/*! 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 26 The force of attraction between ... [FREE SOLUTION] | 91Ó°ÊÓ

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The force of attraction between two particles is given by $$\mathbf{f}_{12}=k\left[\left(\mathbf{r}_{2}-\mathbf{r}_{1}\right)-\frac{r}{v_{0}}\left(\mathbf{\dot { r }}_{2}-\dot{\mathbf{r}}_{1}\right)\right]$$ where \(k\) is a constant, \(v_{0}\) is a constant velocity, and \(r \equiv\left|\mathbf{r}_{2}-\mathbf{r}_{1}\right| .\) Calculate the internal torque for the system; why does this quantity not vanish? Is the system conservative?

Short Answer

Expert verified
The internal torque for the given system of particles is \(\mathbf{Ï„}_{int} = k\left[ \left(\mathbf{r}_1 \times (\mathbf{r}_2 - \mathbf{r}_1)\right) - \left(\mathbf{r}_2 \times (\mathbf{r}_2 - \mathbf{r}_1)\right) - \frac{r}{v_0}\left(\mathbf{r}_1 \times (\dot{\mathbf{r}}_2 - \dot{\mathbf{r}}_1)\right) + \frac{r}{v_0}\left(\mathbf{r}_2 \times (\dot{\mathbf{r}}_2 - \dot{\mathbf{r}}_1)\right) \right]\). The internal torque does not vanish due to the non-zero cross product terms in the expression. This non-vanishing internal torque indicates that the system is not conservative, as mechanical energy will not be conserved.

Step by step solution

01

Determine the individual torque for each particle

For two particles, the torque acting on the first is: \[ \mathbf{Ï„}_{1} = \mathbf{r}_1 \times \mathbf{f}_{12} \] Similarly, for the second particle it is: \[ \mathbf{Ï„}_{2} = \mathbf{r}_2 \times (-\mathbf{f}_{12}) \] where the negative sign is due to the equal and opposite nature of the forces between the particles.
02

Calculate the internal torque

To find the net torque, sum the individual torques on each particle: \[ \mathbf{Ï„}_{int} =\mathbf{Ï„}_{1} +\mathbf{Ï„}_{2} \] which can be rewritten as: \[ \mathbf{Ï„}_{int} = (\mathbf{r}_1 \times \mathbf{f}_{12}) + (\mathbf{r}_2 \times (-\mathbf{f}_{12})) \]
03

Substitute the force equation into torque equation

Now substitute the expression for \(\mathbf{f}_{12}\) given in the problem statement: \[ \mathbf{Ï„}_{int} = (\mathbf{r}_1 \times k[\left(\mathbf{r}_{2}-\mathbf{r}_{1}\right)-\frac{r}{v_{0}}\left(\mathbf{\dot{r}}_{2}-\dot{\mathbf{r}}_{1}\right)]) + (\mathbf{r}_2 \times -k[\left(\mathbf{r}_{2}-\mathbf{r}_{1}\right)-\frac{r}{v_{0}}\left(\mathbf{\dot{r}}_{2}-\dot{\mathbf{r}}_{1}\right)]) \]
04

Simplify the torque expression and find the magnitude

Simplify the expression for the net torque and find the magnitude: \[ \mathbf{Ï„}_{int} = k\left[ \left(\mathbf{r}_1 \times (\mathbf{r}_2 - \mathbf{r}_1)\right) - \left(\mathbf{r}_2 \times (\mathbf{r}_2 - \mathbf{r}_1)\right) - \frac{r}{v_0}\left(\mathbf{r}_1 \times (\dot{\mathbf{r}}_2 - \dot{\mathbf{r}}_1)\right) + \frac{r}{v_0}\left(\mathbf{r}_2 \times (\dot{\mathbf{r}}_2 - \dot{\mathbf{r}}_1)\right) \right] \] Now, we can observe that the cross product terms in the expression for internal torque are not equal to zero, i.e., the internal torque does not vanish. This non-vanishing internal torque means that the system is not conservative, as the mechanical energy will not be conserved.

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Key Concepts

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

Non-conservative Forces
In mechanics, a system is described as conservative if the total mechanical energy is conserved. This means that the potential energy stored in the force fields equals the work done by the forces for any path between two points. However, non-conservative forces cause energy loss, typically in the form of heat or distortions, and they do not allow the energy to be simply stored and recovered.

In the given problem, the force equation provided shows that the force depends on both positions and velocities, implying energy will not simply transfer back and forth like in a conservative system.

The presence of velocity in the expression of force suggests resistive effects, which are hallmark traits of non-conservative forces. This characteristic results in a system where internal forces can create torque and effect changes in angular momentum, unrelated to potential energy alone. Thus, the fact that the internal torque does not vanish aligns with these principles, signifying that our system is non-conservative.
Internal Forces
Internal forces act within a system comprised of multiple particles, such as the attraction between the two particles in this exercise. They arise out of interactions between particles of the system but do not affect the motion of the system's center of mass directly.

According to Newton's third law, internal forces between two particles are equal in magnitude and opposite in direction. But in terms of torque, when calculating it using cross products, these forces may not necessarily cancel out, leading to a non-zero internal torque as shown in the step-by-step solution above.

This non-cancellation can occur because depending on the position vectors and their directions relative to the line of action of force, the torque effect can differ. Thus, despite the forces themselves being internal and balanced, their contributions to torque can lead to a non-vanishing result.
Cross Product
The cross product is a mathematical operation used predominantly in physics to calculate torques or angular quantities. It is a vector multiplication operation where two vectors are multiplied to produce a third vector that is orthogonal (perpendicular) to the plane containing the original two.

In this problem, torque is determined by the cross product of the position vector and force vector. The formula for torque is: \[\mathbf{Ï„} = \mathbf{r} \times \mathbf{f}\]The resulting vector indicates the axis around which rotation tends to occur, with its magnitude providing the torque's strength. The apparent non-zero result when evaluating the system's torque shows that even if the forces are equal and opposite, their cross product with the respective position vectors does not always cancel out. This is because their amplifying effects from displacement and reach can vary within the system.
Particle Dynamics
Particle dynamics is the study of motion (kinematics) and the causes of this motion (forces). In systems involving multiple particles, such dynamics can become complex as they require accounting both for internal forces between particles and external influences.
  • Particle dynamics help us understand how changes in velocity and position occur as a result of acting forces.
  • They take into account the mass of particles and the net external force applied resolving motion through Newton's laws.
In the present exercise, we illustrate particle dynamics by examining how the force between two particles not only affects their linear motion but also introduces changes in rotational aspects through torque. Here, you can see how internal interactions drive particle behavior in a non-conservative setting, where energy is not conserved straightforwardly but gets redistributed differently.

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Most popular questions from this chapter

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