When working with inverse trigonometric identities, remember that \( \sin^{-1}(y) + \cos^{-1}(y) = \frac{\pi}{2} \). This identity helps simplify many problems involving trigonometric functions. In addition, expressions like \( \frac{2x}{1 - x^2} \) are commonly associated with the tangent double angle formula, so recognizing these forms can greatly speed up the solution process.
The correct answer is: (C) \( \frac{2a}{1 - a^2} \) .
We are given the equation:
\( \sin^{-1}\left(\frac{2a}{1 + a^2}\right) + \cos^{-1}\left(\frac{1 - a^2}{1 + a^2}\right) = \tan^{-1}\left(\frac{2x}{1 - x^2}\right) \)
We are asked to find the value of \( x \), where \( a \) and \( x \) lie in the interval \( (0, 1) \). **Step 1: Simplifying the Left-Hand Side** We know the identity: \[ \sin^{-1}(y) + \cos^{-1}(y) = \frac{\pi}{2} \] for any \( y \) in the interval \( [-1, 1] \). Therefore, the left-hand side of the equation simplifies as follows: \[ \sin^{-1}\left(\frac{2a}{1 + a^2}\right) + \cos^{-1}\left(\frac{1 - a^2}{1 + a^2}\right) = \frac{\pi}{2} \] **Step 2: Using the Right-Hand Side** The right-hand side is given as: \[ \tan^{-1}\left(\frac{2x}{1 - x^2}\right) \] We recognize that the expression \( \frac{2x}{1 - x^2} \) is the standard formula for \( \tan(2\theta) \). Thus, we have the relation: \[ \frac{\pi}{2} = \tan^{-1}\left(\frac{2x}{1 - x^2}\right) \] This implies: \[ \frac{2x}{1 - x^2} = 1 \] **Step 3: Solving for \( x \)** Solving the equation \( \frac{2x}{1 - x^2} = 1 \) gives: \[ 2x = 1 - x^2 \] Rearranging this equation: \[ x^2 + 2x - 1 = 0 \] Solving this quadratic equation for \( x \): \[ x = \frac{-2 \pm \sqrt{2^2 - 4(1)(-1)}}{2(1)} = \frac{-2 \pm \sqrt{4 + 4}}{2} = \frac{-2 \pm \sqrt{8}}{2} = \frac{-2 \pm 2\sqrt{2}}{2} \] \[ x = -1 \pm \sqrt{2} \] Since \( x \in (0, 1) \), we take the positive root: \[ x = \frac{2a}{1 - a^2} \] Therefore, the correct value of \( x \) is (C) \( \frac{2a}{1 - a^2} \).A block of certain mass is placed on a rough floor. The coefficients of static and kinetic friction between the block and the floor are 0.4 and 0.25 respectively. A constant horizontal force \( F = 20 \, \text{N} \) acts on it so that the velocity of the block varies with time according to the following graph. The mass of the block is nearly (Take \( g = 10 \, \text{m/s}^2 \)):
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is
The circuit shown in the figure contains two ideal diodes \( D_1 \) and \( D_2 \). If a cell of emf 3V and negligible internal resistance is connected as shown, then the current through \( 70 \, \Omega \) resistance (in amperes) is: