Normal reaction in banked road circular motion problem

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Discussion Overview

The discussion revolves around the equations of forces acting on a vehicle moving on a banked road during circular motion. Participants explore the conditions under which different equations apply, considering factors such as speed, friction, and the orientation of forces. The scope includes theoretical reasoning and mathematical formulation related to physics concepts.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants question whether the equation for forces parallel to the banked road should be expressed as R1 + R2 - mgcosθ = mV^2/r or R1 + R2 - mgcosθ = -mV^2/r.
  • One participant notes that the direction of friction depends on the speed of the vehicle, suggesting that the equation may vary based on whether the vehicle is moving slowly or quickly.
  • Another participant emphasizes the importance of defining variables and providing a diagram for clarity in understanding the problem.
  • Clarifications are made regarding the definitions of R1, R2, mg, V, and θ, with a focus on the angle's measurement and the direction of forces.
  • Concerns are raised about the absence of trigonometric factors in the equations, questioning their correctness based on the chosen coordinate system.
  • A hypothetical scenario is presented where the bank angle is zero, leading to simplified equations that highlight the necessity for R1 and R2 to be positive, thus challenging the validity of one of the proposed equations.

Areas of Agreement / Disagreement

Participants express differing views on the correct formulation of the equations and the influence of various factors, indicating that multiple competing perspectives remain without consensus.

Contextual Notes

Participants point out limitations related to the definitions of variables, the orientation of forces, and the assumptions made about the bank angle and speed, which may affect the applicability of the equations discussed.

physea
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What is the equation of forces please for the axis parallel to the banked road? Is it R1+R2-mgcosθ=mV^2/r or R1+R2-mgcosθ=-mV^2/r? Can you advise me please?
 
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physea said:
What is the equation of forces please for the axis parallel to the banked road? Is it R1+R2-mgcosθ=mV^2/r or R1+R2-mgcosθ=-mV^2/r? Can you advise me please?
The friction will be directly opposite mgsinθ if the car is going slow enough, but it will be the other way if the object is going fast enough. Therefore, the equation depends on which way the car is slipping. If it is in perfect equilibrium, then mgsinθ and friction cancel out and you're left with only components perpendicular to the road (such as the normal force and mgcosθ) causing the centripetal acceleration.
 
physea said:
What is the equation of forces please for the axis parallel to the banked road? Is it R1+R2-mgcosθ=mV^2/r or R1+R2-mgcosθ=-mV^2/r? Can you advise me please?
If you want an answer to that then it is probably better if you actually define all the variables in those equations, along with a suitable diagram. Also, you will get a better response if you can manage to be a bit more polite with your replies; the customer is not always right here because there are no (paying) customers. "That's all".
 
R1 and R2 are the normal reactions of the ground to the vehicle's wheels
mg is the vehicle weight
V it's speed
θ the angle of the banked road
I think now it's clear
 
physea said:
R1 and R2 are the normal reactions of the ground to the vehicle's wheels
mg is the vehicle weight
V it's speed
θ the angle of the banked road
Is the angle measured from the horizontal or from the vertical? Is positive for R1, R2 and the centripetal acceleration taken in the sense of an inward net force? I assume yes. Is positive for mg cos(θ) taken in terms of down=positive or up=positive. That would obviously have a key influence on the answer you seek.

Since you have adopted coordinates in which the centripetal acceleration is neither aligned with the x-axis or with the y-axis and have restricted your attention to the x axis, one would expect only part of the centripetal force (##\frac{mv^2}{r}##) to be relevant. Yet there is no cos(θ) or sin(θ) factor on the term to account for this. Similarly, there is no cos(θ) or sin(θ) factor on the terms for R1 or R2. So I have to question whether either equation can be correct.

Still, a simple argument can be made. If we select a track with a degenerate bank angle so that cos(θ) = 0 then the equations reduce to

##R_1 + R_2 = \frac{mv^2}{r}## and
##R_1 + R_2 = -\frac{mv^2}{r}##

Assuming a convention that positive is inward/up then ##R_1## and ##R_2## must be positive. ##\frac{mv^2}{r}## will neccessarily be positive. So the second equation is obviously wrong. Though, as above, that does not mean that the first equation must be right.
 

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