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19 Questions around this concept.
An empty spherical flask of diameter 15 cm is placed in water of refractive index $4 / 3$. A parallel ray of light strikes the flask. Where does it get focused, if observed from within the flask, when measured from the centre of the surface of the spherical flask surface i.e., pole in cm
A spherical convex surface separates object and image space of refractive index 1 and 4/3 respectively. If radius of curvature of the surface is 0.1 m, its power is:
If an object 0 is placed in front of a curved surface as shown in the above figure, then the Refraction formula is given as
$$
\frac{n_2}{v}-\frac{n_1}{u}=\frac{n_2-n_1}{R}
$$
where
$n_1=\text { Refractive index of the medium from which light rays are coming (from the object). }$.
$n_2=$ Refractive index of the medium in which light rays are entering.
and $n_1<n_2$
and $\mathrm{u}=$ Distance of object, $\mathrm{v}=$ Distance of image, $\mathrm{R}=$ Radius of curvature
Note -
- use sign convention while solving the problem
- Real image forms on the side of a refracting surface that is opposite to the object, and virtual image forms on the same side as the object.
- Using $R=\infty$ (i.e for plane surface)
we get $\frac{n_2}{v}=\frac{n_1}{u} \Rightarrow \frac{n_2}{n_1}=\frac{v}{u}$
If an object AB is placed in front of a curved surface as shown in the above figure, then the lateral Magnification formula is given as
Lateral magnification, $m=\frac{\text { Image height }}{\text { Object height }}=\frac{-\left(A^{\prime} B^{\prime}\right)}{A B}$
$
m=-\frac{A^{\prime} B^{\prime}}{A B}=-\frac{\mu_1}{\mu_2} \times \frac{v}{u}=-\frac{v / \mu_2}{u / \mu_1}
$
where
$\mu_{1}=\text { Refractive index of the medium from which light rays are coming (from the object). }$
$\mu_{2}=\text { Refractive index of the medium in which light rays are entering. }$
and $\mu_1<\mu_2$
and $\mathrm{u}=$ Distance of object, $\mathrm{v}=$ Distance of image, $\mathrm{R}=$ Radius of curvature
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