k transparent slabs are arranged one over another. The refractive indices of the slabs are $\mu_1,\mu_2,\mu_3, \ ...\mu_{\text{k}}$ and the thicknesses are $t_1, t_2, t_3, ... t_k$ . An object is seen through this combination with nearly perpendicular light. Find the equivalent refractive index of the system which will allow the image to be formed at the same place.
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Total no. of slabs = k, thickness $= t_1, t_2, t_3, ... t_k$ Refractive index $=\mu_1,\mu_2,\mu_3, \ ...\mu_{\text{k}}$
$\therefore$ The shift $\Delta\text{t}=\Big(1-\frac{1}{\mu_1}\Big)\text{t}_1+\Big(1-\frac{1}{\mu_2}\Big)\text{t}_2+ \ ... \ \Big(1-\frac{1}{\mu_{\text{k }}}\Big)\text{t}_{\text{k}} \ ...(1)$
If, $\mu\rightarrow$ refractive index of combination of slabs and image is formed at same place,
$\Delta\text{t}=\Big(1-\frac{1}{\mu}\Big)(\text{t}_1+\text{t}_2+...+\text{t}_{\text{k}}) \ ...(2)$
Equation (1) and (2), we get,
$\Big(1-\frac{1}{\mu}\Big)(\text{t}_1+\text{t}_2+...+\text{t}_{\text{k}})$
$=\Big(1-\frac{1}{\mu_1}\Big)\text{t}_1+\Big(1-\frac{1}{\mu_2}\Big)\text{t}_2+ ...+\Big(1-\frac{1}{\mu_{\text{k}}}\Big)\text{t}_{\text{k}}$
$=(\text{t}_1+\text{t}_2+...+\text{t}_{\text{k}})-\Big(\frac{\text{t}_1}{\mu_1}+\frac{\text{t}_2}{\mu_2}+...+\frac{\text{t}_{\text{k}}}{\mu_{\text{k}}}\Big)$
$=-\frac{1}{\mu}\sum\limits_{\text{i}=1}^\text{k}\text{t}_1=-\sum\limits_{\text{i}=1}^\text{k}\Big(\frac{\text{t}_1}{\mu_1}\Big)\Rightarrow\mu=\frac{\sum\limits_{\text{i}=1}^\text{k}\text{t}_1}{\sum\limits_{\text{i}=1}^\text{k}\big(\frac{\text{t}_1}{\mu_1}\big)}.$
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