Banked curves, coefficient of static friction

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Homework Help Overview

The discussion revolves around the physics of banked curves, specifically focusing on the coefficient of static friction and the associated equations of motion. Participants are examining discrepancies in calculated values and the assumptions underlying the equations used.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants are questioning the correctness of the equations used, with one asking for the angle of the bank and another suggesting the need to show work for clarity. There are discussions about the decomposition of forces and the validity of certain simplifications at low speeds.

Discussion Status

The discussion is active, with participants exploring different interpretations of the problem and questioning the assumptions made in the calculations. Some guidance has been offered regarding the equations and their application, but no consensus has been reached on the correct approach or values.

Contextual Notes

There are indications of missing information, such as the specific angle of the bank, and participants are considering whether the equations provided were derived or assumed. The potential for numerical discrepancies due to simplifications is also under discussion.

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Homework Statement
If a car takes a banked curve at less than the ideal speed, friction is needed to keep it from sliding toward the inside of the curve (a problem on icy mountain roads). (a) Calculate the ideal speed to take a 100.0 m radius curve banked at . (b) What is the minimum coefficient of friction needed for a frightened driver to take the same curve at 20.0 km/h?
Relevant Equations
tan(theta)-(v^2)/(rg) = us
where us is coefficient of static friction
The solution in my textbook says that for b, us = 0.234. However when I use the formula above I get 0.2364 which I feel like is too far off. Something must have gone wrong...
Any help would be much appreciated!
Thanks :)
 
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What is the angle of the bank?
 
In any case, your equation doesn't look correct. Can you show your work? You can write two equations by applying Newton's second law vertically and horizontally respectively, putting ##F = \mu N## in this limiting case.

[You should end up with an equation of the form ##\mu = \left(\tan{\theta} - \dfrac{v^2}{rg} \right)/X##, where ##X \sim 1## is a term depending on ##v,r,g## and ##\theta##...].
 
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What you did is that you decomposed the acceleration due to gravity into components normal and perpendicular to the road, but you didn't do the same with the centripetal acceleration.
 
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PeroK said:
What is the angle of the bank?
Is it 15 degrees?
 
In my understanding of how this works, when a student gives a relevant equation it is a given in the problem. I would like to establish if that is true here or if the student derived it first.
 
bob012345 said:
In my understanding of how this works, when a student gives a relevant equation it is a given in the problem. I would like to establish if that is true here or if the student derived it first.
At a guess, the student miscopied it.
 
haruspex said:
At a guess, the student miscopied it.
Perhaps, but it is a reasonable simplification valid at low speeds as shown by @ergospherical in post#3. It could explain the slight numerical discrepancy.
 
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bob012345 said:
Perhaps, but it is a reasonable simplification valid at low speeds as shown by @ergospherical in post#3. It could explain the slight numerical discrepancy.
Have you been thinking about a relativistic solution, then?
 
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PeroK said:
Have you been thinking about a relativistic solution, then?
Just comparing @ergospherical 's slipping equations with and without the ##X## term at 20##\frac{km}{hr}## and a presumed 15 degree bank angle.
 
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