Conservation of energy of a car problem

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Homework Help Overview

The problem involves determining the height a roller coaster car will reach on an incline after being launched with sufficient speed to round the top of a loop without leaving the track. The context is centered around the conservation of energy principles and forces acting on the car during circular motion.

Discussion Character

  • Exploratory, Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the application of conservation of energy equations and the forces acting on the car at the top of the loop, including gravitational and normal forces. There is a focus on understanding the conditions required for the car to maintain contact with the track.

Discussion Status

The discussion is ongoing, with participants exploring the implications of forces at the top of the loop and questioning the assumptions made regarding the speed of the car. Some guidance has been offered regarding the relationship between forces and acceleration in circular motion, but no consensus has been reached.

Contextual Notes

Participants note the importance of considering the minimum speed required for the car to "hug" the track at the top of the loop, which introduces complexities in the problem setup. There is also mention of the need to clarify the definitions of forces involved in the scenario.

myoplex11
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Homework Statement


Determine the height h to the top of the incline D to which the 200-kg roller coaster car will reach, if it is launched at B with a speed just sufficient for it to round the top of the loop at C without leaving the track. The radius of curvature at C is
ρC = 25 m. I have attached a picture of this problem below.



Homework Equations


KE1+PE1=KE2+PE2


The Attempt at a Solution


.5mv1^2+mgh=.5mv^2+mgh
.5mv1^2=mgh
0.5v1^2=gh
 

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… physics for "hug" is "force" …

myoplex11 said:

Homework Equations


KE1+PE1=KE2+PE2

The Attempt at a Solution


.5mv1^2+mgh=.5mv^2+mgh
.5mv1^2=mgh
0.5v1^2=gh

Your method would only give you the speed needed for the car to reach the top with zero speed.

The question requires the speed at the top to be so great that the car still "hugs the track".

Physics for "hug" is "force". :smile:

(Reminds me of: Principal "How is you mathematics?" Groucho Marx: "Sir, I speak it like a native!" :smile:)

So … what are the forces on the car at the top of the track? :smile:
 
centipetal force and the normal force i still have no idea how to do this
 
… the acceleration is always downward …

myoplex11 said:
centipetal force and the normal force i still have no idea how to do this

"Centipetal force" is not a force! :frown:

And you've missed out gravity …

The only two forces are gravity, and the normal force (the reaction force).

Those two forces determine the acceleration.

Paradoxically, they're both downward (at the top of the loop, C) … which means that the acceleration is always downward (centripetal)! :frown:

But that doesn't matter, because circular motion (at the top of the circle) requires downward acceleration! :smile:

This is geometry, not physics (and you can easily prove it using vectors) … an object with speed v in a circle or radius r has an acceleration of v^2/r towards the centre of the circle.

So, at C, you want gravity and the normal force together to equal m.v^2/r (Newtons' second law).

The question asks for the minimum case, which obviously must be when the normal force is zero: then the force from gravity alone equals mv^2/r.

And so … ? :smile:
 

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