Find Banking Angle and Normal/Friction Force on Curved Road

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SUMMARY

The discussion focuses on calculating the banking angle and forces acting on a car navigating a curved road with a radius of curvature of 65 m at a steady speed of 22 m/s. The proper banking angle is determined to be approximately 37 degrees using the formula θ = tan-1(v2 / (gr)). The normal force exerted by the highway on a 750-kg car at this angle is calculated to be approximately 9,200 N, while the friction force is approximately 5,600 N. The analysis emphasizes the distinction between centripetal force and frictional force in the context of banking curves.

PREREQUISITES
  • Understanding of centripetal force and its relationship with banking angles
  • Familiarity with trigonometric functions, specifically tangent
  • Knowledge of Newton's laws of motion
  • Basic principles of friction and normal force calculations
NEXT STEPS
  • Study the derivation of the banking angle formula in detail
  • Explore the effects of varying speeds on friction and banking angles
  • Learn about the role of coefficients of friction in banking scenarios
  • Investigate real-world applications of banking angles in highway engineering
USEFUL FOR

This discussion is beneficial for physics students, highway engineers, and anyone interested in the dynamics of vehicles on curved roads, particularly in understanding the forces at play during banking maneuvers.

logan3
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Homework Statement


A curved portion of highway has a radius of curvature of 65 m. As a highway engineer,
you want to bank this curve at the proper angle for a steady speed of 22 m/s.
(a) What banking angle should you specify for this curve?
(b) At the proper banking angle, what normal force and what friction force does the
highway exert on a 750-kg car going around the curve at the proper speed?

r = 65m
v = 22 m/s
g = 9.8 m/s^2
m = 750 kg

Homework Equations


F_{Ny} = F_N cos\theta = mg \Rightarrow F_N = \frac {mg}{cos\theta}
\vec F_c = \frac {mv^2} {r} = F_N sin\theta \Rightarrow (\frac {mg}{cos\theta}) sin\theta = \frac {mv^2} {r} \Rightarrow gtan\theta = \frac {v^2} {r} \Rightarrow \theta = tan^{-1}(\frac {v^2} {gr})
When the object is moving at constant velocity, the centripetal force will be the same as the force of friction.

The Attempt at a Solution


The wording "radius of curvature" is throwing me off, because we've never had it. I looked it up and pictures showed it as part of the circumference of the curved road, not the distance the to center. Nonetheless, I went ahead and treated "radius of curvature of 65 m" as simply r = 65m.

(a) \theta = tan^{-1}(\frac {(22 m/s)^2} {(9.8 m/s^2)(65m)}) = 37.227^o \sim 37^o
(b) F_N = \frac {mg}{cos\theta} = \frac {(750 kg)(9.8 m/s^2)}{(cos 37.227^o)} = 9,230.949 N \sim 9,200N
\vec F_f = \vec F_c = F_N sin\theta \Rightarrow (9,230.949 N)(sin 37.227^o) = 5,584.48N \sim 5,600N

Thank-you
 
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logan3 said:
\theta = tan^{-1}(\frac {v^2} {gr})
Good.
When the object is moving at constant velocity, the centripetal force will be the same as the force of friction.
That's only true on a horizontal surface. Here, those two forces act in different directions.

The Attempt at a Solution


I went ahead and treated "radius of curvature of 65 m" as simply r = 65m.
Good move.
\vec F_f = \vec F_c
Think about the logic/FBD behind your equation ##\vec F_c = F_N sin\theta##. What does that imply for \vec F_f?
 
I guess I'm a bit confused. Isn't there a different speed in order to prevent the car from sliding down the bank versus sliding up the bank? Where does the 22m/s fit in? Do I set the sliding down and up equations equal to each other and solve for the coefficient of friction, then use that to find the friction force?
 
logan3 said:
I guess I'm a bit confused. Isn't there a different speed in order to prevent the car from sliding down the bank versus sliding up the bank?
For a given coefficient of friction, yes. But what is meant by 'proper angle' here? You solved that part ok, yet friction never appeared in the analysis. Why do you think that is?
 

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