Integrate Acceleration to Find Time?

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Homework Help Overview

The problem involves a particle of mass m attracted to a fixed point with a force inversely proportional to its distance from that point. The task is to determine how long it takes for the particle, released from rest at a distance L, to reach the fixed point.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the need for integration to find time and explore various methods to express the motion of the particle. Some participants suggest deriving an equation for position as a function of time, while others delve into differential equations and integration techniques.

Discussion Status

There are multiple lines of reasoning being explored, including different integration techniques and interpretations of the constants involved. Some participants express uncertainty about the implications of a negative proportionality constant and its effect on the direction of force.

Contextual Notes

Participants note the complexity of the integrals involved and the potential for confusion regarding the setup of the problem, particularly concerning the sign of the proportionality constant k. There is also mention of constraints from class examples that typically assume positive constants.

Trapezoid
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This question is from my calculus assignment but I apologize if it belongs on the a physics board regardless.

Homework Statement



A particle of mass m is attracted towards a fixed point 0 with a force inversely proportional to its instantaneous distance from 0. If a particle is released from rest at a distance L from 0, how long will it take to reach 0?

2. The attempt at a solution
[tex]F = ma = \frac{k}{d}[/tex]
where d is the distance from 0 and k is a proportionality constant. Therefore, [tex]a = \frac{d^2x}{dt^2} = \frac{k}{md}[/tex]
I know that integration is required but I don't see how to use it to find time. Could somebody give me a tip as to how to proceed?

Thanks,
Trapezoid
 
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Well, imagine that the question asked you for an equation that gave the position of the particle as a function of time. E.g. [itex]s(t) = a_0 + a_1t + a_2t^2[/itex]. You know how to do this, right? Now, once you have the equation, just put the distance traveled on the LHS and solve for [itex]t[/itex].
 
Trapezoid said:
This question is from my calculus assignment but I apologize if it belongs on the a physics board regardless.

Homework Statement



A particle of mass m is attracted towards a fixed point 0 with a force inversely proportional to its instantaneous distance from 0. If a particle is released from rest at a distance L from 0, how long will it take to reach 0?

2. The attempt at a solution
[tex]F = ma = \frac{k}{d}[/tex]
where d is the distance from 0 and k is a proportionality constant. Therefore, [tex]a = \frac{d^2x}{dt^2} = \frac{k}{md}[/tex]
I know that integration is required but I don't see how to use it to find time. Could somebody give me a tip as to how to proceed?

Thanks,
Trapezoid
[tex]x\frac{d^2x}{dt^2} = \frac{k}{m}[/tex]
d is x. Is that what you were forgetting?
 
You say "d is the distance from 0 and k is a proportionality constant" but you don't say what "x" is! I think you mean x to be also the distance from 0 at time t so your differential equation is really
[tex]\frac{d^2x}{dt^2}-= \frac{k}{mx}[/tex]

You will have to solve the differential equation for x, then set it equal to 0 and solve for t.

Now, that is not easy to integrate directly but you can use a technique called "quadrature".
Let v= dx/dt so that [itex]d^2x/dt^2= dv/dt[/itex]. By the chain rule, [itex]dv/dt= (dv/dx)(dx/dt)= v dx/dt[/itex]. So your equation is
[tex]v\frac{dv}{dx}= \frac{k}{mx}[/tex]
a separable equation.

[tex]v dv= \frac{k}{m}\frac{dx}{x}[/tex]
Integrating,
[tex](1/2)v^2= \frac{k}{m}ln(|x|)+ C[/tex]
Since the object was released "distance L" (x= L) at rest (v= 0) we have
[tex](1/2)0^2= \frac{k}{m}ln(L)+ C[/tex]
so
[tex]C= -\frac{k}{m}ln(L)[/tex]
and the equation for v becomes
[tex]\frac{1}{2}v^2= \frac{k}{m}ln(x)- \frac{k}{m}ln(L)= \frac{k}{m}ln\left(\frac{x}{L}\right)[/tex]
(I am assuming that L is positive and as x changes from L to 0, it will be positive so we don't need the absolute value.)
[tex]v= \frac{dx}{dt}= \sqrt{\frac{2k}{m}ln\left(\frac{x}{L}\right)}[/tex]

Integrate that, solve for x as a function of t, set it equal to 0, and solve for t.
 
Thanks for all the help everybody. I'll take a closer look to see if I can't find the answer from here.
 
I thought it would just be
[tex]x\frac{d^2x}{dt^2} = \frac{k}{m}[/tex]
[tex]\int \int x dxdx = \frac{k}{m} \int \int dtdt[/tex]
[tex]\frac{x^3}{6}=\frac{k}{m}\frac{t^2}{2}+c[/tex]
[tex]x^3=3\frac{k}{m}t^2+c[/tex]
Here is a nice junction to find c (assuming x = 0 is at the point and x = L is the initial condition, L > 0):
[tex]L^3 = 0 + c \rightarrow c = L^3[/tex]
then
[tex]x^3=3\frac{k}{m}t^2+L^3[/tex]
[tex]x(t)=\left ( 3\frac{k}{m}t^2+L^3 \right )^{1/3}[/tex]

You then solve for the time for which x(t) = 0. Note, k must be < 0 for such a solution.
 
Thanks HallsofIvy and RoshanBBQ,

Unless I've misunderstood, the method outlined by HallsofIvy leaves me with the integral [itex]\int \frac{dx}{\sqrt{\ln(\frac{x}{L})}}[/itex] which I cannot even begin to solve. With regards to RoshanBBQ's solution, it seems odd to me that k would be negative since constants in examples done in class are always specified to be positive. That being said, a negative k would imply that the force acts in the negative direction, which seems consistent with the problem. Is my thinking here correct?

Trapezoid
 
Trapezoid said:
Thanks HallsofIvy and RoshanBBQ,

Unless I've misunderstood, the method outlined by HallsofIvy leaves me with the integral [itex]\int \frac{dx}{\sqrt{\ln(\frac{x}{L})}}[/itex] which I cannot even begin to solve. With regards to RoshanBBQ's solution, it seems odd to me that k would be negative since constants in examples done in class are always specified to be positive. That being said, a negative k would imply that the force acts in the negative direction, which seems consistent with the problem. Is my thinking here correct?

Trapezoid

It just depends on how you set up the problem.I'm not entirely comfortable with the answer I found, though. Consider when t -> infinity. You would expect x -> 0. My solution has x become the 3rd root of an increasingly negative number...
 
Last edited:
Hi all,

Sorry to bump but we got the solutions to the assignment so I thought I'd post some more guidance in case anybody else is having trouble with a similar question.

The method outlined by HallsofIvy is correct. Without giving too much away, to solve the last integral, substitute [itex]u = \frac{L}{x}[/itex] and use the gamma function.
 

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