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Question: In List -I a constant force F is applied on the rod of mass m and length 'l' such that in each case ...

In List -I a constant force F is applied on the rod of mass m and length 'l' such that in each case rod moves. A transverse pulse is created at the end point P in each case. The time to move the pulse from P to Q is given in List -II. Then match the following.

A

(m, l)P→Fμ = 0(m = 4kg, l = 20 m, F = 5N)

B

(m, l)P→Fμ = 1/20(m = 9kg, l = 32 m, F = 8N)

C

↑FQ(m, l)P(m = 7kg, l = 14 m, F = 2N)

D

F(m, l)μα 1/10P(m = 10kg, l = 20 m, F = 2N)

Answer

(I)-(R), (II)-(P), (III)-(S), (IV)-(Q)

Explanation

Solution

The time taken for a transverse pulse to travel along a rod under varying tension T(x)T(x) is given by:

t=0ldxv(x)=0lμT(x)dx=ml0ldxT(x)t = \int_{0}^{l} \frac{dx}{v(x)} = \int_{0}^{l} \sqrt{\frac{\mu}{T(x)}} dx = \sqrt{\frac{m}{l}} \int_{0}^{l} \frac{dx}{\sqrt{T(x)}}

We calculate the tension T(x)T(x) at a distance xx from the starting point P of the pulse by applying Newton's second law to the segment of the rod from P to xx. The forces on this segment in the direction of motion are the tension T(x)T(x) at its end, and other external/internal forces like weight and friction. The net force equals the mass of the segment times the acceleration of the rod.

In all four cases, the tension distribution is found to be linear with distance from P, T(x)=kxT(x) = kx, where kk is a constant.

For cases I, II, III, and IV, we derived T(x)=FefflxT(x) = \frac{F_{eff}}{l} x, where FeffF_{eff} is the effective force responsible for creating tension along the rod.

  • Case I: Horizontal, frictionless. T(x)=FlxT(x) = \frac{F}{l} x. t=2mlFt = 2\sqrt{\frac{ml}{F}}. t=24×205=8t = 2\sqrt{\frac{4 \times 20}{5}} = 8 s.
  • Case II: Horizontal, friction. T(x)=FlxT(x) = \frac{F}{l} x. t=2mlFt = 2\sqrt{\frac{ml}{F}}. t=29×328=12t = 2\sqrt{\frac{9 \times 32}{8}} = 12 s.
  • Case III: Vertical. T(x)=FlxT(x) = \frac{F}{l} x. t=2mlFt = 2\sqrt{\frac{ml}{F}}. t=27×142=14t = 2\sqrt{\frac{7 \times 14}{2}} = 14 s.
  • Case IV: Inclined, horizontal force. T(x)=FcosθlxT(x) = \frac{F \cos\theta}{l} x. t=2mlFcosθt = 2\sqrt{\frac{ml}{F \cos\theta}}. t=210×202cos30=22003t = 2\sqrt{\frac{10 \times 20}{2 \cos 30^\circ}} = 2\sqrt{\frac{200}{\sqrt{3}}}. Approximating 32\sqrt{3} \approx 2, t22002=20t \approx 2\sqrt{\frac{200}{2}} = 20 s.

Matches: (I)-(R), (II)-(P), (III)-(S), (IV)-(Q).

Therefore, the final answer is (I)(R),(II)(P),(III)(S),(IV)(Q)(I)-(R), (II)-(P), (III)-(S), (IV)-(Q).