Frictionless banked turn? What is wrong with my thinking?

AI Thread Summary
The discussion revolves around calculating the speed required for cars to navigate frictionless, banked turns at the Daytona International Speedway, with a maximum radius of 316 meters and a banking angle of 31 degrees. Initial calculations yielded a speed of 36.9 m/s, but the correct speed is actually 43 m/s. Participants clarify that the normal force on a banked turn does not equal mgcosθ, as the car maintains a constant height while providing centripetal force. The conversation emphasizes the importance of understanding the forces acting on the car to maintain circular motion. Accurate force analysis is crucial for solving such physics problems effectively.
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Homework Statement


The Daytona 500 is the major event of the NASCAR season. It is held at the Daytona International Speedway in Daytona, Florida. The turns in this oval track have a maximum radius (at the top) of r = 316, and are banked steeply, with θ = 31°. Suppose these maximum-radius turns were frictionless. At what speed would the cars have to travel around them?


Homework Equations


Fc = mv^2/r



The Attempt at a Solution


εfx = Fac = Nx
(mv^2)/r = sinθN
(mv^2)/r = sinθ(-wcosθ)
(mv^2)/r = sinθ(-mgcosθ)
v = √[sinθ(-gcosθ)r]
v = √[sin31°(-(-9.8))(cos31°)(316)]
v = 36.9m/s

answer is actually 43m/s
 
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hey123a said:

Homework Statement


The Daytona 500 is the major event of the NASCAR season. It is held at the Daytona International Speedway in Daytona, Florida. The turns in this oval track have a maximum radius (at the top) of r = 316, and are banked steeply, with θ = 31°. Suppose these maximum-radius turns were frictionless. At what speed would the cars have to travel around them?

Homework Equations


Fc = mv^2/r

The Attempt at a Solution


εfx = Fac = Nx
(mv^2)/r = sinθN
(mv^2)/r = sinθ(-wcosθ)
(mv^2)/r = sinθ(-mgcosθ)
v = √[sinθ(-gcosθ)r]
v = √[sin31°(-(-9.8))(cos31°)(316)]
v = 36.9m/s

answer is actually 43m/s

Omit the minus signs, as you use magnitudes.

Check the figure. Is N=mgcosθ?



ehild
 
ehild said:
Omit the minus signs, as you use magnitudes.

Check the figure. Is N=mgcosθ?



ehild

yes, on an incline the normal force is equal to the magnitude of the y component of the weight. the y component of the weight is equal to mgcosθ
 
hey123a said:
yes, on an incline the normal force is equal to the magnitude of the y component of the weight. the y component of the weight is equal to mgcosθ

It is true if an object slides on a slope. Now, the car does not slide but stays at a constant hight. The vertical component of the normal force opposes the weight. The horizontal component of the normal force provides the centripetal force.
ehild
 
ehild said:
It is true if an object slides on a slope. Now, the car does not slide but stays at a constant hight. The vertical component of the normal force opposes the weight. The horizontal component of the normal force provides the centripetal force.
ehild

why is it only true if the object slides on a slope?
 
The normal force is a force of constraint. It ensures that the body performs the constrained motion. Its magnitude depends on the motion.

In case of sliding along a slope, the body can not rise from the surface, neither can it penetrate into the surface: there is a force balancing the normal component of gravity: the normal force is equal to -mgcosθ.

Here the car has to travel along a horizontal circle with speed V. If the normal force was equal to -mgcosθ, the resultant force would be parallel to the slope, and downward, with magnitude mgsinθ. But the circular motion to be maintained, the resultant force has to be horizontal, and equal to mV2/R.

ehild
 
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ehild said:
The normal force is a force of constraint. It ensures that the body performs the constrained motion. Its magnitude depends on the motion.

In case of sliding along a slope, the body can not rise from the surface, neither can it penetrate into the surface: there is a force balancing the normal component of gravity: the normal force is equal to -mgcosθ.

Here the car has to travel along a horizontal circle with speed V. If the normal force was equal to -mgcosθ, the resultant force would be parallel to the slope, and downward, with magnitude mgsinθ. But the circular motion to be maintained, the resultant force has to be horizontal, and equal to mV2/R.

ehild
ah okay thanks
 

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