How do I solve this FODE for the particle's velocity?

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The discussion centers on solving a first-order differential equation (FODE) related to a particle's motion along the positive x-axis, where its acceleration is proportional to the negative inverse cube of its displacement. The initial conditions specify that the particle starts at rest when x=1. Participants clarify the correct formulation of the acceleration equation and the integration process, emphasizing the importance of proper handling of derivatives and signs. The conversation highlights the confusion around integrating to find the time taken for the particle to reach x=1/4, with one participant noting the challenge of obtaining a real solution. Ultimately, the discussion underscores the complexities of mechanics problems and the need for careful integration techniques.
mr bob
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Hey.
I've been doing more mechanics recently - further kinematics in M3. I've come across another question I'm confused by.

A particle moves on the positive x-axis. When its displacement from O is x meters, is acceleration is of magnitude x^-3 m/s^2 and directed towards O. Given that initially, when t=0, the particle is at rest with x=1, find the time the particle takes to reach x=1/4.

First i integrate with respect to x to find:

V^2 = x^-2 + C where C = -1
v^2 = x^-2 -1

V = x^-1 - 1

Now i integrate again to find velocity as (dx/dt):

dx/dt = x^-1 - 1

Which is a FODE, however i can't solve it.

Thank you,
Bob
 
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mr bob said:
Hey.
I've been doing more mechanics recently - further kinematics in M3. I've come across another question I'm confused by.

A particle moves on the positive x-axis. When its displacement from O is x meters, is acceleration is of magnitude x^-3 m/s^2 and directed towards O. Given that initially, when t=0, the particle is at rest with x=1, find the time the particle takes to reach x=1/4.

First i integrate with respect to x to find:

V^2 = x^-2 + C where C = -1
v^2 = x^-2 -1

V = x^-1 - 1

Now i integrate again to find velocity as (dx/dt):

dx/dt = x^-1 - 1

Which is a FODE, however i can't solve it.

Thank you,
Bob
That isn't quite right. The problem says the accleration is given by x^{-3} towards the origin, so
\frac{d^2x}{dt^2}=-x^{-3}
Multiplying by x3dt2 gives:
x^3d^2x =-dt^2
Now integrate twice.
 
LeonhardEuler said:
That isn't quite right. The problem says the accleration is given by x^{-3} towards the origin, so
\frac{d^2x}{dt^2}=-x^{-3}
Multiplying by x3dt2 gives:
x^3d^2x =-dt^2
Now integrate twice.

No, you can't treat a second derivative like that, "differentials", dx and dy separately, are only defined for the first derivative: we could separate \frac{dv}{dt}= x^{-3} into cv= x^{-3}dt but then you can't integrate x-3 with respect to t.

You can do this by "quadrature" (looks to me like this is what mr bob did)- since t does not appear explicitly, let v= \frac{dx}{dt}. Then \frac{d^2x}{dt^2}= \frac{dv}{dt} and, by the chain rule, \frac{dv}{dt}= \frac{dv}{dx}\frac{dx}{dt}= v\frac{dv}{dx}

That makes the equation v\frac{dv}{dx}= x^{-3} which we can separate: v dv= x^{-3}dx and, integrating, \frac{1}{2}v^2= -\frac{1}{2}x^{-2}+ C or v^2= -x^{-2}+ C almost what mr bob said (he is missing the "-" as x increases the particle slows). Taking x= 1, v= 0 when t= 0, we get 0= -1+ C so C= 1 and v^2= -x^{-2}+ C again almost as mr bob said.

However, (are you listening mr bob?) taking the square root does NOT give v= 1- x-1! \sqrt{a^2+ b^2} \ne a+ b!

Instead v= \frac{dx}{dt}= \sqrt{1- x^{-1}}= \sqrt{\frac{x^2- 1}{x^2}}= \frac{\sqrt{x^2-1}}{x}. That separates as \frac{xdx}{x^2- 1}= dt which should be easy to integrate.
 
Last edited by a moderator:
LeonhardEuler said:
That isn't quite right. The problem says the accleration is given by x^{-3} towards the origin, so
\frac{d^2x}{dt^2}=-x^{-3}
Multiplying by x3dt2 gives:
x^3d^2x =-dt^2
Now integrate twice.

No, you can't treat a second derivative like that: we could separate \frac{dv}{dt}= x^{-3} into cv= x^{-3}dt but then you can't integrat x-3 with respect to t.

You can do this by "quadrature"- since t does not appear explicitly, let v= \frac{dx}{dt}. Then \frac{d^2x}{dt^2}= \frac{dv}{dt} and, by the chain rule, \frac{dv}{dt}= \frac{dv}{dx}\frac{dx}{dt}= v\frac{dv}{dx}<br /> <br /> That makes the equation v\frac{dv}{dx}= x^{-3} which we can separate: v dv= x^{-3}dx and, integrating, \frac{1}{2}v^2= -\frac{1}{2}x^{-2}+ C or v^2= -x^{-2}+ C <b>almost</b> what mr bob said (he is missing the &quot;-&quot; as x increases the particle slows). Taking x= 1, v= 0 when t= 0, we get 0= -1+ C so C= 1 and v^2= 1 -x^{-2} again almost as mr bob said.<br /> <br /> <b>However, (are you listening mr bob?) taking the square root does NOT give v= 1- x<sup>-1</sup>! \sqrt{a^2+ b^2} \ne a+ b!<br /> <br /> Instead v= \frac{dx}{dt}= \sqrt{1- x^{-1}}= \sqrt{\frac{x^2- 1}{x^2}}= \frac{\sqrt{x^2-1}}{x}. That separates as \frac{xdx}{\sqrt{x^2- 1}}= dt which should be easy to integrate.</b>
 
Thank you very much. I really appreciate the help. Some of these mechanics questions are a bit hard. Need to improve my integration skills abit.
 
I've integrated to t = \sqrt(x^2 - 1) but can't get the answer correct. Find t when x = 1/4, which gives the root of a negative number, not real. But the book's answer is \sqrt(15) which i notice is \sqrt(x^-2 - 1). How is this possible?

Thank you,
Bob
 
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The acceleration is of magnitude x-3 and directed toward O!

I missed that myself: the differential equation is not
\frac{dv}{dt}= x^{-3}
it is
\frac{dv}{dt}= -x^{-3}
!

That's why you had what I (mistakenly) thought was a sign error!
 
Last edited by a moderator:
When i integrate i get t = 1 - (1 - x^2).
I'm getting confused by this now, i think my brain's just died, ah well. Sorry for keeping asking questions, i can see how annoying it would be if the answer was so obvious yet i don't grasp it.

Thanks,
Bob
 

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