For trigonometric functions like \( \cot(x) \), look for values where the denominator of the function becomes zero. For \( \cot(x) = \frac{\cos(x)}{\sin(x)} \), the function is undefined whenever \( \sin(x) = 0 \), which happens at multiples of \( \pi \). These are the points of discontinuity.
The correct answer is: (B) \( \left\{ x = n\pi ;\ n \in \mathbb{Z} \right\} \).
The function \( f(x) = \cot(x) \) is discontinuous at points where the denominator of the cotangent function is zero. The cotangent function is defined as:
\( \cot(x) = \frac{\cos(x)}{\sin(x)} \)
The function \( \cot(x) \) is undefined when \( \sin(x) = 0 \), which occurs at multiples of \( \pi \), i.e., \( x = n\pi \), where \( n \in \mathbb{Z} \) (the set of all integers). Therefore, \( f(x) = \cot(x) \) is discontinuous at \( x = n\pi \), for \( n \in \mathbb{Z} \). Thus, the correct answer is (B) \( \left\{ x = n\pi ;\ n \in \mathbb{Z} \right\} \).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: