What Speed Range is Safe for a Car on a Wet, Banked Curve?

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Homework Help Overview

The problem involves a banked curve with a specified radius and design speed, where the coefficient of static friction is provided for wet pavement. Participants are exploring the range of speeds at which a car can safely navigate the curve without slipping.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to calculate the maximum and minimum speeds using forces and friction, while some participants suggest drawing a free body diagram to clarify the forces involved. There are questions about the correctness of the calculations and the assumptions made regarding the normal force and friction.

Discussion Status

Participants are actively discussing the problem, with some providing guidance on the importance of free body diagrams and the application of Newton's laws. There is a recognition of potential errors in calculations, and the discussion is focused on clarifying concepts rather than reaching a consensus.

Contextual Notes

Participants note the complexity of the problem and the challenges of self-teaching from the course material. There is an emphasis on understanding the forces at play in both frictional and non-frictional scenarios.

Hydroshock
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Homework Statement



A curve of radius 60m is banked for a design speed of 100km/h. If the coefficient of static friction is 0.3 (wet pavement), at what range of speeds can a car safely make the curve?

v = 100km/hr = 27.8m/s
x = ?
r = 60m
a_r = 12.9m/s²
u = 0.3

Homework Equations



tan(x) = v²/rg
a_r = v²/r

The Attempt at a Solution



The part I'm stuck at is I know I'm missing an equation. The one that mass cancels out to find how the forces can give me the max speed etc. with the coefficient of friction.

tan(x) = (27.8)²/(60)(9.8) = 1.31
x = 52.6°

a_r = (27.8)²/60 = 12.9m/s²
 
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Don't go equation hunting; instead, draw a free body diagram showing all forces acting (including friction) for the two cases. Then apply Newton's 2nd law.

(An important first step is to solve for the angle of the road--and you've done that. Good.)
 
Alright, well to help myself out on drawing a free body diagram I made a nominal mass of 1000kg (although I do realize it's possible to do without one). so I got [tex]F_N = (1000)(9.8)sin(52.6) = 12900N[/tex] which in turn the force is the same as [tex]F_R[/tex] which is something I didn't exactly know was meant to happen. Although makes sense as it makes the speed for no friction.

(I'm taking an online course and I find just teaching myself from the book confusing as the work I'm meant to do isn't from the book)

So with [tex]F_N[/tex] I found [tex]F_fr = (.3)(12900) = 3870N[/tex]

From there I added and subtracted the forces to give me max and min for no slipping.

[tex]F_m_a_x = 16770N = (1000kg)A_r = 16.77m/s^2 = v^2/60m[/tex]
[tex]F_m_i_n = 9030N = (1000kg)A_r = 9.03m/s^2 = v^2/60m[/tex]

so

[tex]v_m_a_x = 31.7m/s = 114.1km/hr[/tex]
[tex]v_m_i_n = 23.3m/s = 83.9km/hr[/tex]

I think I did that right? =)
 
Hi Hydroshock,

I believe there are some problems with your calculations.

From your free body diagram for the first case (no friction), which direction is the acceleration in? (Here the normal force will not equal the perpendicular component of the weight.) Which direction is the normal force and weight in? Once you have those, choose components perpendicular and parallel to the acceleration and then use [itex]F_{{\rm net},x}=m a_x[/itex] for the x direction and similarly for the y direction.

The point of the case without friction is to find the angle that the road is banked at, so that you can use that angle for the other two cases.
 

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