Speed at which a car on a banked curve will slide.

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SUMMARY

The discussion centers on calculating the maximum speed at which a car can navigate a banked curve without sliding off. The relevant parameters include a radius (R) of 200 meters, a banking angle (θ) of 10 degrees, and a coefficient of static friction (μs) of 0.60. The derived formula for maximum speed (v) is v > √(gR(tan(θ) + μs)/(1 - μs tan(θ))). A critical error in the initial calculation was identified, leading to an incorrect speed of 88.6 m/s, which was rectified by properly applying the static friction force. The corrected formula eliminates the erroneous tangent function in the friction term.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with circular motion dynamics
  • Knowledge of static friction and its role in motion
  • Ability to manipulate trigonometric functions in physics equations
NEXT STEPS
  • Study the derivation of centripetal acceleration in circular motion
  • Learn about the effects of banking angles on vehicle dynamics
  • Explore the role of static friction in preventing sliding on curves
  • Investigate real-world applications of banked curves in road design
USEFUL FOR

Physics students, automotive engineers, and anyone interested in the dynamics of vehicles on curved paths will benefit from this discussion.

SheldonG
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Homework Statement


If a car goes around a banked curve too fast, the car will slide out of the curve. Find an expression for the car speed v_{max} that puts the car on the verge of sliding out. What is the value for R=200, \theta = 10, \mu_s = 0.60?


Homework Equations



a = v^2/r, F = ma.


The Attempt at a Solution


Place the x-axis along the bank, and write the for equations for x and y:

\sum F_x = \frac{mv^2}{R}\cos\theta = mg\sin\theta + f_s
\sum F_y = 0 = F_n - \frac{mv^2}{R}\sin\theta - mg\cos\theta

It seems that the car should start to slide when
\frac{mv^2}{R}\cos\theta > mg\sin\theta + f_s

Using fs = \mu_s F_n

\frac{mv^2}{R}\cos\theta > mg\sin\theta + \mu_s\left(\frac{mv^2}{R}\sin\theta + mg\cos\theta\right)

Solving for v:

v > \sqrt{\frac{gR(\tan\theta + \mu_s/\tan\theta)}{1-\mu_s\tan\theta}

Unfortunately, the figure I get for v using R = 200, theta = 10, coefficient of static friction = 0.60 is much too high (88.6 m/s).

Could someone give me a hint about where I went wrong?

Thank you,
Sheldon
 
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In this term \mu_s mg\cos\theta, if one divides by cos\theta, then one does not get a tan function, but simply

\mu_s mg


So one would obtain

v > \sqrt{\frac{gR(\tan\theta + \mu_s)}{1-\mu_s\tan\theta}
 
Last edited:
Thank you, Astronuc. I am in your debt. What a stupid error :-)

Sheldon
 

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