Snell's Law

Lenses work because of Snell's law, which expresses how much rays of light bend when entering or exiting a transparent material. Recall that the speed of light in a medium is less than the speed $ c$ in an vacuum. For a given material, let its refractive index be defined as

$\displaystyle n = {c \over s} ,$ (4.2)

in which $ s$ is the speed of light in the medium. For example, $ n = 2$ means that light takes twice as long to traverse the medium than through a vacuum. For some common examples, $ n = 1.000293$ for air, $ n = 1.33$ for water, and $ n = 1.523$ for crown glass.

Figure: Propagating wavefronts from a medium with low refractive index (such as air) to one with a higher index (such as glass). (a) The effect of slower propagation on the wavefronts is shown as they enter the lower medium. (b) This shows the resulting bending of a light ray, which is always perpendicular to the wavefronts. Snell's Law relates the refractive indices and angles as $ n_1 \sin\theta_1 = n_2 \sin\theta_2$.
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(a) & & (b)
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Figure 4.9 shows what happens to incoming light waves and rays. Suppose in this example that the light is traveling from air into glass, so that $ n_1 < n_2$. Let $ \theta_1$ represent the incoming angle with respect to the surface normal, and let $ \theta_2$ represent the resulting angle as it passes through the material. Snell's law relates the four quantities as

$\displaystyle n_1 \sin\theta_1 = n_2 \sin\theta_2 .$ (4.3)

Typically, $ n_1/n_2$ and $ \theta_1$ are given, so that (4.3) is solved for $ \theta_2$ to obtain

$\displaystyle \theta_2 = \sin^{-1} \left({ n_1 \sin\theta_1 \over n_2 }\right) .$ (4.4)

If $ n_1 < n_2$, then $ \theta_2$ is closer to perpendicular than $ \theta_1$. If $ n_1 > n_2$, then $ \theta_2$ is further from perpendicular. The case of $ n_1 > n_2$ is also interesting in that light may not penetrate the surface if the incoming angle $ \theta_1$ is too large. The range of $ \sin^{-1}$ is 0 to $ 1$, which implies that (4.4) provides a solution for $ \theta_2$ only if

$\displaystyle (n_1/n_2)\sin\theta_1 \leq 1.$ (4.5)

If the condition above does not hold, then the light rays reflect from the surface. This situation occurs while under water and looking up at the surface. Rather than being able to see the world above, a swimmer might instead see a reflection, depending on the viewing angle.

Steven M LaValle 2016-12-31