Why Are Sine Functions Changed to Cosine in Deriving the Law of Reflection?

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SUMMARY

The discussion centers on the derivation of the law of reflection for electromagnetic waves and optics, specifically addressing the transition from sine to cosine functions in the equations. The user expresses confusion regarding this change, particularly in contrast to Snell's law. A participant suggests that the source material may contain a misprint, indicating that the equations for the components of wave vectors should align correctly. The conclusion emphasizes that while the sine functions lead to a straightforward equality of angles, the cosine functions introduce ambiguity in the relationship between the angles.

PREREQUISITES
  • Understanding of electromagnetic wave behavior
  • Familiarity with optics principles
  • Knowledge of Snell's law
  • Basic trigonometry, specifically sine and cosine functions
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  • Study the mathematical implications of sine and cosine functions in wave equations
  • Examine the conditions under which Snell's law applies
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KaseyKC
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I'm trying to derive the law of reflection for Electromagnetic Waves and Optics. I'm using some lecture notes that my university provided. I'm confused as to why the two sine functions are changed to cosine functions as you don't do the same when you are deriving Snell's law.

Refer to attached for the equations.

I'm currently stuck at the part just before the sine's are converted into cosine functions.
 

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Hello KKC, and welcome to PF :smile: !

You do want to use the template in the homework forum (it's mandatory, and the good spirits that watch over us get nasty if you don't).

However, for your question: I think it's a misprint in the book. They say ##k_{ Iz} = k_{ Rz}## but they work out ##k_{ Ix} = k_{ Rx}##. The first -- as you correctly point out -- leads to ##\sin \theta_I = \sin \theta_R \Rightarrow \theta_I = \theta_R##.

Personally, I don't really like the second (##k_{ Ix} = k_{ Rx}##), because ##\cos \theta_I = \cos \theta_R \Rightarrow \theta_I = \theta_R## isn't even correct (should be ##\Rightarrow \theta_I = \pm \; \theta_R##).

I leave it to you to discover why the "other solution" of ##\sin \theta_I = \sin \theta_R## does not make it wrong to write ## \Rightarrow \theta_I = \theta_R## :rolleyes: !​
 
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