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A wheel of radius \(0.250 \mathrm{~m}\), moving initially at \(43.0 \mathrm{~m} / \mathrm{s}\), rolls to a stop in \(225 \mathrm{~m}\). Calculate the magnitudes of its (a) linear acceleration and (b) angular acceleration. (c) Its rotational inertia is \(0.155\) \(\mathrm{kg} \cdot \mathrm{m}^{2}\) about its central axis. Find the magnitude of the torque about the central axis due to friction on the wheel.

Short Answer

Expert verified
(a) Linear acceleration: \(-4.11 \text{ m/s}^2\); (b) Angular acceleration: \(-16.44 \text{ rad/s}^2\); (c) Torque: \(2.548 \text{ N·m}\).

Step by step solution

01

Find Linear Acceleration

Use the formula for linear acceleration: \( a = \frac{v^2 - u^2}{2s} \), where \( v = 0 \) m/s (final velocity), \( u = 43.0 \) m/s (initial velocity), and \( s = 225 \) m (distance). Substituting the values: \[a = \frac{0 - (43.0)^2}{2 \times 225} = \frac{-1849}{450} = -4.11 \text{ m/s}^2.\]Thus, the linear acceleration is \(-4.11 \text{ m/s}^2\).
02

Find Angular Acceleration

Angular acceleration \( \alpha \) can be obtained from linear acceleration \( a \) using the formula: \( \alpha = \frac{a}{r} \), where \( r = 0.250 \) m. Substituting the values:\[\alpha = \frac{-4.11}{0.250} = -16.44 \text{ rad/s}^2.\]Thus, the angular acceleration is \(-16.44 \text{ rad/s}^{2}\).
03

Calculate the Torque

Torque \( \tau \) can be calculated using the formula \( \tau = I \alpha \), where \( I = 0.155 \) kg·m² is the rotational inertia. Substituting the values:\[\tau = 0.155 \times (-16.44) = -2.548 \text{ N·m}.\]The magnitude of the torque is \(2.548 \text{ N·m}\).

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Key Concepts

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

Understanding Linear Acceleration
Linear acceleration is a vital concept when studying motion. It's defined as the rate of change of velocity with respect to time. In simpler terms, it tells us how quickly an object speeds up or slows down. The formula for linear acceleration in this exercise is presented as:
  • \( a = \frac{v^2 - u^2}{2s} \)
  • \( v \) is the final velocity, which is 0 m/s here since the wheel comes to a stop.
  • \( u \) is the initial velocity, 43.0 m/s.
  • \( s \) represents the distance, 225 m, over which the wheel stops.
The negative acceleration value of \(-4.11 \text{ m/s}^2\) calculated in this exercise indicates the wheel is decelerating as it rolls to a stop.ul>{Physics Problem]
Sections will start with text and you will find each Orignal Exercise in it .ORIGINAL EXERCISE: A wheel of radius \ [ 0.250 \, metr ] , moving initially at \[ 43.0 \, m \/ s \], rolls to a stop in \[ 225 \, m \]. Calculate the magnitudes of its (a) linear acceleration and (b) angular acceleration. Scheme For more understanding, think of applying brakes when driving a car. The car's speed lowers, marking linear acceleration due to the force applied through brakes.
Exploring Angular Acceleration
Angular acceleration relates closely to linear acceleration, especially in the context of rotating objects, like wheels or gears. Angular acceleration indicates how quickly an object changes its rotational speed. The relationship between angular and linear acceleration is vital for understanding how rotational motion translates from an object's edge to its entire structure.
  • Angular acceleration \( \alpha \) can be computed directly from linear acceleration \( a \) using the formula \( \alpha = \frac{a}{r} \).
  • Here, \( r \) is the radius of the wheel, given as 0.250 m.
  • The angular acceleration results in \(-16.44 \text{ rad/s}^2\) for the wheel in this problem.
The negative value signifies a decrease in the wheel's rotational speed, much like when a spinning top gradually stops due to resisting forces like friction. The faster the angular speed changes, the greater the angular acceleration.
The Role of Torque in Rotational Motion
Torque is the force that causes an object to rotate around an axis. It can be thought of as the rotational equivalent of linear force. Torque involves three main elements:
  • The amount of force applied.
  • The distance from the axis of rotation, often called a lever arm.
  • The angle at which the force is applied.
In this exercise, torque \( \tau \) is calculated by multiplying rotational inertia \( I \) by angular acceleration \( \alpha \):
  • \( \tau = I \alpha \)
  • \( I \) given as \( 0.155 \text{ kg·m}^2 \), and \( \alpha = -16.44 \text{ rad/s}^2 \)
By plugging in these values, the torque results in a magnitude of \(2.548 \text{ N·m}\), indicating the resistive force of friction causing the wheel to stop. Understanding torque helps clarify how forces contribute not just to the start or stop of motion, but to its rotation as well.

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Most popular questions from this chapter

A \(140 \mathrm{~kg}\) hoop rolls along a horizontal floor so that the hoop's center of mass has a speed of \(0.150 \mathrm{~m} / \mathrm{s}\). How much work must be done on the hoop to stop it?

A solid sphere of weight \(36.0 \mathrm{~N}\) rolls up an incline at an angle of \(30.0^{\circ}\). At the bottom of the incline the center of mass of the sphere has a translational speed of \(4.90 \mathrm{~m} / \mathrm{s}\). (a) What is the kinetic energy of the sphere at the bottom of the incline? (b) How far does the sphere travel up along the incline? (c) Does the answer to (b) depend on the sphere's mass?

At one instant, force \(\vec{F}=4.0 \hat{\mathrm{j}} \mathrm{N}\) acts on a \(0.25 \mathrm{~kg}\) object that has position vector \(\vec{r}=(2.0 \hat{\mathrm{i}}-2.0 \hat{\mathrm{k}}) \mathrm{m}\) and velocity vector \(\vec{v}=(-5.0 \hat{\mathrm{i}}+5.0 \hat{\mathrm{k}}) \mathrm{m} / \mathrm{s}\). About the origin and in unit-vector notation, what are (a) the object's angular momentum and (b) the torque acting on the object?

A \(2.50 \mathrm{~kg}\) particle that is moving horizontally over a floor with velocity \((-3.00 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{j}}\) undergoes a completely inelastic collision with a \(4.00 \mathrm{~kg}\) particle that is moving horizontally over the floor with velocity \((4.50 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{i}}\). The collision occurs at \(x y\) coordinates \((-0.500 \mathrm{~m},-0.100 \mathrm{~m})\). After the collision and in unit- vector notation, what is the angular momentum of the stuck-together particles with respect to the origin?

In unit-vector notation, what is the torque about the origin on a jar of jalapeño peppers located at coordinates \((3.0 \mathrm{~m},-2.0 \mathrm{~m},\), \(4.0 \mathrm{~m}\) ) due to (a) force \(\vec{F}_{1}=(3.0 \mathrm{~N}) \hat{\mathrm{i}}-(4.0 \mathrm{~N}) \hat{\mathrm{j}}+(5.0 \mathrm{~N}) \hat{\mathrm{k}}\), (b) force \(\vec{F}_{2}=(-3.0 \mathrm{~N}) \hat{\mathrm{i}}-(4.0 \mathrm{~N}) \hat{\mathrm{j}}-(5.0 \mathrm{~N}) \hat{\mathrm{k}}\), and \((\mathrm{c})\) the vector sum of \(\vec{F}_{1}\) and \(\vec{F}_{2} ?\) (d) Repeat part (c) for the torque about the point with coordinates \((3.0 \mathrm{~m}, 2.0 \mathrm{~m}, 4.0 \mathrm{~m})\).

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