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 rolls down a loop track. The ball is released on the linear portion at a vertical height from the lowest point. The circular part shown has a radius . Evaluate the normal force and the frictional force acting on the ball if , , and .
Options
- A, upward
- B, upward
- C, downward
- D, upward
Correct answer
A. , upward
Step-by-step solution
Let the horizontal position on the loop track correspond to . At this point, the ball is at a height from the lowest point.
By the principle of conservation of mechanical energy from the release point to the horizontal position:
For a solid spherical ball, the moment of inertia is . For rolling without slipping, . Substituting these into the energy equation:
The normal force at the horizontal position provides the necessary centripetal force:
m = 70 0.07 g = 9.8 , \text{ cm} =\text{ m}, and \text{ cm} =\text{ m}:
\dfrac{10}{7} \times\times\times \left(\dfrac{0.6 - 0.1}{0.1}\right) =\times\times\text{ N}
To find the frictional force , we analyze the tangential motion. Let act in the upward direction. The downward tangential force is gravity . The equation of linear motion is:
The torque about the center of mass is provided by the frictional force, which causes angular deceleration:
\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}fma_tmg - f = \dfrac{5}{2}f \Rightarrow \dfrac{7}{2}f = mg \Rightarrow f = \dfrac{2}{7}mgf = \dfrac{2}{7} \times0.07 \times9.8 = 0.02 \times9.8 = 0.196 \text{ N}f4.9 \text{ N},0.196 \text{ N}upward
By the principle of conservation of mechanical energy from the release point to the horizontal position:
For a solid spherical ball, the moment of inertia is . For rolling without slipping, . Substituting these into the energy equation:
The normal force at the horizontal position provides the necessary centripetal force:
m = 70 0.07 g = 9.8 , \text{ cm} =\text{ m}, and \text{ cm} =\text{ m}:
\dfrac{10}{7} \times\times\times \left(\dfrac{0.6 - 0.1}{0.1}\right) =\times\times\text{ N}
To find the frictional force , we analyze the tangential motion. Let act in the upward direction. The downward tangential force is gravity . The equation of linear motion is:
The torque about the center of mass is provided by the frictional force, which causes angular deceleration:
\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}fma_tmg - f = \dfrac{5}{2}f \Rightarrow \dfrac{7}{2}f = mg \Rightarrow f = \dfrac{2}{7}mgf = \dfrac{2}{7} \times0.07 \times9.8 = 0.02 \times9.8 = 0.196 \text{ N}f4.9 \text{ N},0.196 \text{ N}upward