
The critical angle of glass-air is \[45{}^\circ \] for the light of yellow colour. State whether it will be less than, equal to, or more than \[45{}^\circ \] for blue light?
\[A)\] more than \[45{}^\circ \]
\[B)\] less than \[45{}^\circ \]
\[C)\] same as \[45{}^\circ \]
\[D)\] can’t say
Answer
586.2k+ views
Hint: We must know that the critical angle is the angle of incidence that provides an angle of refraction equal to \[90{}^\circ \]. The relation between refractive indices and angle of incidence and angle of refraction is given by Snell’s law as \[\dfrac{\sin \left( i \right)}{\sin \left( r \right)}=\dfrac{{{n}_{2}}}{{{n}_{1}}}\]. The refractive index of a particular medium may differ for light waves with different frequencies. The relation between this is that refractive index is directly proportional to frequency.
Complete step by step answer:
Firstly we will calculate the refractive index of this particular glass for yellow light. The expression is given by snell’s law as,
\[\dfrac{\sin \left( i \right)}{\sin \left( r \right)}=\dfrac{{{n}_{2}}}{{{n}_{1}}}\]
Here, the angle of refraction is equal to \[90{}^\circ \] , because incident angle is critical angle which is equal to \[45{}^\circ \] for yellow light. Now, this is given for glass-air medium. So our refractive index if the first medium will be one.
\[\Rightarrow \dfrac{\sin \left( 45{}^\circ \right)}{\sin \left( 90{}^\circ \right)}=\dfrac{{{n}_{2}}}{1}\]
Therefore, refractive index for yellow light will be,
\[{{n}_{yellow}}=\sin \left( 45{}^\circ \right)=\dfrac{1}{\sqrt{2}}\]
Now, if we change this with yellow light with blue, the refractive index of this glass will increase a little. We can understand this from the relation that refractive index is directly proportional to frequency. We know blue light has a higher frequency than that of yellow light. So the refractive index increases.
That means, \[{{n}_{blue}}>\dfrac{1}{\sqrt{2}}\] .
So, from this we can understand the critical angle when we use blue light.
\[\Rightarrow {{n}_{blue}}=\sin \left( {{\theta }_{c}} \right)>\dfrac{1}{\sqrt{2}}\]
\[\begin{align}
& {{\theta }_{c}}>{{\sin }^{-1}}\left( \dfrac{1}{\sqrt{2}} \right) \\
& {{\theta }_{c}}>45{}^\circ \\
\end{align}\]
Therefore, the critical angle when we use blue light here will be more than \[45{}^\circ \] .
So, the correct answer is “Option A”.
Note:
We can also solve this question on the basis of wavelength. As we know, wavelength is given by \[\lambda =\dfrac{c}{\upsilon }\] . So, as the wavelength increases, the refractive index will be decreasing. We can clearly understand the dependence of the refractive index on frequency by looking at dispersion of white light by a prism. There, the light waves are dispersed because different frequencies will have different refractive indices. Blue wave will be at the bottom because it will be having the largest refractive index.
Complete step by step answer:
Firstly we will calculate the refractive index of this particular glass for yellow light. The expression is given by snell’s law as,
\[\dfrac{\sin \left( i \right)}{\sin \left( r \right)}=\dfrac{{{n}_{2}}}{{{n}_{1}}}\]
Here, the angle of refraction is equal to \[90{}^\circ \] , because incident angle is critical angle which is equal to \[45{}^\circ \] for yellow light. Now, this is given for glass-air medium. So our refractive index if the first medium will be one.
\[\Rightarrow \dfrac{\sin \left( 45{}^\circ \right)}{\sin \left( 90{}^\circ \right)}=\dfrac{{{n}_{2}}}{1}\]
Therefore, refractive index for yellow light will be,
\[{{n}_{yellow}}=\sin \left( 45{}^\circ \right)=\dfrac{1}{\sqrt{2}}\]
Now, if we change this with yellow light with blue, the refractive index of this glass will increase a little. We can understand this from the relation that refractive index is directly proportional to frequency. We know blue light has a higher frequency than that of yellow light. So the refractive index increases.
That means, \[{{n}_{blue}}>\dfrac{1}{\sqrt{2}}\] .
So, from this we can understand the critical angle when we use blue light.
\[\Rightarrow {{n}_{blue}}=\sin \left( {{\theta }_{c}} \right)>\dfrac{1}{\sqrt{2}}\]
\[\begin{align}
& {{\theta }_{c}}>{{\sin }^{-1}}\left( \dfrac{1}{\sqrt{2}} \right) \\
& {{\theta }_{c}}>45{}^\circ \\
\end{align}\]
Therefore, the critical angle when we use blue light here will be more than \[45{}^\circ \] .
So, the correct answer is “Option A”.
Note:
We can also solve this question on the basis of wavelength. As we know, wavelength is given by \[\lambda =\dfrac{c}{\upsilon }\] . So, as the wavelength increases, the refractive index will be decreasing. We can clearly understand the dependence of the refractive index on frequency by looking at dispersion of white light by a prism. There, the light waves are dispersed because different frequencies will have different refractive indices. Blue wave will be at the bottom because it will be having the largest refractive index.
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