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A 2.80-kg grinding wheel is in the form of a solid cylinder of radius 0.100 m. (a) What constant torque will bring it from rest to an angular speed of 1200 rev/min in 2.5 s? (b) Through what angle has it turned during that time? (c) Use Eq. (10.21) to calculate the work done by the torque. (d) What is the grinding wheel's kinetic energy when it is rotating at 1200 rev/min ? Compare your answer to the result in part (c).

Short Answer

Expert verified
(a) 0.224\(\pi\) Nm; (b) 50\(\pi\) radians; (c) 11.2\(\pi^2\) J; (d) 11.2\(\pi^2\) J, same as (c).

Step by step solution

01

Convert Units

First, convert the angular speed from revolutions per minute to radians per second. Since 1 revolution is \(2\pi\) radians and 1 minute is 60 seconds, we have:\[\omega = 1200 \, \text{rev/min} = 1200 \times \frac{2\pi}{60} \, \text{rad/s} = 40\pi \, \text{rad/s}\]
02

Calculate Moment of Inertia

The moment of inertia \(I\) for a solid cylinder is given by \(I = \frac{1}{2} m r^2\), where \(m = 2.80 \, \text{kg}\) and \(r = 0.100 \, \text{m}\).\[I = \frac{1}{2} \times 2.80 \times (0.100)^2 = 0.014 \, \text{kg} \, \text{m}^2\]
03

Calculate Angular Acceleration

To find the angular acceleration \(\alpha\), use the formula \(\alpha = \frac{\Delta \omega}{\Delta t}\), where \(\Delta \omega = 40\pi \, \text{rad/s}\) and \(\Delta t = 2.5 \, \text{s}\):\[\alpha = \frac{40\pi}{2.5} = 16\pi \, \text{rad/s}^2\]
04

Calculate Torque

Use the relationship between torque \(\tau\) and angular acceleration \(\alpha\), given by \(\tau = I \alpha\).\[\tau = 0.014 \times 16\pi = 0.224\pi \, \text{Nm}\]
05

Calculate Angle Turned

The angle \(\theta\) through which the wheel turns is given by \(\theta = \omega_0 t + \frac{1}{2} \alpha t^2\). Since \(\omega_0 = 0\), it simplifies to:\[\theta = \frac{1}{2} \times 16\pi \times (2.5)^2 = 50\pi \, \text{radians}\]
06

Calculate the Work Done by the Torque

Work done by the torque \(W\) is given by \(W = \tau \theta\).\[W = 0.224\pi \times 50\pi = 11.2\pi^2 \, \text{J}\]
07

Calculate Kinetic Energy

The kinetic energy \(K\) when the wheel is rotating is \(K = \frac{1}{2}I \omega^2\).\[K = \frac{1}{2} \times 0.014 \times (40\pi)^2 = 11.2\pi^2 \, \text{J}\]The kinetic energy is the same as the work done by the torque.

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Key Concepts

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

Torque
In the realm of angular mechanics, torque is a fundamental concept. It is essentially the rotational counterpart of force and dictates how effectively an object can be set into rotational motion. Torque (\( \tau \)) is calculated using the formula \( \tau = I \alpha \), where \( I \) is the moment of inertia and \( \alpha \) is the angular acceleration. It is measured in Newton-meters (Nm).
In our example, to calculate the torque required to spin the grinding wheel, we first found the moment of inertia and the angular acceleration. Then, by multiplying these two, we determined the torque. This technique is used frequently in machinery design, where precise levels of torque must be applied to achieve desired rotation rates.
Torque reflects not just the force applied but also the distance from the pivot point. When the distance from the axis of rotation increases, the potential for greater torque is present. This relationship is akin to using a wrench, where a longer handle allows for easier turning due to increased torque.
Moment of Inertia
The moment of inertia (\( I \)) is crucial in understanding how an object resists changes in its rotational motion. For different shapes and mass distributions, the moment of inertia varies. For a solid cylinder like our grinding wheel, the formula is \( I = \frac{1}{2}mr^2 \), where \( m \) is the mass and \( r \) is the radius.
In essence, it's the measure of how spread out an object's mass is in relation to the axis of rotation. As the mass moves further away, the moment of inertia increases, requiring more torque to achieve the same angular acceleration. Imagine spinning an empty wheel versus one filled with a heavy liquid; the second one spins more reluctantly because of the higher moment of inertia.
Understanding the moment of inertia is vital in applications ranging from designing car engines to understanding how to optimize the spins of athletic moves.
Angular Acceleration
Angular acceleration (\( \alpha \)) describes how quickly an object changes its rotational speed. Mathematically, it is defined as the change in angular velocity over time: \( \alpha = \frac{\Delta \omega}{\Delta t} \).
In our example, we calculated that the angular acceleration required to bring the grinding wheel to the desired speed was \( 16\pi \) radians per second squared. This tells us how fast the wheel reaches its peak speed from rest within the timeframe of 2.5 seconds.
Angular acceleration plays a critical role in many engineering systems, such as conveyor belts, where a controlled increase in speed is necessary for proper operation. It is also crucial in robotics, where precise movement and adjustments are essential for the efficient running of tasks.
Kinetic Energy
Once an object is rotating, it possesses kinetic energy due to its motion. The rotational kinetic energy (\( K \)) can be expressed using the formula \( K = \frac{1}{2}I \omega^2 \).
For our rotating grinding wheel, we calculated the kinetic energy to verify that it matches the work done by the torque used to accelerate the wheel. Both calculations resulted in \( 11.2\pi^2 \) Joules, confirming the conservation of energy principle.
Kinetic energy is an essential concept in physics and engineering. It allows us to quantify how much work an object in motion can do. Understanding kinetic energy is necessary for everything from designing efficient industrial machines to calculating the impacts during vehicular accidents.

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Most popular questions from this chapter

We can roughly model a gymnastic tumbler as a uniform solid cylinder of mass 75 kg and diameter 1.0 m. If this tumbler rolls forward at 0.50 rev/s, (a) how much total kinetic energy does he have, and (b) what percent of his total kinetic energy is rotational?

You are designing a simple elevator system for an old warehouse that is being converted to loft apartments. A 22,500-N elevator is to be accelerated upward by connecting it to a counterweight by means of a light (but strong!) cable passing over a solid uniform disk- shaped pulley. The cable does not slip where it is in contact with the surface of the pulley. There is no appreciable friction at the axle of the pulley, but its mass is 875 kg and it is 1.50 m in diameter. (a) What mass should the counterweight have so that it will accelerate the elevator upward through 6.75 m in the first 3.00 s, starting from rest? (b) What is the tension in the cable on each side of the pulley?

When an object is rolling without slipping, the rolling friction force is much less than the friction force when the object is sliding; a silver dollar will roll on its edge much farther than it will slide on its flat side (see Section 5.3). When an object is rolling without slipping on a horizontal surface, we can approximate the friction force to be zero, so that \(a_x\) and \(a_z\) are approximately zero and \(v_x\) and \(\omega_z\) are approximately constant. Rolling without slipping means \(v_x = r\omega_z\) and \(a_x = r\alpha_z\) . If an object is set in motion on a surface \(without\) these equalities, sliding (kinetic) friction will act on the object as it slips until rolling without slipping is established. A solid cylinder with mass \(M\) and radius \(R\), rotating with angular speed \(\omega_0\) about an axis through its center, is set on a horizontal surface for which the kinetic friction coefficient is \(\mu_k\). (a) Draw a free-body diagram for the cylinder on the surface. Think carefully about the direction of the kinetic friction force on the cylinder. Calculate the accelerations \(a_x\) of the center of mass and \(a_z\) of rotation about the center of mass. (b) The cylinder is initially slipping completely, so initially \(\omega_z = \omega_0\) but \(v_x =\) 0. Rolling without slipping sets in when \(v_x = r\omega_z\) . Calculate the \(distance\) the cylinder rolls before slipping stops. (c) Calculate the work done by the friction force on the cylinder as it moves from where it was set down to where it begins to roll without slipping.

A thin uniform rod has a length of 0.500 m and is rotating in a circle on a frictionless table. The axis of rotation is perpendicular to the length of the rod at one end and is stationary. The rod has an angular velocity of 0.400 rad/s and a moment of inertia about the axis of 3.00 \(\times 10^{-3}\) kg \(\cdot\) m\(^2\). A bug initially standing on the rod at the axis of rotation decides to crawl out to the other end of the rod. When the bug has reached the end of the rod and sits there, its tangential speed is 0.160 m/s. The bug can be treated as a point mass. What is the mass of (a) the rod; (b) the bug?

A machine part has the shape of a solid uniform sphere of mass 225 g and diameter 3.00 cm. It is spinning about a frictionless axle through its center, but at one point on its equator it is scraping against metal, resulting in a friction force of 0.0200 N at that point. (a) Find its angular acceleration. (b) How long will it take to decrease its rotational speed by 22.5 rad/s ?

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