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 $\sin^{-1} \alpha = A$, $\sin^{-1} \beta = B$, $\sin^{-1} \gamma = C$
$A + B + C = \pi$
$(\alpha + \beta)^2 - \gamma^2 = 3 \alpha \beta$
$\alpha^2 + \beta^2 - \gamma^2 = \alpha \beta$
$\frac{\alpha^2 + \beta^2 - \gamma^2}{2 \alpha \beta} = \frac{1}{2}$
$\Rightarrow \cos C = \frac{1}{2}$
$\sin C = \gamma$
$\cos C = \sqrt{1 - \gamma^2} = \frac{1}{2}$
$\gamma = \frac{\sqrt{3}}{2}$
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,