How Is the Minimum Radius at Point B Calculated for Rollercoaster Safety?

In summary: I'm not sure if you are asking about the initial or final states, but in either case, the cart has 0 kinetic energy at the top of point B. When it goes down to 0 meters, it gains kinetic energy, and when it goes back up to 5 meters, it loses kinetic energy again. So the centripetal force at point B would be =mv2/r with the mass divided out.
  • #1
d0rk
8
0
the question is:

The figure below shows the plan for a proposed rollercoaster track. Each car will start from rest at point A and will roll with negligible friction. For safety, it is important that there be at least some small positive normal force (a push) exerted by the track on the car at all points. What is the minimum safe value for the radius at point B?

the picture shows a cart at the top of the track with a heigh of 15.0meters signified by point A. it then goes down and back up to a point B which is 5.0meters high.

if someone can just start me off in the right direction i would greatly appreciate it.
 
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  • #2
Edit: I misread the question.
 
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  • #3
I know Normal force will be consistent throughout...so should I use the Work Energy Theorem for the external forces...because I know it can't just be mg...
 
  • #4
Edit: NM I thought it was a circular loop.
 
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  • #5
Think of centripetal force.

Fcentripetal = mv2/r, which must be less than the weight of the car in order to assure + force down onto the track.

http://hyperphysics.phy-astr.gsu.edu/Hbase/cf.html#cf

Then one has to determine the speed (magnitude of velocity) at B.
 
  • #6
if its a circular motion problem shouldn't the net force be 0?..and there is no loop in the diagram...its just point a at 15.0 meters that goes down to 0 meters then back up another hump 5 meters tall...
 
  • #7
d0rk said:
if its a circular motion problem shouldn't the net force be 0?..and there is no loop in the diagram...its just point a at 15.0 meters that goes down to 0 meters then back up another hump 5 meters tall...
Oh my bad. I misunderstood the problem. For some reason I assumed that it was a circular loop.
 
  • #8
without any mass how would i be able to incorporate the centripetal force...
 
  • #9
One does not need mass if all equations can be written on a per mass basis or specific energy. For example,

gravitational potential energy = mgh, but specific GPE = gh.

kinetic energy = 1/2 mv2, but specific KE = v2/2,

graviational force (weight) = mg, but in specific terms = g (which is just acceleration), and

centripetal force F = ma = mv2/r, is simply v2/r with the mass divided out, and actually one determines when centripetal acceleration = gravitational acceleration, or

g > v2/r for a net downward force, or use = for minimum radius.
 
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  • #10
Please check if this is right

Astronuc said:
Think of centripetal force.

Fcentripetal = mv2/r, which must be less than the weight of the car in order to assure + force down onto the track.

http://hyperphysics.phy-astr.gsu.edu/Hbase/cf.html#cf

Then one has to determine the speed (magnitude of velocity) at B.


this is what i have so far

v^2/R<g
K=U
1/2mv^2=mgh
v^2=2gh
g>2gh/r

i put my reference line at the bottom which = 0
the car starts at the top at 15m high then goes down to 0 then back up another hump, point B, at 5.0meters. for h do i subtract 15-5=10m if i do this is what i get...

g>2g(10)/r
r=20m?

could that be the minimum safe value for the radius at point B??
 
  • #11
ok...now after thinking about it...i solved for the velocity at the bottom of the track right before it hits the hump B...

mgh=1/2mv^2
mg(15)=1/2mv^2
30g=v^2
v=sqrt(30g)

is this the velocity at the bottom of the track for the first part?
 
  • #12
mgh=1/2mv^2
mg(15)=1/2mv^2
30g=v^2
v=sqrt(30g)

is this the velocity at the bottom of the track for the first part?
That would be the velocity at an elevation of 0.

You seem to be headed in the right direction.

Basically at 15 m, and v=0, the energy for this system is all potential. Then at 0 m elevation, the energy is all kinetic.

The cart loses some KE, while it regains some GPE as it increases elevation again to 5 m.

From conservation of energy, one can determine the change in KE from the change in PE, and from KE, one obtains the velocity (at the elevation of interest), and from velocity on uses the balance of force (gravity and centripetal) to get the corresponding radius.
 
  • #13
so with the velocity at sqrt(30g)...

with that when the cart starts to go over the second hump (B) the velocity needs to equal:

mg(5)=1/2mv^2
10g=v^2
v=sqrt(10g)

I'm assuming that this equals the velocity at the top of hump B...

conservation of energy states that PE(final)+KE(final)=PE(initial)+KE(initial)

Fcen=mv^2/r

so at the top of point B would it be correct to say that it is all potential? and that i would just need to take the difference of the velocity at 0 meters and at 5 meters and substitute v in the the Centripetal force equation and solve for r? but then again for the mass in the equation i would need to use g>v^2/r??
 
  • #14
so at the top of point B would it be correct to say that it is all potential?
The total energy at B is a combination of potential and kinetic, since the cart has increased elevation, but is still moving. The minimum potential is at 0 m.

To find the velocity at B, the KE at B should be just the difference in potential between the start (where KE = 0) and the potential energy at B.

So find the corresponding velocity.

Then mg = mv2/r.

Here is an example of the principle with which we are working - http://hyperphysics.phy-astr.gsu.edu/hbase/flobj.html

Gravitational potential energy (a linear function of elevation - mgh) is converted to kinetic energy. The course simply affects the direction in which the vehicle travels - assuming no dissipative forces like air resistance or friction with the surface.
 
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  • #15
This is what I got:

PE(final)+KE(final)=PE(initial)+KE(initial)
1/2mv^2 + mg(5) = 0 + mg(15)
1/2v^2 + 5g = 0 + 15g
1/2v^2 = 10g
v^2 = 20g

mg = mv^2/r
g = 20g/r
r = 20?

Is that correct??
 
  • #16
20 m is correct - and I am assuming that the track at point B has a horizontal tangent. This is important because the centripetal force acts perpendicular to the tangent on a curve, which can have any orientation with respect to horizontal (or vertical), but gravity is always downward.

Is there a diagram of the track? Is the tangent of the curve at point B horizontal?

One has to remember that forces and acceleration are vector quantities.
 

1. What is normal force?

Normal force is the force that a surface or object exerts on an object that is in contact with it. It is always perpendicular to the surface and acts in the opposite direction of the force applied by the object.

2. How is normal force different from other types of forces?

Normal force is different from other types of forces because it is a reactive force, meaning it is only present when an object is in contact with a surface. Other forces, such as gravity and friction, can act at a distance without direct contact.

3. What factors affect the magnitude of normal force?

The magnitude of normal force is affected by the weight of the object, the angle at which the object is placed on the surface, and the surface's characteristics (such as roughness or elasticity).

4. How is normal force related to weight?

Normal force is equal in magnitude to the weight of an object when it is placed on a horizontal surface. However, if the surface is at an angle, the normal force will be less than the weight of the object.

5. Can normal force be negative?

No, normal force cannot be negative. It always acts in the direction perpendicular to the surface and opposes the force applied by the object. If the force applied by the object is greater than the normal force, the object will either sink into the surface or slide along it.

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