/*! 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 57 (II) An atomic nucleus of mass \... [FREE SOLUTION] | 91Ó°ÊÓ

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(II) An atomic nucleus of mass \(m\) traveling with speed \(v\) collides elastically with a target particle of mass \(2 m\) (initially at rest) and is scattered at \(90^{\circ} .(a)\) At what angle does the target particle move after the collision? \((b)\) What are the final speeds of the two particles? ( \(c\) ) What fraction of the initial kinetic energy is transferred to the target particle?

Short Answer

Expert verified
(a) 45°; (b) both \(\frac{v}{\sqrt{2}}\); (c) 50%

Step by step solution

01

Understand the Problem

We need to determine three things: (a) the angle at which the target particle moves after the elastic collision, (b) the final speeds of both particles, and (c) the fraction of the initial kinetic energy transferred to the target particle. The collision is elastic, and the mass and speed relationships are given.
02

Use Elastic Collision Equations

In an elastic collision, both momentum and kinetic energy are conserved. For momentum, we have:\[ m \cdot v + 2m \cdot 0 = m \cdot v' + 2m \cdot v_{2}' \]where \(v'\) is the final speed of the nucleus and \(v_{2}'\) is the final speed of the target particle. Kinetic energy conservation gives:\[ \frac{1}{2}m v^2 = \frac{1}{2}m v'^2 + \frac{1}{2}(2m) v_{2}'^2 \]
03

Apply Scattering at 90 Degrees

For scattering at a 90-degree angle, vectors create a right triangle with the final velocities, so: \[ v'^2 + v_{2}'^2 = v^2 \]. Solve for \(v_{2}'\) using the equations, and substitute into the other equations.
04

Solve for Angles and Speeds

Using the momentum conservation equation focused on directions:\[ v_x = v'; \quad v_y = 2v_{2}' \cos(\theta) - 0 \] where \(\theta\) is the angle of the target particle. Using the 90-degree information, along with trigonometry, deduce that \(\theta = 45^{\circ}\). For speeds, solve the system to find:\[ v' = \frac{v}{\sqrt{2}}, \quad v_{2}' = \frac{v}{\sqrt{2}} \].
05

Calculate Kinetic Energy Transfer

Use the kinetic energy equations to find the initial and final kinetic energies and the energy transferred:\[ E_{initial} = \frac{1}{2}mv^2 \]\[ E_{final\_target} = \frac{1}{2}(2m) \left(\frac{v}{\sqrt{2}}\right)^2 = mv^2/2 \]The fraction of energy transferred to the target is 0.5 or 50%.

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Key Concepts

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

Momentum Conservation
In an elastic collision, one of the key principles is the conservation of momentum. This fundamental law of physics states that the total momentum of a closed system remains constant if no external forces act upon it. It is expressed mathematically as:
  • Initial momentum = Final momentum
  • \[m imes v + 2m imes 0 = m imes v' + 2m imes v_{2}'\]
Here, the system involves a nucleus of mass \(m\) with speed \(v\), colliding with a particle of mass \(2m\) initially at rest. This equation represents the conservation of momentum where \(v'\) and \(v_{2}'\) are the final velocities of the nucleus and the target particle respectively.
When an elastic collision occurs, the momentum before the collision equals the momentum after the collision, even if the objects change direction. This property allows us to solve for unknowns like the final speeds or angles at which objects deflect.
In our situation, since the initial target particle is at rest, the initial momentum is carried solely by the nucleus. This information is pivotal when you compute the outcomes of such collisions.
Kinetic Energy Conservation
Besides conserving momentum, elastic collisions are characterized by the conservation of kinetic energy. In simple terms, the kinetic energy before the collision is equal to the kinetic energy after the collision. The equation for kinetic energy conservation is expressed as follows:
  • \[\frac{1}{2}m v^2 = \frac{1}{2}m v'^2 + \frac{1}{2}(2m) v_{2}'^2\]
Kinetic energy is the energy that an object possesses due to its motion. In elastic collisions, no kinetic energy is converted into other forms of energy, like heat or sound.
By using this conservation principle, the actual speeds of the particles after the collision can be calculated. Remember that since these quantities also satisfy momentum conservation, it's all about solving the equations simultaneously. For our specific problem, this results in finding that both particles acquire a final speed of \(\frac{v}{\sqrt{2}}\).
Understanding how energy is conserved enables us to track how energy moves through the system during the collision, allowing us to determine the distribution of energy between the colliding objects.
Angle of Deflection in Collisions
The angle at which particles deflect after an elastic collision is an important aspect of the collision dynamics. In our case, where a nucleus scatters off its target at a right angle or 90 degrees, this creates a right triangle with the velocities.
  • This means that the velocities suddenly take a new direction but the vector sum equals the initial velocity.
The deflection angle can be interpreted and calculated using trigonometric principles:
  • Knowing that for a right angle collision, \[v'^2 + v_{2}'^2 = v^2\]considers both the conservation laws and vector relationships.
In many collision scenarios, the angle is fundamental as it helps in understanding how the motion is altered.
In our problem, due to a perfect right angle formed, the resulting vector analysis shows that the target particle moves at 45 degrees after the collision. Understanding angles of deflection provides insight into how particles interact and distribute their motion through space during a collision.

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Most popular questions from this chapter

(II) A ball of mass \(0.220 \mathrm{~kg}\) that is moving with a speed of \(7.5 \mathrm{~m} / \mathrm{s}\) collides head-on and elastically with another ball initially at rest. Immediately after the collision, the incoming ball bounces backward with a speed of \(3.8 \mathrm{~m} / \mathrm{s}\). Calculate (a) the velocity of the target ball after the collision, and (b) the mass of the target ball.

You have been hired as an expert witness in a court case involving an automobile accident. The accident involved car A of mass \(1500 \mathrm{~kg}\) which crashed into stationary car \(\mathrm{B}\) of mass \(1100 \mathrm{~kg} .\) The driver of car \(\mathrm{A}\) applied his brakes \(15 \mathrm{~m}\) before he skidded and crashed into car \(\mathrm{B}\). After the collision, car A slid \(18 \mathrm{~m}\) while car \(\mathrm{B}\) slid \(30 \mathrm{~m}\). The coefficient of kinetic friction between the locked wheels and the road was measured to be \(0.60 .\) Show that the driver of car A was exceeding the \(55-\mathrm{mi} / \mathrm{h}(90 \mathrm{~km} / \mathrm{h})\) speed limit before applying the brakes.

(III) \(\mathrm{A}\) neon atom \((m=20.0 \mathrm{u})\) makes a perfectly elastic collision with another atom at rest. After the impact, the neon atom travels away at a \(55.6^{\circ}\) angle from its original direction and the unknown atom travels away at a \(-50.0^{\circ}\) angle. What is the mass (in u) of the unknown atom? [Hint: You could use the law of sines.

A ball is dropped from a height of 1.50 \(\mathrm{m}\) and rebounds to a height of 1.20 \(\mathrm{m} .\) Approximately how many rebounds will the ball make before losing 90\(\%\) of its energy?

You are the design engineer in charge of the crashworthiness of new automobile models. Cars are tested by smashing them into fixed, massive barriers at \(45 \mathrm{~km} / \mathrm{h}\). A new model of mass 1500 kg takes 0.15 s from the time of impact until it is brought to rest. \((a)\) Calculate the average force exerted on the car by the barrier. (b) Calculate the average deceleration of the car.

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