Banked Roadway Design for Ice Conditions: Solving for Optimal Angle

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Homework Help Overview

The discussion revolves around the design of a banked roadway intended for icy conditions, specifically focusing on calculating the optimal angle for banking a curve so that a car can navigate it without relying on friction. The parameters include a designated speed of 13.4 m/s and a curve radius of 35.0 m.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between forces acting on a car on a banked curve, questioning the relevance of centripetal acceleration and the appropriate use of equations involving angles and forces. Some participants discuss the implications of measuring the radius to the center of mass of the car.

Discussion Status

The discussion is active, with participants providing insights into the forces at play and clarifying misconceptions about the direction of centripetal acceleration. There is an ongoing exploration of different approaches to defining the problem and the forces involved.

Contextual Notes

Participants note the importance of considering the frame of reference when discussing forces, particularly distinguishing between centrifugal force and inertial frames. There is also mention of an attached sheet that offers an intuitive solution, though its contents are not detailed in the discussion.

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Homework Statement


A civil engineer wishes to redesign the curved roadway in Interactive Example 5.7 in such a way that a car will not have to rely on friction to round the curve without skidding. In other words, a car moving at the desig- nated speed can negotiate the curve even when the road is covered with ice. Such a curve is usually banked, meaning that the roadway is tilted toward the inside of the curve. Suppose the designated speed for the curve is to be 13.4 m/s (30.0 mi/h) and the radius of the curve is 35.0 m. At what angle should the curve be banked?

5-13.gif


Homework Equations


nsin(theta) = mv2 /r
ncos(theta) = mg
tan(theta) = v2/rg

The Attempt at a Solution


I had thought that looking at horizontal movement on the slope you would use mgsin(theta) = mv2/r, so that the force is parallel with the slope. Why are we not doing this? Thanks.
 
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Wouldn't it depend on how you measured r?
 
You can assume r is measured to the COM of the car.

scharry03 said:

The Attempt at a Solution


I had thought that looking at horizontal movement on the slope you would use mgsin(theta) = mv2/r, so that the force is parallel with the slope. Why are we not doing this? Thanks.

For problems like this it is often easier to define an axis parallel to the slope and work that way. Then you can ignore the normal force as it makes no contribution to what you are interested in; what theta is when all forces parallel to the slope sum to zero.

With that said, the force due to the centripetal acceleration is not parallel to the slope, it's horizontal. so your expression mgsin(theta) = mv2/r will not give the correct answer. Those two force vectors are not collinear.
 
Okay, I didn't realize that centripetal acceleration wasn't parallel with the slope, but now that I think about it, that makes complete sense. Thanks!
 
Have a look at the sheet i have attached, note that its an intuitive solution.
 

Attachments

dean barry said:
Have a look at the sheet i have attached, note that its an intuitive solution.
For neutral banking, the banking will be perpendicular to the force resultant (F3)
You should clarify that that is using the centrifugal force view, not an inertial frame.
 

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