Car turning on a bank (circular motion problem)

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SUMMARY

The discussion focuses on a physics problem involving a racecar turning on a bank inclined at 15%, traveling at a speed of 225 km/h with a mass of 1450 kg. Key calculations include determining the radius of curvature, centripetal acceleration, the magnitude of static friction, and the coefficient of static friction. The equations of motion are analyzed, revealing that the problem presents two unknowns with only one equation, indicating insufficient information to derive a solution. Additionally, the role of static friction is clarified, emphasizing that it is not always equal to the coefficient of static friction times the normal force unless the surfaces are on the verge of sliding.

PREREQUISITES
  • Understanding of centripetal acceleration and its formula
  • Knowledge of forces acting on an inclined plane
  • Familiarity with static friction and its coefficient
  • Ability to solve equations involving multiple variables
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  • Study the derivation of centripetal acceleration formulas
  • Learn about forces on inclined planes in physics
  • Explore the conditions for static friction in circular motion
  • Investigate the relationship between speed, radius, and friction in banked curves
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Homework Statement


A racecar is turning on a bank inclined at 15%. It's speed is 225 km/h and it's mass is 1450kg.
1. Calculate the radius of curvature
2. Calculate the centripetal acceleration.
3. If the car mantains circular traction, what is the magnitude of the force of static friction
4. What is the coefficient of static friction.


Homework Equations





The Attempt at a Solution


Is it just me or is there too many unknowns to be able to solve this question? (The answers are supposed to be actual numbers, not expressions in terms of unknowns)

So , I will have the force of gravity pointing straight down, I will have the Normal Force pointing perpendicular to the bank, and I will have the static friction force (fs) pointing parallel to the bank towards the centre.

So my Fy's are supposed to balance so we have:
Ny - fy - mg = 0
Ncosθ - μNsinθ - mg = 0
N (cosθ - μsinθ) = mg

And for Fx we have
fx + Nx = mv^2/R
μNcosθ + Nsinθ = mv^2/R

N(μcosθ + sinθ) = mv^2/R
plug in the N i got from the Fy equations:

g(μcosθ + sinθ) / (cosθ - μsinθ) = v^2/R

Now, I'm somehow supposed to provide the radius of curvature, and μ, (centripetl acceleration and magnitude of friction will then just come from those 2), but this is a single equation with 2 unknowns, how can i possibly be able to figure out both?
 
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I would agree with you that more information is needed to solve this problem.

In addition, I should point out that you are not justified in saying that the force of static friction is equal to the coefficient of static friction times the normal force. This is the case only if the two surfaces in contact are on the verge of sliding past each other. There is no language in the problem saying that this is the case.

Finally, the direction of the force of static friction is not necessarily down slope. If the speed is low enough (lower than what is necessary for the car to make it round the curve on a friction-free road) then static friction up slope is needed to maintain the car on track.
 

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