Find Banking Angle and Normal/Friction Force on Curved Road

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Homework Help Overview

The problem involves determining the banking angle for a curved highway with a specified radius of curvature and speed, as well as calculating the normal and friction forces acting on a car traveling along this curve. The subject area includes dynamics and circular motion.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the interpretation of the radius of curvature and its application in the problem. There are attempts to calculate the banking angle and forces involved, with some questioning the role of friction in the analysis. Others raise concerns about the implications of different speeds for sliding up or down the bank.

Discussion Status

The discussion is ongoing, with participants exploring various interpretations of the problem and the relationships between forces. Some guidance has been offered regarding the treatment of forces on a banked curve, but there is no explicit consensus on the role of friction or the implications of the given speed.

Contextual Notes

Participants note confusion regarding the definition of "proper angle" and the absence of friction in certain analyses. There is also mention of the need to consider different speeds to prevent sliding in either direction on the banked curve.

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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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