Answer
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Hint: According to Snell’s law the ratio of the sine of the angle of incidence to the sine of the angle of refraction is a constant. All the rays that come out from an object that is kept at the centre of a transparent sphere will be normal to the surface of the sphere. The light will be reflected inside the sphere.
Complete step by step answer:
When light falls normally on the boundary surface then the angle if incidence will be $0$,
We will apply the lens formula considering the refractive indices of the medium involved
According to this formula;
$\dfrac{{{\mu _2}}}{v} - \dfrac{{{\mu _1}}}{u} = \dfrac{{\left( {{\mu _2} - {\mu _1}} \right)}}{R}$ ……………………………………… (i)
As we know that refractive index of glass is will be constant ${\mu _1} = \mu $,
${\mu _2}$(refractive index of surrounding) will be 1, $u = - R$ = {Radius of sphere} and \[R = - R\] is the radius of sphere
Substituting these values in equation (i)
We get,
$\dfrac{1}{v} - \dfrac{\mu }{{ - R}} = \dfrac{{\left( {1 - \mu } \right)}}{{ - R}}$………………………………………………(ii)
On solving above equation, we get,
$\dfrac{1}{v} = \dfrac{1}{{ - R}}$ …………………………………………………………….(iii)
From above relation, we can say that the "there will be no change in the position of an opaque dot at the centre of a transparent glass sphere when a person observes it from the outside."
Note:
When light falls normally on the boundary surface, then we have angle of incidence $i = 0$ and
According to Snell's law \[{\mu _1}\sin i\; = {\mu _2}\sin r.\] So, there will be no refraction, i.e. r is also zero. Thus, the light will be totally internally reflected.
Hence the object will be observed at the same position from outside, and this and will be independent of the refractive index of the sphere
Complete step by step answer:
When light falls normally on the boundary surface then the angle if incidence will be $0$,
We will apply the lens formula considering the refractive indices of the medium involved
According to this formula;
$\dfrac{{{\mu _2}}}{v} - \dfrac{{{\mu _1}}}{u} = \dfrac{{\left( {{\mu _2} - {\mu _1}} \right)}}{R}$ ……………………………………… (i)
As we know that refractive index of glass is will be constant ${\mu _1} = \mu $,
${\mu _2}$(refractive index of surrounding) will be 1, $u = - R$ = {Radius of sphere} and \[R = - R\] is the radius of sphere
Substituting these values in equation (i)
We get,
$\dfrac{1}{v} - \dfrac{\mu }{{ - R}} = \dfrac{{\left( {1 - \mu } \right)}}{{ - R}}$………………………………………………(ii)
On solving above equation, we get,
$\dfrac{1}{v} = \dfrac{1}{{ - R}}$ …………………………………………………………….(iii)
From above relation, we can say that the "there will be no change in the position of an opaque dot at the centre of a transparent glass sphere when a person observes it from the outside."
Note:
When light falls normally on the boundary surface, then we have angle of incidence $i = 0$ and
According to Snell's law \[{\mu _1}\sin i\; = {\mu _2}\sin r.\] So, there will be no refraction, i.e. r is also zero. Thus, the light will be totally internally reflected.
Hence the object will be observed at the same position from outside, and this and will be independent of the refractive index of the sphere
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