The greatest integer function [x] takes any real number x and rounds it down to the nearest integer.
The range of the greatest integer function is the set of all integers.
The domain of the inverse cosine function, \(\cos^{-1}(x)\), is [-1, 1], where x is a real number.
To find the domain of \(\cos^{-1}[x]\), we need to determine the values of x for which [x] lies within the range of [-1, 1].
Since the range of [x] is the set of all integers, we need to find the integers that lie within the range of [-1, 1].
The integers that lie within the range of [-1, 1] are -1, 0, and 1.
Therefore, the domain of \(\cos^{-1}[x]\) is the set of values for which [x] is equal to -1, 0, or 1.
So, the domain of \(\cos^{-1}[x]\) is [-1, 2) (option D).
Let \( f(x) = \cos^{-1}([x]) \), where \([x]\) is the greatest integer function. The domain of \( \cos^{-1}(x) \) is \( [-1, 1] \). So, \([x]\) must lie in \( [-1, 1] \). That means possible values of \([x]\) are \( -1, 0, 1 \) For:
Combining all: \[ x \in [-1, 2) \] So, the domain is: \([-1, 2)\)
We need to find the domain of \(cos^{-1}[x]\), where [x] denotes the greatest integer function.
The domain of the inverse cosine function, cos-1(y), is -1 ≤ y ≤ 1. Therefore, for cos-1[x] to be defined, we must have:
-1 ≤ [x] ≤ 1
This means that the greatest integer function of x must be between -1 and 1, inclusive. Let's consider the possible values of [x]:
Combining these intervals, we get:
-1 ≤ x < 0, 0 ≤ x < 1, 1 ≤ x < 2
This is equivalent to -1 ≤ x < 2
Therefore, the domain of cos-1[x] is [-1, 2).
Answer: [-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: