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In the figure, a ray is incident on one face of a triangular glass prism in air. The angle of incidence θis chosen so that the emerging ray also makes the same angle θwith the normal to the other face. Show that the index ofrefraction of the glass prism is given by

ψn=sin12(ψ+ϕ)sin12ϕ

whereϕ is the vertex angle of the prism and ψis thedeviation angle, the total angle through which the beam is turned in passing through the prism. (Under these conditions the deviation angle has the smallest possible value, which is called theangle of minimum deviation.)

Figure:

Short Answer

Expert verified

The index of refraction of the glass prism in given byn=sin12(ψ+ϕ)sin12ϕ is shown in theexplanation part.

Step by step solution

01

Given

The figure is given in which a ray is incident on one face of a triangular glass prism in the air.

02

Understanding the concept

Write for the angle of refraction in terms of thevertex angle from the geometry of the prism and the ray diagram. Thenusing the formula for theexterior angle of triangle,solve for the angle of incidence in terms of thevertex angle. Then, using Snell’s law of refraction, show that the index of refraction of the glass prism in given by n=sin12(ψ+f)sin12f.

Formula:

n1sinθ1=n2sinθ2
03

Show that the index of refraction  n of the glass prism is given by n=sin12(ψ+f)sin12f 

Consider the diagram for the condition as:

Letθ2be the angle of refraction.

From the figure, we can write

θ2+α=900θ2=900−α

Consider the equation for the angle as:

ϕ+2α=1800

Hence,

α=(1800−ϕ)2

Solve for the second angle as:

θ2=90°−(180°−ϕ)2θ2=(180°−180°+ϕ)2

θ2=ϕ2

Using the formula for the exterior angle of triangle and solve as:

ψ=2(θ−θ2)ψ=2(θ−ϕ2)2θ=ψ+ϕθ=12(ϕ+ψ)

Snell’s law given as:

n1sinθ1=n2sinθ2

Here, n1=1,θ1=θ,n2=n,θ2=θ2. Therefore,

sinθ=nsinθ2n=sinθsinθ2n=sin12(ϕ+ψ)sinϕ2

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Most popular questions from this chapter

Figure 33-32 shows four long horizontal layers ´¡â€“D of different materials, with air above and below them. The index of refraction of each material is given. Rays of light are sent into the left end of each layer as shown. In which layer is there the possibility of totally trapping the light in that layer so that, after many reflections, all the light reaches the right end of the layer?

In Fig.33-52a, a beam of light in material1is incident on a boundary at an angle ofθ1=30°. The extent of refraction of the light into material2depends, in part, on the index of refractionn2of material 2. Fig.33-52bgives the angle of refractionθ2versusn2for a range of possiblen2values. The vertical axis scale is set byθ2a=20.0°andθ2b=40.0°

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