan(\theta_o)^2}}[/tex][tex]= \frac{1}{\sqrt{1 + frac{\gamma*2}{cos{\theta_o)^2} - \gamma^2}}[/tex]

I'm not seeing how this can reduce to my answer I'm suppose to get yet?
 
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csnsc14320 said:

Homework Statement


A light beam is emitted at an angle [tex]\theta_o[/tex] with respect to the x' axis in S'

a) Find the angle [tex]\theta[/tex] the beam makes with respect to the x-axis in S.
- Ans. : [tex]cos\theta = (cos\theta_o + \frac{v}{c})(1 + \frac{v}{c} cos\theta_o)[/tex]
That answer doesn't look right. It should be:

[tex]cos\theta = \frac{(cos\theta_o + \frac{v}{c})}{(1 + \frac{v}{c} cos\theta_o)}[/tex]

The easy way to derive it is to use the velocity transformations.
 
Doc Al said:
That answer doesn't look right. It should be:

[tex]cos\theta = \frac{(cos\theta_o + \frac{v}{c})}{(1 + \frac{v}{c} cos\theta_o)}[/tex]

The easy way to derive it is to use the velocity transformations.

oops I missed the divide sign in my book - your answer is the right one.

I'll give that a shot
 

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