Static and dynamic analysis of a crank with pedal

Click For Summary

Discussion Overview

The discussion revolves around the static and dynamic analysis of a bike's crank and pedal system, focusing on stress concentrations in the pin connecting the crank and pedal. Participants explore the implications of static versus dynamic forces on stress levels, considering both theoretical and practical aspects of the analysis.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant asserts that the stress concentration of 121.3 MPa in the pin remains the same in both static and dynamic scenarios, given a constant force of 210 N applied to the pedal.
  • Another participant agrees, suggesting that unless there is significant acceleration of the pedal, the stress levels should not differ between static and dynamic analyses.
  • A third participant notes that while static and dynamic stress levels may not differ significantly for realistic acceleration rates, the method of restraining the crank could affect the reaction forces and load paths.
  • Concerns are raised about how the crank is restrained, with suggestions that fixing it at multiple points may not accurately represent real-world conditions.
  • Participants discuss the effects of chain tension on stress distribution, considering extreme cases of sprocket and chain interaction that could influence local stresses.
  • Another participant highlights that the mass of the assembly is small compared to the bike's overall mass, indicating that acceleration effects on stress may be negligible.
  • Discussion includes considerations of rotational acceleration and its potential impact on stress, though participants agree that the effects are likely small.

Areas of Agreement / Disagreement

Participants generally agree that the stress levels in the pin may not significantly differ between static and dynamic scenarios under typical conditions. However, there is no consensus on the exact impact of different restraining methods or the specifics of chain interaction with the sprocket.

Contextual Notes

Participants express uncertainty about the correct method for restraining the crank and how this may affect the analysis. There are also unresolved considerations regarding the influence of chain dynamics on stress distribution.

boblefisk
Messages
4
Reaction score
0
Hi.

me and my friend have a problem that we can't really agree upon.

we are doing an analysis study on a bike's crank and pedal.

the first picture shows how we put the force of 210 N.
picture 2 shows how we used "fixed geometry" to lock the part in place.

now, this is the static analyses, where we get a stress consentration of 121.3 MPa in the pin connecting the crank and the pedal.

our unagreement comes here:

she belives that the stress consentration in the same spot in a dynamic "real" event could be reduced.
because instead of the part beeing fixed and locked where the gear is, it would rater have a force working against the pedal force.

i believe the stresses in the pin would be the same nomatter if its static or dynamic in that excact position. The force used on the pedal will still be 210 N and therefor the max stress in that area would remain the same.
i can't imagine how the stresses at that location can be reduced due to the change from static to dynamic, when all paramters are the same except for resitance insted of it beeing locked.

(im know the stresses would change due to the change in position in dynamic, but that isn't what we are asking for)


im not sure if i made my self understandable here. please ask if anything is unclare:)
 

Attachments

  • force event 1.PNG
    force event 1.PNG
    45.4 KB · Views: 943
  • låsinger.PNG
    låsinger.PNG
    39.5 KB · Views: 884
  • jern vonmises 2.PNG
    jern vonmises 2.PNG
    21.8 KB · Views: 773
Physics news on Phys.org
i believe the stresses in the pin would be the same nomatter if its static or dynamic in that excact position. The force used on the pedal will still be 210 N and therefor the max stress in that area would remain the same.
I agree, unless you have a significant acceleration of your pedal. Force on it has to cancel if its mass*acceleration is negligible in the setup.
 
I agree there would not be any significant change between a static and dynamic stress levels, for a realistic acceleration rate of the bike.

However you might want to think a bit more about how you restrained the crank against rotating, so you get the correct reaction forces on it. You seem to have fixed the chain wheel at three points around its circumference, which doesn't correspond to the real situation.

The force propelling the bike comes from the tension in the top part of the chain, which is applied tangentially to the top of the gear wheel. You can probablly ignore the tension in the bottom part of the chain which should be much smaller. The other forces on the crank are all through its bearings.

To model the fact that the crank can turn in the bearing, you can restrain it in the X Y and Z directions all the way along the axis of rotation. You then need to stop it spinning freely, by restraining it tangentially at the top, where the chain starts to wrap around it.

Without making a model I don't know if that will actually make any difference, but these details can be important if they create the wrong load paths through the structure. Restraining the model the right way is no harder than doing it wrong, except for a bit more thought to decide what is "right".
 
it is true what you are saying. we shouldn't restrain it at all the way around the gear.
thanks for the heads up;)

So can someone explain why the stresses at the given point will be equal at that excact position in the two different scenarios?

i need to know why, (given my theory is right) so i can explain it to her:) or vice versa
 
boblefisk said:
So can someone explain why the stresses at the given point will be equal at that excact position in the two different scenarios?

Which two scenarios are you asking about? Accelerating and not accelerating? Or two different ways of restraining the model?
 
Accelerating and not accelerating.
 
The mass of the assembly is very small compared to mass of the wheel and the bicycle, so acceleration will not make any difference here. Nearly all of the stress will come from action between chain, axis on which sprocket is mounted, and the crank/pedal itself.

As far as stress from the chain, I see two extreme cases that should be considered. First, it's possible that spacing between teeth of the sprocket is slightly shorter than spacing between links of the chain. In that case, chain will mostly pull on the top of the sprocket. On the other hand, if the spacing between teeth is slightly longer, the stress will be distributed more evenly, with more tangential force at the bottom of the sprocket, and radial force through half of the revolution in between. Of course, rounded grooves will help reduce the significance of this effect, so it might be ok to just assume even pull.
 
K^2 said:
As far as stress from the chain, I see two extreme cases that should be considered. First, it's possible that spacing between teeth of the sprocket is slightly shorter than spacing between links of the chain. In that case, chain will mostly pull on the top of the sprocket. On the other hand, if the spacing between teeth is slightly longer, the stress will be distributed more evenly, with more tangential force at the bottom of the sprocket, and radial force through half of the revolution in between. Of course, rounded grooves will help reduce the significance of this effect, so it might be ok to just assume even pull.

The way the chain fits onto the sprocket teeth will affect the local stresses around the rim of the sprocket, but not the way the chain "pulls" on the sprocket as a whole.

Think about a free body diagram of the sprocket and pedal crank, plus a short piece of the chain from the sprocket towards the rear wheel. You have three statically determinate forces acting (ignoring the weight of the object, which will be small compared with the other forces): the pull in the direction of the chain, the force on the pedal, and the reaction force at the bearing. Those forces are not affected by the details of how the chain interacts with the sprocket.
 
boblefisk said:
Accelerating and not accelerating.

The acceleration of the bike is limited by the friction force between the tires and the ground, and the maximum will be of the order of 1g (10m/s). So the maximum force required for the linear acceleration of the crank is the same order of magnitude as the weight of the crank. That is much smaller than the force applied to the pedal, etc.

There is also the rotational acceleration to consider, and you need more numbers about the size of the bike wheels and the gear ratios to estimate that, but you would get to the same conclusion - the effect would be small. That's not really surprising, since these parts were designed to be as light as possible to minimize the amount of "wasted" energy propelling the bike.
 
  • #10
True. I was thinking about net moment of force around a point other than center of the sprocket, but yeah, that still works out the same. So if you are not interested in stress on the sprocket, but only the pedal and the crank, then it doesn't matter how the chain interacts with the sprocket.
 
  • #11
Thank you very much, both of you. That helped a lot:D
 

Similar threads

Replies
6
Views
6K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 23 ·
Replies
23
Views
15K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 16 ·
Replies
16
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 2 ·
Replies
2
Views
8K