Find the min. velocity for which a particle will remain on the loop

Click For Summary
SUMMARY

The minimum velocity required for a particle to remain on a vertical circular track without losing contact is derived from the principles of conservation of energy and centripetal force. The key equation is derived from the balance of forces at the top of the loop, leading to the expression v = sqrt(v0^2 - 4gr). Here, v0 represents the initial speed at the lowest point, g is the acceleration due to gravity, and r is the radius of the circle. Understanding the role of the angle theta in the context of radial and tangential components of weight is crucial for solving this problem.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with centripetal force equations
  • Knowledge of conservation of energy principles
  • Basic trigonometry, particularly involving angles in circular motion
NEXT STEPS
  • Study the derivation of centripetal force equations in circular motion
  • Learn about the conservation of mechanical energy in physics
  • Explore the role of radial and tangential components in circular motion
  • Investigate the effects of friction in circular motion scenarios
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and circular motion, as well as educators looking for practical examples of energy conservation and force balance in vertical circular tracks.

holezch
Messages
251
Reaction score
0

Homework Statement


A particle m is moving in a vertical circle of radius R inside a track. There is no friction. When m is at its lowest position, its speed is v0. What is the lowest value of v0 for which m will go completely around the circle without losing contact of the track?

Homework Equations



F= mv^2/r

conservation of energy

The Attempt at a Solution



Is this correct:

The min velocity will be at the top, where 1/2mv^2 + U(max height) = 1/2 mv0^2 ( from the bottom where U(0) = 0 ). So, if the particle is going to "fall off" the track, it should be where there isn't enough kinetic energy / speed. So.. if it DOES fall off, we would have N = 0, mv^2/r = mgsintheta - N = mgsintheta.

From 1/2 mv^2 + U(max height) = 1/2 mv^2 + mg2r = 1/2 mv0^2 we can solve for v from the top

and it turns out to be v = sqrt( v0^2 - 4gr )

then plug that into mv^2/r = mgsintheta and that would be the min. speed of the particle's total movement.. and you can solve for the initial speed from there. so if the min. speed is larger than the value that would have N = 0 , then it won't fall off.

thanks
 
Last edited:
Physics news on Phys.org
I think that should work; however, I don't know what theta represents in this problem.
 
JaWiB said:
I think that should work; however, I don't know what theta represents in this problem.

thanks, I just had to split my weight into radial and tangential components
 

Similar threads

Replies
8
Views
4K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
Replies
5
Views
2K
Replies
7
Views
3K
  • · Replies 13 ·
Replies
13
Views
2K
Replies
2
Views
1K
  • · Replies 6 ·
Replies
6
Views
3K
Replies
40
Views
3K