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Physics · Ch 6 — Optics

Proof for Laws of Refraction Using Huygens' Principle

6.9.4

Proof for Laws of Refraction Using Huygens' Principle

The same Huygens' construction, applied at a refracting rather than a reflecting boundary, proves Snell's law. A plane wavefront ABAB in medium (1), perpendicular to incident rays L,ML,M, strikes a plane refracting surface XYXY obliquely and enters medium (2), where the wave travels at a different speed. Because the two media give different speeds v1≠v2v_1\neq v_2, the two secondary wavelets from AA and BB grow by different distances in the same elapsed time: AA′/v2=BB′/v1AA'/v_2=BB'/v_1. Working through the resulting right-triangle ratio gives sin⁡i/sin⁡r=BB′/AA′=v1/v2\sin i/\sin r=BB'/AA' = v_1/v_2; substituting the refractive indices c/v1=n1c/v_1=n_1 and c/v2=n2c/v_2=n_2 recovers Snell's law, n1sin⁡i=n2sin⁡rn_1\sin i=n_2\sin r. Because light travels faster in a rarer medium and slower in a denser one, this same construction shows the wavelength itself is longer in the rarer medium and shorter in th …

Figure 6.51Law of refraction (Huygens' construction)

What this figure shows. A plane wavefront AB in medium (1), perpendicular to incident rays L and M, strikes a plane refracting boundary XY obliquely, entering medium (2) where the wave travels at a different speed. As in the reflection proof, point A reaches the boundary first; by the time B reaches it at B', the secondary wavelet from A has expanded into medium (2), but now by a different distance AA' than BB' (since the two media give the two rays different speeds v1 and v2 over the very same elapsed time). Setting up the resulting right-triangle ratio sin i/sin r = (BB'/AB')/(AA'/AB') = v1/v2, and substituting the refractive indices n1 = c/v1 and n2 = c/v2, recover …

Misc Example 6.23-noteFrequency stays constant while wavelength changes with the medium

Worked out. Building directly on the wavelength/speed relations derived from Huygens' construction (lambda1/lambda2 = n2/n1), the accompanying worked calculation for sodium light entering water (vacuum wavelength 5893 angstrom, n=1.33) computes the frequency two independent ways -- once from v(vacuum)/lambda(vacuum) and once from v(water)/lambda(water) -- and finds exactly the same value both times, about 5.091 times 10 to the 14 hertz. This numerically confirms the general rule already stated in words in the section: a light wave's frequency is fixed by its source and never changes as the wave crosses from one medium into another, no matter how different the two media's refractive indices are; only the wave's speed …