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(a) Draw a ray diagram for formation of image of a point object by a thin double convex lens having radii of curvatures R1 and R2 and hence derive lens maker’s formula. 

(b) Define power of a lens and give its S.I. units. 

If a convex lens of focal length 50cm is placed in contact coaxially with a concave lens of focal length 20cm, what is the power of the combination?

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(a) 

From lens maker formula,

\(\frac 1f = (\mu - 1) \left(\frac 1{R_1} - \frac 1{R_2}\right)\)

Assumptions

The following assumptions are taken for the derivation of lens maker formula.

• Let us consider the thin lens shown in the image above with 2 refracting surfaces having the radii of curvatures R1 and R2 respectively. 

• Let the refractive indices of the surrounding medium and the lens material be n1 and n2 respectively.

Derivation

The complete derivation of lens maker formula is described below. Using the formula for refraction at a single spherical surface we can say that,

For the first surface,

\(\frac{n_2}{v_1} - \frac{n_1}u = \frac{n_2 - n_1}{R_1} \)   .......(1)

For the second surface,

\(\frac{n_1}{v} - \frac{n_2}{v_1} = \frac{n_1 - n_2}{R_2} \)    .....(2)

Now adding equation (1) and (2),

\(\frac {n_1}v - \frac {n_1}u = \left({n_2}-{n_1} \right) \left[\frac 1{R_1} - \frac 1{R_2}\right]\)

⇒ \(\frac 1v - \frac 1u = \left(\frac{n_2}{n_1} - 1\right) \left[\frac 1{R_1} - \frac 1{R_2}\right]\)

When u = \(\infty\) and v = f

\(\frac 1f = \left(\frac{n_2}{n_1} - 1\right) \left[\frac 1{R_1} - \frac 1{R_2}\right]\)

But also,

\(\frac 1v - \frac 1u = \frac 1f\)

Therefore we can say that,

\(\frac 1f = (u - 1) \left(\frac 1{R_1} - \frac 1{R_2}\right)\)

Where µ is the refractive index of the material.

This is the lens maker formula derivation.

(b) Power of a lens is its ability to converge or diverge the rays of light falling on it. Power of a lens is equal to reciprocal of the focal length of the lens.

SI unit of power is dioptre (D).

Given the focal length of convex lens, f1 = 50 cm = 0.5 m

The focal length of concave lens, f2 = 20 cm = 0.2 m

The equivalent focal length of the combination of lenses is given by the sum of individual focal lengths.

\(\frac 1{f_c} = \frac 1{f_1} + \frac 1{f_2}\)

Since the focal length of concave lens is negative, hence

\(\frac 1{f_c} = \frac 1{f_1}- \frac 1{f_2}\)

Substituting the values,

\(\frac 1{f_c} = \frac 1{0.5}- \frac 1{0.2}\)

\(= \frac{0.2 - 0.5}{0.5 \times 0.2}\)

⇒ \(\frac 1{f_c} = \frac{-0.3}{0.1} = -3\)

Thus, the power of the combination is

\(P_c = \frac 1{f_c } = -3D\)

Hence, the power of the combination of the lenses is -3D.

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(a) Lens Maker’s Formula: Suppose L is a thin lens. The refractive index of the material of lens is n2 and it is placed in a medium of refractive index n1. The optical centre of lens is C and X ' X is principal axis. The radii of curvature of the surfaces of the lens are R1  and R2  and their poles are P1  and P2. The thickness of lens is t, which is very small. O is a point object on the principal axis of the lens. The distance of O from pole P1  is u. The first refracting surface forms the image of O at I' at a distance v' from P1.From the refraction formula at spherical surface

The image I' acts as a virtual object for second surface and after refraction at second surface, the final image is formed at I. The distance of I from pole P2  of second surface is v. The distance of virtual object (I') from pole P2  is (v' - t). 

For refraction at second surface, the ray is going from second medium (refractive index n2 ) to first medium (refractive index n1 ), therefore from refraction formula at spherical surface

For a thin lens t is negligible as compared to v', therefore from (ii)

Adding equations (i) and (iii), we get 

where 1n2 = n2/n1 = is refractive index of second medium (i.e. medium of lens) with respect to first medium. 

If the object O is at infinity, the image will be formed at second focus i.e. if u= , v = f2 = f

Therefore from equation (iv)

This is the formula of refraction for a thin lens. This formula is called Lens-Maker’s formula. 

If first medium is air and refractive index of material of lens be n, then 1n2 = n, therefore equation (v) may be written as

(b) Power of a Lens: The power of a lens is its ability to deviate the rays towards its principal axis. It is defined as the reciprocal of focal length in metres.

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