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Question: The critical angle of medium for specific wavelength, if the medium has relative permittivity \(3\) ...

The critical angle of medium for specific wavelength, if the medium has relative permittivity 33 and relative permeability 43\dfrac{4}{3} for this wavelength, will be:
A) 45{45^ \circ }
B) 30{30^ \circ }
C) 15{15^ \circ }
D) 60{60^ \circ }

Explanation

Solution

Use the formula of the refractive index of the medium and substitute the formula of velocity of light in air and medium. Substitute the angles, and the obtained refractive index of the medium in the snell’s law to know the critical angle of the medium.

Useful formula:
(1) The relative permittivity is given by
r=0{ \in _r} = \dfrac{{{ \in _{}}}}{{{ \in _0}}}
Where 0{ \in _0} is the permittivity of free space and \in is the permittivity of the medium.

(2) The relative permeability of the medium is given by
μr=μμ0{\mu _r} = \dfrac{{{\mu _{}}}}{{{\mu _0}}}
Where μ\mu is the permeability of the medium and μ0{\mu _0} is the permeability of the free space.

(3) The refractive index of the medium is given by
μ2=cv{\mu _2} = \dfrac{c}{v}
Where cc is the velocity of the light in vacuum and vv is the velocity of the light in medium.

(4) The snell’s law states that
μ2sinθi=μ1sinθr{\mu _2}\sin {\theta _i} = {\mu _1}\sin {\theta _r}
Where μ1{\mu _1} is the refractive index of free space and μ2{\mu _2} is the refractive index of the medium.

Complete step by step solution:
It is given that the
Relative permittivity of the medium, r=3{ \in _r} = 3
The relative permeability of the medium, μ=43\mu = \dfrac{4}{3}
By taking the formula (3),
μ2=cv{\mu _2} = \dfrac{c}{v}
Substituting the values of c=1vo0c = \dfrac{1}{{\sqrt {{v_o}{ \in _0}} }} and the v=1μrv = \dfrac{1}{{\sqrt {\mu { \in _r}} }} in the above formula,

μ2=1vo01μr{\mu _2} = \dfrac{{\dfrac{1}{{\sqrt {{v_o}{ \in _0}} }}}}{{\dfrac{1}{{\sqrt {\mu { \in _r}} }}}}
By simplifying the above equation, and also using the formula (1) and (2) in it, we get
μ2=μrr{\mu _2} = \sqrt {{\mu _r}{ \in _r}}
μ2=3×43{\mu _2} = \sqrt {3 \times \dfrac{4}{3}}
μ2=2{\mu _2} = 2
Using the formula (4),
μ2sinθi=μ1sinθr{\mu _2}\sin {\theta _i} = {\mu _1}\sin {\theta _r}
The critical angle θr=90{\theta _r} = {90^ \circ }, so
μ2sinθi=μ1sin90{\mu _2}\sin {\theta _i} = {\mu _1}\sin {90^ \circ }
μ2sinθi=2×12{\mu _2}\sin {\theta _i} = 2 \times \dfrac{1}{2}
Substituting the value of the angles and the refractive index of the medium
2sinθi=12\sin {\theta _i} = 1
sinθi=12\sin {\theta _i} = \dfrac{1}{2}
Hence the value of the critical angle of the medium is 30{30^ \circ }.

Thus the option (B) is correct.

Note: The snell’s law has the relation, in which the ratio of the sine of the angles of incidence and the refraction is equal to the ratio of the refractive indexes. It is mainly used in fiber optics. Always remember that the critical angle of the free space is 90{90^ \circ } .