How Do You Derive the Constraint Equation for a Disc Rolling Along a Parabola?

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SUMMARY

The discussion focuses on deriving the constraint equation for a disc of radius R rolling without slipping along the parabola defined by the equation y = ax². The key equations established are R dθ = ds and ds = √(1 + 4a²x²) dx, which must be equated to derive the constraint equation. The conversation also references a generalization of the constraint equation for arbitrary curves, emphasizing the importance of understanding the angles θ and φ in relation to the disc's motion. A visual diagram is recommended for clarity in understanding the relationships between these angles.

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  • Understanding of calculus, particularly derivatives and integrals.
  • Familiarity with the geometry of curves, specifically parabolas.
  • Knowledge of angular motion and rolling without slipping conditions.
  • Ability to interpret and manipulate equations involving trigonometric functions.
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  • Study the derivation of constraint equations for different types of curves.
  • Learn about the dynamics of rolling motion in physics, focusing on non-slip conditions.
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QuantumDuality
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Homework Statement


A disc of radius R rolls without slipping along the parabola y= ax2. Obtain the constrain equation

Homework Equations


Because there's no slipping, then:
##R d \theta = ds (1)##
Where ##\theta ## is the angle between the line from the center of the disc to a fixed point and the line from the center of the disc to the contract point with the parabola
Also:
##ds = \sqrt{(dx)^2 + (dy)^2} = \sqrt{1 + 4a^2 x^2} dx (2)##

The Attempt at a Solution


So I just have to equate (1) and (2) to get the constraint equation?, Because I have seen a generalization of the constraint equation for an arbitrary curve that use

##ds = R(d\theta + d\phi) ##

Where ##\theta## is an angle between a radius to a fixed point and the radius parallel to the y axis, while ##\phi## is an angle between the radius parallel to the y-axis and the radius to the contact point
Here's the generalization:

https://campus.mst.edu/physics/courses/409/Problem-Solutions/HW#4/HW4_prob3_ hoop on curve.pdf
 
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Your problem statement says, "... rolls along ... the parabola..." Is the disk in the plane of the parabola, perhaps normal to the plane of the parabola, or something else again?
 
QuantumDuality said:
Because there's no slipping, then:
##R d \theta = ds (1)##
Where ##\theta ## is the angle between the line from the center of the disc to a fixed point and the line from the center of the disc to the contract point with the parabola
Took me a while to realize you meant a point fixed on the perimeter of the disc.
QuantumDuality said:
Where θ is an angle between a radius to a fixed point and the radius parallel to the y axis, while ϕ is an angle between the radius parallel to the y-axis and the radius to the contact point
I think if you draw a diagram you will find that your θ equals their θ+φ+constant.
 
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