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Two particles with masses \(m_{1}, m_{2}\) and velocities \(v_{1}, v_{2}\) collide and stick together. Find the velocity of this composite particle and show that the loss in kinetic energy due to the collision is $$ \frac{m_{1} m_{2}}{2\left(m_{1}+m_{2}\right)}\left|v_{1}-v_{2}\right|^{2} $$.

Short Answer

Expert verified
The final velocity of the composite particle is \(V = \frac{m_{1} * v_{1} + m_{2} * v_{2}}{m_{1} + m_{2}}\) and the loss in kinetic energy due to the collision is given by \(\frac{m_{1} m_{2}}{2\left(m_{1}+m_{2}\right)} \left|v_{1}-v_{2}\right|^{2}\).

Step by step solution

01

Find Final Velocity

By Conservation of momentum, the total momentum before the collision is equal to the total momentum after the collision. This gives us the equation \(m_{1} * v_{1} + m_{2} * v_{2} = (m_{1} + m_{2}) * V\) where \(V\) is the final velocity of the combined particle. Solving for \(V\) we get \(V = \frac{m_{1} * v_{1} + m_{2} * v_{2}}{m_{1} + m_{2}}\).
02

Compute Initial and Final Kinetic Energy

The initial kinetic energy \(K_{i}\) is given by \(\frac{1}{2} m_{1} * v_{1}^{2} + \frac{1}{2} m_{2} * v_{2}^{2}\). After the collision, the final kinetic energy \(K_{f}\) is \(\frac{1}{2} (m_{1} + m_{2}) * V^{2}\).
03

Calculate the Loss in Kinetic Energy

The loss in kinetic energy due to the collision is given by \(K_{i} - K_{f}\). Substituting the expressions for \(K_{i}\), \(K_{f}\) and \(V\) obtained in previous steps and simplifying should yield \(\frac{m_{1} m_{2}}{2\left(m_{1}+m_{2}\right)} \left|v_{1}-v_{2}\right|^{2}\).

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Key Concepts

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

Conservation of Momentum
In physics, the concept of conservation of momentum plays a vital role when analyzing collisions. Simply put, momentum is a product of an object's mass and its velocity, and it is a conserved quantity. This means that in a closed system, the total momentum before a collision will be the same as the total momentum after.

In the problem presented, two particles with masses \(m_1\) and \(m_2\) and velocities \(v_1\) and \(v_2\) collide and stick together. It is a classic example of an inelastic collision. To find the velocity \(V\) of the composite particle post-collision, we use the principle of conservation of momentum:

\[m_1 \cdot v_1 + m_2 \cdot v_2 = (m_1 + m_2) \cdot V\]

By solving for \(V\), we find that the velocity of the composite particle is:

\[V = \frac{m_1 \cdot v_1 + m_2 \cdot v_2}{m_1 + m_2}\]

This equation tells us that the final velocity is essentially a mass-weighted average of the initial velocities of the particles.
Kinetic Energy
Kinetic energy is the energy an object possesses due to its motion, and it can be calculated as \( \frac{1}{2} m v^2 \) for any object of mass \(m\) moving at velocity \(v\).

Before the collision, each particle has its own initial kinetic energy. The sum of these is the total initial kinetic energy \(K_i\):

\[K_i = \frac{1}{2} m_1 v_1^2 + \frac{1}{2} m_2 v_2^2\]

After the collision, when the particles stick together and move as one body with velocity \(V\), their combined kinetic energy is:

\[K_f = \frac{1}{2} (m_1 + m_2) V^2\]

Given the inelastic nature of the collision (where the objects stick together), it's essential to note that some kinetic energy is "lost" or transformed into other forms of energy, such as heat or sound.
Collision Energy Loss
The difference between the initial kinetic energy \(K_i\) and the final kinetic energy \(K_f\) post-collision gives us the energy lost during the collision.

In inelastic collisions, like the one in this exercise, not all kinetic energy is conserved as it is transferred into other forms. The energy loss can be calculated by finding the difference:

\[\text{Energy Loss} = K_i - K_f\]

Substituting the expressions for \(K_i\) and \(K_f\), and incorporating the derived final velocity \(V\), we get a simplified expression for the kinetic energy loss:

\[\text{Energy Loss} = \frac{m_1 m_2}{2(m_1 + m_2)} |v_1 - v_2|^2\]

This formula shows that the energy lost is dependent on the mass of the particles and the square of their velocity difference. In simpler terms, the greater the discrepancy in velocities, the higher the kinetic energy lost in the collision. This underscores how energy behaves in inelastic collisions, making it a profound learning point in understanding energy transformations.

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Most popular questions from this chapter

A boat of mass \(M\) is at rest in still water and a man of mass \(m\) is sitting at the bow. The man stands up, walks to the stem of the boat and then sits down again. If the water offers a resistance to the motion of the boat proportional to the velocity of the boat, show that the boat will eventually come to rest at its orginal position. [This remarkable result is independent of the resistance constant and the details of the man's motion.]

Show that, if a system moves from one state of rest to another over a certain time interval, then the average of the total external force over this time interval must be zero. An hourglass of mass \(M\) stands on a fixed platform which also measures the apparent weight of the hourglass. The sand is at rest in the upper chamber when, at time \(t=0\), a tiny disturbance causes the sand to start running through. The sand comes to rest in the lower chamber after a time \(t=\tau\). Find the time average of the appararent weight of the hourglass over the time interval \([0, \tau]\). [The apparent weight of the hourglass is however not constant in time. One can advance an argument that, when the sand is steadily running through, the apparent weight of the hourglass exceeds the real weight!]

A body of mass \(4 m\) is at rest when it explodes into three fragments of masses \(2 m, m\) and \(m\). After the explosion the two fragments of mass \(m\) are observed to be moving with the same speed in directions making \(120^{\circ}\) with each other. Find the proportion of the total kinetic energy carried by each fragment.

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Equal masses Show that, when the particles are of equal mass, the elastic scattering formulae take the simple form $$ \theta_{1}=\frac{1}{2} \psi \quad \theta_{2}=\frac{1}{2} \pi-\frac{1}{2} \psi \quad \theta=\frac{1}{2} \pi \quad \frac{E_{1}}{E_{0}}=\cos ^{2} \frac{1}{2} \psi \quad \frac{E_{2}}{E_{0}}=\sin ^{2} \frac{1}{2} \psi $$ where \(\psi\) is the scattering angle in the \(Z M\) frame. In the scattering of neutrons of energy \(E\) by neutrons at rest, in what directions should the experimenter look to find neutrons of energy \(\frac{1}{4} E ?\) What other energies would be observed in these directions?

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