/*! 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 5 A child is pushing a merry-go-ro... [FREE SOLUTION] | 91Ó°ÊÓ

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A child is pushing a merry-go-round. The angle through which the merry-go- round has turned varies with time according to \(\theta(t)=\gamma t+\beta t^{3},\) where \(\gamma=0.400 \mathrm{rad} / \mathrm{s}\) and \(\beta=\) 0.0120 \(\mathrm{rad} / \mathrm{s}^{3}\) (a) Calculate the angular velocity of the merry-go-round as a function of time. (b) What is the initial value of the angular velocity? (c) Calculate the instantaneous value of the angular velocity \(\omega_{z}\) at \(t=5.00\) s and the average angular velocity \(\omega_{\mathrm{av}-z}\) for the time interval \(t=0\) to \(t=5.00\) s. Show that \(\omega_{\mathrm{av}-z \text { is }}\) not equal to the average of the instantaneous angular velocities at \(t=0\) and \(t=5.00 \mathrm{s},\) and explain why it is not.

Short Answer

Expert verified
(a) \(\omega(t) = 0.400 + 0.036t^2\). (b) \(\omega(0) = 0.400\, \mathrm{rad/s}\). (c) \(\omega(5) = 1.300\, \mathrm{rad/s}\); \(\omega_{\mathrm{av}} = 0.700\, \mathrm{rad/s}\); average and instantaneous values differ due to quadratic nature.

Step by step solution

01

Differentiate to find Angular Velocity

Angular velocity \(\omega(t)\) is the time derivative of angle \(\theta(t)\). Differentiating \(\theta(t) = \gamma t + \beta t^3\), we get: \[ \omega(t) = \frac{d}{dt}(\gamma t + \beta t^3) = \gamma + 3\beta t^2. \] Substituting the given values \(\gamma = 0.400\, \mathrm{rad/s}\) and \(\beta = 0.0120\, \mathrm{rad/s^3}\), the equation becomes: \[ \omega(t) = 0.400 + 3(0.0120)t^2 = 0.400 + 0.036t^2. \]
02

Calculate Initial Angular Velocity

The initial angular velocity is \(\omega(0)\). Substitute \(t = 0\) into the angular velocity equation: \[ \omega(0) = 0.400 + 0.036 \times 0^2 = 0.400\, \mathrm{rad/s}. \]
03

Find Instantaneous Angular Velocity at t = 5 s

Substitute \(t = 5\, \mathrm{s}\) into the angular velocity equation to find \(\omega(5)\): \[ \omega(5) = 0.400 + 0.036 \times (5)^2 = 0.400 + 0.036 \times 25 = 1.300\, \mathrm{rad/s}. \]
04

Calculate Average Angular Velocity for t = 0 to t = 5 s

Average angular velocity over a time interval is given by: \[ \omega_{\text{av}} = \frac{\theta(t_{\text{final}}) - \theta(t_{\text{initial}})}{t_{\text{final}} - t_{\text{initial}}}. \]\( \theta(5) = \gamma (5) + \beta (5)^3 = 0.400 \times 5 + 0.0120 \times 125 = 2.000 + 1.500 = 3.500 \, \mathrm{rad}\) and \(\theta(0) = 0\). Thus, \[\omega_{\text{av}} = \frac{3.500 - 0}{5 - 0} = 0.700\, \mathrm{rad/s}. \]
05

Compare Average Angular Velocity with Instantaneous Values

The average of instantaneous angular velocities at \(t = 0\) and \(t = 5\) is: \[\frac{\omega(0) + \omega(5)}{2} = \frac{0.400 + 1.300}{2} = 0.850\, \mathrm{rad/s}.\] Since \(0.850\, \mathrm{rad/s} eq 0.700\, \mathrm{rad/s}\), they are not equal. This discrepancy is because average angular velocity considers the entire trajectory, not just start and end points, and \(\omega(t)\) is not linear over time but quadratic.

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Key Concepts

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

Angular Velocity
Angular velocity is a measure of how quickly an object rotates or revolves around an axis. It is an essential concept in rotational motion, akin to linear velocity in linear motion. Angular velocity specifies both direction and rate of rotation.

In the exercise, the angular velocity of the merry-go-round is obtained by differentiating the angular displacement function, \(\theta(t)=\gamma t+\beta t^3\), with respect to time. This yields the angular velocity function \(\omega(t) = \gamma + 3\beta t^2\). Here's what it means:
  • \(\gamma\) represents the constant part of angular velocity, similar to a starting pace.
  • The term \(+ 3\beta t^2\) introduces a time-dependent change, suggesting that the rate of rotation increases as time progresses.
To understand this better, think of the merry-go-round spinning faster over time due to the \(t^2\) term, showing non-linear acceleration in the rotation.
Differentiation in Physics
Differentiation is a powerful mathematical tool used in physics to find rates of change, especially in motion-related problems. In the context of the exercise, differentiation helps derive the angular velocity from the displacement function.

Here's how differentiation works in this scenario:
  • The angular displacement \(\theta(t)=\gamma t+\beta t^3\) represents how far the merry-go-round has turned over time.
  • When you differentiate \(\theta(t)\) with respect to time \(t\), you obtain the time rate of change of angle, known as angular velocity \(\omega(t)\).
This process highlights how instantaneous changes (e.g., how fast something is spinning at any given moment) are extracted from a time-dependent position or displacement function.
Average Velocity
In rotational motion, average velocity describes how far an object rotates over a certain time period. It provides a simpler, overall picture of motion within an interval, rather than detailing speed at every instant.

For the merry-go-round, the average angular velocity is calculated using the formula:
  • \(\omega_{\text{av}} = \frac{\theta(t_{\text{final}}) - \theta(t_{\text{initial}})}{t_{\text{final}} - t_{\text{initial}}}\)
This equation takes the total angular displacement over a given time interval and divides it by the time difference. It’s the rotational counterpart to the linear average velocity, which you'd use on a straight path.

The average velocity is a straightforward way to grasp the overall spin effect during that period without analyzing motion step-by-step.
Instantaneous Velocity
Instantaneous velocity reveals the exact rate of rotation at a specific time. It is akin to checking your speedometer over time during a car ride to see exactly how fast you are going at that moment.

In the merry-go-round problem, the instantaneous angular velocity is found from the angular velocity function \(\omega(t) = 0.400 + 0.036t^2\). To explore this:
  • By substituting a specific time into \(\omega(t)\), for instance at \(t=5s\), you determine the merry-go-round's precise spinning speed at that second.
In contrast to average velocity, which covers a whole time span, instantaneous velocity focuses on now, allowing us to capture how the speed varies instantaneously.

Understanding instantaneous velocity is crucial when analyzing motion that changes over time, as it provides insight into the dynamism of rotational motion.

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Most popular questions from this chapter

The motor of a table saw is rotating at 3450 rev/min. A pulley attached to the motor shaft drives a second pulley of half the diameter by moans of a V-belt. A circular saw blade of diameter 0.208 \(\mathrm{m}\) is mounted on the same rotating shaft as the second pulley. (a) The operator is careless and the blade catches and throws back a small piece of wood. This piece of wood moves with linear speed equal to the tangential speed of the rim of the blade. What is this speed? (b) Calculate the radial acceleration of points on the outer edge of the blade to see why sawdust doesn't to its teeth.

A flywheel has angular acceleration \(\alpha_{z}(t)=$$8.60 \mathrm{rad} / \mathrm{s}^{2}-\left(2.30 \mathrm{rad} / \mathrm{s}^{3}\right) t,\) where counterclockwise rotation is positive. (a) If the flywheel is at rest at \(t=0,\) what is its angular velocity at 5.00 s? (b) Through what angle (in radians) does the flywheel turn in the time interval from \(t=0\) to \(t=5.00\) s?

A meter stick with a mass of 0.180 \(\mathrm{kg}\) is pivoted about one end so it can rotate without friction about a horizontal axis. The meter stick is held in a horizontal position and released. As it swings through the vertical, calculate (a) the change in gravitational potential energy that has occurred; (b) the angular speed of the stick; (c) the linear speed of the end of the stick opposite the axis. (d) Compare the answer in part (c) to the speed of a particle that has fallen \(1.00 \mathrm{m},\) starting from rest.

How \(I\) Scales. If we multiply all the design dimensions of an object by a scaling factor \(f,\) its volume and mass will be multiplied by \(f^{3}\) (a) By what factor will its moment of inertia be multiplied? (b) If a \(\frac{1}{48}-\) scale model has a rotational kinetic energy of \(2.5 \mathrm{J},\) what will be the kinetic energy for the full-scale object of the same material rotating at the same angular velocity?

The Kinetic Energy of Walking. If a person of mass \(M\) simply moved forward with speed \(V\), his kinetic energy would be \(\frac{1}{2} M V^{2}\).However, in addition to possessing a forward motion, various parts of his body (such as the arms and legs) undergo rotation. Therefore, his total kinetic energy is the sum of the energy from his forward motion plus the rotational kinetic energy of his arms and legs. The purpose of this problem is to see how much this rotational motion contributes to the person's kinetic energy. Biomedical measurements show that the arms and hands together typically make up 13\(\%\) of a person's mass, while the legs and feet together account for 37\(\%\) . For a rough (but reasonable) calculation, we can model the arms and legs as thin uniform bars pivoting about the shoulder and hip, respectively. In a brisk walk, the arms and legs each move through an angle of about \(\pm 30^{\circ}\) (a total of \(60^{\circ} )\) from the vertical in approximately 1 second. We shall assume that they are held straight, rather than being bent, which is not quite true. Let us consider a 75 -kg person walking at 5.0 \(\mathrm{km} / \mathrm{h}\) , having arms 70 \(\mathrm{cm}\) long and legs 90 \(\mathrm{cm}\) long. (a) What is the average angular velocity of his arms and legs? (b) Using the average angular velocity from part (a), calculate the amount of rotational kinetic energy in this person's arms and legs as he walks. (c) What is the total kinetic energy due to both his forward motion and his rotation? (d) What percentage of his kinetic energy is due to the rotation of his legs and arms?

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