Solve Integration Problem: a=(-2v)m/s^2, v=20m/s, s=0, t=0

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Homework Help Overview

The problem involves a particle moving along a straight line with an acceleration defined as a=(-2v) m/s², where the initial conditions specify that the velocity is 20 m/s when the position and time are both zero. The objective is to determine the particle's velocity as a function of position and the distance it moves before stopping.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss various methods to express velocity as a function of position, including integration techniques and the use of kinematic equations. Some participants express confusion regarding the application of certain equations due to the non-constant nature of acceleration.

Discussion Status

The discussion is ongoing, with participants exploring different approaches to the problem. Some guidance has been offered regarding the exponential decay model, while others are questioning the validity of using specific kinematic equations in this context.

Contextual Notes

There is a noted concern about the implications of the acceleration being dependent on velocity, which complicates the use of standard kinematic equations. Participants are also grappling with the integration process and the interpretation of results.

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Homework Statement


A particle is moving along a straight line such that its acceleration is defined as a=(-2v)m/s^2.
If v=20 m/s when s=0 and t=0, determine the particle's velocity as a function of position and the distance the particle moves before it stops.

The answer is v=(20-2s)m/s ; s=10m

Homework Equations


a=\frac{dv}{dt}

a=\frac{dv}{ds}*\frac{ds}{dt} which becomes...

ads=vdv


The Attempt at a Solution


given: a=(-2v) m/s
v=20 m/s
t=0
s=0
solution attempt:

a=\frac{dv}{dt}

-2v*dt=dv

dt=-\frac{dv}{-2v}

\int dt = \int\frac{dv}{-2v}


That's as far as I can get. If I evaluate the left hand side from 0 to t, I get t.
If I evaluate the left, I get messed up. If I pull out the -\frac{1}{2},
I am left with \frac{1}{v}. I think the integral of that is ln v.
I need some direction on this one please.
 
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This problem is about damping. You have an object moving against a force proportional to its velocity, but directed opposite to it: F = -bv. The solution is an exponentially decaying one. This is what you got!

-2t = ln v + C ===> v = v_0 e^{-2t}
 
I need velocity as a function of position.
How about this?
Can I use the equation v^2=v0^2+2a(\Delta s)

then I get v= \sqrt{200-4s}

which would give me v=20-2s which is the answer in the book.

My concern here is the "s" and the value for "a" is -2v not just -2.
How do I deal with this under the square root sign?
 
You can't use that equation because that only applies when one has constant acceleration.

(1) v= v_0 e^{-t/\tau}

(2) x = v_0\int_0^t e^{-\frac{t'}{\tau}} dt' = v_0\tau(1 - e^{-\frac{t}{\tau}})

Solve for time in second equation (2). Then you can substitute that into (1). It will get hairy, but you should get an answer like the one in your book. Remember: e^{\ln{x}} = x.
 

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