What velocity does a train need to go up and down the hill

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The discussion centers on determining the velocity a train must achieve to ascend and descend a hill of height h and length l, given its kinetic and potential energy equations. Participants explore the relationship between the train's center of mass and its position on the hill, concluding that the center of mass must be at the hill's peak for maximum potential energy. The minimum velocity requirement is established as v > 0, assuming the train coasts without engine power. A derived formula suggests that the velocity must exceed sqrt(g⋅h(2-d/2l), with the caveat that the train's length d must be less than twice the hill's length l for the calculations to hold. The conversation highlights the complexities involved when the train's length exceeds the hill's dimensions, leading to potential contradictions in energy calculations.
  • #31
So yeah, the answer i got is v > sqrt(g⋅h(2-d/2l) from similar triangles and their ratios. New height on which the center of mass is, is h((hl-d)/4l) so then we plug it as height in equation mv2/2 > mgh and rearrange it to get velocity.
 
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  • #32
Jorgen1224 said:

Homework Equations


Ek=m⋅v2/2
Ep=m⋅g⋅h

The Attempt at a Solution


I'm basically stuck at conversation of energy. Train needs to have kintetic energy equivalent to potential energy mgh, but calculating v from this equation seems pointless since it doesn't include either length. I have no idea how to include either of them.

if there is no friction then those are the only 2 equations that you need, because the length of l does not matter.
 
  • #33
mrsmitten said:
if there is no friction then those are the only 2 equations that you need, because the length of l does not matter.
As has been thoroughly discussed in this thread already, what you just wrote is not correct.
 
  • #34
Jorgen1224 said:
So yeah, the answer i got is v > sqrt(g⋅h(2-d/2l)).
Right.
 
  • #35
Orodruin said:
As has been thoroughly discussed in this thread already, what you just wrote is not correct.

sorry I was thinking of the train as a rigid body.

i see what you are talking about now.
 
  • #36
Jorgen1224 said:
So yeah, the answer i got is v > sqrt(g⋅h(2-d/2l)

haruspex said:
Right.
With the proviso that the train is not long enough to span the entire hill. That is, as long as d < 2l.

As drawn, the train appears to only be long enough to span about half of the hill, so the proposed solution above appears to be the intended one.

If the train is longer than two hill-spans (d > 4l ), the proposed solution goes really wonky and predicts an imaginary required speed. [If you draw it out, that's because scenario assumed by the formula would have the front and back ends of the train dangling underground. The center of gravity would be below ground when the midpoint of the train hits the peak of the hill].
 
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  • #37
jbriggs444 said:
osed solution goes really wonky and predicts an imaginary required speed.
(At the risk of derailing thread,is that literally an imaginary number? As in i?)
 
  • #38
DaveC426913 said:
(At the risk of derailing thread,is that literally an imaginary number? As in i?)
Yes.

A sufficiently long train has less potential energy when draped over the top of a hill than when it is flat at a specific level below the hilltop. To end up with zero kinetic energy you therefore have to start with negative kinetic energy. Which means an imaginary starting velocity. The square root of minus 1 sort of "imaginary".
 
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