Determine a formula for the angle at which a road should be banked

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Homework Help Overview

The discussion revolves around determining a formula for the angle at which a road should be banked for a car traveling around a curve without relying on friction. The problem involves concepts from dynamics and circular motion, specifically centripetal force and the forces acting on an inclined plane.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster attempts to derive a formula using free body diagrams and equations related to forces acting on the car. Some participants question the clarity of the original poster's notation and reasoning, while others suggest focusing on the components of forces involved in circular motion.

Discussion Status

Participants have explored different approaches to the problem, with one suggesting a formula involving arctangent for calculating the banking angle. There is acknowledgment of confusion in the original calculations, and some guidance has been provided to clarify the relationships between forces.

Contextual Notes

There is a mention of unit conversion from kilometers per hour to meters per second, which is relevant for the calculations involved in determining the banking angle.

HawKMX2004
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I'm having some problem on my forces homework. Please help, I believe my answer is wrong, and I'm starting to get frustrated :mad:

Q: For a car traveling with speed 's' around a curve of radius 'r', determine a formula for the angle at which a road should be banked so that no friction is required to keep the car on the road. Then, find the angle for a curve of radius 50 m at a speed of 50 km/h.

I drew a Free Body diagram of an Inclined Plane, and the Circle the car is traveling. The following is my equations

NetForce(Y-direction)=Fn(ForceNatural) - Fgy(ForceGravity*Ydirection*) = 0
Nfy = Fn = Fgy
Nfy = Fn = Fg(Cos(Theta))

Nfc(Netforcecentrifical) = Ff(ForceFriction) = m(v^2)/r
Nfc = FnUs = m(v^2)/r
Nfc = Fg(Cos(Theta))Us = m(v^2)/r
Nfc = ma(cos(Theta))Us = m(v^2)/r mass cancels out
Nfc = a(cos(Theta))Us = v^2/r
Nfc = cos(Theta)Us = v^2/r(a) Us = V^2/r(a)
Nfc = cos(Theta) = (v^2)Us/r(a)
Nfc = Theta = cos^-1[(v^2)Us/r(a)]
Nfc = Thata = cos^-1[v^2(v^2)/ra(ra)]
Nfc = Thata = cos^-1[v^4/r^2(a^2)] <------ Final Equation

Nfc = Thata = cos^-1[50^4/50^2(9.8^2)]
Nfc = Theta = 89.9 Degrees <---- Final Answer


I think i did something terribly wrong, that answer doesn't seem right. Help would be very greatly appreciated...Thankz
 
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I'm afraid I gave up following your solution early on. Not your fault - it's just difficult to read without the standard notation. *sigh* One of these days, I have to take the time to learn to do that.

Anyway - think about the problem. The car is traveling in a circle, which means that there must be a centripetal force directed towards the center of the circle. You have two questions to answer: 1) Where is the center of that circle and 2) What provides the centripetal force?

The answer to 1 is pretty easy: envision the path of the car. It'll make a circle, and the center of the circle is the center for which you're looking. Note that the center will not be on the ground. One mistake some students make is putting the center on the ground in the middle of the curve.

For 2, there's really only one answer as well: the centripetal force is provided by the component of the normal force pointing towards that center. That component will be parallel to the ground. You have to find the banking angle that makes that component equal to the centripetal force necessary to hold the car in the circle.

I hope that helps - if not, post again and tell me where it fails, and we'll try it again.
 


I got that, that was 89.9 degrees, which i find wrong...do you have any other suggestions or equations i might be able to use?
 
OK - I did the problem quickly and ended up with

theta = Arctan(v^2/rg)

Keeping proper track of the units (remember - you have the speed in kph and you need it in m/s), I end up with an angle of 21.5 degrees.

Part of the key to this is realizing that the component of the normal force perpendicular to the ground has to cancel out the weight.

Does this help any?
 
Yes it does! I understand it now, somewhere I lost track of what i was doing but yes now it makes sense. Thank you very much!
 

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