Vertical circular motion minimum speed proof

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Discussion Overview

The discussion centers around the minimum speed required for a body to successfully complete a vertical circular motion. Participants explore the conditions under which a body can maintain its path through the circle, particularly focusing on the speed at the top of the circle and the implications of that speed for the entire motion. The conversation includes theoretical considerations, mathematical formulations, and conceptual clarifications.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that the minimum speed for a body to finish a vertical circle is given by v = (rg)^0.5, particularly at the top of the circle.
  • Others question the assumption that reaching this speed at the top guarantees completion of the circle, seeking further explanation on why this is the case.
  • One participant suggests that if the speed is less than (rg)^0.5 at the top, the body would fall off the path earlier.
  • Another participant introduces equations for minimum speed as a function of angle and actual speed, indicating that the curves of minimum required speed and actual speed intersect at the top of the circle.
  • Some participants discuss the implications of velocity changes throughout the circular path and how they affect centripetal acceleration and normal force.
  • There are mentions of analyzing the motion in reverse to argue that if the body can complete the first half of the circle, it should also complete the second half under certain conditions.

Areas of Agreement / Disagreement

Participants express differing views on the implications of the minimum speed at the top of the circle, with some agreeing on the mathematical formulation while others challenge the conclusions drawn from it. The discussion remains unresolved regarding the necessity of the body completing the circle at the minimum speed and the conditions under which this occurs.

Contextual Notes

Participants note that the acceleration is changing throughout the motion, and the analysis relies on specific assumptions about forces acting on the body at different points in the circular path. There are unresolved questions about the relationship between speed at the top and the ability to maintain circular motion.

Mad_Eye
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hi,
i've read in a lot of places that the minimum speed fora body to "finish" a vertical circle is (rg)^0.5, but I've never understood why.. they assume the if the body passes the top, it will finish the whole circle.. but i can't actually see it... can someone explain/proof it to me?

secondly, is the mentioned speed is for the bottom or for the top?
this is the proof I've seen:
(the top point)
mg + N = ma
a = v^2 / r

assume N=0

mg = mv^2 / r
v = (rg)^0.5my problem is with this formula
a = v^2 / r

the acceleration is changing, thus this is true for momentary velocity.

so v = (rg)^0.5
must be for v of the top.. not the bottom...sorry about my english :)
 
Last edited:
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v is the speed the object must have as it passes the top of the circle

for example, if it was 0 the object would just drop vertically to the floor...
 
YellowTaxi said:
v is the speed the object must have as it passes the top of the circle

for example, if it was 0 the object would just drop vertically to the floor...

fine, but why the body will necessarily complete the circle? (if the speed is such)
p.s. so it is possible the body get to the top point at speed 0? or any thing below (rg)^0.5 ?
 
Last edited:
Mad_Eye said:
fine, but why the body will necessarily complete the circle? (if the speed is such)
The top point is critical because v and a are minimal and Fg is acting fully to reduce N, therefore N is minmal. After passing the top v and a increase and Fg acts only partly to reduce N, so N increases too.
Mad_Eye said:
p.s. so it is possible the body get to the top point at speed 0? or any thing below (rg)^0.5 ?
No, it would fall off earlier.
 
The equation for minimum speed as a function of angle is:

v_min(ang) = (r*g*sin(ang))^0.5

ang = 0 when the body reaches a quarter of the circle
ang = pi/2 when the body reaches the top of the circle

The equation for actual speed as a function of v_top (speed at the top of circle) and angle is: (solved using conservation of energy)

v_act(v_top,ang) = (v_top^2 + 2*g*r*(1-sin(ang))^0.5

For the case of v_top = (r*g)^0.5, the plot of these two equations looks like this:

_|
_|._________________________________.
_|_._______________________________.
_|____._________________________.
_|_________._______________.
v|_________________.
_|_________._______________.
_|____._________________________.
_|_._______________________________.
_|._________________________________.
0|______________________________________
_0________________pi/2_________________pi

ang

The top curve is actual speed. The bottom curve is minimum required speed. They meet at pi/2 (top of the circle) with the value of v = (r*g)^0.5. If you lowered the actual speed curve, the curves would intersect. The point at which they first intersect is the angle at which the body would fall. This is what "A.T." meant when he said "it would fall off earlier."
 
Last edited:
another way is you know if it falls, then it'll fall along a parabola not along a circle. So just compare the shape of the given parabola that would form (at that instantaneous velocity) if the circle wasn't there.
 
YellowTaxi said:
another way is you know if it falls, then it'll fall along a parabola not along a circle. So just compare the shape of the given parabola that would form (at that instantaneous velocity) if the circle wasn't there.

i've thought about it.. but that just a proof it won't fall at the top, but a moment after that, it has different velocity..
 
I meant you could take the velocity anywhere on the cirlce and show whether it's fast enough at that point to stay on the circle or fall parabolically inside of it.
 
Mad_Eye said:
but that just a proof it won't fall at the top, but a moment after that, it has different velocity.
yes, a higher velocity, resulting in higher centripetal acceleration and higher normal force. so it cannot fall anymore, if it got that far.
 
  • #10
bluelava0207 said:
The equation for minimum speed as a function of angle is:

v_min(ang) = (r*g*sin(ang))^0.5

ang = 0 when the body reaches a quarter of the circle
ang = pi/2 when the body reaches the top of the circle

The equation for actual speed as a function of v_top (speed at the top of circle) and angle is: (solved using conservation of energy)

v_act(v_top,ang) = (v_top^2 + 2*g*r*(1-sin(ang))^0.5

For the case of v_top = (r*g)^0.5, the plot of these two equations looks like this:

_|
_|._________________________________.
_|_._______________________________.
_|____._________________________.
_|_________._______________.
v|_________________.
_|_________._______________.
_|____._________________________.
_|_._______________________________.
_|._________________________________.
0|______________________________________
_0________________pi/2_________________pi

ang

The top curve is actual speed. The bottom curve is minimum required speed. They meet at pi/2 (top of the circle) with the value of v = (r*g)^0.5. If you lowered the actual speed curve, the curves would intersect. The point at which they first intersect is the angle at which the body would fall. This is what "A.T." meant when he said "it would fall off earlier."

i've just thought about a simpler one..
so the body reached the top.. let's take what happened so far, in reverse.. now the body has velocity of (rg)^0.5 to the other side, mg is still downward.. we KNOW the body will complete the half circle reversed motion, because we've just seen it complete it...
now the second half of the circle, is exact the same as the first half reversed... so the body will necessarily complete the second half because we know it complete the first half reversed...
 
  • #11
Mad_Eye said:
..
now the second half of the circle, is exact the same as the first half reversed... so the body will necessarily complete the second half because we know it complete the first half reversed...
Yeah, but how do you know that it can get to the top with v = (rg)^0.5 ? :smile: The analysis by bluelava0207 shows that.
 
  • #12
A.T. said:
Yeah, but how do you know that it can get to the top with v = (rg)^0.5 ? :smile: The analysis by bluelava0207 shows that.

i know it can get to the top at (rg)^0.5, according to what I've write in the first post
 

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