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Worked Examples · Example 1.5

Q.Semi-vertical angle of the conical section of a funnel is 37°. There is a small ball kept inside the funnel. On rotating the funnel, the maximum speed that the ball can have in order to remain in the funnel is 2 m/s. Calculate inner radius of the brim of the funnel. Is there any limit upon the frequency of rotation? How much is it? Is it lower or upper limit? Give a logical reasoning. (Use g = 10 m/s² and sin 37° = 0.6)

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Resolving N for a ball on the funnel wall gives r=v2tan⁡θgr=\dfrac{v^2\tan\theta}{g}; as v→0v\to0, r→0r\to0 with frequency INCREASING, so only a lower limit on n exists — reached at the brim.

Forces on the ball inside the rotating funnel: N perpendicular to the wall with components N sin θ (vertical) and N cos θ (horizontal), and the weight mg
Forces on the ball inside the rotating funnel: N perpendicular to the wall with components N sin θ (vertical) and N cos θ (horizontal), and the weight mg

A conical funnel of semi-vertical angle 37∘37^\circ holds a small ball that can rotate along the inside surface of the funnel; the MAXIMUM speed the ball can have while still remaining inside the funnel is given as 2 m/s (use g = 10 m/s^2, sin⁡37∘=0.6\sin37^\circ=0.6). Since a rotating ball inside a funnel behaves exactly like a conical pendulum with the normal reaction N playing the role of the string tension, tan⁡θ=v2/(rg)\tan\theta=v^2/(rg) gives the inner radius r at the brim (where the maximum speed is reached) as r=vmax2gtan⁡θ=410×0.75≈0.3r=\frac{v_{max}^2}{g\tan\theta}=\frac{4}{10\times0.75}\approx0.3 m. The example's discussion then notes that as the ball approaches the (narrower) base of the funnel its linear speed decreases but its angular speed/frequenc …

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