A rather interesting type of coupled oscillator.

dHannibal
Messages
10
Reaction score
0

Homework Statement


The problem can be found here. http://wopho.org/dl.php?id=17&dirfile=selection-problem/helical_rope.pdf" I am attempting to solve part 3.

Homework Equations


The Lagrangian of the system is: L= \frac{m\dot{x}^2}{2}+\frac{mr^2\dot{\theta}^2}{2}-k \left( x^2+(r\theta)^2-2x_0\sqrt{x^2+(r\theta)^2} \right)
Also,the equations of motion are:
\ddot{x}=\frac{2k}{m} \left(\frac{x_0}{\sqrt{x^2+(r\theta)^2}} -1 \right)x
\ddot{\theta}=\frac{2k}{m} \left(\frac{x_0}{\sqrt{x^2+(r\theta)^2}} -1 \right) \theta

The Attempt at a Solution


I need to solve the equations of motion for x(t) and \theta (t). First I tried assuming r \theta << x but it leads to equations of motion of the form

<br /> \ddot{x}=\frac{2k}{m} \left(\frac{x_0}{x+\frac{(r \theta)^2}{2x}} -1 \right)x<br />
which is not particulaly useful. Pointing out that \frac{\ddot{x}}{x} = \frac{\ddot{\theta}}{\theta} I tried assuming solutions of the form x= Ae^{(iwt + \phi)} and \theta= Be^{(iwt + \phi)} but I was again unsuccessful. I was stuck at this point.
Thank you.
 
Last edited by a moderator:
Physics news on Phys.org
hi dHannibal! :smile:

try putting x'' = v dv/dx and integrating :wink:
 
Hi tinytim,
but how do i get rid of \theta's in the square root when integrating?
 
Hello everyone, I’m considering a point charge q that oscillates harmonically about the origin along the z-axis, e.g. $$z_{q}(t)= A\sin(wt)$$ In a strongly simplified / quasi-instantaneous approximation I ignore retardation and take the electric field at the position ##r=(x,y,z)## simply to be the “Coulomb field at the charge’s instantaneous position”: $$E(r,t)=\frac{q}{4\pi\varepsilon_{0}}\frac{r-r_{q}(t)}{||r-r_{q}(t)||^{3}}$$ with $$r_{q}(t)=(0,0,z_{q}(t))$$ (I’m aware this isn’t...
Hi, I had an exam and I completely messed up a problem. Especially one part which was necessary for the rest of the problem. Basically, I have a wormhole metric: $$(ds)^2 = -(dt)^2 + (dr)^2 + (r^2 + b^2)( (d\theta)^2 + sin^2 \theta (d\phi)^2 )$$ Where ##b=1## with an orbit only in the equatorial plane. We also know from the question that the orbit must satisfy this relationship: $$\varepsilon = \frac{1}{2} (\frac{dr}{d\tau})^2 + V_{eff}(r)$$ Ultimately, I was tasked to find the initial...
Back
Top