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At time \(t=0\), a \(3.0 \mathrm{~kg}\) particle with velocity \(\vec{v}=(5.0 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{i}}-(6.0 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{j}}\) is at \(x=3.0 \mathrm{~m}, y=8.0 \mathrm{~m} .\) It is pulled by a \(7.0 \mathrm{~N}\) force in the negative \(x\) direction. About the origin, what are (a) the particle's angular momentum, (b) the torque acting on the particle, and (c) the rate at which the angular momentum is changing?

Short Answer

Expert verified
a) 66 kg m²/s b) -56 Nm c) -56 kg m²/s²

Step by step solution

01

Understand the Provided Information

We have a particle with a mass of \(3.0 \text{ kg}\), initial velocity \(\vec{v} = (5.0 \text{ m/s}) \hat{\mathbb{i}} - (6.0 \text{ m/s}) \hat{\mathbb{j}}\), and initial position \((x, y) = (3.0 \text{ m}, 8.0 \text{ m})\). There is also a constant force of \(7.0 \text{ N}\) in the negative \(x\)-direction acting on it.
02

Calculate Initial Angular Momentum

Angular momentum \(L\) about the origin is given by \(\vec{L} = \vec{r} \times \vec{p}\), where \(\vec{r}\) is the position vector and \(\vec{p} = m\vec{v}\) is the momentum. Here, \(\vec{r} = 3.0 \hat{\mathbb{i}} + 8.0 \hat{\mathbb{j}}\) and \(\vec{p} = 3.0\text{ kg} \times ((5.0 \hat{\mathbb{i}} - 6.0 \hat{\mathbb{j}}) \text{m/s}) = (15 \hat{\mathbb{i}} - 18 \hat{\mathbb{j}}) \text{ kg m/s}\). The cross product \(\vec{r} \times \vec{p}\) then is \((3.0 \hat{\mathbb{i}} + 8.0 \hat{\mathbb{j}}) \times (15 \hat{\mathbb{i}} - 18 \hat{\mathbb{j}}) = -54 \hat{\mathbb{k}} + 120 \hat{\mathbb{k}} = 66 \hat{\mathbb{k}} \text{ kg m}^2 \text{/s}\). So, \(L = 66 \text{ kg m}^2 \text{/s}\).
03

Find Torque on the Particle

Torque \(\vec{\tau}\) is given by \(\vec{\tau} = \vec{r} \times \vec{F}\), where \(\vec{F} = - 7.0 \hat{\mathbb{i}}\) (since the force is in the negative \(x\)-direction). Then \(\vec{r} = 3.0 \hat{\mathbb{i}} + 8.0 \hat{\mathbb{j}}\), so \(\vec{\tau} = (3.0 \hat{\mathbb{i}} + 8.0 \hat{\mathbb{j}}) \times (-7.0 \hat{\mathbb{i}}) = (0) \hat{\mathbb{i}} - (0) \hat{\mathbb{j}} + (-56) \hat{\mathbb{k}} = -56 \hat{\mathbb{k}} \text{ Nm}\). Thus, \(\vec{\tau} = -56 \hat{\mathbb{k}} \text{ Nm}\).
04

Determine the Rate of Change of Angular Momentum

The relation between torque and the rate of change of angular momentum \(\frac{d\vec{L}}{dt}\) is given by \(\vec{\tau} = \frac{d\vec{L}}{dt}\). Since \(\vec{\tau} = -56 \hat{\mathbb{k}} \text{ Nm}\), the rate of change of angular momentum is also \(-56 \hat{\mathbb{k}} \text{ kg m}^2/\text{s}^2\).

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Key Concepts

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

Torque
Torque is a fundamental concept in rotational dynamics. It measures how much a force causes an object to rotate about an axis. Think of it as a twisting force. The formula for torque \( \vec{\tau} \) is the cross product of the position vector \( \vec{r} \) and the force vector \( \vec{F} \):
  • \( \vec{\tau} = \vec{r} \times \vec{F} \)

In our particle's scenario, the force is acting in the negative \( x \)-direction with a magnitude of 7 N. The position vector \( \vec{r} \) at the time of interest is \(3.0 \hat{\mathbb{i}} + 8.0 \hat{\mathbb{j}}\). To find the torque, calculate the cross product between these vectors.
The result, \( -56 \hat{\mathbb{k}} \text{ Nm}\), signifies that the torque causes a rotation in the negative \( k \)-direction, perpendicularly to the \( xy \)-plane. Thus, knowing how to compute torque using the cross product helps us predict how forces influence rotational motion of objects.
Cross Product
The cross product is a mathematical operation used to find a vector perpendicular to two given vectors in three-dimensional space. It's an essential tool in vector physics, particularly in torque and angular momentum calculations.
In our exercise, we utilize the cross product to find both the angular momentum and torque.
  • To calculate angular momentum \( \vec{L} \), we use \( \vec{L} = \vec{r} \times \vec{p} \), where \( \vec{p} = m\vec{v} \) is the linear momentum.
  • For torque, the formula is \( \vec{\tau} = \vec{r} \times \vec{F} \).
The cross product results in a new vector that is orthogonal to the plane formed by the original vectors.
This perpendicular nature is fundamental in determining the direction of angular quantities, which is why you'll encounter it often in particle dynamics and rotational mechanics.
Rate of Change
The rate of change is a concept that describes how quickly something evolves over time. In the context of angular momentum, this change is directly influenced by torque. Mathematically, it is expressed as:
  • \( \frac{d\vec{L}}{dt} = \vec{\tau} \)

This equation shows a direct relationship between torque and the rate of change of angular momentum. If a constant torque acts on a particle, its angular momentum changes at a steady rate.
In our exercise, the torque \( -56 \hat{\mathbb{k}} \text{ Nm} \) implies that the rate of change of angular momentum is \( -56 \hat{\mathbb{k}} \text{ kg m}^2/\text{s}^2 \). This information can help us understand how the particle's state of rotation will alter over time due to the applied force.
Particle Dynamics
Particle dynamics deals with the motion of objects subjected to various forces. It encompasses concepts like velocity, force, torque, angular momentum, and energy, providing a comprehensive understanding of particle motion.
In this problem, we consider how forces and initial velocities affect a particle's rotational and translational motion.
  • The particle begins with a specific velocity and position and is subjected to a constant force.
  • To fully understand its dynamics, we examine both linear and angular aspects.
The interplay of these forces determines the particle's future motion, including how it rotates around a point and moves linearly.
Grasping particle dynamics enables you to predict motion accurately, which is crucial in fields from engineering to astrophysics.

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Most popular questions from this chapter

A disk with a rotational inertia of \(7.00 \mathrm{~kg} \cdot \mathrm{m}^{2}\) rotates like a merry-go-round while undergoing a time-dependent torque given by \(\tau=(5.00+2.00 t) \mathrm{N} \cdot \mathrm{m} .\) At time \(t=1.00 \mathrm{~s}\), its angular momentum is \(5.00 \mathrm{~kg} \cdot \mathrm{m}^{2} / \mathrm{s}\). What is its angular momentum at \(t=3.00 \mathrm{~s}\) ?

Two disks are mounted (like a merry-go-round) on lowfriction bearings on the same axle and can be brought together so that they couple and rotate as one unit. The first disk, with rotational inertia \(3.30 \mathrm{~kg} \cdot \mathrm{m}^{2}\) about its central axis, is set spinning counterclockwise at 450 rev/min. The second disk, with rotational inertia \(6.60 \mathrm{~kg} \cdot \mathrm{m}^{2}\) about its central axis, is set spinning counterclockwise at 900 rev/min. They then couple together. (a) What is their angular speed after coupling? If instead the second disk is set spinning clockwise at \(900 \mathrm{rev} / \mathrm{min}\), what are their (b) angular speed and (c) direction of rotation after they couple together?

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.

A body of radius \(R\) and mass \(m\) is rolling smoothly with speed \(v\) on a horizontal surface. It then rolls up a hill to a maximum height \(h\). (a) If \(h=3 v^{2} / 4 g\), what is the body's rotational inertia about the rotational axis through its center of mass? (b) What might the body be?

Figure 11-51 shows an overhead view of a ring that can rotate about its center like a merrygo-round. Its outer radius \(R_{2}\) is \(0.800 \mathrm{~m}\), its inner radius \(R_{1}\) is \(R_{2} / 2.00\), its mass \(M\) is \(8.00 \mathrm{~kg}\), and the mass of the crossbars at its center is negligible. It initially rotates at an angular speed of \(8.00 \mathrm{rad} / \mathrm{s}\) with a cat of mass \(m=M / 4.00\) on its outer edge, at radius \(R_{2}\). By how much does the cat increase the kinetic energy of the cat-ring system if the cat crawls to the inner edge, at radius \(R_{1}\) ?

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