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Concepts Of Physics MCQ Edition [Volume 1]
Exam
Concepts Of Physics MCQ Edition [Volume 1]
Subject
Physics
Chapter
Rotational Mechanics

Concepts Of Physics MCQ Edition [Volume 1] · Physics · Rotational Mechanics

A small spherical ball of mass m rolls down a loop track. The ball...

A small spherical ball of mass mm rolls down a loop track. The ball is released on the linear portion at a vertical height HH from the lowest point. The circular part shown has a radius RR. Evaluate the normal force and the frictional force acting on the ball if H=60 cmH = 60 \text{ cm}, R=10 cmR = 10 \text{ cm}, θ=0\theta = 0 and m=70 gm = 70 \text{ g}.

Options

  1. A4.9 N4.9 \text{ N}, 0.196 N0.196 \text{ N} upward
  2. B9.8 N9.8 \text{ N}, 0.392 N0.392 \text{ N} upward
  3. C4.9 N4.9 \text{ N}, 0.196 N0.196 \text{ N} downward
  4. D2.45 N2.45 \text{ N}, 0.098 N0.098 \text{ N} upward

Correct answer

A. 4.9 N4.9 \text{ N}, 0.196 N0.196 \text{ N} upward

Step-by-step solution

Let the horizontal position on the loop track correspond to θ=0\theta = 0. At this point, the ball is at a height RR from the lowest point.

By the principle of conservation of mechanical energy from the release point to the horizontal position:

mgH=mgR+12mv2+12Iω2mgH = mgR + \dfrac{1}{2}mv^2 + \dfrac{1}{2}I\omega^2

For a solid spherical ball, the moment of inertia is I=25mr2I = \dfrac{2}{5}mr^2. For rolling without slipping, v=ωrv = \omega r. Substituting these into the energy equation:

mg(H−R)=12mv2+12(25mr2)(vr)2mg(H - R) = \dfrac{1}{2}mv^2 + \dfrac{1}{2}\left(\dfrac{2}{5}mr^2\right)\left(\dfrac{v}{r}\right)^2

mg(H−R)=710mv2⇒v2=107g(H−R)mg(H - R) = \dfrac{7}{10}mv^2 \Rightarrow v^2 = \dfrac{10}{7}g(H - R)

The normal force NN at the horizontal position provides the necessary centripetal force:

N=mv2R=107mg(H−RR)<br><br>GivenN = \dfrac{mv^2}{R} = \dfrac{10}{7}mg \left(\dfrac{H - R}{R}\right)<br><br>Givenm = 70  g=\text{ g} =0.07  kg,\text{ kg},g = 9.8  m/s2\text{ m/s}^2, H=60H = 60\text{ cm} =0.60.6\text{ m}, and R=10R = 10\text{ cm} =0.10.1\text{ m}:

N=N =\dfrac{10}{7} \times0.070.07\times9.89.8\times \left(\dfrac{0.6 - 0.1}{0.1}\right) =0.10.1\times9.89.8\times5=4.95 = 4.9\text{ N}

To find the frictional force ff, we analyze the tangential motion. Let ff act in the upward direction. The downward tangential force is gravity mgmg. The equation of linear motion is:

mg−f=matmg - f = ma_t

The torque about the center of mass is provided by the frictional force, which causes angular deceleration:

τ=fr=I\tau = f r = I\alpha = \left(\dfrac{2}{5}mr^2\right)\left(\dfrac{a_t}{r}\right) \Rightarrowf = \dfrac{2}{5}ma_t \Rightarrow ma_t = \dfrac{5}{2}f<br><br>Substituting<br><br>Substitutingma_tintothelinearmotionequation:<br><br>into the linear motion equation:<br><br>mg - f = \dfrac{5}{2}f \Rightarrow \dfrac{7}{2}f = mg \Rightarrow f = \dfrac{2}{7}mg<br><br>Calculatingthemagnitudeofthefrictionalforce:<br><br><br><br>Calculating the magnitude of the frictional force:<br><br>f = \dfrac{2}{7} \times0.07 \times9.8 = 0.02 \times9.8 = 0.196 \text{ N}<br><br>Sincethecalculatedvalueof<br><br>Since the calculated value offispositive,theassumedupwarddirectioniscorrect.Thefrictionactsupwardtoprovidethetorquerequiredtoslowdowntheball′srotationasitascends.<br><br>Answer:is positive, the assumed upward direction is correct. The friction acts upward to provide the torque required to slow down the ball's rotation as it ascends.<br><br>Answer:4.9 \text{ N},0.196 \text{ N}upward
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