Explore refraction, reflection, and Snell's Law
Light bends when it crosses a boundary between materials with different indices of refraction. Snell's Law quantifies this: n₁sinθ₁ = n₂sinθ₂. When light travels from a denser medium to a less dense medium at an angle greater than the critical angle, total internal reflection occurs — the basis for fiber optics. The speed of light in a medium is c/n.
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Sign in →Refraction is what makes a straw look broken in a glass of water, what makes a swimming pool seem shallower than it really is, and what lets eyeglasses bring blurry text into focus. When light crosses from one transparent material into another — air into water, water into glass — its speed changes, and that speed change forces the wavefront to tilt at the boundary. Snell's Law captures the geometry exactly: n₁ sinθ₁ = n₂ sinθ₂, where n is the index of refraction and θ is measured from the normal. The simulation lets you fire a beam at any angle into materials with any pair of indices, watch the refracted ray bend toward or away from the normal, push the angle past the critical angle to trigger total internal reflection, and recover Snell's Law from raw measurements. Total internal reflection is what keeps light bouncing inside fiber optic cables.
MisconceptionLight bends because the boundary itself pushes or repels it, like a wall deflecting a ball.
CorrectThere's no surface force kicking the ray sideways. Light's phase speed changes inside the denser medium because the electromagnetic wave interacts with bound charges in the material, and when one side of an obliquely incident wavefront enters first it slows before the rest, forcing the whole front to tilt. That tilt is what we see as bending — wave geometry, no shove from the boundary.
MisconceptionThe angle of refraction is always smaller than the angle of incidence.
CorrectOnly when the beam goes from a less dense medium into a denser one (n₂ > n₁). Going the other way — glass into air, water into air — the refracted angle is bigger than the incident angle, and once it hits the critical angle the beam stops refracting altogether and totally reflects.
MisconceptionTotal internal reflection is just regular reflection that happens when the surface is shiny enough.
CorrectTotal internal reflection is a wave-optics effect, not a coating effect. Above the critical angle Snell's Law has no transmitted-ray solution (sinθ₂ would exceed 1), so an ideal boundary reflects the energy back inside the denser medium while an evanescent field exists just beyond the surface. Real fibers still have small absorption and scattering losses, but the reflection can be efficient enough for signals to travel kilometers.
MisconceptionAll colors of light bend by the same amount when they refract.
CorrectThe index of refraction depends slightly on wavelength (this is called dispersion), so red light bends a little less than blue light in the same glass. That tiny difference, accumulated through a prism, splits white light into a rainbow.
MisconceptionSnell's Law only works for one specific kind of light, like lasers.
CorrectSnell's Law holds for any electromagnetic wave at a boundary between two transparent media — visible light, infrared, microwaves, even radio waves. The simulation uses a clean laser only because it is easy to draw a single ray.
Light slows down in denser materials because the electromagnetic field drives bound charges in the material, and that collective response lowers the wave's phase speed. When part of a wavefront enters the new material before the rest, that side slows first and the whole front pivots, which we see as bending. Snell's Law gives the exact geometry.
The critical angle is the incident angle (going from a denser medium into a less dense one) above which all the light reflects back instead of refracting through. It is given by θ_c = arcsin(n₂/n₁). For glass (n=1.5) to air (n=1), θ_c ≈ 41.8°; for water (n=1.33) to air, θ_c ≈ 48.6°; for diamond (n=2.42) to air, θ_c ≈ 24.4°, which is why diamonds sparkle so aggressively.
Frequency stays the same — it is set by the source and cannot change at a passive boundary. Wavelength shrinks in the denser medium because λ = v/f and v drops. That's why color is set by frequency, not wavelength: a red laser stays red whether it is in air, water, or glass.
GO-1.A asks students to relate the index of refraction to the speed of light in a medium. GO-1.B requires applying Snell's Law to predict ray paths at boundaries. GO-1.C covers total internal reflection and the critical angle. The simulation gives a controllable lab where each of these can be measured directly and the predictions can be verified.
Two reasons. First, diamond has a much higher index (2.42 vs ~1.5), so its critical angle is small (~24°) — light entering through a facet is very likely to hit the next facet above the critical angle and totally reflect, bouncing inside the stone before exiting. Second, diamond has strong dispersion, so the trapped light splits into colors before it escapes. Cut quality is engineered to maximize both effects.