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

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SUMMARY

The discussion centers on determining the minimum velocity required for a train of length d to ascend and descend a hill of height h and length l. The key conclusion is that the train must maintain a velocity greater than zero (v > 0) to successfully navigate the hill, assuming negligible power from the engine during ascent. The derived formula for the minimum velocity is v > sqrt(g⋅h(2-d/2l), which incorporates gravitational acceleration g and the dimensions of the train and hill.

PREREQUISITES
  • Understanding of kinetic energy (Ek = m⋅v²/2)
  • Understanding of potential energy (Ep = m⋅g⋅h)
  • Familiarity with the concept of center of mass
  • Basic knowledge of similar triangles and ratios
NEXT STEPS
  • Explore the implications of train length on potential energy and velocity requirements
  • Study the effects of friction on kinetic and potential energy calculations
  • Learn about the dynamics of flexible bodies in motion, particularly in relation to center of mass
  • Investigate the mathematical implications of imaginary numbers in physical scenarios
USEFUL FOR

Students of physics, engineers working on transportation systems, and anyone interested in the mechanics of motion and energy conservation in dynamic systems.

  • #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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