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Question: A point particle of mass M is attached to one end of a massless rigid non-conducting rod of length L...

A point particle of mass M is attached to one end of a massless rigid non-conducting rod of length L. Another point particle of the same mass is attached to other end of the rod. The two particles carry charges +q and – q respectively. This arrangement is held in a region of a uniform electric field E such that the rod makes a small angle θ (say of about 5 degrees) with the field direction (see figure). Will be minimum time, needed for the rod to become parallel to the field after it is set free

A

t=2πmL2pEt = 2\pi\sqrt{\frac{mL}{2pE}}

B

t=π2mL2qEt = \frac{\pi}{2}\sqrt{\frac{mL}{2qE}}

C

t=3π2mL2pEt = \frac{3\pi}{2}\sqrt{\frac{mL}{2pE}}

D

t=π2mLqEt = \pi\sqrt{\frac{2mL}{qE}}

Answer

t=π2mL2qEt = \frac{\pi}{2}\sqrt{\frac{mL}{2qE}}

Explanation

Solution

In the given situation system oscillate in electric field with maximum angular displacement θ.

It’s time period of oscillation (similar to dipole)

T=2πIpET = 2\pi\sqrt{\frac{I}{pE}} where I = moment of inertia of the

system and p=qLp = qL

Hence the minimum time needed for the rod becomes parallel to the field is t=T4=π2IpEt = \frac{T}{4} = \frac{\pi}{2}\sqrt{\frac{I}{pE}}

Here I=M(L2)2+M(L2)2=ML22I = M\left( \frac{L}{2} \right)^{2} + M\left( \frac{L}{2} \right)^{2} = \frac{ML^{2}}{2}

t=π2ML22×qL×E=π2ML2qEt = \frac{\pi}{2}\sqrt{\frac{ML^{2}}{2 \times qL \times E}} = \frac{\pi}{2}\sqrt{\frac{ML}{2qE}}