Lagrange constraint mechanics problem

In summary, the conversation discusses the relationship between rotational kinetic energy and the angular position of a point on a smaller sphere in relation to the centers of two spheres. The formula for Trot is given as 1/5 ma2(thetaDOT + phiDOT)2, where theta is the angular position and phi is the orientation of the joining line between the two spheres. The inclusion of the phiDOT term accounts for the changing orientation of the joining line over time.
  • #1
DylanG
5
0
http://img221.imageshack.us/img221/3754/capturetp.png

Just a simple question. I can see that for this to work I need:

Trot = 1/5 ma2(thetaDOT + phiDOT)2

Just can't work out what phi has to do with rotational kinetic energy. I would have thought it would need to be simply the same thing but without the phiDOT term.
 
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  • #2
[itex]\theta[/itex] is the angular position of an identified point on the smaller sphere, measured with respect to the line joining the centers of the two spheres, right? Note that not only does [itex]\theta[/itex] change with time, but so does the orientation of that joining line, so you need to take that into account as well. That's where the [tex]\dot\phi[/tex] comes from.
 

1. What is the Lagrange constraint mechanics problem?

The Lagrange constraint mechanics problem is a mathematical framework used to analyze the motion of a system while taking into account any constraints that may limit the motion of the system. It was developed by Joseph-Louis Lagrange in the late 1700s and is a fundamental tool in classical mechanics.

2. How does the Lagrange constraint mechanics problem differ from Newton's laws of motion?

Newton's laws of motion describe the behavior of a system without any restrictions or constraints, while the Lagrange constraint mechanics problem takes into account any constraints that may limit the motion of the system. This allows for a more accurate and comprehensive analysis of the system's motion.

3. What are some common examples of systems that can be analyzed using the Lagrange constraint mechanics problem?

The Lagrange constraint mechanics problem can be applied to a wide range of systems, including pendulums, planetary orbits, and rigid bodies. It is particularly useful in analyzing systems with multiple degrees of freedom.

4. How does the Lagrange constraint mechanics problem handle non-conservative forces?

The Lagrange constraint mechanics problem can easily incorporate non-conservative forces, such as friction or air resistance, into the equations of motion. This allows for a more realistic and accurate analysis of the system's behavior.

5. Are there any limitations to using the Lagrange constraint mechanics problem?

The Lagrange constraint mechanics problem is a powerful tool, but it does have some limitations. It assumes that the system is in equilibrium and that the constraints are holonomic (can be described by equations). It may not be applicable to systems with non-holonomic constraints or systems that are constantly changing.

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