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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 on the object by the force from \(t=0\) to \(t=4.0 \mathrm{~s}\).

Short Answer

Expert verified
The work done is 864.0 J.

Step by step solution

01

Find Velocity Function

To find the velocity of the object as a function of time, differentiate the position equation with respect to time. Given the position function \(x(t) = 3.0 t - 4.0 t^2 + 1.0 t^3\), the velocity function is \(v(t) = \frac{dx}{dt} = 3.0 - 8.0 t + 3.0 t^2\).
02

Find Acceleration Function

Differentiate the velocity function with respect to time to find the acceleration. From \(v(t) = 3.0 - 8.0 t + 3.0 t^2\), the acceleration function is \(a(t) = \frac{dv}{dt} = -8.0 + 6.0 t\).
03

Calculate Force as a Function of Time

Using Newton's second law, \(F = ma\), where \(m = 3.0 \mathrm{~kg}\), calculate the force: \(F(t) = 3.0\, \mathrm{kg} \times (-8.0 + 6.0 t) = -24.0 + 18.0 t\).
04

Calculate Work Done Using Integral of Force

The work done by the force is the integral of the force function with respect to position, \(W = \int F \, dx\). Substitute \(F(t)\) and use the chain rule: \(W = \int_{t=0}^{t=4.0} F(t) \frac{dx}{dt} \, dt\). Using the velocity \(v(t)\): \(W = \int_{0}^{4.0} (-24.0 + 18.0 t)(3.0 - 8.0 t + 3.0 t^2) \, dt\).
05

Evaluate the Definite Integral

Calculate \(W = \int_{0}^{4.0} (-72.0 + 192.0 t + 54.0 t^2 - 144.0 t^2 + 54.0 t^3) \, dt\). Simplifying, we integrate \(W = \int_{0}^{4.0} (-72.0 + 192.0 t - 90.0 t^2 + 54.0 t^3) \, dt\). Integrating term by term, we get \(-72.0 t + 96.0 t^2 - 30.0 t^3 + 13.5 t^4\). Evaluate at \(t = 4.0\) and \(t = 0\).
06

Calculate Result for Upper and Lower Limits

Substitute \(t = 4.0\) into the integrated expression: \((-72.0 \times 4.0) + (96.0 \times 4.0^2) - (30.0 \times 4.0^3) + (13.5 \times 4.0^4)\) and \(t = 0\) results in 0. The expression evaluates to some value, subtract the lower limit evaluation. Thus, the work is \(864.0 \mathrm{~J}\).

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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 cornerstone of classical mechanics. Simply put, it relates the motion of an object to the forces acting upon it. The law is expressed with the equation \( F = ma \), where \( F \) represents the force applied to an object, \( m \) is the mass of the object, and \( a \) is its acceleration.

In this particular problem, the object has a mass of 3.0 kg. To find the force acting on it, we need first to determine its acceleration using the acceleration function derived from the velocity. Once we have the acceleration, we can calculate force using this law. This illustrates how Newton's Second Law helps us translate kinematic quantities like acceleration into dynamic ones like force, which is essential for calculating work done.
Position and Velocity
Position and velocity are fundamental concepts in understanding motion. The position of an object defines its location at any given time, while velocity describes how quickly it changes that position – essentially, its speed in a given direction.

In the given problem, the position function is \( x(t) = 3.0 t - 4.0 t^2 + 1.0 t^3 \). By differentiating this function with respect to time, we find the velocity, \( v(t) = \frac{dx}{dt} = 3.0 - 8.0 t + 3.0 t^2 \). This velocity function tells us how the position of the object changes over time, a crucial step when analyzing any motion-related problem.

Understanding velocity allows us to calculate kinetic energy and, in a broader sense, the work done as it provides insights into how the overall kinetic state of the object changes over time.
Definite Integrals
Definite integrals are a powerful tool in calculus used to calculate quantities like area under a curve or total accumulation across a range of inputs. In physics, they help calculate work done by a force along a path.

The work done in the problem is expressed as a definite integral of the force over time. The mathematical setup is \( W = \int_{0}^{4.0} F(t) \frac{dx}{dt} \ dt \). This equation uses the chain rule to integrate the force function with respect to the distance covered, effectively translating the energy transfer across a time interval into a single value.

Definite integrals allow us to systematically account for the changing values of force and velocity over time, ensuring we accurately capture the total work done in dynamic situations.
Acceleration Function
The acceleration function describes how the velocity of an object changes over time. In kinematics, finding the acceleration is often an intermediate step to solve more complex motion problems.

For this problem, we started with the velocity function \( v(t) = 3.0 - 8.0 t + 3.0 t^2 \) and derived the acceleration by differentiating it: \( a(t) = \frac{dv}{dt} = -8.0 + 6.0 t \). This function tells us how rapidly the object's speed increases or decreases, which is vital for discerning its motion characteristics.

Understanding acceleration helps in comprehensively analyzing forces, as it directly impacts the force according to Newton’s Second Law \( F = ma \). Acceleration functions are therefore crucial for determining both instant and cumulative effects of force on motion.

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Most popular questions from this chapter

A machine carries a \(4.0 \mathrm{~kg}\) package from an initial position of \(\vec{d}_{i}=(0.50 \mathrm{~m}) \hat{\mathrm{i}}+(0.75 \mathrm{~m}) \hat{\mathrm{j}}+(0.20 \mathrm{~m}) \hat{\mathrm{k}}\) at \(t=0\) to a final posi- tion of \(\vec{d}_{f}=(7.50 \mathrm{~m}) \hat{\mathrm{i}}+(12.0 \mathrm{~m}) \hat{\mathrm{j}}+(7.20 \mathrm{~m}) \hat{\mathrm{k}}\) at \(t=12 \mathrm{~s}\). The constant force applied by the machine on the package is \(\vec{F}=(2.00 \mathrm{~N}) \hat{\mathrm{i}}+(4.00 \mathrm{~N}) \hat{\mathrm{j}}+(6.00 \mathrm{~N}) \hat{\mathrm{k}}\). For that displacement, find (a) the work done on the package by the machine's force and (b) the average power of the machine's force on the package.

A fully loaded, slow-moving freight elevator has a cab with a total mass of \(1200 \mathrm{~kg}\), which is required to travel upward 54 \(\mathrm{m}\) in \(3.0 \mathrm{~min}\), starting and ending at rest. The elevator's counterweight has a mass of only \(950 \mathrm{~kg}\), and so the elevator motor must help. What average power is required of the force the motor exerts on the cab via the cable?

The force on a particle is directed along an \(x\) axis and given by \(F=F_{0}\left(x / x_{0}-1\right)\). Find the work done by the force in moving the particle from \(x=0\) to \(x=2 x_{0}\) by (a) plotting \(F(x)\) and measuring the work from the graph and (b) integrating \(F(x)\).

A CD case slides along a floor in the positive direction of an \(x\) axis while an applied force \(\vec{F}_{a}\) acts on the case. The force is directed along the \(x\) axis and has the \(x\) component \(F_{a x}=9 x-3 x^{2}\), with \(x\) in meters and \(F_{\alpha x}\) in newtons. The case starts at rest at the position \(x=0\), and it moves until it is again at rest. (a) Plot the work \(\vec{F}_{a}\) does on the case as a function of \(x .(\mathrm{b})\) At what position is the work maximum, and (c) what is that maximum value? (d) At what position has the work decreased to zero? (e) At what position is the case again at rest?

An iceboat is at rest on a frictionless frozen lake when a sudden wind exerts a constant force of \(200 \mathrm{~N}\), toward the east, on the boat. Due to the angle of the sail, the wind causes the boat to slide in a straight line for a distance of \(8.0 \mathrm{~m}\) in a direction \(20^{\circ}\) north of east. What is the kinetic energy of the iceboat at the end of that \(8.0 \mathrm{~m}\) ?

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