List-I | List-II | ||
P | The capacitance between S1 and S4, with S2 and S3 not connected, is | I | \(3C_0\) |
Q | The capacitance between S1 and S4, with S2 shorted to S3, is | II | \(\frac{C_0}{2}\) |
R | The capacitance between S1 and S3, with S2 shorted to S4, is | III | \(\frac{C_0}{3}\) |
S | The capacitance between S1 and S2, with S3 shorted to S1, and S2 shorted to S4, is | IV | \(2\frac{C_0}{3}\) |
\[2C_0\] |
P → 2; Q → 3; R → 2; S → 1
P → 3; Q → 2; R → 2; S → 5
P. The capacitance between S1 and S4, with S2 and S3 not connected:
Effectively, this is the series combination of 3 capacitances, each \(\frac{C_0}{2}\):
\(\frac{1}{C} = \frac{1}{(\frac{C_0}{2})} + \frac{1}{(\frac{C_0}{2})} + \frac{1}{(\frac{C_0}{2})}\)
Thus, the total capacitance \(C = \frac{C_0}{3/2} = \frac{2C_0}{3}\).
Q. The capacitance between S1 and S4, with S2 shorted to S3:
By shorting S2 to S3, the central plates form a single capacitor leaving two capacitors in series:
\(\frac{1}{C} = \frac{1}{C_0} + \frac{1}{C_0}\), therefore, the capacitance becomes \(C = \frac{C_0}{2}\).
R. The capacitance between S1 and S3, with S2 shorted to S4:
When S2 and S4 are shorted, it becomes a system of capacitors in series equivalent to \(\frac{C_0}{3}\).
S. The capacitance between S1 and S2, with S3 shorted to S1, and S2 shorted to S4:
In this configuration, S3 to S1 shorted, S2 to S4 shorted forms two parallel configurations resulting in \(2C_0\).
Based on calculations, match each case:
P | The capacitance between S1 and S4, with S2 and S3 not connected, is | III | \(\frac{2C_0}{3}\) |
Q | The capacitance between S1 and S4, with S2 shorted to S3, is | II | \(\frac{C_0}{2}\) |
R | The capacitance between S1 and S3, with S2 shorted to S4, is | IV | \(\frac{C_0}{3}\) |
S | The capacitance between S1 and S2, with S3 shorted to S1, and S2 shorted to S4, is | I | \(2C_0\) |
Thus, the correct option is: \(P → 3; Q → 2; R → 4; S → 1\).
To solve the problem, we need to find the capacitance values for different configurations of four identical thin, square metal sheets arranged parallel to each other.
1. Understanding the Capacitance of a Single Capacitor:
The capacitance of two parallel plates each of side \(a\) separated by distance \(d\) is given by:
\( C_0 = \varepsilon_0 \frac{a^2}{d} \)
2. Analyzing the Different Configurations:
(P) Capacitance between \( S_1 \) and \( S_4 \), with \( S_2 \) and \( S_3 \) not connected:
Here, three capacitors \( C_0 \) are in series between the plates:
\( C = \frac{C_0}{3} \)
This corresponds to option (3).
(Q) Capacitance between \( S_1 \) and \( S_4 \), with \( S_2 \) shorted to \( S_3 \):
Shorting \( S_2 \) and \( S_3 \) makes them a single plate, so two capacitors \( C_0 \) in series remain:
\( C = \frac{C_0}{2} \)
This corresponds to option (2).
(R) Capacitance between \( S_1 \) and \( S_3 \), with \( S_2 \) shorted to \( S_4 \):
Shorting \( S_2 \) and \( S_4 \) makes them a single conductor.
The effective capacitance is two capacitors in parallel but with adjusted distances, resulting in:
\( C = \frac{2C_0}{3} \)
This corresponds to option (4).
(S) Capacitance between \( S_1 \) and \( S_2 \), with \( S_3 \) shorted to \( S_1 \) and \( S_2 \) shorted to \( S_4 \):
Shorting these plates creates two capacitors \( C_0 \) in parallel:
\( C = 2C_0 \)
This corresponds to option (1).
Final Matching:
\( P \to 3; Q \to 2; R \to 4; S \to 1 \)
Final Answer:
Option (C) \( P \to 3; Q \to 2; R \to 4; S \to 1 \)
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
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):