1. Understand the problem:
We need to differentiate the expression \( \cos^2 \left( \cot^{-1} \sqrt{\frac{2+x}{2-x}} \right) \) with respect to \( x \).
2. Simplify the expression:
Let \( \theta = \cot^{-1} \sqrt{\frac{2+x}{2-x}} \). Then, \( \cot \theta = \sqrt{\frac{2+x}{2-x}} \).
Construct a right triangle with adjacent side \( \sqrt{2+x} \) and opposite side \( \sqrt{2-x} \). The hypotenuse is:
\[ \sqrt{(\sqrt{2+x})^2 + (\sqrt{2-x})^2} = \sqrt{2+x + 2-x} = \sqrt{4} = 2 \]
Thus, \( \cos \theta = \frac{\sqrt{2+x}}{2} \), and:
\[ \cos^2 \theta = \left( \frac{\sqrt{2+x}}{2} \right)^2 = \frac{2+x}{4} \]
3. Differentiate with respect to \( x \):
Now, the expression simplifies to \( \frac{2+x}{4} \). Differentiate:
\[ \frac{d}{dx} \left( \frac{2+x}{4} \right) = \frac{1}{4} \]
Correct Answer: (D) \( \frac{1}{4} \)
1. Let's simplify the expression first
Let $ \theta = \cot^{-1}\left(\frac{\sqrt{2+x}}{\sqrt{2-x}}\right) $.
Then, $ \cot(\theta) = \frac{\sqrt{2+x}}{\sqrt{2-x}} $.
Consider a right-angled triangle where the adjacent side is $ \sqrt{2+x} $ and the opposite side is $ \sqrt{2-x} $.
Then the hypotenuse is:
\[ \sqrt{\left(\sqrt{2+x}\right)^2 + \left(\sqrt{2-x}\right)^2} = \sqrt{(2+x) + (2-x)} = \sqrt{4} = 2 \]
Therefore, $ \cos(\theta) = \frac{\text{Adjacent}}{\text{Hypotenuse}} = \frac{\sqrt{2+x}}{2} $.
So, $ \cos^2\left(\cot^{-1}\left(\frac{\sqrt{2+x}}{\sqrt{2-x}}\right)\right) = \cos^2(\theta) = \left(\frac{\sqrt{2+x}}{2}\right)^2 = \frac{2+x}{4} $.
2. Now differentiate:
\[ \frac{d}{dx} \left[\cos^2\left(\cot^{-1}\left(\frac{\sqrt{2+x}}{\sqrt{2-x}}\right)\right)\right] = \frac{d}{dx} \left[\frac{2+x}{4}\right] = \frac{1}{4} \]
Therefore, the derivative is $ \frac{1}{4} $.
A stationary tank is cylindrical in shape with two hemispherical ends and is horizontal, as shown in the figure. \(R\) is the radius of the cylinder as well as of the hemispherical ends. The tank is half filled with an oil of density \(\rho\) and the rest of the space in the tank is occupied by air. The air pressure, inside the tank as well as outside it, is atmospheric. The acceleration due to gravity (\(g\)) acts vertically downward. The net horizontal force applied by the oil on the right hemispherical end (shown by the bold outline in the figure) is:
Draw a rough sketch for the curve $y = 2 + |x + 1|$. Using integration, find the area of the region bounded by the curve $y = 2 + |x + 1|$, $x = -4$, $x = 3$, and $y = 0$.
Let \[ I(x) = \int \frac{dx}{(x-11)^{\frac{11}{13}} (x+15)^{\frac{15}{13}}} \] If \[ I(37) - I(24) = \frac{1}{4} \left( b^{\frac{1}{13}} - c^{\frac{1}{13}} \right) \] where \( b, c \in \mathbb{N} \), then \[ 3(b + c) \] is equal to:
In an experiment to determine the figure of merit of a galvanometer by half deflection method, a student constructed the following circuit. He applied a resistance of \( 520 \, \Omega \) in \( R \). When \( K_1 \) is closed and \( K_2 \) is open, the deflection observed in the galvanometer is 20 div. When \( K_1 \) is also closed and a resistance of \( 90 \, \Omega \) is removed in \( S \), the deflection becomes 13 div. The resistance of galvanometer is nearly:
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