Unicycle straight line motion/time dependent acceleration Problem

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Homework Help Overview

The problem involves a unicycle moving in a straight line along the x-axis, starting from an initial position D with a time-dependent acceleration that increases over time. The cyclist initially accelerates backwards, and the acceleration is defined as ax(t) = -2a + 6dt, where a and d are constants. Participants are exploring how to derive the velocity and position functions based on this acceleration.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss integrating the acceleration to find velocity and then integrating velocity to find position. There are questions about the appropriateness of setting the integral of velocity equal to the initial position D and concerns about the initial conditions provided, particularly regarding the initial velocity and position.

Discussion Status

Some participants have offered guidance on the integration process and the need to consider initial conditions. There is an ongoing exploration of how to correctly apply the definitions of velocity and position in relation to the given acceleration function. Multiple interpretations of the initial conditions and the integration process are being discussed.

Contextual Notes

There is uncertainty regarding the initial velocity of the unicycle, as it is not explicitly defined in the problem statement. Participants are also questioning the assumptions made about the initial position and the implications of the backward acceleration.

chiamocha
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Homework Statement


Here is the problem I have been trying to figure out for the past hour.
A unicycle is traveling in a straight line, along the x axis. At t=0, the unicycle is at x = D. Initially the cyclist is accelerating backwards, in the minus x direction. Over time, the acceleration increases. The time-dependent acceleration is ax(t) = -2a + 6dt The quantities a and d are constants.

Homework Equations



All I know is the equations of constant acceleration vx(t) = v0x + ax(t)

position x(t) = x0 + v0xt + (1/2)axt2

vx2= v02x+2ax(x-x0)

The Attempt at a Solution



What I did to attempt this equation (sorry I am not very good at coding this properly so I will just write it out) is to integrate the equation for time dependent acceleration that was given to get equations for velocity [v = v(initial) +(from 0 to t) ∫ (a) dt'] and then for position[ x = x(initial) + (from 0 to t) ∫(v)dt']. And then since it is given that at time t=0 the object is at position D I plugged that in and since I assume (I am not sure I am correct in this assumption) that the initial position of the object is 0, I set the integral of v from 0 to t equal to D. And I am not sure where to go from there. And I am not sure how to account for the backwards acceleration in the minus x direction, and then change when over time the acceleration increases.
 
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chiamocha said:
I set the integral of v from 0 to t equal to D.
That's a strange thing to do.
X(0)=D. X(t)=D+integral of v from 0 to t.
Please post what you get for those integrals.
 
Hmmm... not sure what you're getting at.

If your looking for the position function, integrate it, plug in your initial conditions for your velocity (I don't recall you giving a magnitude, just a direction? ) then integrate again and use your initial conditions for position to solve for your constant if integration again.

From what you gave, I'm not sure that integrating from 0 to t should give you zero. Definitely not on your velocity (unless you're trying to solve for when it DOES equal 0), which is not t-0 as you stated that the cyclist was moving backwards.

Also I believe you said at t-0 the position was D, also not necessarily 0. If it was zero, likely your prof would use 0 and not D. Can't really do a whole lot other than limiting your first constant of integration with the given conditions, and thus limiting your second one (or getting it in terms of the first)

But again... you really didn't ask a question.
 
Also, these numbers look really cooked, just pointing that out.
 
Sorry, the question is to find the velocity and position of the unicycle as a function of time.
 
If you know the position of the unicycle as a function of time, what is the velocity of said unicycle as a function of time? Hint: there are no integrals involved. Look at the definition of velocity.
 
Isn't it the derivative of the position?
 
Chiamocha, in the OP you mentioned integrating acceleration to get velocity and integrating that to get position. That was all correct. Please post what you got for those integrals and where you went from there.
 
The problem statement defines acceleration versus time:

[tex]a_x(t) = (-2a \ + \ 6)\ \Delta t[/tex]
Integrate this twice adding a constant of integration (v0 for the first integration, x0 for the second integration) for each integration step. The problem states that the unicycle is traveling in a straight line, but doesn't define the initial velocity v0. It does define the initial postion x0 as D.
 
Last edited:
  • #10
chiamocha said:
Isn't it the derivative of the position?

Yes, it is.

Given the information in the OP, write the position of the unicycle as a function of time. Use the acceleration (as a function of time) you were given.
 

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