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- 1 What is a double pendulum?
- 2 No analytical solution ?
- 3 chaos
- 4 the period of a double pendulum with a small angle
- 5 Human Double Pendulum?
- 6 Animated Picture
- 7 Chaotic motion: time elapsed until the double pendulum "flips over"
- 8 Why we use the inertia about the centre of mass, not about the end
- 9 removed horology definition
- 10 Error in Lagrangian
- 11 Article citation
What is a double pendulum?
This article states that "a double pendulum is a pendulum with another pendulum attached to its end", with link to pendulum. Looking at "pendulum", I see that it consists of two masses connected by two massless rods. Here, however, pendulum consists of two massive rods. I think, by double pendulum, people usually think about the case with two massless rods and two masses, see most of the references given at the end of the article. Understanding that this case might also be called double pendulum, not even mentioning the more usual meaning is not satisfactory.
Cumi 13:41, 24 March 2006 (UTC)
I agree with the previous poster. The usual "simple" double pendulum is masses at the ends of massless rods, and the figure suggests this. However the derivation here is for something different, i.e. a "compound" double pendulum consisting of rods with mass but with no masses at their ends. It is quite odd. —Preceding unsigned comment added by 22.214.171.124 (talk) 00:46, 3 November 2007 (UTC)
I suggest the following terms :
- "punctual pendulum" for a pendulum made of a massive point and a massless rod ;
- "solid pendulum" for a pendulum made of a massive rod.
- On WP we are obliged to use standard terminology, and not invent our own. However there are other ways (parenthetical explanations), to avoid forcing the reader to follow links for the definition of the terms. --catslash (talk) 15:39, 9 March 2013 (UTC)
No analytical solution ?
I wonder if there is really no known analytical solution to the double punctual pendulum move.
- Is there an exact analytical solution ?
- If no, is there an approximate analytical solution ?
- If no, what are the precise obstacles to overcome to find an analytical solution ?
- No analytical solution is not quite what it says.
- The trivial solution θ1(t) = θ2(t) = 0 is exact though somewhat dull.
- More interestingly, the double pendulum displays periodic behaviour for certain initial conditions, and any particular instance of this could surely be represented to arbitrary accuracy with a fourier series.
- The chaotic behaviour for other initial conditions makes a general analytic solution seem unlikely (though I don't know whether this proves anything).
- The article would benefit greatly from some proof of chaotic behaviour and/or non-integrability if such exist. Perhaps you could read-up on this topic and fix the article? --catslash (talk) 14:58, 9 March 2013 (UTC)
What units are used for angles < θ1, θ2; CHAOTIC MOTION, Double pendulum >
in the x-y graph where: x axis: angle θ1 is plotted for -3 to +3 (left to right) y axis: angle θ2 is plotted for -3 to +3 (top to bottom)
the graph is described as: < Graph of the time for the pendulum to flip over as a < function of initial conditions
thanks for the information!
veritus 16:15, 24 February 2007 (UTC)
the period of a double pendulum with a small angle
Ok what is the period of a double pendulum with a small angle?
Human Double Pendulum?
Hello, As a dance and movement experiment, I am interested in constructing a human double pendulum - that is, with humans as bobs or masses. I want to hang the first person in a climbing harness by a rope suspended from a truss. Then I want to hang the second person from the first person. Any suggestions?
Scroll down the page a bit. This an animation of a compound double pendulum (because it's an integration of the equations given in the article). I should think the motion of a simple double pendulum would look pretty similar though. --catslash (talk) 09:50, 6 August 2008 (UTC)
Chaotic motion: time elapsed until the double pendulum "flips over"
1) I assume that "to flip over" means to have the bar l2 vercital (θ2 = π).
- Someone should verify the first assumption and clarify in the article. It is not apparent. LokiClock (talk) 17:24, 22 December 2009 (UTC)
3) I don't understand how this plot was produced. What is the source of this plot? As explained the pendulum is a chaotic dynamical system. From some simulations I did, if one perturbs the initial condition by some small delta, the trajectory diverges quickly. In non-dimensional units, at t=10, the perturbation grows to about 10 delta (to simplify). This means that for example if delta = 10^-12, around time t=120, this delta has grown to about 1 and the two trajectories become completely different. The exact numbers are not important. The point is that it is very difficult to integrate exactly the equations of motion beyond t=100 or 200. One needs to use extended precision arithmetic. Even then, here there is a mention of 10,000. I did not attempt that calculation but that seems like a very challenging problem. Therefore back to my question, how was this plot produced? It would be easy to consider a numerical integrator with some fixed time step and produce such a plot without considering the accuracy. However this plot would then completely depends on the choice of numerical integrator and time step. I suspect this is what is happening here. This plot is not showing the exact solution to this problem but rather the behavior of some approximate numerical integrator. I might be wrong but I would like to have a clarification of this point. Zirhom (talk) 18:36, 5 March 2013 (UTC)
Why we use the inertia about the centre of mass, not about the end
Of the two bodies the first pendulum is certainly rotating about its end. The second pendulum is only rotating about its end when the when the first one is stationary. When the first pendulum is moving, then the second is rotating about some point in space which is harder to locate.
The quantity wanted to write the Lagrangian is the total kinetic energy of the two the pendulums. We could write the KE of the first pendulum as
where (as you stated)
Alternatively we could write this energy (and have written it) as the sum of the kinetic energy due to the motion of the centre of mass of the pendulum, plus the kinetic energy due to rotation about this centre of mass (see the kinetic energy article). That is
(the centre of mass being halfway along the rod, and hence at a radius of from the pivot), and where
Either way we get
Both ways are correct. The first way (using the moment of inertia about the end) is simpler, and therefore the preferred way to do it for a single pendulum.
The motion of the second pendulum is more complicated, it's both swinging and moving as whole. To use the first method we'd have to work out the centre of rotation for the combined motion, and then the moment of inertia about that point. This seems difficult, so we use the second method.
Of course we could use one method for the first pendulum and another method for the second, and write
but somebody has decided that it's neater to write
which comes to the same thing.
- Thank you for this clarification, it was really helpful. User:Nillerdk (talk) 14:12, 22 January 2009 (UTC)
removed horology definition
It seemed to be talking about a clock with two pendulums hanging down, that are swinging precisely in anti-phase. That's not what this article is about, the pendulums are hung end-to-end in this article. The maths and everything else would be completely different. Because it was unreferenced and clearly distinct, I removed it.-17:08, 1 April 2010 (UTC)
Error in Lagrangian
Why do you include the "rotational energy" in the Lagrangian? Kinetic energy in terms of x1,y1 and y1,y2 is enough to specify the Lagrangian => transform to theta1 and theta2. Seems to be an error, unless I'm missing something. Someone should look into that and fix it. Danski14(talk) 20:10, 12 September 2010 (UTC)
- I see the description above, but that is a very confusing way to do it. I would recommend changing to the normal way of solving this problem.Danski14(talk) 20:12, 12 September 2010 (UTC)
- You may have overlooked the fact that the analysis and description relate to compound pendulums of equal length, while the first diagram shows simple pendulums of unequal length. For simple pendulums there need be no rotational energy terms since they are point masses. The article history shows that the diagram was removed in April for this reason - but it was then replaced. There is probably less work in replacing the first diagram, rather than rest of the article. --catslash (talk) 21:02, 12 September 2010 (UTC)
- If you are not in a hurry, I could make an appropriate SVG diagram. --catslash (talk) 21:12, 12 September 2010 (UTC)
- Done: the diagram now exactly matches the text of the analysis. It should make more sense now. --catslash (talk) 01:25, 22 September 2010 (UTC)
Most of the content of this article appear to be copied directly from this paper: http://tabitha.phas.ubc.ca/wiki/images/archive/3/37/20080811183757!Double.pdf — Preceding unsigned comment added by 126.96.36.199 (talk) 17:16, 4 January 2014 (UTC)
- The paper is dated 11 Aug 2008, so if anything the article includes material copied from this article (check the Jun 2008 version of this article). Another possibility is that the author of the paper and the relevant contributor to this article is the one and the same person. --catslash (talk) 21:59, 4 January 2014 (UTC)
- In fact a contributor to this article gives on his user-page a real name and affiliation identical to that of the author of the paper (caution: read WP:OUTING before mentioning real names). --catslash (talk) 22:29, 4 January 2014 (UTC)