
Column I | Column II | ||
|---|---|---|---|
I | $\frac{1}{\sqrt{2}}(\sin \omega t \hat{j}+\cos \omega t \hat{k})$ | P | 0 |
II | $\frac{1}{\sqrt{2}}(\sin \omega t \hat{i}+\cos \omega t \hat{j})$ | Q | $-\frac{\alpha}{4} \hat{i}$ |
III | $\frac{1}{\sqrt{2}}(\sin \omega t \hat{i}+\cos \omega t \hat{k})$ | R | $\frac{3 \alpha}{4} \hat{i}$ |
IV | $\frac{1}{\sqrt{2}}(\cos \omega t \hat{i}+\sin \omega t \hat{k})$ | S | $\frac{\alpha}{4} \hat{j}$ |
|
| T | $-\frac{3 \alpha}{4} \hat{i}$ |
Which one of the following options is correct?
Step 1: Understanding the Magnetic Field and Torque
We are dealing with a small circular loop of area \( A \) and resistance \( R \), placed in a solenoid carrying a time-varying current. The magnetic field inside the solenoid is given by \( B(t) = B_0 \cos(\omega t) \), where \( B_0 \) is the amplitude of the magnetic field, and \( \omega \) is the angular frequency.
The torque on the loop is given by: \[ \tau = \mu \times B \] where \( \mu = I A \hat{n} \) is the magnetic moment of the loop, and \( B \) is the magnetic field. The time-varying magnetic field induces a torque on the loop, which varies with time.
Step 2: Analyzing Column I Expressions
The expressions in Column I represent the time-varying magnetic field and the corresponding torques in Column II.
Expression I: \( \frac{1}{\sqrt{2}} (\sin(\omega t) + \cos(\omega t)) \)
This expression represents the time-varying magnetic field. Since both the sine and cosine terms oscillate with the same frequency, their combination results in a net zero average torque over one complete cycle. Therefore, the torque corresponding to this field is \({Q} \), which indicates zero torque.
Expression II: \( \frac{1}{\sqrt{2}} (\sin(\omega t) + \cos(\omega t)) \)
This expression is similar to Expression I. Given the same sinusoidal time-dependence, the net torque is again zero over one complete cycle, so the corresponding torque is \({P} \), which is also zero.
Expression III: \( \frac{1}{\sqrt{2}} (\sin(\omega t) + \cos(\omega t)) \)
This time-varying field produces a torque that is proportional to the angular frequency \( \omega \), which gives a non-zero torque that oscillates. The corresponding torque expression is \({S} \).
Expression IV: \( \frac{1}{\sqrt{2}} (\cos(\omega t) + \sin(\omega t)) \)
Like Expression III, this expression also results in a non-zero torque but with a different time-dependence. The corresponding torque expression for this is \({R} \).
Step 3: Final Answer
Based on the analysis, the correct matching is:
Final Answer: The correct option is: C: I → Q, II → P, III → S, IV → R.

As shown in the figures, a uniform rod $ OO' $ of length $ l $ is hinged at the point $ O $ and held in place vertically between two walls using two massless springs of the same spring constant. The springs are connected at the midpoint and at the top-end $ (O') $ of the rod, as shown in Fig. 1, and the rod is made to oscillate by a small angular displacement. The frequency of oscillation of the rod is $ f_1 $. On the other hand, if both the springs are connected at the midpoint of the rod, as shown in Fig. 2, and the rod is made to oscillate by a small angular displacement, then the frequency of oscillation is $ f_2 $. Ignoring gravity and assuming motion only in the plane of the diagram, the value of $\frac{f_1}{f_2}$ is:
The reaction sequence given below is carried out with 16 moles of X. The yield of the major product in each step is given below the product in parentheses. The amount (in grams) of S produced is ____. 
Use: Atomic mass (in amu): H = 1, C = 12, O = 16, Br = 80
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.
Let $ \mathbb{R} $ denote the set of all real numbers. Then the area of the region $$ \left\{ (x, y) \in \mathbb{R} \times \mathbb{R} : x > 0, y > \frac{1}{x},\ 5x - 4y - 1 > 0,\ 4x + 4y - 17 < 0 \right\} $$ is
Electromagnetic Induction is a current produced by the voltage production due to a changing magnetic field. This happens in one of the two conditions:-
The electromagnetic induction is mathematically represented as:-
e=N × d∅.dt
Where