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Question: A glass sphere, refractive index 1.5 and radius 10cm, has a spherical cavity of radius 5cm concentri...

A glass sphere, refractive index 1.5 and radius 10cm, has a spherical cavity of radius 5cm concentric with it. A narrow beam of light is directed into the sphere. Find the final image and its nature.

A. 25cm left of S4, virtual\text{A}\text{. 25cm left of }{{\text{S}}_{\text{4}}}\text{, virtual}
B. 25cm right of S4, virtual\text{B}\text{. 25cm right of }{{\text{S}}_{\text{4}}}\text{, virtual}
C. 15cm left of S4, virtual\text{C}\text{. 15cm left of }{{\text{S}}_{\text{4}}}\text{, virtual}
D. 20cm right of S4, virtual\text{D}\text{. 20cm right of }{{\text{S}}_{\text{4}}}\text{, virtual}

Explanation

Solution

Hint: The will be four images formed due the refraction of the light rays at the four surfaces. The first three are intermediate and the last one is the final image. The image found due to one surface will act as an object for the surface. Use the formula μ2vμ1u=μ2μ1R\dfrac{{{\mu }_{2}}}{v}-\dfrac{{{\mu }_{1}}}{u}=\dfrac{{{\mu }_{2}}-{{\mu }_{1}}}{R} to locate the positions of the images.
Formula used:
μ2vμ1u=μ2μ1R\dfrac{{{\mu }_{2}}}{v}-\dfrac{{{\mu }_{1}}}{u}=\dfrac{{{\mu }_{2}}-{{\mu }_{1}}}{R}

Complete step by step answer:
When rays of light from an object pass into a different medium, the rays refract and an image of the object is created. If the refracted rays of light intersect at a point, then the image is called a real image. If the rays of light appear to be emerging from a point, then the image is called a virtual image.
If the rays light pass through a spherical surface, the relation between the positions of the object and its image is given as μ2vμ1u=μ2μ1R\dfrac{{{\mu }_{2}}}{v}-\dfrac{{{\mu }_{1}}}{u}=\dfrac{{{\mu }_{2}}-{{\mu }_{1}}}{R}.
Here, μ1{{\mu }_{1}} and μ2{{\mu }_{2}} are the refractive indices of the incident medium and refracted medium respectively. v and u are the positions of the object and image respectively, according to the sign convection. R is the radius of the spherical surface.
Here, the rays of light will refract at all the four surfaces. Therefore, there will be four images formed. The final image of the object will form when the light is refracted at surface S1{{S}_{1}}.
First, it will refract at surface S1{{S}_{1}}.
Here, μ1=1{{\mu }_{1}}=1, μ2=1.5{{\mu }_{2}}=1.5, u=u=-\infty and R=10cm. Let v=v1v={{v}_{1}}
Hence, we get
1.5v11=1.5110\dfrac{1.5}{{{v}_{1}}}-\dfrac{1}{-\infty }=\dfrac{1.5-1}{10}
1.5v10=0.510\Rightarrow \dfrac{1.5}{{{v}_{1}}}-0=\dfrac{0.5}{10}
1v1=0.515=130\Rightarrow \dfrac{1}{{{v}_{1}}}=\dfrac{0.5}{15}=\dfrac{1}{30}
v1=30cm\Rightarrow {{v}_{1}}=30cm
Therefore, the first image is formed at a distance of 30cm from surface S1{{S}_{1}}, towards right.
Now, this image will act as an object from surface S2{{S}_{2}} as the light will again refract at surface S2{{S}_{2}}.
The first image are formed at a position +30cm from S1{{S}_{1}} and the distance between S1{{S}_{1}} and S2{{S}_{2}} is 5cm. Therefore, the position of the first image from S2{{S}_{2}} is +25cm.
Hence, this case, u=25cmu=25cm, μ1=1.5{{\mu }_{1}}=1.5, μ2=1{{\mu }_{2}}=1and R=5cm. Let v=v2v={{v}_{2}}
This implies that
1v21.525=11.55\dfrac{1}{{{v}_{2}}}-\dfrac{1.5}{25}=\dfrac{1-1.5}{5}
1v20.35=0.55\Rightarrow \dfrac{1}{{{v}_{2}}}-\dfrac{0.3}{5}=\dfrac{-0.5}{5}
1v2=0.350.55\Rightarrow \dfrac{1}{{{v}_{2}}}=\dfrac{0.3}{5}-\dfrac{0.5}{5}
1v2=0.25\Rightarrow \dfrac{1}{{{v}_{2}}}=-\dfrac{0.2}{5}
v2=50.2=25cm\Rightarrow {{v}_{2}}=-\dfrac{5}{0.2}=-25cm
This means the second image is formed towards the left of S2{{S}_{2}} at a distance of 25cm.
Now, this image will act as an object for surface S3{{S}_{3}}.
The second image is formed at a distance of 25cm towards left of S2{{S}_{2}} and the distance between S2{{S}_{2}} and S3{{S}_{3}} is 10cm. Therefore, the position of the second image from S3{{S}_{3}} is -35cm.
Hence, now u=35cmu=-35cm, μ1=1{{\mu }_{1}}=1, μ2=1.5{{\mu }_{2}}=1.5and R= -5cm. Let v=v3v={{v}_{3}}
This implies that
1.5v3135=1.515\dfrac{1.5}{{{v}_{3}}}-\dfrac{1}{-35}=\dfrac{1.5-1}{-5}
1.5v3+135=0.55\Rightarrow \dfrac{1.5}{{{v}_{3}}}+\dfrac{1}{35}=-\dfrac{0.5}{5}
1.5v3=0.55135\Rightarrow \dfrac{1.5}{{{v}_{3}}}=-\dfrac{0.5}{5}-\dfrac{1}{35}
1.5v3=3.5135=4.535=0.97\Rightarrow \dfrac{1.5}{{{v}_{3}}}=\dfrac{-3.5-1}{35}=\dfrac{-4.5}{35}=\dfrac{-0.9}{7}
v3=1.5×70.9=353cm\Rightarrow {{v}_{3}}=-\dfrac{1.5\times 7}{0.9}=-\dfrac{35}{3}cm
This means the third image is formed towards the left of S3{{S}_{3}} at a distance of 353-\dfrac{35}{3}cm.
Now, this image will act as an object for surface S4{{S}_{4}}.
The third image is formed at a distance of 353-\dfrac{35}{3}cm towards left of S3{{S}_{3}} and the distance between S3{{S}_{3}} and S4{{S}_{4}} is 5cm. Therefore, the position of the second image from S3{{S}_{3}} is (353+5)=503cm-\left( \dfrac{35}{3}+5 \right)=-\dfrac{50}{3}cm.
Hence, now u=503cmu=-\dfrac{50}{3}cm, μ1=1.5{{\mu }_{1}}=1.5, μ2=1{{\mu }_{2}}=1 and R= -10cm. Let v=v4v={{v}_{4}}
This implies that
1v41.5503=11.510\dfrac{1}{{{v}_{4}}}-\dfrac{1.5}{\dfrac{-50}{3}}=\dfrac{1-1.5}{-10}
1v4+4.550=0.510\Rightarrow \dfrac{1}{{{v}_{4}}}+\dfrac{4.5}{50}=\dfrac{-0.5}{-10}
1v4=0.5104.550\Rightarrow \dfrac{1}{{{v}_{4}}}=\dfrac{0.5}{10}-\dfrac{4.5}{50}
1v4=2.54.550=2.550=125\Rightarrow \dfrac{1}{{{v}_{4}}}=\dfrac{2.5-4.5}{50}=\dfrac{-2.5}{50}=\dfrac{-1}{25}
v4=25cm\Rightarrow {{v}_{4}}=-25cm
This means that the fourth and the final image is towards the left of S4{{S}_{4}} at the distance of 25 cm. Since, the image is towards the left, the light will diverge at the surface and will appear to emerge from a point. Hence, the image is a virtual image.
Hence, the correct option is A.

Note: Students can make mistakes while writing the values of u, v and R. These values can be positive as well as negative, according to the sign convection.
The positions from the refracting surface that are directed along the direction of the incident rays, are positive. If the direction of the positions are towards the opposite direction of incident rays, then the positions are considered to be negative.