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The light beam in the figure below strikes surface 2 at the critical angle, θc =...

uploaded imageThe light beam in the figure below strikes surface 2 at the critical angle, θc = 42°. Determine the angle of incidence, θi.
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Concepts and reason

The concept required to solve the given problem is Snell’s law of refraction.

Initially, find the refractive index of glass when light strikes surface 2 using equation of Snell’s law. After that, use the triangle law to find the angle of refraction when light strikes surface 1. Use the angle of refraction and refractive index value to find the angel of incidence.

Fundamentals

The Snell’s law of refraction relates the angle of incidence and refraction with the refractive index value. Mathematically, it is given as follows:

n1sinθ1=n2sinθ2{n_1}\sin {\theta _1} = {n_2}\sin {\theta _2}

Here, n1{n_1} is the refractive index of first medium, n2{n_2} is the refractive index of second medium, θ1{\theta _1} is the angle that ray makes with the normal in medium 1 and θ2{\theta _2} is the angle that ray makes with the normal in medium 2.

The following figure shows the angle made by light beam with surface 1 and 2.

Surface
102)
60.00
Surface ?
Uc

Here, n1{n_1} is the refractive index of first medium (air), n2{n_2} is the refractive index of second medium(glass), θr{\theta _r} is the angle of refraction when light strikes surface 1 and θc{\theta _c} is the critical angle.

Snell’s law equation when light beam strikes surface 2 is,

n2sinθc=n1sin90n2=n1sinθc\begin{array}{c}\\{n_2}\sin {\theta _c} = {n_1}\sin 90^\circ \\\\{n_2} = \frac{{{n_1}}}{{\sin {\theta _c}}}\\\end{array}

Substitute 1 for n1{n_1} and 4242^\circ for θc{\theta _c} in equation n2=n1sinθc{n_2} = \frac{{{n_1}}}{{\sin {\theta _c}}} .

n2=1sin42=1.49\begin{array}{c}\\{n_2} = \frac{1}{{\sin 42^\circ }}\\\\ = 1.49\\\end{array}

In ΔABC\Delta ABC ,

θ1+60+θ2=180θ1+θ2=120\begin{array}{c}\\{\theta _1} + 60^\circ + {\theta _2} = 180^\circ \\\\{\theta _1} + {\theta _2} = 120^\circ \\\end{array}

From figure,

θc+θ1=90θ1=90θc\begin{array}{c}\\{\theta _c} + {\theta _1} = 90^\circ \\\\{\theta _1} = 90^\circ - {\theta _c}\\\end{array}

Substitute 4242^\circ for θc{\theta _c} in equation θ1=90θc{\theta _1} = 90^\circ - {\theta _c} .

θ1=9042=48\begin{array}{c}\\{\theta _1} = 90^\circ - 42^\circ \\\\ = 48^\circ \\\end{array}

Substitute 4848^\circ for θ1{\theta _1} in equation θ1+θ2=120{\theta _1} + {\theta _2} = 120^\circ .

48+θ2=120θ2=72\begin{array}{c}\\48^\circ + {\theta _2} = 120^\circ \\\\{\theta _2} = 72^\circ \\\end{array}

From figure,

θr+θ2=90θr=90θ2\begin{array}{c}\\{\theta _r} + {\theta _2} = 90^\circ \\\\{\theta _r} = 90^\circ - {\theta _2}\\\end{array}

Substitute 7272^\circ for θ2{\theta _2} in equation θr=90θ2{\theta _r} = 90^\circ - {\theta _2} and calculate the angle of refraction as follows:.

θr=9072=18\begin{array}{c}\\{\theta _r} = 90^\circ - 72^\circ \\\\ = 18^\circ \\\end{array}

Snell’s law equation when light beam strikes surface 1 is,

n1sinθi=n2sinθrθi=sin1(n2n1sinθr)\begin{array}{c}\\{n_1}\sin {\theta _i} = {n_2}\sin {\theta _r}\\\\{\theta _i} = {\sin ^{ - 1}}\left( {\frac{{{n_2}}}{{{n_1}}}\sin {\theta _r}} \right)\\\end{array}

Substitute 1 for n1{n_1} , 1.49 for n2{n_2} and 1818^\circ for θr{\theta _r} in equation θi=sin1(n2n1sinθr){\theta _i} = {\sin ^{ - 1}}\left( {\frac{{{n_2}}}{{{n_1}}}\sin {\theta _r}} \right) .

θi=sin1(1.491sin18)=27.4\begin{array}{c}\\{\theta _i} = {\sin ^{ - 1}}\left( {\frac{{1.49}}{1}\sin 18^\circ } \right)\\\\ = 27.4^\circ \\\end{array}

Ans:

The angle of incidence is 27.427.4^\circ .

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