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.
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