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At time \(t=0\), force \(\vec{F}_{1}=(-4.00 \hat{\mathrm{i}}+5.00 \hat{\mathrm{j}}) \mathrm{N}\) acts on an initially stationary particle of mass \(2.00 \times 10^{-3} \mathrm{~kg}\) and force \(\vec{F}_{2}=(2.00 \hat{i}-4.00 \mathrm{j}) \mathrm{N}\) acts on an initially stationary particle of mass \(4.00 \times 10^{-3} \mathrm{~kg}\). From time \(t=0\) to \(t=2.00 \mathrm{~ms}\), what are the (a) magnitude and (b) angle (relative to the positive direction of the \(x\) axis) of the displacement of the center of mass of the twoparticle system? (c) What is the kinetic energy of the center of mass at \(t=2.00 \mathrm{~ms}\) ?

Short Answer

Expert verified
(a) Magnitude: 0.745 mm, (b) Angle: -26.6°, (c) Kinetic energy: 0.0267 J.

Step by step solution

01

Calculate individual accelerations

The acceleration of each particle can be computed using Newton's second law: \[a = \frac{F}{m}\].First particle:\[\vec{a}_1 = \frac{\vec{F}_1}{m_1} = \frac{(-4.00 \hat{\mathrm{i}} + 5.00 \hat{\mathrm{j}})}{2.00 \times 10^{-3}} = (-2000 \hat{\mathrm{i}} + 2500 \hat{\mathrm{j}}) \, \mathrm{m/s^2}\] Second particle:\[\vec{a}_2 = \frac{\vec{F}_2}{m_2} = \frac{(2.00 \hat{\mathrm{i}} - 4.00 \hat{\mathrm{j}})}{4.00 \times 10^{-3}} = (500 \hat{\mathrm{i}} - 1000 \hat{\mathrm{j}}) \, \mathrm{m/s^2}\].
02

Calculate the displacements of each particle

Displacement due to constant acceleration is given by: \(s = \frac{1}{2} a t^2 \).For the first particle:\[\vec{s}_1 = \frac{1}{2} \vec{a}_1 t^2 = \frac{1}{2} (-2000 \hat{\mathrm{i}} + 2500 \hat{\mathrm{j}})(2.00 \times 10^{-3})^2\]\[= (-4.00 \hat{\mathrm{i}} + 5.00 \hat{\mathrm{j}}) \times 10^{-3} \, \mathrm{m}\]For the second particle:\[\vec{s}_2 = \frac{1}{2} \vec{a}_2 t^2 = \frac{1}{2} (500 \hat{\mathrm{i}} - 1000 \hat{\mathrm{j}})(2.00 \times 10^{-3})^2\]\[= (1.00 \hat{\mathrm{i}} - 2.00 \hat{\mathrm{j}}) \times 10^{-3} \, \mathrm{m}\].
03

Calculate the center of mass displacement

The center of mass (\(\vec{s}_{cm}\)) is obtained using the formula:\[\vec{s}_{cm} = \frac{m_1 \vec{s}_1 + m_2 \vec{s}_2}{m_1 + m_2}\].Substitute the known values:\[\vec{s}_{cm} = \frac{(2.00 \times 10^{-3})(-4.00 \hat{\mathrm{i}} + 5.00 \hat{\mathrm{j}}) + (4.00 \times 10^{-3})(1.00 \hat{\mathrm{i}} - 2.00 \hat{\mathrm{j}})}{2.00 \times 10^{-3} + 4.00 \times 10^{-3}}\]\[= \frac{(-8.00 \hat{\mathrm{i}} + 10.00 \hat{\mathrm{j}} + 4.00 \hat{\mathrm{i}} - 8.00 \hat{\mathrm{j}})}{6.00 \times 10^{-3}}\]\[= (-0.667 \hat{\mathrm{i}} + 0.333 \hat{\mathrm{j}}) \times 10^{-3} \, \mathrm{m}\].
04

Calculate the magnitude and direction of displacement

With \(\vec{s}_{cm}\) from Step 3:The magnitude of displacement is:\[|\vec{s}_{cm}| = \sqrt{(-0.667 \times 10^{-3})^2 + (0.333 \times 10^{-3})^2} = 0.745 \times 10^{-3} \, \mathrm{m}\].The angle relative to the positive \(x\)-axis is:\[\theta = \tan^{-1}\left(\frac{0.333}{-0.667}\right) = -26.6^\circ\].
05

Calculate the kinetic energy of the center of mass

First, calculate the velocities of the center of mass:\(\vec{v}_{cm} = \frac{m_1 \vec{a}_1 + m_2 \vec{a}_2}{m_1 + m_2} \times t \).Substitute the accelerations:\[\vec{v}_{cm} = \frac{(2 \times 10^{-3})(-2000 \hat{\mathrm{i}} + 2500 \hat{\mathrm{j}}) + (4 \times 10^{-3})(500 \hat{\mathrm{i}} - 1000 \hat{\mathrm{j}})}{2 \times 10^{-3} + 4 \times 10^{-3}}(2 \times 10^{-3})\]\[= (-2.67 \hat{\mathrm{i}} + 1.33 \hat{\mathrm{j}}) \, \mathrm{m/s}\].The kinetic energy is:\[KE_{cm} = \frac{1}{2} M_{total} v_{cm}^2 = \frac{1}{2} (6.00 \times 10^{-3})(\sqrt{(-2.67)^2 + 1.33^2})^2\]\[= 0.0267 \, \mathrm{J}\].

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Key Concepts

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

Newton's Second Law
Newton's Second Law is a fundamental principle in physics that relates the force exerted on an object to its acceleration. The law is succinctly expressed in the formula \( F = ma \), where \( F \) is the force applied, \( m \) is the mass of the object, and \( a \) is its acceleration. In this exercise, we are looking at a system of particles subjected to known forces. By applying Newton's Second Law, we can determine how these forces cause the particles to accelerate.
For instance, when a force \( \vec{F}_1 = (-4.00 \hat{\mathrm{i}} + 5.00 \hat{\mathrm{j}}) \text{ N} \) acts on a particle with mass \( 2.00 \times 10^{-3} \text{ kg} \), we find its acceleration by rearranging our equation: \( a_1 = \frac{F_1}{m_1} \).
This results in an acceleration \( \vec{a}_1 = (-2000 \hat{\mathrm{i}} + 2500 \hat{\mathrm{j}}) \text{ m/s}^2 \) for the first particle. Understanding this relationship supports the analysis of motion, explaining how varying forces influence particle behavior.
Center of Mass
The center of mass of a system of particles is a point that behaves as if all the system's mass and external forces are concentrated there. It's a crucial concept for solving dynamics problems involving multiple particles. The position of the center of mass \( \vec{s}_{cm} \) can be determined by weighing individual positions by their respective masses and then summing and normalizing across the total mass.
In the given problem, we calculate the displacement of the center of mass, \( \vec{s}_{cm} \), as follows: \( \vec{s}_{cm} = \frac{m_1 \vec{s}_1 + m_2 \vec{s}_2}{m_1 + m_2} \).
This formula tells us how the entire system shifts based on individual particle displacements. By plugging in the known values, we determine the center of mass displacement as \((-0.667 \hat{\mathrm{i}} + 0.333 \hat{\mathrm{j}}) \times 10^{-3} \text{ m} \). This displacement helps analyze how the system's orientation changes under applied forces across a short period (\(t = 2.00 \text{ ms}\)).
Kinetic Energy
Kinetic Energy (KE) quantifies the motion of an object or system of particles. It's calculated using the formula \( KE = \frac{1}{2} mv^2 \), where \( m \) is the mass and \( v \) is the velocity. For a system of particles, we often consider the kinetic energy of the center of mass, which represents the overall movement of the system.
To find the kinetic energy of the center of mass at \( t = 2.00 \text{ ms} \), we first compute the center of mass velocity \( \vec{v}_{cm} \) resulting from applied forces. The velocity can be found from: \( \vec{v}_{cm} = \frac{m_1 \vec{a}_1 + m_2 \vec{a}_2}{m_1 + m_2} \times t \).
Putting values in the equation provides us with \( \vec{v}_{cm} = (-2.67 \hat{\mathrm{i}} + 1.33 \hat{\mathrm{j}}) \text{ m/s} \). Subsequently, the kinetic energy is calculated: \[ KE_{cm} = \frac{1}{2}M_{total}(\sqrt{(-2.67)^2 + 1.33^2})^2 \].
This results in a kinetic energy of \( 0.0267 \text{ J} \), offering insight into the dynamic behavior of the system influenced by the particles' combined forces and mass.

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