Optics - index of refraction and phase lag

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Homework Help Overview

The discussion revolves around the behavior of light as it passes through different media, specifically focusing on the index of refraction and phase lag when a light beam transitions from vacuum to glass. The original poster presents a problem involving a light beam of wavelength 500nm traveling through a glass sheet with a known thickness and refractive index.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the relationship between wavelength in vacuum and in glass, questioning how to calculate the number of waves in different media. There are attempts to derive expressions for the number of cycles and phase lag, with some participants checking the correctness of units and definitions.

Discussion Status

Some participants have provided feedback on the calculations and expressions used, pointing out potential errors in unit handling and terminology. There is ongoing exploration of how to accurately express the number of waves in glass versus vacuum, with various interpretations being discussed.

Contextual Notes

Participants are navigating through the implications of using different symbols for wave numbers and ensuring that their calculations yield unitless results, reflecting the constraints of the problem setup.

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Homework Statement



A light beam of wavelength 500nm travels from A to B in vacuum. (AB = 10mm)
If we put a glass sheet with n=1.5 and 1mm thick, calculate how change the number of periods. Calculate the phase lag too.


Homework Equations



k0 = 2Pi/λ (vacuum)

k= k0·n

The Attempt at a Solution



If in the vacuum the wave gas a wavelength λ=2Pi/k0, into a n=1.5 glass, it will have λ'=2Pi·n/k0 (?)

Thanks
 
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Yes, that's correct.
 
How many more waves are there in 1 mm of glass than there are in 1 mm of free space?
 
SammyS said:
How many more waves are there in 1 mm of glass than there are in 1 mm of free space?

If the wavelength is λ, in a free space of d=1mm there will be k=λd waves, and in d'=1mm glass (index n) there will be k'=λnd', so if we put the glass into de space d, this leads to

k=λ(d-d')

k'=λd'n

therefore the number of waves (total) will be

K = k+k'

Is this correct?

thanks
 
No, you didn't calculate the number of cycles correctly. Both λ and d have units of length, so using your expression, k would have units of length squared. The number, however, should be unitless.

(k isn't the best letter to use since k is typically used to denote the spatial frequency.)
 
vela said:
No, you didn't calculate the number of cycles correctly. Both λ and d have units of length, so using your expression, k would have units of length squared. The number, however, should be unitless.

(k isn't the best letter to use since k is typically used to denote the spatial frequency.)

If k = 2Pi/λ [meters^(-1)], then kd, with [d=meters] is unitless, isn't it?

Thanks
 
vela said:
(k isn't the best letter to use since k is typically used to denote the spatial frequency.)

Ok, my mistake, but is K = k+k' as we define k and k' [uniteless] the number of waves?
 
SammyS said:
How many more waves are there in 1 mm of glass than there are in 1 mm of free space?

The number of waves in a thickness d of glass, is: d/(λ) = d/(λ0/n) = nd/λ0, where λ0 is the wavelength in a vacuum.

So, the number of EXTRA cycles is: nd/λ0-d/λ0 = (n-1)(d/λ0)
 

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