We need to find the value of \(\cos(\sin^{-1}(\frac{\pi}{3}) + \cos^{-1}(\frac{\pi}{3}))\).
First, note that the domain of both \(\sin^{-1}(x)\) and \(\cos^{-1}(x)\) is \([-1, 1]\). However, \(\frac{\pi}{3} \approx \frac{3.14}{3} > 1\). Therefore, \(\sin^{-1}(\frac{\pi}{3})\) and \(\cos^{-1}(\frac{\pi}{3})\) are not defined.
Since \(\sin^{-1}(\frac{\pi}{3})\) and \(\cos^{-1}(\frac{\pi}{3})\) do not exist, the entire expression does not exist.
Thus, the correct option is (D) Does not exist.
\[ \cos\left( \sin^{-1}\left( \frac{\pi}{3} \right) + \cos^{-1}\left( \frac{\pi}{3} \right) \right) \]
- \( \sin^{-1}\left( \frac{\pi}{3} \right) \) and \( \cos^{-1}\left( \frac{\pi}{3} \right) \) are angles whose sine and cosine are \( \frac{\pi}{3} \), respectively.
However, the values of \( \sin^{-1}(x) \) and \( \cos^{-1}(x) \) are defined only for arguments between \(-1\) and \( 1\).
Since \( \frac{\pi}{3} \approx 1.047 \) is greater than 1, neither \( \sin^{-1} \left( \frac{\pi}{3} \right) \) nor \( \cos^{-1} \left( \frac{\pi}{3} \right) \) is defined.
The value does not exist.
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
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: