Period of Anharmonic Oscillator

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Homework Statement



Hi,

For a certain oscillator the net force on a body, with mass m, is given by F=-cx^3.

One quarter of a period is the time taken for the body to move from x=0 to x=A (where A is the amplitude of the oscillation). Calculate this time and hence the period.

Homework Equations



[tex]U(x)=(cx^4)/4[/tex], where U(x) represents the potential energy of the body.


The Attempt at a Solution



In order to solve this I used a homogeneity of units argument as follows,

Units of time are [tex](s)[/tex]

Units of potential energy are [tex](kg*m^2)/(s^2)[/tex]

In order to get from the potential energy units to the time units,

[tex](s)=\sqrt{((kg*m^2)/(s^2))}[/tex]

in terms of the above equations this is,

[tex]\sqrt{(m*x^2/U(x))}[/tex]=[tex]\sqrt{((4*m*x^2)/(c*x^4))}[/tex]

let x=A and the equation =T/4,

[tex]T/4=\sqrt{((4*m)/(cA^2))}[/tex]

hence, [tex]T=4*\sqrt{((4*m)/(cA^2))}[/tex]

However this is incorrect, my answer is wrong by a multiplicative factor. Please could someone show me where I have gone wrong?
 
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You can not use dimensional analysis to find multiplicative factors.

There is no closed form analytical solution to this question (?)

Use conservation of energy ## \dfrac{m(x')^2}{2} + U(x) = U(A) ## where ##m## is the mass of a weight attached to the oscillator. With some algebra, you should end up with this ## \dfrac{d x}{ dt } =\sqrt{ \dfrac{c(A^4 - x^4) }{ 2m }} ## which is a separable differential equation. Integrate t from 0 to T/4 and x from 0 to A.
 
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Well the ODE as a function of time doesn't have closed form solution indeed. Instead the ODE as a function of x (and velocity v as unknown function) has a closed form solution $$m\frac{dv}{dt}=-cx^3\Rightarrow m\frac{dv}{dx}\frac{dx}{dt}=-cx^3\Rightarrow m\frac{dv}{dx}v=-cx^3$$
 
Nvm what I said in post #3, doesn't help us find the period, seems one way to approximately solve the ode of post #2 is to find a Taylor series approximation of the integral $$\frac{T}{4}=\sqrt{2m}\int_0^A \frac{dx}{\sqrt{c(A^4-x^4)}}$$. Wolfram gives the first two terms of this approximation as $$\frac{x^4}{c^{1/2}A^2}+\frac{x^6}{10c^{3/2}A^6}$$
 
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Delta2 said:
Taylor series approximation of the integral

Don't you mean "Tayloer series of the integrand"?
The integral is not a function of x...
 
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drmalawi said:
Don't you mean "Tayloer series of the integrand"?
The integral is not a function of x...
Yes well, I mean the respective indefinite integral.
 
and a Taylor series always have a point which you expand around, I guess you took x=0.
 
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Delta2 said:
here is what I get from wolfram, judge for yourself

I am not questioning whether it is correct or not, I am just nitpicking about nomenclature ;)
 
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Since this is a very old thread, I think it would OK to continue on from @drmalawi 's setup in post #2 and finish it:

##T = \large \frac{4}{A} \sqrt{\frac{m}{2c}} \int_0^1 \frac{du}{\sqrt{1-u^4}}##

Mathematica expresses the value of the integral in terms of the gamma function:

##\large \int_0^1 \frac{du}{\sqrt{1-u^4}} = \sqrt \pi \frac{\Gamma(5/4)}{\Gamma(3/4)}## ## \approx 1.311##

Then ##T \approx 3.708 \large \frac{\sqrt{m/c}}{A}##
 
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Yeah I was hesitaded not to give away too much.

One can also integrate numerically from 0 to 1-ε where ε is a small positive number

Or, just plug it into wolfram alpha :oldsmile:
1657206972319.png
 
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