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 $\sin^{-1} \alpha = A$, $\sin^{-1} \beta = B$, $\sin^{-1} \gamma = C$
$A + B + C = \pi$
$(\alpha + \beta)^2 - \gamma^2 = 3 \alpha \beta$
$\alpha^2 + \beta^2 - \gamma^2 = \alpha \beta$
$\frac{\alpha^2 + \beta^2 - \gamma^2}{2 \alpha \beta} = \frac{1}{2}$
$\Rightarrow \cos C = \frac{1}{2}$
$\sin C = \gamma$
$\cos C = \sqrt{1 - \gamma^2} = \frac{1}{2}$
$\gamma = \frac{\sqrt{3}}{2}$
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).

Match the LIST-I with LIST-II for an isothermal process of an ideal gas system. 
Choose the correct answer from the options given below:
Which one of the following graphs accurately represents the plot of partial pressure of CS₂ vs its mole fraction in a mixture of acetone and CS₂ at constant temperature?
