The index of refraction of light in passing from a vacuum into water is 1.33. If the angle of incidence is 40°, determine the angle of refraction.

Short Answer

Expert verified

The angle of refraction is28.9o.

Step by step solution

01

Step 1. Given Information  

The index of refraction of light in passing from a vacuum into water is 1.33. If the angle of incidence is 40°.

We have to determine the angle of refraction.

02

Step 2. The Snell's law tell us that when you have two medium with refraction index n1 and n2 the equation is src="data:image/svg+xml;base64,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" role="math" localid="1647100147718" src="https://studysmarter-mediafiles.s3.amazonaws.com/media/textbook-exercise-images/e8ea34e5-f688-4097-b73b-79648fff8fe9.svg?X-Amz-Algorithm=AWS4-HMAC-SHA256&X-Amz-Credential=AKIA4OLDUDE42UZHAIET%2F20220312%2Feu-central-1%2Fs3%2Faws4_request&X-Amz-Date=20220312T155858Z&X-Amz-Expires=90000&X-Amz-SignedHeaders=host&X-Amz-Signature=b1d1d780bcd7cfc5992e5b55f72626883cc0c8fee4ca348b236948ddefa16646" n1sinθ1=n2sinθ2

With θ1andθ2the angle in the first medium and in second medium respectively.

For us the initial angle θ1=40oandn2=1.33.

In order to find θ2we need to know n1.

Assume n1=1for air.

03

Step 3. Then our equation is

1·sin40o=1.33·sinθ2

Divide by 1.33 on both side

sin40o1.33=1.331.33·sinθ2sin40o1.33=sinθ2sinθ2=sin40o1.33θ2=sin-1sin40o1.33

04

Step 4. After solving the equation is θ2=sin-1sin40o1.33

θ2sin-10.6431.33θ2sin-10.483θ228.9o

The angle of refraction is 28.9o.

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