/*! 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 71 The acceleration of a particle i... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

The acceleration of a particle is given by \(a_{x}(t)=\) \(-2.00 \mathrm{~m} / \mathrm{s}^{2}+\left(3.00 \mathrm{~m} / \mathrm{s}^{3}\right) t\) Find the initial velocity \(v_{0 x}\) such that the particle will have the same \(x\) coordinate at \(t=4.00 \mathrm{~s}\) as it had at t=0 . \text { (b) What will be the velocity at } t=4.00 \mathrm{~s} ?

Short Answer

Expert verified
The initial velocity (\(v_{0x}\)) is 0. The velocity at \(t = 4.00s\) is 4 m/s.

Step by step solution

01

Integration of Acceleration Function

Firstly, the acceleration function \(a_{x}(t)=-2.00 \mathrm{~m} / \mathrm{s}^{2}+\left(3.00 \mathrm{~m} / \mathrm{s}^{3}\right) t\) needs to be integrated with respect to time in order to obtain the velocity function. The integral of the function \(a_{x}(t)\) will give the equation: \[v_{x}(t) = -2.00t + (3.00/2)t^2 + C\]where C is the constant of integration which in this context represents the initial velocity \(v_{0 x}\).
02

Calculate Initial Velocity

To calculate the initial velocity, we need to set up the equation derived from the previous step such that the \(x\) coordinate of the particle is same at \(t=0\) and \(t=4.00 s\). That gives us the equation:\[-2.00t + \frac{3.00}{2}t^2=0\]On simplifying and solving the equation, we get \(t=0\) and \(t=4.00s\). So, our initial assumption was correct and we can use it in velocity equation to obtain the initial velocity.
03

Find Velocity at Certain Time Point

To find the velocity at certain time point, simply substitute the time in the equation obtained for velocity. We are interested in velocity at \(t=4.00 s\), substitute \(t = 4.00s\) in \(v_{x}(t) = -2.00t + (3.00/2)t^2 + C\). Solve the equation to obtain the velocity at \(t=4.00s\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

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

Integration of Acceleration
When we talk about the motion of a particle, its velocity and position at any time can be determined if the acceleration is known. The process of finding velocity from acceleration involves integration, a fundamental concept in calculus. Integration is essentially the reverse operation of differentiation and can be thought of as the 'summing up' of small pieces to find the whole.

For acceleration described by a function of time, such as the given exercise, integrating acceleration over time yields velocity. In this specific scenario, the function is a polynomial in time, making it straightforward to integrate. After integrating the given function, the result is an expression for velocity that includes a constant of integration, denoted by 'C'. This constant represents the initial velocity, which is yet to be determined based on the conditions specified in the exercise.

It is crucial to remember that integrating an acceleration function doesn't just give us speed—it gives us velocity, which is speed with a direction. In this case, our velocity function will tell us how fast the particle is moving and in what direction, along the x-axis, at any instant in time. For students looking to fully understand this process, practicing integration on various acceleration functions and confirming their results with the velocity-time relationship can be quite educational.
Initial Velocity Calculation
In motion problems like the one in our exercise, calculating the initial velocity is a key step in understanding the complete motion of the particle. Initial velocity is the velocity of the particle when time equals zero, also denoted as \( v_{0} \). In this exercise, the initial velocity is the 'C' from the integrated acceleration function.

To calculate the initial velocity, \( v_{0x} \), we apply the given boundary condition: the particle’s position at \( t = 4.00s \) should be the same as at \( t = 0s \). In essence, this implies the displacement of the particle over the 4-second period should be zero. Because velocity is the integral of acceleration, the displacement is the integral of velocity. Setting up the integral of the velocity function from \( t = 0s \) to \( t = 4.00s \) and solving for when the displacement is zero provides us with the value of \( v_{0x} \).

This calculation equips students with the skill to analyze motion scenarios where the initial conditions can be uniquely determined by later events. Essentially, it’s like 'working backwards' to find a missing piece of a puzzle: knowing the end situation helps us figure out how things started. For students, this concept proves useful when dealing with more complex physics problems as well as real-life situations where deducing unknown past conditions from present information is required.
Velocity-Time Relationship
Understanding the interplay between velocity and time is essential in solving motion problems. The velocity-time relationship is fundamental in kinematics, the branch of physics that deals with the motion of objects without considering the forces causing the motion. In our exercise, the velocity function \(v_{x}(t)\) describes how the velocity of the particle depends on time.

To find the velocity at any given time, one simply substitutes that time value into the velocity function. Doing so for \( t = 4.00s \) will yield the velocity at that moment. Furthermore, when we take the derivative of the velocity-time function, we get the acceleration, reinforcing the concept of derivatives and integrals being inverse operations.

This velocity-time relationship can be represented graphically, often resulting in a slope that indicates acceleration. For example, if the velocity-time graph is a straight line, the acceleration is constant, while a curved line would mean the acceleration is changing over time. By exploring various motion equations and their respective velocity-time graphs, students can develop an intuitive and practical understanding of how an object's motion is represented mathematically and visually. Such skills are not just academic; they are applicable in a range of fields from engineering to computer animation.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

You are standing at rest at a bus stop. A bus moving at a constant speed of \(5.00 \mathrm{~m} / \mathrm{s}\) passes you. When the rear of the bus is \(12.0 \mathrm{~m}\) past you, you realize that it is your bus, so you start to run toward it with a constant acceleration of \(0.960 \mathrm{~m} / \mathrm{s}^{2}\). How far would you have to run before you catch up with the rear of the bus, and how fast must you be running then? Would an average college student be physically able to accomplish this?

You are on the roof of the physics building, \(46.0 \mathrm{~m}\) above the ground (Fig. \(\mathbf{P 2 . 7 0}\) ). Your physics professor, who is \(1.80 \mathrm{~m}\) tall, is walking alongside the building at a constant speed of \(1.20 \mathrm{~m} / \mathrm{s}\). If you wish to drop an egg on your professor's head, where should the professor be when you release the egg? Assume that the egg is in free fall.

The acceleration of a bus is given by \(a_{x}(t)=\alpha t,\) where \(\alpha=1.2 \mathrm{~m} / \mathrm{s}^{3} .\) (a) If the bus's velocity at time \(t=1.0 \mathrm{~s}\) is \(5.0 \mathrm{~m} / \mathrm{s}\) what is its velocity at time \(t=2.0 \mathrm{~s} ?\) (b) If the bus's position at time \(t=1.0 \mathrm{~s}\) is \(6.0 \mathrm{~m},\) what is its position at time \(t=2.0 \mathrm{~s} ?(\mathrm{c})\) Sketch \(a_{y}-t\) \(v_{y}-t,\) and \(x-t\) graphs for the motion.

A flowerpot falls off a windowsill and passes the window of the story below. Ignore air resistance. It takes the pot \(0.380 \mathrm{~s}\) to pass from the top to the bottom of this window, which is \(1.90 \mathrm{~m}\) high. How far is the top of the window below the windowsill from which the flowerpot fell?

A 15 kg rock is dropped from rest on the earth and reaches the ground in \(1.75 \mathrm{~s}\). When it is dropped from the same height on Saturn's satellite Enceladus, the rock reaches the ground in \(18.6 \mathrm{~s}\). What is the acceleration due to gravity on Enceladus?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.