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QJEEAdv17Ph2eaa: JEE Advanced 2017 Physics - Class 11 JEEAdv17Ph2eaa Solution: The minimum value of 0 below which the ring will drop down is

The minimum value of ω\omega 0 below which the ring will drop down is

Multiple Choice Options

  • A g2μ(R−r)\sqrt {{g \over {2\mu (R - r)}}}
  • B 3g2μ(R−r)\sqrt {{{3g} \over {2\mu (R - r)}}}
  • C gμ(R−r)\sqrt {{g \over {\mu (R - r)}}}
  • D 2gμ(R−r)\sqrt {{{2g} \over {\mu (R - r)}}}

Step-by-Step Verified Solution

Let the ring makes an angle α\alpha with the horizontal and the finger makes an angle β\beta with the vertical (see figure). The forces acting on the ring are its weight mg at the centre C, normal reaction N and the frictional force f at the contact point P. Resolve the forces in the horizontal and the vertical directions. The centre of mass C rotates with an angular velocity ω\omega 0 in a horizontal circle of radius (R −- r) cos α\alpha centred at O. Apply Newton's second law in the horizontal and the vertical directions to get

fcos⁡β−Nsin⁡β−Mg=0f\cos \beta - N\sin \beta - Mg = 0 ..... (1)

Ncos⁡β+fsin⁡β=Mω02(R−r)cos⁡αN\cos \beta + f\sin \beta = M\omega _0^2(R - r)\cos \alpha .... (2)

JEE Advanced 2017 Paper 2 Offline Physics - Rotational Motion Question 31 English Explanation
The minimum value of ω\omega 0 occurs when the frictional force attains its limiting value i.e.,

f=μNf = \mu N ....... (3)

Eliminate f and N from equations (1) - (3) to get

ω0, min⁡=[(cos⁡β+μsin⁡β)g(μcos⁡β−sin⁡β)(R−r)cos⁡α]1/2{\omega _{0,\,\min }} = {\left[ {{{(\cos \beta + \mu \sin \beta )g} \over {(\mu \cos \beta - \sin \beta )(R - r)\cos \alpha }}} \right]^{1/2}}

≈[gμ(R−r)]1/2\approx {\left[ {{g \over {\mu (R - r)}}} \right]^{1/2}} ( ∵\because α\alpha = 0 and β\beta = 0).

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