To solve the problem, we need to find the value of \( \gamma \) given the equations:
Let's work through these step-by-step:
The sum of the inverse sine functions equals \(\pi\). Since the range of \(\sin^{-1} x\) is \([-\frac{\pi}{2}, \frac{\pi}{2}]\), we deduce that it is possible if:
If \(\alpha = 1\), then \(\sin^{-1} \alpha = \frac{\pi}{2}\). Therefore:
Apply the identity where \(\sin^{-1} \beta + \sin^{-1} \gamma = \frac{\pi}{2}\) implies \(\beta = \cos \theta\) and \(\gamma = \cos \left(\frac{\pi}{2} - \theta\right) = \sin \theta\).
The equation given is:
Substitute values:
Expanding the left-hand side, we get:
Simplifying using trigonometrical identity \((\cos^2 \theta + \sin^2 \theta = 1)\), the expression becomes \(1 + 2 \cos \theta\).
Equate it to the right-hand side:
Simplifying gives:
Thus after substituting back for \(\gamma\):\(\gamma = \sin \theta = \frac{\sqrt{3}}{2}\)
Thus, the value of \(\gamma\) is \(\frac{\sqrt{3}}{2}\).
Let $\sin^{-1} \alpha = A$, $\sin^{-1} \beta = B$, $\sin^{-1} \gamma = C$
$A + B + C = \pi$
$(\alpha + \beta)^2 - \gamma^2 = 3 \alpha \beta$
$\alpha^2 + \beta^2 - \gamma^2 = \alpha \beta$
$\frac{\alpha^2 + \beta^2 - \gamma^2}{2 \alpha \beta} = \frac{1}{2}$
$\Rightarrow \cos C = \frac{1}{2}$
$\sin C = \gamma$
$\cos C = \sqrt{1 - \gamma^2} = \frac{1}{2}$
$\gamma = \frac{\sqrt{3}}{2}$

A biconvex lens is formed by using two plano-convex lenses as shown in the figure. The refractive index and radius of curvature of surfaces are also mentioned. When an object is placed on the left side of the lens at a distance of \(30\,\text{cm}\), the magnification of the image will be: 