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Two identical balls traveling parallel to the \(x\) -axis have speeds of 30 \(\mathrm{cm} / \mathrm{s}\) and are oppositely directed. They collide off center perfectly elastically. After the collision, one ball is moving at an angle of \(30^{\circ}\) above the \(+x\) -axis. Find its speed and the velocity of the other ball.

Short Answer

Expert verified
The first ball's speed is 30 cm/s; the second ball's speed is also 30 cm/s.

Step by step solution

01

Understanding the Problem

Two identical balls collide elastically. One ball initially moves at 30 cm/s along the positive x-axis and the other at 30 cm/s along the negative x-axis. After collision, one ball moves at 30° above the +x-axis.
02

Conservation of Momentum in X-direction

For an elastic collision, momentum is conserved. Let the speeds of the balls after collision be \(v_1\) and \(v_2\). The total momentum in the x-direction before collision is \(m \times 30 - m \times 30 = 0\) (where \(m\) is the mass). Therefore, \[m v_1 \cos(30^{\circ}) + m v_2 \cos(\theta_2) = 0\] where \(\theta_2\) is the angle of the second ball.
03

Conservation of Momentum in Y-direction

In the y-direction, the initial momentum is 0, so after the collision: \[m v_1 \sin(30^{\circ}) - m v_2 \sin(\theta_2) = 0\] This implies \[v_1 \sin(30^{\circ}) = v_2 \sin(\theta_2)\]
04

Conservation of Kinetic Energy

Because the collision is elastic, the total kinetic energy is conserved:\[0.5 m (30^2) + 0.5 m (30^2) = 0.5 m (v_1^2) + 0.5 m (v_2^2)\]Simplifying this gives:\[1800 = v_1^2 + v_2^2\]
05

Solve System of Equations

Substituting from Step 3 into Steps 2 and 4 allows solving the equations.1. From Step 2: \(v_2 = -v_1 \cos(30^{\circ}) / \cos(\theta_2)\)2. Simplify Step 4: \(1800 = v_1^2 + (-v_1 \cos(30^{\circ}) / \cos(\theta_2))^2\)Combine with Step 3 to solve for \(v_1\) and \(v_2\).
06

Simplify Calculations

Since the balls are identical and the collision is symmetric, they simply exchange velocities. This symmetry implies:\[v_1 = 30\] cm/s, and \(v_2 = 30\) cm/s.

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Key Concepts

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

Conservation of Momentum
The Conservation of Momentum is a crucial principle that dictates how objects interact during collisions. Put simply, momentum is a measure of the quantity of motion an object has, and for a closed system, total momentum remains constant before and after the collision. In our case, with two identical balls:
  • Before collision: One ball moves at 30 cm/s in the positive x-direction and the other at 30 cm/s in the negative x-direction.
  • Total momentum is calculated as: \( m \times 30 - m \times 30 = 0 \).
This is because the two momenta of equal magnitude but opposite direction cancel each other out.

After the collision, the situation remains symmetrical. Therefore, the momentum in both x and y directions must satisfy the equations that ensure total momentum remains zero. In the x-direction, the equation is:
  • \( m v_1 \cos(30^{\circ}) + m v_2 \cos(\theta_2) = 0 \)
In the y-direction, since no initial y momentum exists, the equation becomes:
  • \( m v_1 \sin(30^{\circ}) = m v_2 \sin(\theta_2) \)
These equations allow us to explore the results of the collision and derive the speed and direction of the two balls after the collision.
Conservation of Kinetic Energy
When a collision is described as elastic, this means that the total kinetic energy is conserved. Kinetic energy quantifies an object's energy due to its motion, and in a closed system, it remains constant when the collision doesn't result in permanent deformation or heat loss. For the problem with our two balls:
  • Before the collision, each ball has a kinetic energy of \( 0.5 \times m \times (30^2) \).
  • The total initial kinetic energy of the system is \( 2 \times 0.5 \times m \times (30^2) = 1800 m \).


Following the collision, the sum of the kinetic energies of both balls must still total 1800, allowing us to write the following equation:
  • \( 0.5 m (v_1^2) + 0.5 m (v_2^2) = 1800 \)
By solving this equation simultaneously with those derived from the conservation of momentum, we arrive at the velocities of the two balls post-collision. Importantly, conservation of kinetic energy provides a reality check that ensures calculations involving speed and kinetic motion are correct.
Collision Angles
In the context of our exercise, collision angles play a pivotal role in determining the trajectory of each ball post-collision. Collision angles refer to the direction each object takes relative to a reference axis, often chosen to simplify calculations.

In our scenario:
  • One ball is given to move at \(30^{\circ}\) above the \(+x\)-axis after collision.
  • This result provides one constraint for our momentum and kinetic energy equations.
The secondary ball, although not explicitly stated in the problem, will have a symmetric angle due to conservation laws and the nature of elastic collisions.

The use of angles helps decompose vector quantities like velocity into orthogonal components, generally the x and y components. This allows the problem to easily align with conservation laws, as components can then be analyzed separately. In our case, you can focus on splitting the speed of each ball after the collision into components using the given angle for a precise understanding of the collision dynamics.

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Most popular questions from this chapter

A force of \(1000 \mathrm{~N}\) is applied to a small space satellite for a time of \(10.0\) minutes. If the craft has a mass of \(200 \mathrm{~kg}\), what will be its final speed? [Hint: Be careful with those exponents when using a calculator.]

Two balls of equal mass, moving with speeds of \(3 \mathrm{~m} / \mathrm{s}\), collide head-on. Find the speed of each after impact if \((a)\) they stick together, \((b)\) the collision is perfectly elastic, \((c)\) the coefficient of restitution is \(1 / 3\).

Three masses are placed on the \(y\) -axis: \(2 \mathrm{~kg}\) at \(y=300 \mathrm{~cm}, 6 \mathrm{~kg}\) at \(y\) \(=150 \mathrm{~cm}\), and \(4 \mathrm{~kg}\) at \(y=-75 \mathrm{~cm}\). Find their center of mass.

During a soccer game a ball (of mass \(0.425 \mathrm{~kg}\) ), which is initially at rest, is kicked by one of the players. The ball moves off at a speed of \(26 \mathrm{~m} / \mathrm{s}\). Given that the impact lasted for \(8.0 \mathrm{~ms}\), what was the average force exerted on the ball?

A 15 -g bullet moving at \(300 \mathrm{~m} / \mathrm{s}\) passes through a \(2.0\) -cm-thick sheet of foam plastic and emerges with a speed of \(90 \mathrm{~m} / \mathrm{s}\). Assuming that the speed change takes place uniformly, what average force impeded the bullet's motion through the plastic? We can determine the change in momentum, and that suggests using the impulse equation to find the force \(F\) on the bullet as it takes a time \(\Delta t\) to pass through the plastic. Taking the initial direction of motion to be positive, $$ F \Delta t=m v_{f}-m v_{i} $$ We can find \(\Delta t\) by assuming uniform deceleration and using \(x=\) \(v_{a v} t\), where \(x=0.020 \mathrm{~m}\) and \(v_{a v}=\frac{1}{2}\left(v_{i}+v_{f}\right)=195 \mathrm{~m} / \mathrm{s}\). This gives \(\Delta t=1.026 \times 10^{-4} \mathrm{~s}\). Then \((F)\left(1.026 \times 10^{-4} \mathrm{~s}\right)=(0.015 \mathrm{~kg})(90 \mathrm{~m} / \mathrm{s})-(0.015 \mathrm{~kg})(300 \mathrm{~m} / \mathrm{s})\) which yields \(F=-3.1 \times 10^{4} \mathrm{~N}\) as the average retarding force. How could this problem have been solved using \(F=\) ma instead of the impulse equation? By using energy methods?

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