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\(\mathrm{A}\) barge with mass \(1.50 \times\) \(10^{5} \mathrm{~kg}\) is proceeding downriver at \(6.2 \mathrm{~m} / \mathrm{s}\) in heavy fog when it collides with a barge heading directly across the river (see Fig. 7-31). The second barge has mass \(2.78\) \(\times 10^{5} \mathrm{~kg}\) and before the collision is moving at \(4.3\) \(\mathrm{m} / \mathrm{s} . \quad\) Immediately after impact, the second barge finds its course deflected by \(18^{\circ}\) in the downriver direction and its speed increased to \(5.1 \mathrm{~m} / \mathrm{s}\). The river current is approximately zero at the time of the accident. What are the speed and direction of motion of the first barge immediately after the collision?

Short Answer

Expert verified
The speed of the first barge after the collision is approximately 5.77 m/s at an angle of approximately 118.5 degrees from the positive x-axis.

Step by step solution

01

Understand the problem

We have two barges colliding in a foggy environment. The first barge has mass \(1.50 \times 10^{5} \text{ kg}\) and an initial speed of \(6.2 \text{ m/s}\). The second barge has mass \(2.78 \times 10^{5} \text{ kg}\) and an initial speed of \(4.3 \text{ m/s}\). After the collision, the second barge's speed is \(5.1 \text{ m/s}\) at an angle of \(18^{\circ}\). We need to find the speed and direction of motion of the first barge after the collision.
02

- Calculate initial momentum

Determine the x- and y-components of the initial momentum for both barges. Let the downriver direction be the x-axis, and the direction directly across the river be the y-axis. For barge 1 (x-direction): \[ p_{1x\text{initial}} = m_{1} v_{1x} = 1.50 \times 10^{5} \text{ kg} \times 6.2 \text{ m/s} = 9.3 \times 10^{5} \text{ kg} \cdot \text{m/s} \] and for barge 2 (y-direction): \[ p_{2y\text{initial}} = m_{2} v_{2y} = 2.78 \times 10^{5} \text{ kg} \times 4.3 \text{ m/s} = 1.1954 \times 10^{6} \text{ kg} \cdot \text{m/s} \] Since barge 2 initially has no x-component and barge 1 no y-component, it simplifies our calculations.
03

- Calculate final momentum for barge 2

Post-collision, find the x- and y-components of the final momentum for barge 2. Using its given speed and deflected angle: \[ p_{2x\text{final}} = m_{2} v_{2\text{final}} \cos(18^{\circ}) = 2.78 \times 10^{5} \text{ kg} \times 5.1 \text{ m/s} \cos(18^{\circ}) = 1.34622 \times 10^{6} \text{ kg} \cdot \text{m/s} \] \[ p_{2y\text{final}} = m_{2} v_{2\text{final}} \sin(18^{\circ}) = 2.78 \times 10^{5} \text{ kg} \times 5.1 \text{ m/s} \sin(18^{\circ}) = 4.36431 \times 10^{5} \text{ kg} \cdot \text{m/s} \]
04

- Apply conservation of momentum

Since momentum is conserved in both x and y directions: In the x-direction: \[ p_{1x\text{initial}} + 0 = p_{1x\text{final}} + p_{2x\text{final}} \] \[ 9.3 \times 10^{5} \text{ kg} \cdot \text{m/s} = p_{1x\text{final}} + 1.34622 \times 10^{6} \text{ kg} \cdot \text{m/s} \] Rearrange to find \(p_{1x\text{final}}\): \[ p_{1x\text{final}} = (9.3 \times 10^{5} - 1.34622 \times 10^{6}) \text{ kg} \cdot \text{m/s} = -4.1622 \times 10^5 \text{ kg} \cdot \text{m/s} \] And in the y-direction: \[ 0 + p_{2y\text{initial}} = p_{1y\text{final}} + p_{2y\text{final}} \] \[ 1.1954 \times 10^{6} \text{ kg} \cdot \text{m/s} = p_{1y\text{final}} + 4.36431 \times 10^{5} \text{ kg} \cdot \text{m/s} \] Rearrange to find \(p_{1y\text{final}}\): \[ p_{1y\text{final}} = (1.1954 \times 10^{6} - 4.36431 \times 10^{5}) \text{ kg} \cdot \text{m/s} = 7.58969 \times 10^5 \text{ kg} \cdot \text{m/s} \]
05

- Determine speed of first barge

Use the components of final momentum to find the speed of the first barge. Recall: \[ p = m \cdot v \text{, hence} \; \vec{v}_1 = \frac{\vec{p}_1}{m_1} \] Therefore, \( v_{1\text{final}} = \sqrt{(\frac{p_{1x\text{final}}}{m_{1}})^2 + (\frac{p_{1y\text{final}}}{m_{1}})^2} \) \[ v_{1\text{final}} = \sqrt{(\frac{-4.1622 \times 10^5}{1.50 \times 10^5})^2 + (\frac{7.58969 \times 10^5}{1.50 \times 10^5})^2} \] \[ v_{1\text{final}} = \sqrt{(-2.7748)^2 + (5.0598)^2} \] \[ v_{1\text{final}} \approx \sqrt{7.7 + 25.6} = \sqrt{33.3} \approx 5.77 \text{ m/s} \]
06

- Determine direction of the first barge

Find the angle of the first barge's velocity after the collision. \[ \theta = \tan^{-1}(\frac{p_{1y\text{final}}}{p_{1x\text{final}}}) = \tan^{-1}(\frac{7.58969 \times 10^5}{-4.1622 \times 10^5}) \approx \tan^{-1}(-1.824) \approx -61.5^{\circ} \] The negative angle indicates the direction is 180° - 61.5° = 118.5° counterclockwise from the positive x-axis.

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Key Concepts

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

momentum conservation
In physics, the law of momentum conservation is vital when analyzing collisions. This law states that the total momentum of a closed system remains constant before and after a collision. Think of momentum as the 'quantity of motion' an object has. In mathematical terms, we write it as \( \boldsymbol{p} = m \times v \) where \( m \) is mass and \( v \) is velocity.
This law allows us to set up equations that help us solve for unknown variables, such as the final velocities of colliding objects.

For instance, in the given barge collision problem, we used initial and final momenta's x- and y-components to solve for the first barge's speed and direction post-collision. By doing this, we considered momentum conservation in both directions separately, ensuring that the total momentum remains unchanged.
vector components
Vectors in physics represent quantities with both magnitude and direction. Most of the time, vectors are broken down into their x (horizontal) and y (vertical) components. This step is essential for simplifying calculations especially in two-dimensional problems, like our barge collision.

For vector breakdown, we use trigonometry: \( v_x = v \times \text{cos(θ)} \) and \( v_y = v \times \text{sin(θ)} \).

In our case, each barge's speed was split into components along the directions of interest (downriver and across). This approach enabled us to apply the momentum conservation principle more effectively, as we could deal with straight lines rather than complex angles.
collision analysis
Analyzing collisions involves understanding how the interacting bodies behave before and after impact. We categorize collisions into elastic and inelastic.

An elastic collision retains both kinetic energy and momentum, while an inelastic collision retains only momentum. Both kinds involve calculating the initial and final states of the objects involved.

For our exercise, distinguishing these principles was crucial. Despite the lack of specific kinetic energy conservation details, knowing it allowed us to focus on momentum conservation rules for calculation. Understanding collision types helps determine what principles to apply when solving problems.
problem-solving in physics
Solving physics problems often entails breaking them down into smaller, manageable steps. Here's a concise strategy:
  • Read and understand the problem.
  • Identify given data and required unknowns.
  • Apply relevant principles and laws (e.g., conservation laws, kinematic equations).
  • Break complex problems into simpler components using vector analysis where necessary.
  • Use mathematical tools to derive solutions and verify the results.

These steps helped solve our barge collision problem efficiently. First, we determined the initial and final momenta components for each barge. Next, we conserved momentum to find unknown variables. Lastly, calculations were verified for consistency.
kinematics
Kinematics focuses on describing motion without considering its causes. It uses equations that connect displacement, velocity, acceleration, and time.
In many collision problems, we prioritize velocity and sometimes acceleration.

In our exercise, kinematic principles were implicitly applied, especially when calculating the new speeds and directions post-collision. The barges' velocities pre- and post-impact helped break the motion into understandable parts, enabling further analysis using momentum conservation. Remember, kinematics helps describe how objects move, aiding deeper dynamic studies.

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Most popular questions from this chapter

Vessel at Rest Explodes A vessel at rest explodes, breaking into three pieces. Two pieces, having equal mass, fly off perpendicular to one another with the same speed of \(30 \mathrm{~m} / \mathrm{s}\). The third piece has three times the mass of each other piece. What are the magnitude and direction of its velocity immediately after the explosion?

A \(2.00 \mathrm{~kg}\) "particle" traveling with velocity \(\vec{v}_{A 1}=(4.0 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{i}}\) collides with a \(4.00 \mathrm{~kg}\) "particle" traveling with velocity \(\vec{v}_{B 1}=(2.0 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{j}}\). The collision connects the two particles. What then is their velocity in (a) unit-vector notation and (b) magnitude-angle notation?

Two balls \(A\) and \(B\), having different but unknown masses, collide. Initially, \(A\) is at rest and \(B\) has speed \(v_{B}\). After the collision, \(B\) has speed \(v_{B} / 2\) and moves perpendicularly to its original motion. (a) Find the direction in which ball \(A\) moves after the collision. (b) Show that you cannot determine the speed of \(A\) from the information given.

A rocket, which is in deep space and initially at rest relative to an inertial reference frame, has a mass of \(2.55 \times 10^{5} \mathrm{~kg}\), of which \(1.81 \times 10^{5} \mathrm{~kg}\) is fuel. The rocket engine is then fired for \(250 \mathrm{~s}\), during which fuel is consumed at the rate of \(480 \mathrm{~kg} / \mathrm{s}\). The speed of the exhaust products relative to the rocket is \(3.27 \mathrm{~km} / \mathrm{s}\). (a) What is the rocket's thrust? After the \(250 \mathrm{~s}\) firing, what are the (b) mass and (c) speed of the rocket?

The force of air resistance on a sphere of radius \(R\) can plausibly be argued to have the form $$ \vec{F} \text { drag }=-\frac{1}{2} C \rho R^{2}|v| \vec{v}=-b|v| \vec{v} $$ where \(\vec{v}\) is the vector velocity and \(|\vec{v}|\) is its magnitude (the speed). The density of the air, \(\rho\), is about \(1 \mathrm{~kg} / \mathrm{m}^{3}-1 / 1000\) that of water. The parameter \(C\) is a dimensionless constant. If we drop a steel ball and a styrofoam ball from a height of \(s\). the steel ball reaches the ground when the styrofoam ball is still a bit above the ground. Call this distance \(h .\) Estimate the air resistance coefficient \(C\) as follows: (a) Assume the effect of air resistance on the steel sphere is negligible. Calculate approximately how long the steel sphere takes to fall to the ground \(\left(\Delta t_{\text {ste }}\right)\) and how fast it is traveling just before it hits \(\left(v_{\text {ste }}\right) .\) Express your answers in terms of \(s, g\), and \(m\). (b) Since the steel and styrofoam were not very different, use \(\left\langle\vec{v}_{\text {ste }}\right.\), the average velocity of the steel ball during its fall to calculate an average air resistance force, \((\vec{F}\) drag \()=-b\left\langle\left.\vec{v}\right|^{2}\right.\) acting on the styrofoam sphere during its fall. Express this force in terms of \(b, m\) (the mass of the styrofoam sphere), \(g, s\), and \(h\). (c) The average velocity of the steel ball is \(\left\langle\vec{v}_{\text {ste }}\right\rangle=s / \Delta t_{\text {ste }} .\) The average velocity of the styrofoam sphere was \(\left\langle\vec{v}_{\text {sty }}\right\rangle=(s-h) / \Delta t_{\text {ste }}\) Assume this difference, \(\Delta(\vec{v})\), is caused by the average air resistance force acting over the time \(\Delta t_{\text {ste }}\) with our basic Newton's law formula: $$ \left\langle\vec{F}^{\text {drag }}\right\rangle \Delta t_{\text {ste }}=m \Delta(\vec{v}) . $$ Use this to show that $$ b \cong \frac{m h}{s^{2}} $$ (d) A styrofoam ball of radius \(R=5 \mathrm{~cm}\) and mass \(m=50 \mathrm{~g}\) is dropped with a steel ball from a height of \(s=2 \mathrm{~m}\). When the steel ball hits, the styrofoam is about \(h=10 \mathrm{~cm}\) above the ground. Calculate \(b\) (for the styrofoam sphere) and \(C\) (for any sphere).

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