We are given the function \(f(x) = \cos^{-1}(\sqrt{x-1})\) and need to find its domain.
There are two conditions that must be satisfied for the function to be defined:
Since \(\sqrt{x-1}\) is always non-negative, we can rewrite the second condition as:
\(0 \le \sqrt{x-1} \le 1\)
Squaring all parts, we get:
\(0 \le x - 1 \le 1\)
Adding 1 to all parts, we get:
\(1 \le x \le 2\)
Combining both conditions \(x \ge 1\) and \(1 \le x \le 2\), we find that the domain is \(1 \le x \le 2\).
Thus, the correct option is (A) \([1, 2]\).
The function is \( f(x) = \cos^{-1}(\sqrt{x - 1}) \). For \( \sqrt{x - 1} \) to be real, we require: \[ x - 1 \geq 0 \quad \Rightarrow \quad x \geq 1 \] The range of \( \cos^{-1}(y) \) is \( [0, \pi] \), so the argument \( \sqrt{x - 1} \) must lie within the range \( [0, 1] \). Thus, we need: \[ 0 \leq \sqrt{x - 1} \leq 1 \] Squaring both sides: \[ 0 \leq x - 1 \leq 1 \] This simplifies to: \[ 1 \leq x \leq 2 \]
The domain of the function is \( [1, 2] \).
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
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: