/*! 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 2 A 16 -g mass is moving in the \(... [FREE SOLUTION] | 91Ó°ÊÓ

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A 16 -g mass is moving in the \(+x\) -direction at \(30 \mathrm{~cm} / \mathrm{s}\), while a \(4.0\) -g mass is moving in the \(-x\) -direction at \(50 \mathrm{~cm} / \mathrm{s}\). They collide headon and stick together. Find their velocity after the collision. Assume negligible friction. This is a completely inelastic collision for which KE is not conserved, although momentum is. Let the 16 -g mass be \(m_{1}\) and the 4.0-g mass be \(m_{2}\). Take the \(+x\) -direction to be positive. That means that the velocity of the \(4.0\) -g mass has a scalar value of \(u_{2 x}\) \(=-50 \mathrm{~cm} / \mathrm{s}\). We apply the law of conservation of momentum to the system consisting of the two masses: $$ \begin{array}{l} \text { Momentum before impact = Momentum after impact }\\\ \begin{aligned} m_{1} v_{1 x}+m_{2} v_{2 x} &=\left(m_{1}+m_{2}\right) v_{x} \\ (0.016 \mathrm{~kg})(0.30 \mathrm{~m} / \mathrm{s})+(0.0040 \mathrm{~kg})(-0.50 \mathrm{~m} / \mathrm{s}) &=(0.020 \mathrm{~kg}) v_{x} \\ v_{x} &=+0.14 \mathrm{~m} / \mathrm{s} \end{aligned} \end{array} $$ (Notice that the \(4.0\) -g mass has negative momentum.) Hence, \(\overrightarrow{\mathbf{v}}=\) \(0.14 \mathrm{~m} / \mathrm{s}\) - POSITIVE \(X\) -DIRECTION

Short Answer

Expert verified
The final velocity is \(0.14 \, \text{m/s}\) in the positive x-direction.

Step by step solution

01

Understand the Conservation of Momentum

Momentum is always conserved in a closed system. This means that the total momentum before the collision equals the total momentum after the collision. For two masses, this is expressed as: \[ m_1 v_{1x} + m_2 v_{2x} = (m_1 + m_2) v_x \] where \(v_x\) is the velocity after collision.
02

Convert Mass and Velocity into Compatible Units

For calculations, mass should be in kilograms and velocity in meters per second. Convert: - 16 g to 0.016 kg - 30 cm/s to 0.30 m/s - 4 g to 0.004 kg - 50 cm/s to 0.50 m/s.
03

Substitute Given Values into the Momentum Equation

Plug the values of mass and velocity into the conservation of momentum formula: \[ (0.016 \, \text{kg})(0.30 \, \text{m/s}) + (0.0040 \, \text{kg})(-0.50 \, \text{m/s}) = (0.020 \, \text{kg}) v_x \].
04

Calculate the Momentum Before Collision

Calculate the momentum for each object: - Momentum of the 16-g mass is \(0.016 \times 0.30 = 0.0048 \, \text{kg m/s}\).- Momentum of the 4-g mass is \(0.004 \times (-0.50) = -0.002 \, \text{kg m/s}\). - Total momentum before is \(0.0048 - 0.002 = 0.0028 \, \text{kg m/s}\).
05

Solve for the Final Velocity \(v_x\)

Set the total initial momentum equal to the momentum after collision and solve for \(v_x\): \[ 0.0028 = (0.020) v_x \]Rearrange to find \(v_x\): \[ v_x = \frac{0.0028}{0.020} = 0.14 \, \text{m/s} \].
06

Determine the Direction of the Velocity

Since the final velocity \(v_x = 0.14 \, \text{m/s}\) is positive, the direction is in the +x direction.

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Key Concepts

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

Conservation of Momentum
When it comes to understanding physics, the principle of conservation of momentum is foundational. Momentum, which is the product of an object's mass and velocity, is conserved in an isolated system. This means that just before and just after any collision, the total momentum remains unchanged. For our specific problem, the sum of the initial momenta of both masses before they collide is equal to the combined momentum of both masses after they stick together. This is represented by the equation: \[ m_1 v_{1x} + m_2 v_{2x} = (m_1 + m_2) v_x \].Key points about conservation of momentum:
  • It applies to all kinds of collisions, whether elastic or inelastic.
  • Momentum is a vector quantity, which means it has both magnitude and direction.
  • In our problem, even though the individual momenta may change, the total system momentum stays constant.
Understanding this principle helps in solving many collision-related problems and is crucial for calculating post-collision velocities.
Inelastic Collision
In the realm of physics, collisions can be classified as elastic or inelastic, based on whether kinetic energy is conserved. In the scenario presented, we deal with a completely inelastic collision. Here, the two colliding masses stick together after they crash, making them move as one unit thereafter. Important points to note about inelastic collisions are:
  • Kinetic energy is not conserved, but momentum is.
  • After the collision, the objects do not bounce off each other but instead cling together, sharing a common velocity.
  • This change in system behavior affects how velocities and forces are modified post-collision.
  • In this enabled problem, the final merged mass moves with a common velocity that can be determined using the conservation of momentum.
Recognizing the type of collision is critical for selecting the right physics principles to apply.
Unit Conversion
An essential part of solving physics problems is ensuring that all units are compatible for calculation. This process, known as unit conversion, requires careful attention. Variables like mass and velocity often need adjustments to maintain consistency across equations. For the given exercise, mass in grams must be converted to kilograms, and velocities in centimeters per second converted to meters per second: - Mass: Convert 16 g to 0.016 kg and 4 g to 0.004 kg. - Velocity: Convert 30 cm/s to 0.30 m/s and 50 cm/s to 0.50 m/s. Key considerations when performing unit conversions:
  • Use familiar conversion factors (e.g., 1 kg = 1000 g, 1 m = 100 cm) to simplify the process.
  • Ensure all related terms in equations reflect the same unit type (e.g., meters, kilograms) before solving.
  • Regular consistency checks can prevent errors that might arise from incorrect unit application.
Mastering unit conversion is vital to obtaining accurate and meaningful results from calculations in physics.

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Most popular questions from this chapter

A billiard ball moving at a speed \(v_{1 i}\) strikes, head-on, another billiard ball that is at rest. Assuming the collision is completely elastic, show that $$ v_{1 i}=v_{1 f}+v_{2 f} $$

Two balls of equal mass approach the coordinate origin, one moving downward along the \(y\) -axis at \(2.00 \mathrm{~m} / \mathrm{s}\) and the other moving to the right along the \(-x\) -axis at \(3.00 \mathrm{~m} / \mathrm{s}\). After they collide, one ball moves out to the right along the \(+x\) -axis at \(1.20\) \(\mathrm{m} / \mathrm{s}\). Find the scalar \(x\) and \(y\) velocity components of the other ball. This is a two-dimensional collision and momentum must be conserved independently in each perpendicular direction, \(x\) and \(y\). Take up and to the right as positive. Accordingly, keeping in mind that before impact only one ball had an \(x\) -component of velocity, or \(m(3,00 \mathrm{~m} / \mathrm{s})+0=m(1.20 \mathrm{~m} / \mathrm{s}+m v\) Here \(u_{x}\) is the unknown \(x\) -component of velocity of the second ball acquired on impact. Since we know that the first ball lost some of its \(x\) -momentum, the second ball must have gained it. Moreover, \(0 r\) Here \(u_{y}\) is the \(y\) -component of velocity of the second ball. (Why the minus sign?) Solving each equation, after cancelling the mass we find that \(v_{x}=1.80 \mathrm{~m} / \mathrm{s}\) and \(v_{y}=-2.00 \mathrm{~m} / \mathrm{s}\).

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Imagine a space vehicle floating in the void. It fires a small thruster that delivers a forward force of \(2000 \mathrm{~N}\) for \(25.0 \mathrm{~s}\). Determine the resulting change in momentum of the craft. Do you need the mass of the ship?

Typically, a tennis ball hit during a serve travels away at about 51 \(\mathrm{m} / \mathrm{s}\). If the ball is at rest mid-air when struck, and it has a mass of \(0.058 \mathrm{~kg}\), what is the change in its momentum on leaving the racket?

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