Motion in Nonlinear Differential Equations

Click For Summary
SUMMARY

The discussion focuses on deriving the time-dependent velocity equation for a uniform sphere of mass m and radius r rolling down a semicircular half pipe with radius R, specifically when R > r. The participants emphasize the importance of modeling the motion using differential equations, particularly in the absence of friction and when considering the sphere's rotation. The equation for velocity is suggested to be analogous to that of a simple pendulum, with the need to derive the ordinary differential equation (ODE) through a free body approach.

PREREQUISITES
  • Understanding of nonlinear differential equations
  • Familiarity with the concepts of motion in physics, specifically pendulum motion
  • Knowledge of free body diagrams and forces acting on objects
  • Basic calculus for integration and differential equations
NEXT STEPS
  • Research the derivation of ordinary differential equations for motion on curved paths
  • Study the dynamics of rolling objects, particularly the effects of rotational inertia
  • Explore the mathematical modeling of pendulum motion and its applications
  • Learn about the impact of friction on motion in differential equations
USEFUL FOR

Students and professionals in physics, particularly those studying mechanics and dynamics, as well as mathematicians interested in differential equations and their applications in real-world scenarios.

kgns
Messages
1
Reaction score
0

Homework Statement



How do you derive the time-dependent velocity equation for motion along a curve, such as a skateboarder on a half pipe?

For the sake of abstraction, I ask myself the following:

A uniform sphere of mass m and radius r is set free from the top edge of a semicircle half pipe with radius R. If R > r, what is the time-dependent velocity equation v(t) for the sphere in terms of t, m, r, R and g?

(i) ignoring any effects of friction?
(ii) if the sphere is rotating?2. The attempt at a solution

If it were an inclined plane, we'd have no problem with
[itex]v(t)=gtsin(\alpha)[/itex]

Considering the halfpipe an infinitesimal sum of inclined planes we'd get
[itex]\int^{0}_{t}gsin\alpha(t)\partial\alpha[/itex]

However I've failed to derive [itex]\alpha[/itex] in terms of t.

How can I model such a problem in differential equations?
 
Physics news on Phys.org
I assume this is all in the plane at right angles to the trough's axis.
If you ignore friction then the object will slide, so its shape is somewhat irrelevant. The problem becomes a simple pendulum, but using the exact equation, not the approximation for small angles that makes it effectively SHM. You should be able to derive the ODE using the usual free body approach.
For a rolling sphere, I don't expect it to be much different. Should be equivalent to reduced gravity. Again, do try to obtain the equation.
 

Similar threads

Replies
10
Views
2K
Replies
4
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K
Replies
3
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
5
Views
3K
  • · Replies 6 ·
Replies
6
Views
3K
Replies
7
Views
2K
Replies
1
Views
2K
  • · Replies 8 ·
Replies
8
Views
6K