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Question:(II) A ball of radius rrolls on the inside of a track of radius R(see Fig. 8鈥53). If the ball starts from rest at the vertical edge of the track, what will be its speed when it reaches the lowest point of the track, rolling without slipping?

Short Answer

Expert verified

The speed of the ball when it reaches the lowest point of the track is \(\sqrt {\frac{{10}}{7}g\left( {R - r} \right)} \).

Step by step solution

01

Identification of given data

The given data can be listed below as:

  • The radius of the ball is r.
  • The radius of the track is R.
  • The acceleration due to gravity is \(g = 9.81{\rm{ m/}}{{\rm{s}}^2}\).
02

Understanding the motion of the ball on the track

The ball is rolling inside the track.Therefore, the total energy of the ball on the track is the sum of the energy of the ball in a vertical circle, its translational kinetic energy, and its rotational kinetic energy.The acceleration due to gravity also acts on the ball during its motion on the track.

03

Representation of the track along with the ball

The diagram of the track can be shown as:

Here, A is the highest position of the ball on the circular track as the motion can be considered in the vertical circle. B is the lowest position of the ball on the track.

04

Determination of the speed of the ball when it reaches the lowest point of the track

The moment of inertia of the spherical ball can be expressed as:

\(I = \frac{2}{5}m{r^2}\)

Here, m is the mass of the ball.

It is given that the ball is rolling without slipping. The speed of the ball can be expressed as:

\(v = r\omega \)

Here,\(\omega \)is the angular speed of the ball.

At the lowest position (B) of the track, the ball has both types of speed, namely angular and linear speed.

The total energy of the ball in the vertical circle can be expressed as:

\(\begin{aligned}{c}{E_T} &= {E_b} + K.{E_t} + K.{E_r}\\mgR &= mgr + \frac{1}{2}m{v^2} + \frac{1}{2}I{\omega ^2}\\mg\left( {R - r} \right) &= \frac{1}{2}m{v^2} + \frac{1}{2} \times \frac{2}{5}m{r^2}{\omega ^2}\\g\left( {R - r} \right) &= \frac{1}{2}{v^2} + \frac{1}{5}{v^2}\end{aligned}\)

Here,\({E_T}\)is the total energy of the ball on the track,\({E_b}\)is the ball's energy in the vertical circle at point (A),\(K.{E_t}\)is the translational kinetic energy of the ball,\(K.{E_r}\)is the rotational kinetic energy of the ball, and g is the acceleration due to gravity.

The above equation can be further solved as:

\(\begin{aligned}{c}g\left( {R - r} \right) &= \frac{7}{{10}}{v^2}\\{v^2} &= \frac{{10}}{7}g\left( {R - r} \right)\\v &= \sqrt {\frac{{10}}{7}g\left( {R - r} \right)} \end{aligned}\)

Thus, the speed of the ball when it reaches the lowest point of the track is \(\sqrt {\frac{{10}}{7}g\left( {R - r} \right)} \).

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Most popular questions from this chapter

The angular velocity of a wheel rotating on a horizontal axle points west. In what direction is the linear velocity of a point on the top of the wheel? If the angular acceleration points east, describe the tangential linear acceleration of this point at the top of the wheel. Is the angular speed increasing or decreasing?

A cyclist accelerates from rest at a rate of \({\bf{1}}{\bf{.00}}\;{\bf{m/}}{{\bf{s}}^{\bf{2}}}\). How fast will a point at the top of the rim of the tire (diameter = 0.80 cm) be moving after 2.25 s? [Hint: At any moment, the lowest point on the tire is in contact with the ground and is at rest 鈥 sees Fig. 8鈥57.]

FIGURE 8-57 Problem 79

If the coefficient of static friction between a car鈥檚 tires and the pavement is 0.65, calculate the minimum torque that must be applied to the 66-cm-diameter tire of a 1080-kg automobile in order to 鈥渓ay rubber鈥 (make the wheels spin, slipping as the car accelerates). Assume each wheel supports an equal share of the weight.

A merry-go-round with a moment of inertia equal to \({\bf{1260}}\;{\bf{kg}} \cdot {{\bf{m}}{\bf{2}}}\) and a radius of 2.5 m rotates with negligible friction at \({\bf{1}}{\bf{.70}}\;{{{\bf{rad}}} \mathord{\left/ {\vphantom {{{\bf{rad}}} {\bf{s}}}} \right. \\{\bf{s}}}\). A child initially standing still next to the merry-go-round jumps onto the edge of the platform straight toward the axis of rotation, causing the platform to slow to \({\bf{1}}{\bf{.35}}\;{{{\bf{rad}}} \mathord{\left/{\vphantom {{{\bf{rad}}} {\bf{s}}}} \right.

\\{\bf{s}}}\). What is her mass?

A small mass m on a string is rotating without friction in a circle. The string is shortened by pulling it through the axis of rotation without any external torque, Fig. 8鈥39. What happens to the angular velocity of the object?

(a) It increases.

(b) It decreases.

(c) It remains the same.

FIGURE 8-39

Mis-Conceptual Questions 10 and 11.

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