Monochromatic Light Frequency in Glass (5.20 x 10^2 nm, n=1.50)

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SUMMARY

The discussion centers on calculating the frequency of monochromatic light with a wavelength of 5.20 x 102 nm as it enters glass with a refractive index (n) of 1.50. The relevant formulas include the relationship between wavelength, frequency, and refractive index. The frequency of light remains constant when transitioning between media, while the wavelength changes. Thus, the frequency of light in glass is the same as outside, calculated using the formula: frequency = speed of light / wavelength.

PREREQUISITES
  • Understanding of the wave equation: v = frequency × wavelength
  • Knowledge of refractive index and its implications on light behavior
  • Familiarity with the properties of monochromatic light
  • Basic grasp of light speed in different media
NEXT STEPS
  • Calculate the frequency of light in glass using the formula: frequency = speed of light / wavelength
  • Explore the concept of refractive index and its effect on wavelength
  • Investigate the behavior of light as it transitions between different media
  • Learn about the implications of frequency consistency across media
USEFUL FOR

Students studying optics, physics educators, and anyone interested in the properties of light and its behavior in different materials.

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Homework Statement



Monochromatic light of a wavelength of 5.20 x 10^2 nm enters glass (n=1.50). What is the frequency of light in the glass?

Homework Equations


I am thinking I am supposed to use the formula : wave length = d(sin ( ) )/n
and then v=Frequency(wave length)


The Attempt at a Solution


This is where i got lost...

I attempted to use the formulas but got really confused.
 
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Forget the formulas. What's the frequency outside of the glass? Can the frequency inside of the glass be different? Frequency counts the number of waves passing per second. If the number outside and inside are different, where are the extra waves going?? This may be more of an understanding question than a formula question.
 

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