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← JEE Advanced 2016 · Paper 2
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JEE Advanced 2016 · Paper 2, Physics question 16

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PARAGRAPH 1

A frame of reference that is accelerated with respect to an inertial frame of reference is called a non-inertial frame of reference. A coordinate system fixed on a circular disc rotating about a fixed axis with a constant angular velocity ω\omega is an example of a non-inertial frame of reference.

The relationship between the force F⃗rot\vec F_{rot} experienced by a particle of mass mm moving on the rotating disc and the force F⃗in\vec F_{in} experienced by the particle in an inertial frame of reference is
F⃗rot=F⃗in+2m(v⃗rot×ω⃗)+m(ω⃗×r⃗)×ω⃗,\vec F_{rot}=\vec F_{in}+2m(\vec v_{rot}\times\vec\omega)+m(\vec\omega\times\vec r)\times\vec\omega,
where v⃗rot\vec v_{rot} is the velocity of the particle in the rotating frame of reference and r⃗\vec r is the position vector of the particle with respect to the centre of the disc.

Now consider a smooth slot along a diameter of a disc of radius RR rotating counter-clockwise with a constant angular speed ω\omega about its vertical axis through its center. We assign a coordinate system with the origin at the center of the disc, the xx-axis along the slot, the yy-axis perpendicular to the slot and the zz-axis along the rotation axis (ω⃗=ωk^)(\vec\omega=\omega\hat k). A small block of mass mm is gently placed in the slot at r⃗=(R/2)i^\vec r=(R/2)\hat i at t=0t=0 and is constrained to move only along the slot.

A horizontal disc of radius R rotating counter-clockwise with angular speed ω about a vertical axis through its centre. A straight slot runs along a diameter; a small block of mass m sits in the slot at distance R/2 from the centre.

The net reaction of the disc on the block is

Choose one option
Answer and worked solution

Official answer: B

Velocity in the slot. x˙=Rω4(eωt−e−ωt)\dot x=\dfrac{R\omega}4\left(e^{\omega t}-e^{-\omega t}\right).

Coriolis force.
2m(v⃗rot×ω⃗)=2mx˙ω(i^×k^)=−2mωx˙ j^.2m(\vec v_{rot}\times\vec\omega)=2m\dot x\omega(\hat i\times\hat k)=-2m\omega\dot x\,\hat j.
The slot wall must supply +2mωx˙ j^+2m\omega\dot x\,\hat j to keep the block in the slot. The disc's floor supports the weight with mgk^mg\hat k.

Net reaction.
N⃗=12mω2R(eωt−e−ωt)j^+mgk^.\vec N=\frac12m\omega^2R\left(e^{\omega t}-e^{-\omega t}\right)\hat j+mg\hat k.

(B)