Can you solve the pendulum with obstacles? Find the equation of movement!

  • Thread starter Thread starter carllacan
  • Start date Start date
  • Tags Tags
    Pendulum
carllacan
Messages
272
Reaction score
3

Homework Statement


We have a pendulum, with length 4a. It is placed between two rounded obstacles (see image) described by x = a(θ+sinθ) and z = a(-3-cosθ), which disturb its natural movement. Find the equation of movement.
https://www.dropbox.com/s/q1y4gzmnv0mm9c0/2014-01-27 20.19.03.jpg

Homework Equations


x = a(θ+sinθ) and z = a(-3-cosθ) are the parametrized coordinates of the obstacles


The Attempt at a Solution


I have no idea where to start.
 
Physics news on Phys.org
Okay, I've just had an idea for this, but I would appreciate if you gave me any opinion before I try to apply it.

I think I could treat the pendulum as a regular one, with the twist that its lentgh changues over time, from L to L minus the portion of the obstacles the rope is incontact with. Does that make any sense?
 
I can note that the obstacle is a cycloid.

This might help.

http://www.17centurymaths.com/contents/huygens/horologiumpart1.pdf
 
Not much, but thanky you.

I found an expression for the length of the rope not touching the obstacles, but I don't know what else to do.

Do you think the parameter θ is the polar coordinate of the mass? This would make things infinitely easier.
 
No, the introduction of theta is a parametrisation as you say. Basically the angle over which the circle to describe the obstacle has rotated. Work towards the angle between the tangent to the obstacle and the vertical.

And read up on the cycloid (what you found is OK, but it's a little verbose. In the years since 1673 shorter exposes were put on the net...)
 
##|\Psi|^2=\frac{1}{\sqrt{\pi b^2}}\exp(\frac{-(x-x_0)^2}{b^2}).## ##\braket{x}=\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dx\,x\exp(-\frac{(x-x_0)^2}{b^2}).## ##y=x-x_0 \quad x=y+x_0 \quad dy=dx.## The boundaries remain infinite, I believe. ##\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dy(y+x_0)\exp(\frac{-y^2}{b^2}).## ##\frac{2}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,y\exp(\frac{-y^2}{b^2})+\frac{2x_0}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,\exp(-\frac{y^2}{b^2}).## I then resolved the two...
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