Banked curves, coefficient of static friction

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SUMMARY

The discussion centers on the calculation of the coefficient of static friction (us) for banked curves, specifically addressing discrepancies between textbook values and user calculations. The textbook states us = 0.234, while a user calculates 0.2364, prompting inquiries into the correctness of their equations. Key insights include the application of Newton's second law and the need to properly account for centripetal acceleration in the equations. The angle of the bank is suggested to be 15 degrees, with considerations for simplifications at low speeds.

PREREQUISITES
  • Understanding of Newton's second law of motion
  • Familiarity with banked curve dynamics
  • Knowledge of static friction coefficients
  • Basic trigonometry for angle calculations
NEXT STEPS
  • Study the derivation of equations for banked curves
  • Learn about the effects of speed on friction in banked turns
  • Explore the role of centripetal acceleration in motion on curves
  • Investigate the implications of low-speed approximations in physics
USEFUL FOR

Students of physics, engineers working on vehicle dynamics, and anyone interested in the mechanics of banked curves and frictional forces.

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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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