Safe Speed of Frictionless Banked Turn

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SUMMARY

The discussion focuses on calculating the "safe speed" for a frictionless banked turn with a radius of 40.3 meters and a banking angle of 20.4 degrees. The key equations involve the components of the normal force and gravitational force acting on a car, with the centripetal force derived from these components. The correct approach involves setting up two equations based on the vertical and horizontal forces, leading to the final calculation of safe speed as 11.7 m/s. The initial attempt incorrectly calculated the parallel component of the weight, which led to an erroneous result.

PREREQUISITES
  • Understanding of centripetal force and its relation to circular motion
  • Familiarity with free-body diagrams and force components
  • Knowledge of trigonometric functions, specifically sine and cosine
  • Basic principles of Newton's laws of motion
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  • Study the derivation of centripetal force in banked turns
  • Learn how to construct and analyze free-body diagrams for various scenarios
  • Explore the effects of friction on banked turns and how it alters safe speed
  • Investigate the application of Newton's second law in circular motion problems
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Physics students, educators, and anyone interested in understanding the dynamics of banked turns and centripetal motion in real-world applications.

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Homework Statement



On banked turns, the horizontal component of the normal force exerted by the road reduces the need for friction to prevent skidding. In fact, for a turn banked at a certain angle, there is one speed for which no friction is required! The horizontal component of the normal force can provide all of the needed centripetal force. Find the so-called "safe speed" of a turn of radius 40.3 meters banked at 20.4 degrees. Hint: Draw a free-body diagram for a car on a frictionless banked turn. Then consider the net vertical force and the net horizontal force.

Homework Equations



2(pi)r/T = V
a = V^2/r
Fc = mac
w = mg
weight parallel = 9.8 * x * sin(20.4)
weight perp = 9.8 * x * cos(20.4)



The Attempt at a Solution



So what I start to do is I first find the weight
I assign m = 100kg to the car

so w = (100)(9.8)
so w = 980 N

then I find weight parallel to road

so 980 * sin (20.4)
= 341.6006064 N

so weight parallel to road will be equal in magnitude to parallel component of the normal force

so N = 341.6006064

which will need to equal centripetal force to keep it from slipping

so Fc = 341.6006064

so Fc = ma
so 341.6006064N/100 kg = a

a = 3.416006064

and a = V^2.r
so 3.416006064*40.3m = V^2

so V^2 = 137.7750444 m/s
so V = 11.7 m/s

but its wrong ...
 
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I think it is a mistake to find the component of mg parallel to the road.
The question suggests you find the x and y components of the normal force. Draw N perpendicular to the road and show its components N*sinθ and N*cosθ.
In the vertical direction, the forces on the car are one of those components and the force of gravity. Their total must be zero because the car does not accelerate upward or downward. That gives you equation [1].

In the horizontal direction, the question says the x component of N provides the centripetal force. Equation [2]. You can put the two equations together to eliminate N and find a nice simple expression for Fc which you can use to find the velocity.
 

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