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A single force acts on a \(3.0 \mathrm{~kg}\) particle-like object whose position is given by \(x=3.0 t-4.0 t^{2}+1.0 t^{3},\) with \(x\) in meters and \(t\) in seconds. Find the work done by the force from \(t=0\) to \(t=4.0 \mathrm{~s}\).

Short Answer

Expert verified
The work done by the force is \(-528.0 \, \text{J}\).

Step by step solution

01

Determine the Velocity Function

Start by taking the derivative of the position function with respect to time to find the velocity function. The position function is given by \(x(t) = 3.0t - 4.0t^2 + 1.0t^3\). Differentiating with respect to \(t\) gives:\[ v(t) = \frac{dx}{dt} = 3.0 - 8.0t + 3.0t^2 \]
02

Find the Force Using Newton's Second Law

Since force is related to acceleration (the second derivative of position) through Newton's second law \( F = ma \), find the acceleration by differentiating the velocity function:\[ a(t) = \frac{dv}{dt} = -8.0 + 6.0t \]Then, the force is:\[ F(t) = m \cdot a(t) = 3.0 \cdot (-8.0 + 6.0t) = -24.0 + 18.0t \]
03

Compute the Work Done by Integrating the Force

The work done by a force over a displacement is the integral of the force with respect to the displacement:\[ W = \int_{0}^{4} F(t) \cdot v(t) \, dt \]Substitute \(F(t) = -24.0 + 18.0t\) and \(v(t) = 3.0 - 8.0t + 3.0t^2\) into the integral:\[ W = \int_{0}^{4} (-24.0 + 18.0t) \cdot (3.0 - 8.0t + 3.0t^2) \, dt \]
04

Evaluate the Integral

Expand the expression and integrate term by term:\[W = \int_{0}^{4} (-72.0 + 192.0t - 72.0t^2) \, dt + \int_{0}^{4} (54.0t - 144.0t^2 + 54.0t^3) \, dt \]Compute each integral separately:- \(\int_{0}^{4} (-72.0) \, dt = -72.0t \bigg|_{0}^{4} = -288.0\)- \(\int_{0}^{4} (192.0t) \, dt = 96.0t^2 \bigg|_{0}^{4} = 1536.0\)- \(\int_{0}^{4} (-72.0t^2) \, dt = -24.0t^3 \bigg|_{0}^{4} = -1536.0\)- \(\int_{0}^{4} (54.0t) \, dt = 27.0t^2 \bigg|_{0}^{4} = 432.0\)- \(\int_{0}^{4} (-144.0t^2) \, dt = -48.0t^3 \bigg|_{0}^{4} = -1536.0\)- \(\int_{0}^{4} (54.0t^3) \, dt = 13.5t^4 \bigg|_{0}^{4} = 864.0\)Adding these results gives:\[ W = -288.0 + 1536.0 - 1536.0 + 432.0 - 1536.0 + 864.0 = -528.0 \, \text{J} \]
05

Conclusion

After computing the integrals and summing them, the net work done by the force from \(t=0\) to \(t=4.0\, s\) is \(-528.0 \, \text{J}\). This indicates that the force performed negative work, which often implies it opposed the motion overall.

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Key Concepts

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

Kinematics
In physics, kinematics is the branch that deals with the motion of objects. It describes how an object's position changes over time without considering the causes of motion.
When solving problems related to kinematics, the first step is to find the position, velocity, and sometimes acceleration functions. These help us track an object's motion:
  • The position function, denoted as \( x(t) \), gives the location of the object at any given time \( t \).
  • Velocity, \( v(t) \), is the rate of change of position. It's found by differentiating the position function with respect to time.
This particular exercise starts with a position function \( x(t) = 3.0t - 4.0t^2 + 1.0t^3 \). By differentiating it, we obtain the velocity: \[ v(t) = \frac{dx}{dt} = 3.0 - 8.0t + 3.0t^2 \]This velocity function tells us how fast and in which direction the object moves as time varies. It's a foundational concept used to understand more complex physics problems such as calculating work and energy.
Newton's Second Law
Newton's second law is crucial in connecting the concepts of force and motion. It states that the force exerted on an object is equal to the mass of the object multiplied by its acceleration: \[ F = ma \]Here, acceleration is the rate of change of velocity over time. So to find the acceleration function, we differentiate the velocity function: \[ a(t) = \frac{dv}{dt} = -8.0 + 6.0t \]In this exercise, multiplying the mass of the object (\(3.0 \, \text{kg}\)) with its acceleration function gives us the force as a function of time: \[ F(t) = 3.0 \times (-8.0 + 6.0t) = -24.0 + 18.0t \]This function illustrates how the force changes over time as the particle accelerates. By understanding this, we also grasp how forces influence motion, an essential principle not just in academics, but in real-world physics applications.
Calculus in Physics
Calculus is a mathematical tool that is indispensable in physics for solving problems involving change. In this exercise, calculus allows us to determine the work done by a force as the object moves over time.
  • Work is calculated by integrating the force over the displacement it causes. This is shown by the integral \[ W = \int F(t) \cdot v(t) \, dt \]
  • The force function \( F(t) = -24.0 + 18.0t \) and velocity function \( v(t) = 3.0 - 8.0t + 3.0t^2 \) are multiplied before integration.
Evaluating this integral from \( t=0 \) to \( t=4.0 \, \text{s} \), we find the work done on the particle:\[ W = \int_{0}^{4} (-24.0 + 18.0t)(3.0 - 8.0t + 3.0t^2) \, dt = -528.0 \, \text{J} \]The result is negative, indicating that the force applied opposes the motion. Calculus not only aids in evaluating such integrals; it also provides a deeper understanding of how different physical quantities interrelate dynamically, a key aspect in advanced physics studies.

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Most popular questions from this chapter

A father racing his son has half the kinetic energy of the son, who has half the mass of the father. The father speeds up by \(1.0 \mathrm{~m} / \mathrm{s}\) and then has the same kinetic energy as the son. What are the original speeds of (a) the father and (b) the son?

In 1975 the roof of Montreal's Velodrome, with a weight of \(360 \mathrm{kN},\) was lifted by \(10 \mathrm{~cm}\) so that it could be centered. How much work was done on the roof by the forces making the lift? (b) In 1960 a Tampa, Florida, mother reportedly raised one end of a car that had fallen onto her son when a jack failed. If her panic lift effectively raised \(4000 \mathrm{~N}\) (about \(\frac{1}{4}\) of the car's weight) by \(5.0 \mathrm{~cm},\) how much work did her force do on the car?

A horse pulls a cart with a force of 40 lb at an angle of \(30^{\circ}\) above the horizontal and moves along at a speed of \(6.0 \mathrm{mi} / \mathrm{h}\). (a) How much work does the force do in \(10 \mathrm{~min} ?\) (b) What is the average power (in horsepower) of the force?

A force \(\quad \vec{F}=(3.00 \mathrm{~N}) \hat{\mathrm{i}}+(7.00 \mathrm{~N}) \hat{\mathrm{j}}+(7.00 \mathrm{~N}) \hat{\mathrm{k}}\) acts on a \(2.00 \mathrm{~kg}\) mobile object that moves from an initial position of \(\vec{d}_{i}=(3.00 \mathrm{~m}) \hat{\mathrm{i}}-(2.00 \mathrm{~m}) \hat{\mathrm{j}}+(5.00 \mathrm{~m}) \hat{\mathrm{k}}\) to a final position of \(\vec{d}_{f}=-(5.00 \mathrm{~m}) \hat{\mathrm{i}}+(4.00 \mathrm{~m}) \hat{\mathrm{j}}+(7.00 \mathrm{~m}) \hat{\mathrm{k}}\) in \(4.00 \mathrm{~s} .\) Find \((\mathrm{a})\) the work done on the object by the force in the 4.00 s interval, (b) the average power due to the force during that interval, and (c) the angle between vectors \(\vec{d}_{i}\) and \(\vec{d}_{f}\)

In the block-spring arrangement of Fig. \(7-10,\) the block's mass is \(4.00 \mathrm{~kg}\) and the spring constant is \(500 \mathrm{~N} / \mathrm{m} .\) The block is released from position \(x_{i}=0.300 \mathrm{~m} .\) What are \((\mathrm{a})\) the block's speed at \(x=0,\) (b) the work done by the spring when the block reaches \(x=0,\) (c) the instantaneous power due to the spring at the release point \(x_{i}\), (d) the instantaneous power at \(x=0,\) and \((\mathrm{e})\) the block's position when the power is maximum?

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