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| n1 sin θ1= n2 sin θ2. |
| The figure on the left shows light bending toward the normal as it enters the denser medium of water. Explain why the light bends in this direction using physical arguments rather than any equations. | |
| As described earlier in the module, the edge of the wavefronts closest to the water slows down first. Since the edge away from the water is still moving at the faster speed, the wavefront swings around and becomes more parallel to the surface. This makes the direction of motion more parallel to the normal. | |
| Which angle, θ2 measured in the water or θ1 measured in air, will be greater if the light bends toward the normal? | |
| Looking at the figure, we can see that the angle measured in air, θ1, will be larger; the angle decreases in a denser medium. | |
| Will a denser medium have a larger or a smaller index of refraction than a rarer medium? | |
| A denser medium provides more matter from which the light can scatter, so light will travel more slowly in a dense medium. A slower speed means a higher index of refraction, so n2 > n1, as indicated in the image on the left. | |
| Use Snell's Law combined with your answer to the previous question to mathematically predict which angle will be greater when light moves into a denser medium. How does this compare with your answer to the second question that was based on physical arguments? | |
| Snell's Law says
n1/n2 = (sin θ2)/(sin θ1) (sin θ2)/(sin θ1) <1. |
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| Use Snell's Law to predict what will happen to the light as it enters the water if it approaches the surface along the normal to the surface, as shown in the figure on the right. | |
| If the light approaches along the
normal, the angle of incidence between the light and the normal is
θ2 = 0 = θ1. |
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| Now explain why this occurs using physical arguments rather than equations. | |
| If the light travels along the normal, the wavefronts are parallel to the surface. Since no point on a wavefront enters the denser medium earlier than any other point on the wavefront, no bending occurs. |
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