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Question
Draw a ray diagram for the formation of the image of a point object by a thin double convex lens having radii of curvature R1 and R2. Hence derive lens maker’s formula.
Solution
Lensmaker’s Formula:
When a ray refracts from a lens (double convex), in the above figure, then its image formation can be seen in terms of two steps:
Step 1: The first refracting surface forms the image l1 of the object O.
Step 2: The image of object O for the first surface acts like a virtual object for the second surface. Now for the first surface ABC, the ray will move from a rarer to a denser medium, and then
`n_2/(BI_1) + n_1/(OB) = (n_2 - n_1)/(BC_1)` ...(i)
Similarly for the second interface, ADC we can write.
`n_1/(DI) - n_2/(DI_1) = (n_2 - n_1)/(DC_2)` ...(ii)
DI1 is negative as the distance is measured against the direction of incident light.
Adding equation (1) and equation (2), we get
`n_2/(BI_1) + n_1/(OB) + n_1/(DI) - n_2/(DI_1) = (n_2 - n_1)/(BC_1) + (n_2 - n_1)/(DC_2)`
Or `n_1/(DI) + n_1/(OB) = (n_2 - n_1)(1/(BC_1) + 1/(DC_2))` ...(iii) (∵ for the thin lens BI1 = DI1)
Now, if we assume the object to be at infinity i.e. OB → ∞, then its image will form at focus F (with focal length f), i.e.
DI = f, thus equation (iii) can be rewritten as:
`n_1/f + n_1/∞ = (n_2 - n_1)(1/(BC_1) + 1/(DC_2))`
or `n_1/f = (n_2 - n_1)(1/(BC_1) + 1/(DC_2))` ...(iv)
Now according to the sign conventions,
BC1 = +R1 and DC2 = -R2 ...(v)
Substituting equation (v) in equation (iv), we get
`n_1/f = (n_2 - n_1)(1/R_1 - 1/R_2)`
`1/f = (n_2/n_1 - 1)(1/R_1 - 1/R_2)`
`1/f = (n_{21} - 1)(1/R_1 - 1/R_2)`