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(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.

Short Answer

Expert verified
The mass of the unknown atom is approximately 21.5 u.

Step by step solution

01

Understand the Situation

A neon atom of mass \( m = 20.0 \, \text{u} \) makes a perfectly elastic collision with a stationary atom, resulting in two angles of travel post-collision. The known angle for the neon atom is \( 55.6^{\circ} \) and the unknown mass atom's angle is \(-50.0^{\circ}\). You are tasked with finding the mass of the unknown atom.
02

Establish the Momentum Conservation Equations

In any elastic collision, the conservation of linear momentum applies for both the x and y components.\[p_{\text{x initial}} = p_{\text{x final}} \quad \text{and} \quad p_{\text{y initial}} = p_{\text{y final}}\]Initially, the system's momentum in the y direction is zero as both atoms are moving horizontally.
03

Express Momentum Components

The initial x-axis momentum is due only to the neon atom:\[20.0 \, \text{u} \times v = 20.0 \, \text{u} \times v_{ ext{Ne}} \cos(55.6^{\circ}) + m_u \times v_{\text{u}} \cos(50^{\circ})\]The initial y-axis momentum:\[0 = 20.0 \, \text{u} \times v_{ ext{Ne}} \sin(55.6^{\circ}) - m_u \times v_{ ext{u}} \sin(50^{\circ})\]where \( m_u \) is the unknown mass, \( v_{\text{Ne}} \) is the velocity of the neon atom, and \( v_{\text{u}} \) is the velocity of the unknown atom.
04

Utilize the Law of Sines from Geometry of Collision

Apply the Law of Sines within the triangle of velocity vectors:\[\frac{v_{\text{Ne}} \cos(55.6^{\circ})}{\sin(50^{\circ})} = \frac{v_{\text{u}} \cos(50^{\circ})}{\sin(55.6^{\circ})}\]This simplifies the problem by relating the velocity components, allowing us to focus just on relative velocities.
05

Solve for Mass using Equations

Given the geometry and conservation of momentum:\[\frac{m}{m_u} = \frac{\sin(50^{\circ})}{\sin(55.6^{\circ})}\]Using trigonometric values,\[\frac{20}{m_u} \approx \frac{\sin(50)}{\sin(55.6)}\]Suppose \( \sin(50) \approx 0.766 \) and \( \sin(55.6) \approx 0.826 \), so \( \frac{20}{m_u} \approx \frac{0.766}{0.826} \) which implies \( m_u \approx 21.5 \, \text{u} \).

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Key Concepts

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

law of sines
The Law of Sines is a mathematical relationship in trigonometry that helps solve for unknown sides or angles in a non-right triangle. It's particularly useful in physics problems involving angles, like when objects collide and scatter in multiple directions.

In the given exercise, the collision of atoms results in a triangular relationship between the velocities and their angles of deflection. The Law of Sines comes into play by equating the ratios of sides to the sines of their opposite angles. It is expressed as:
  • \( \frac{a}{\sin A} = \frac{b}{\sin B} = \frac{c}{\sin C} \)
For this specific problem, the law is used to find a ratio between the velocities of the two atoms:
  • \( \frac{v_{\text{Ne}} \cos(55.6^{\circ})}{\sin(50^{\circ})} = \frac{v_{\text{u}} \cos(50^{\circ})}{\sin(55.6^{\circ})} \)
This equation relates the velocity of the neon atom and the unknown atom after the collision through a geometric viewpoint, often unseen in simple linear problems. Nevertheless, such an approach helps to determine the relationship between different velocity components, showcasing the beauty of trigonometry in physics.
momentum conservation
Momentum conservation is a fundamental principle in physics stating that the total momentum of a closed system remains constant if not acted upon by an external force. This principle is crucial during collisions, both elastic and inelastic.

In perfectly elastic collisions such as the one in this exercise, both momentum and kinetic energy are conserved. The principle can be broken down into maintaining momentum along individual axes:
  • x-axis: \( p_{\text{x initial}} = p_{\text{x final}} \)
  • y-axis: \( p_{\text{y initial}} = p_{\text{y final}} \)
During the collision shown, the neon atom initially possesses all the system's momentum, moving horizontally. Thus, for momentum conservation:
  • The total initial x-axis momentum is: \( 20.0 \, \text{u} \times v \)
  • The total final x-axis momentum: \( 20.0 \, \text{u} \times v_{\text{Ne}} \cos(55.6^{\circ}) + m_u \times v_{\text{u}} \cos(50^{\circ}) \)
  • The total initial and final y-axis momentum: 0, balancing as \( 20.0 \, \text{u} \times v_{\text{Ne}} \sin(55.6^{\circ}) = m_u \times v_{\text{u}} \sin(50^{\circ}) \)
By setting up these equations for both axes, we can solve for unknown entities, like the mass of the second atom in this case, relying on the profound principle of momentum staying constant through collisions.
velocity vectors
Velocity vectors are a keystone in understanding movement, especially in interactions like collisions. A vector has both magnitude and direction, which in physics translates to speed and line of travel.

In this problem, the velocity vectors change direction post-collision due to the forces exchanged between atoms. Thus, the directions they take are not arbitrary, but angle-specific:
  • Neon atom: deflects at a \(55.6^{\circ}\) angle
  • Unknown atom: deflects at \(-50.0^{\circ}\) angle
These directions form the basis of velocity vector triangles, where the Law of Sines can apply.

When breaking down velocity into its components:
  • The x-component measures side-to-side movement:
  • The y-component measures up-and-down movement:
These angles and splits of velocity account for achieving momentum conservation in both axes. In every collision where vectors are involved, seeing each as a having x and y parts helps make sense of how paths and speeds change. Properly understanding and representing velocity vectors is crucial both in predicting the outcomes of interactions and in practically calculating unknown factors, like the mass here.

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Most popular questions from this chapter

(II) A \(0.450-\mathrm{kg}\) hockey puck, moving east with a speed of \(4.80 \mathrm{~m} / \mathrm{s},\) has a head-on collision with a \(0.900-\mathrm{kg}\) puck initially at rest. Assuming a perfectly elastic collision, what will be the speed and direction of each object after the collision?

(II) A rocket of mass \(m\) traveling with speed \(v_{0}\) along the \(x\) axis suddenly shoots out fuel equal to one-third its mass, perpendicular to the \(x\) axis (along the \(y\) axis) with speed \(2 v_{0}\). Express the final velocity of the rocket in \(\hat{\mathbf{i}}, \hat{\mathbf{j}}, \hat{\mathbf{k}}\) notation.

(III) A particle of mass \(m_{\mathrm{A}}\) traveling with speed \(v_{\mathrm{A}}\) collides elastically head-on with a stationary particle of smaller mass \(m_{\mathrm{B}} \cdot(a)\) Show that the speed of \(m_{\mathrm{B}}\) after the collision is $$ v_{\mathrm{B}}^{\prime}=\frac{2 v_{\mathrm{A}}}{1+m_{\mathrm{B}} / m_{\mathrm{A}}} $$ (b) Consider now a third particle of mass \(m_{\mathrm{C}}\) at rest between \(m_{\mathrm{A}}\) and \(m_{\mathrm{B}}\) so that \(m_{\mathrm{A}}\) first collides head on with \(m_{\mathrm{C}}\) and then \(m_{\mathrm{C}}\) collides head on with \(m_{\mathrm{B}}\). Both collisions are elastic. Show that in this case, $$ v_{\mathrm{B}}^{\prime}=4 v_{\mathrm{A}} \frac{m_{\mathrm{C}} m_{\mathrm{A}}}{\left(m_{\mathrm{C}}+m_{\mathrm{A}}\right)\left(m_{\mathrm{B}}+m_{\mathrm{C}}\right)} $$ (c) From the result of part (b), show that for $$ \operatorname{maximum} v_{\mathrm{B}}^{\prime}, m_{\mathrm{C}}=\sqrt{m_{\mathrm{A}} m_{\mathrm{B}}} $$ \((d)\) Assume \(m_{\mathrm{B}}=2.0 \mathrm{~kg}\) \(m_{\mathrm{A}}=18.0 \mathrm{~kg}\) and \(v_{\mathrm{A}}=2.0 \mathrm{~m} / \mathrm{s}\). Use a spreadsheet to calculate and graph the values of \(v_{\mathrm{B}}^{\prime}\) from \(m_{\mathrm{C}}=0.0 \mathrm{~kg}\) to \(m_{\mathrm{C}}=50.0 \mathrm{~kg}\) in steps of \(1.0 \mathrm{~kg} .\) For what value of \(m_{\mathrm{C}}\) is the value of \(v_{\mathrm{B}}^{\prime}\) maximum? Does your numerical result agree with your result in part \((c) ?\)

A \(4800-\mathrm{kg}\) open railroad car coasts along with a constant speed of \(8.60 \mathrm{~m} / \mathrm{s}\) on a level track. Snow begins to fall vertically and fills the car at a rate of \(3.80 \mathrm{~kg} / \mathrm{min}\). Ignoring friction with the tracks, what is the speed of the car after \(60.0 \mathrm{~min} ?\) (See Section 9-2.)

(III) Prove that in the elastic collision of two objects of identical mass, with one being a target initially at rest, the angle between their final velocity vectors is always \(90^{\circ} .\)

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