A string of length $L$ fixed at one end carries a body of mass $m$ at the other end. The mass is revolved in a circle in horizontal plane making angle $\theta$ with vertical. The angular frequency of the body is $\omega$. The tension in the string is
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Physics Tip: For conical pendulum: $T\sin\theta=m\omega^2r$ and $T\cos\theta=mg$.
Step 1: Recognize the motion.
This is a conical pendulum. The mass moves in a horizontal circle while the string makes constant angle $\theta$ with vertical.
Step 2: Forces acting on mass.
Two forces act:
• Weight $mg$ downward
• Tension $T$ along string
Horizontal component of tension provides centripetal force.
Step 3: Radius of circular path.
If string length is $L$:
$$
r=L\sin\theta
$$
Step 4: Centripetal force equation.
Required centripetal force:
$$
T\sin\theta=m\omega^2r
$$
Substitute $r=L\sin\theta$:
$$
T\sin\theta=m\omega^2(L\sin\theta)
$$
Step 5: Simplify.
Cancel $\sin\theta$ from both sides:
$$
T=mL\omega^2
$$
Thus tension is independent of angle $\theta$ in this form.
$$
\therefore \text{Correct option is (B).}
$$