/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 35 What net torque is required to g... [FREE SOLUTION] | 91Ó°ÊÓ

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What net torque is required to give a uniform \(20-\mathrm{kg}\) solid ball with a radius of \(0.20 \mathrm{~m}\) an angular acceleration of \(20 \mathrm{rad} / \mathrm{s}^{2} ?\)

Short Answer

Expert verified
The net torque required is 6.4 N·m.

Step by step solution

01

Identify the Given Values

We are given:- Mass of the ball, \( m = 20 \text{ kg} \).- Radius of the ball, \( r = 0.20 \text{ m} \).- Angular acceleration, \( \alpha = 20 \text{ rad/s}^2 \).
02

Determine the Moment of Inertia for the Solid Ball

The moment of inertia \( I \) for a solid ball about an axis through its center is given by\[ I = \frac{2}{5} m r^2. \]Substituting the given values:\[ I = \frac{2}{5} \times 20 \times (0.20)^2 = \frac{2}{5} \times 20 \times 0.04 = \frac{2}{5} \times 0.8 = 0.32 \text{ kg} \cdot \text{m}^2. \]
03

Use the Formula for Net Torque

The net torque \( \tau \) required is related to the moment of inertia \( I \) and angular acceleration \( \alpha \) by the formula:\[ \tau = I \cdot \alpha. \]
04

Calculate the Net Torque

Substitute the values obtained into the net torque formula:\[ \tau = 0.32 \times 20 = 6.4 \text{ N} \cdot \text{m}. \]

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Moment of Inertia
Understanding the moment of inertia helps explain why some objects are harder to spin than others. It represents how mass is distributed relative to the rotational axis. For a solid ball, which is symmetric and has mass distributed evenly all around, the moment of inertia is determined using a specific formula.
  • For a solid ball, this formula is \( I = \frac{2}{5} mr^2 \), where \( m \) is the mass and \( r \) is the radius.
  • This formula arises from integrating the distribution of mass at varying distances from the axis of rotation.
For the example with a 20 kg ball having a radius of 0.20 meters, we calculated the moment of inertia as 0.32 kg \( \cdot \) m\(^2\). This helps us understand the ball's resistance to changes in its rotational state. Recognizing how mass and radius affect inertia is crucial in various physical applications, from mechanics to engineering.
Angular Acceleration
Angular acceleration is a critical concept for understanding how quickly an object can change its rotation. It's the rotational equivalent of linear acceleration and is denoted by \( \alpha \).
  • Angular acceleration defines how an object's rotational velocity changes over time.
  • In our problem, we have an angular acceleration of 20 rad/s\(^2\), which means that the ball's rotational speed increases by 20 radians per second every second.
Understanding angular acceleration is essential when calculating the net torque, as it directly influences how much torque is required to achieve the desired rotational velocity. The relationship between torque and angular acceleration is linear, meaning that doubling the torque will double the angular acceleration, assuming the mass distribution (moment of inertia) remains constant. This relationship is crucial when designing systems that involve rotational motion, such as engines or gears.
Solid Ball Mechanics
In solid ball mechanics, the principles of physics governing rotation help us predict how a solid sphere behaves under various forces. A solid ball, unlike a hollow sphere, has its entire mass evenly distributed throughout its volume.
  • This uniform distribution influences its moment of inertia, making it easier or harder to change its rotational speed.
  • The rigid nature of a solid ball ensures that its shape and size remain constant, regardless of the forces acting on it.
The mechanics of a solid sphere include understanding how it responds to applied torques and the resulting effects on motion. For example, when torque is applied, it causes angular acceleration, altering the ball's rotation. By comprehending these mechanics, we can apply the right amount of force to achieve desired outcomes in various applications, from sports like bowling to sophisticated machinery. This fundamental understanding of solid ball mechanics is critical in fields like engineering and physics.

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Most popular questions from this chapter

(a) How many uniform, identical textbooks of width \(25.0 \mathrm{~cm}\) can be stacked on top of each other on a level surface without the stack falling over if each successive book is displaced \(3.00 \mathrm{~cm}\) in width relative to the book below it? (b) If the books are \(5.00 \mathrm{~cm}\) thick, what will be the height of the center of mass of the stack above the level surface?

A ball with a radius of \(15 \mathrm{~cm}\) rolls on a level surface, and the translational speed of the center of mass is \(0.25 \mathrm{~m} / \mathrm{s}\). What is the angular speed about the center of mass if the ball rolls without slipping?

A kitten stands on the edge of a lazy Susan (a turntable). Assume that the lazy Susan has frictionless bearings and is initially at rest. (a) If the kitten starts to walk around the edge of the lazy Susan, the lazy Susan will (1) remain lazy and stationary, (2) rotate in the direction opposite that in which the kitten is walking, or (3) rotate in the direction the kitten is walking. Explain. (b) The mass of the kitten is \(0.50 \mathrm{~kg},\) and the lazy Susan has a mass of \(1.5 \mathrm{~kg}\) and a radius of \(0.30 \mathrm{~m}\). If the kitten walks at a speed of \(0.25 \mathrm{~m} / \mathrm{s},\) relative to the ground, what will be the angular speed of the lazy Susan? (c) When the kitten has walked completely around the edge and is back at its starting point, will that point be above the same point on the ground as it was at the start? If not, where is the kitten relative to the starting point? (Speculate on what might happen if everyone on the Earth suddenly started to run eastward. What effect might this have on the length of a day?)

Telephone and electrical lines are allowed to sag between poles so that the tension will not be too great when something hits or sits on the line. (a) Is it possible to have the lines perfectly horizontal? Why or why not? (b) Suppose that a line were stretched almost perfectly horizontally between two poles that are \(30 \mathrm{~m}\) apart. If a \(0.25-\mathrm{kg}\) bird perches on the wire midway between the poles and the wire sags \(1.0 \mathrm{~cm},\) what would be the tension in the wire? (Neglect the mass of the wire.)

A bowling ball with a radius of \(15.0 \mathrm{~cm}\) travels down the lane so that its center of mass is moving at \(3.60 \mathrm{~m} / \mathrm{s} .\) The bowler estimates that it makes about 7.50 complete revolutions in 2.00 seconds. Is it rolling without slipping? Prove your answer, assuming that the bowler's quick observation limits answers to two significant figures.

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