Frictionless banked turn? What is wrong with my thinking?

Click For Summary

Homework Help Overview

The discussion revolves around a physics problem related to a frictionless banked turn at the Daytona International Speedway, specifically focusing on the speed required for cars to navigate a turn with a given radius and banking angle. Participants are analyzing the forces acting on the car and the conditions for maintaining circular motion.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the relationship between the normal force and gravitational components on a banked turn, questioning the assumptions made in the original calculations. There are attempts to clarify the role of the normal force in providing centripetal acceleration.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the forces involved. Some guidance has been offered regarding the treatment of normal force and its relation to the motion of the car on the banked turn, but no consensus has been reached on the correct approach.

Contextual Notes

Participants are working under the assumption that the turns are frictionless, which influences their analysis of the forces acting on the car. There is also a focus on the implications of the car maintaining a constant height while navigating the turn.

hey123a
Messages
37
Reaction score
0

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
 
Physics news on Phys.org
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 height. 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 height. 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
 
Last edited:
  • Like
Likes   Reactions: 1 person
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
 

Similar threads

  • · Replies 11 ·
Replies
11
Views
3K
  • · Replies 28 ·
Replies
28
Views
4K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 4 ·
Replies
4
Views
14K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 16 ·
Replies
16
Views
9K
  • · Replies 5 ·
Replies
5
Views
4K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 7 ·
Replies
7
Views
4K
  • · Replies 6 ·
Replies
6
Views
2K