List - I | List - II | ||
(P) | If a = 0, b = 1, c = 0 and d = 0, then | (1) | h is one-one. |
(Q) | If a = 1, b = 0, c = 0 and d = 0, then | (2) | h is onto. |
(R) | If a = 0, b = 0, c = 1 and d = 0, then | (3) | h is differentiable on \(\R\) |
(S) | If a = 0, b = 0, c = 0 and d = 1, then | (4) | the range of h is [0, 1]. |
(5) | the range of h is {0, 1}. |
To solve the problem, we analyze the function \( h(x) \) under the given conditions and match each case in List-I to the correct properties in List-II.
1. Understanding the Functions \( f(x) \) and \( g(x) \):
The function \( f(x) \) is defined as:
\( f(x) = \begin{cases} x|x|\sin\left(\frac{1}{x}\right), & x \neq 0, \\ 0, & x = 0. \end{cases} \)
The function \( g(x) \) is defined as:
\( g(x) = \begin{cases} 1 - 2x, & 0 \leq x \leq \frac{1}{2}, \\ 0, & \text{otherwise}. \end{cases} \)
2. Analyzing \( h(x) \) for Each Case:
The function \( h(x) \) is given by:
\( h(x) = a f(x) + b \left(g(x) + g\left(\frac{1}{2} - x\right)\right) + c (x - g(x)) + d g(x) \).
Case (P): \( a = 0, b = 1, c = 0, d = 0 \)
Here, \( h(x) = g(x) + g\left(\frac{1}{2} - x\right) \).
- For \( 0 \leq x \leq \frac{1}{2} \), \( g(x) = 1 - 2x \) and \( g\left(\frac{1}{2} - x\right) = 1 - 2\left(\frac{1}{2} - x\right) = 2x \). Thus, \( h(x) = 1 \).
- For \( x < 0 \) or \( x > \frac{1}{2} \), \( g(x) = 0 \) and \( g\left(\frac{1}{2} - x\right) = 0 \). Thus, \( h(x) = 0 \).
The range of \( h(x) \) is \( \{0, 1\} \), and \( h(x) \) is not one-one, not onto, and not differentiable everywhere (due to discontinuities at \( x = 0 \) and \( x = \frac{1}{2} \)).
Match: (P) → (5).
Case (Q): \( a = 1, b = 0, c = 0, d = 0 \)
Here, \( h(x) = f(x) \).
- The function \( f(x) \) is differentiable everywhere, including at \( x = 0 \) (as \( \lim_{x \to 0} x|x|\sin\left(\frac{1}{x}\right) = 0 \)).
- The range of \( f(x) \) is \( \mathbb{R} \) because \( x|x|\sin\left(\frac{1}{x}\right) \) oscillates between \( -x|x| \) and \( x|x| \), covering all real values as \( x \) varies.
Thus, \( h(x) \) is differentiable on \( \mathbb{R} \) and onto.
Match: (Q) → (3).
Case (R): \( a = 0, b = 0, c = 1, d = 0 \)
Here, \( h(x) = x - g(x) \).
- For \( 0 \leq x \leq \frac{1}{2} \), \( h(x) = x - (1 - 2x) = 3x - 1 \).
- For \( x < 0 \) or \( x > \frac{1}{2} \), \( h(x) = x \).
The function \( h(x) \) is one-one because it is strictly increasing (its derivative is positive where defined). It is also onto because as \( x \to \infty \), \( h(x) \to \infty \), and as \( x \to -\infty \), \( h(x) \to -\infty \).
Match: (R) → (2).
Case (S): \( a = 0, b = 0, c = 0, d = 1 \)
Here, \( h(x) = g(x) \).
- The range of \( g(x) \) is \( [0, 1] \) because for \( 0 \leq x \leq \frac{1}{2} \), \( g(x) \) decreases linearly from 1 to 0, and \( g(x) = 0 \) otherwise.
- The function \( g(x) \) is not one-one, not onto \( \mathbb{R} \), and not differentiable at \( x = 0 \) and \( x = \frac{1}{2} \).
Match: (S) → (4).
Final Answer:
The correct matching is:
\(\boxed{(P) \rightarrow (5); (Q) \rightarrow (3); (R) \rightarrow (2); (S) \rightarrow (4)}\).
To solve the matching problem, we need to analyze the function \(h(x)=af(x)+b(g(x)+g(\frac{1}{2}-x))+c(x-g(x))+d\ g(x)\) for each set of parameters given in List-I.
Analysis:
Final Matches:
(P) → (5), (Q) → (3), (R) → (2), (S) → (4)
Let \( f(x) = \sqrt{4 - x^2} \), \( g(x) = \sqrt{x^2 - 1} \). Then the domain of the function \( h(x) = f(x) + g(x) \) is equal to:
Figure 1 shows the configuration of main scale and Vernier scale before measurement. Fig. 2 shows the configuration corresponding to the measurement of diameter $ D $ of a tube. The measured value of $ D $ is:
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):