Step 1: Find the inverse of \( f(x) = \tan x \)
The function \( f(x) = \tan x \) is periodic, with a period of \( \pi \). The inverse function \( f^{-1}(x) \) gives us the angle whose tangent is \( x \).
Step 2: Find \( f^{-1}(1) \)
We need to find \( x \) such that:
\[ \tan x = 1. \]
The solution to \( \tan x = 1 \) is \( x = \frac{\pi}{4} + n\pi \), where \( n \in \mathbb{Z} \) because the tangent function repeats every \( \pi \).
Step 3: Conclusion
Thus, \( f^{-1}(1) = \{ n\pi + \frac{\pi}{4} : n \in \mathbb{Z} \} \).
The function \( f(x) = \tan x \) is a periodic function with a period of \( \pi \).
The range of the tangent function is all real numbers, i.e., \( (-\infty, \infty) \).
However, the function is not one-to-one (injective) on its entire domain, so it does not have an inverse function on the whole real line.
To find the inverse function, we restrict the domain of the tangent function to the interval \( \left(-\frac{\pi}{2}, \frac{\pi}{2}\right) \). On this interval, the tangent function is strictly increasing and has a range of \( (-\infty, \infty) \).
The inverse function is denoted as \( \arctan(x) \) or \( \tan^{-1}(x) \).
The principal value of \( x \) for which \( \tan x = 1 \) is \( x = \frac{\pi}{4} \).
However, since the tangent function is periodic with period \( \pi \), there are infinitely many values of \( x \) for which \( \tan x = 1 \).
These values are given by \( x = n\pi + \frac{\pi}{4} \), where \( n \) is an integer.
Therefore, \( f^{-1}(1) \) is the set \( \{n\pi + \frac{\pi}{4} : n \in \mathbb{Z}\} \).
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