Finding the Radius of Gyration of a Racquet?

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Discussion Overview

The discussion revolves around calculating the radius of gyration of a racquet modeled as a uniform lamina, specifically focusing on its geometry defined by the equation r² = cos(2θ) and the implications of rotating it around different axes. Participants explore the mathematical formulation required for this calculation, including the determination of mass and moment of inertia, as well as the concept of the "sweet spot" related to the center of mass.

Discussion Character

  • Homework-related
  • Mathematical reasoning
  • Technical explanation

Main Points Raised

  • One participant seeks clarification on the formula for mass, suggesting it involves a double integral over specified limits.
  • Another participant notes that rotating about x=0 will yield a different moment of inertia compared to rotating around x=-1.
  • There is a suggestion to use area formulas for calculating the radius of gyration, specifically referencing the moment of inertia relative to the x-axis.
  • A correction is made regarding the limits of integration for θ, indicating they should be between -π/4 and π/4.
  • Discussion includes the need to find the mass moment of inertia with respect to the center of mass of the area, emphasizing the massless nature of the handle.
  • Participants mention the parallel axis theorem for calculating the moment of inertia when shifting the axis of rotation.
  • There is a note on how the distance from the centroid affects the radius of gyration and the resistance to rotation.

Areas of Agreement / Disagreement

Participants express various viewpoints on the limits of integration and the formulas to use, indicating that there is no consensus on the exact approach to take for calculating the radius of gyration and the sweet spot.

Contextual Notes

Participants highlight the importance of correctly identifying the limits of integration and the implications of the axis of rotation on the moment of inertia, but do not resolve these issues fully.

justagirl
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Radius of Gyration? REALLY need help ASAP!

Hey -

If any of you can help me with the following problem asap that would be awesome!

A racquet consists of uniform lamina that occupies the region inside the right-hand loop of r^2 = cos 2theta on the end of a handle (assumed to be of neglible mass) corresponding to the interval -1<=x<=0. Find the radius of gyration of the racquet around the line x = -1. Where is its sweet spot?

I know the radius of gyration around the y-axis can be found by the using the formula: radius of g = sqrt(Inertia around y-axis / mass)

Is this the correct formula for mass?

m = int(0...pi/4)int (0...sqrt(cos2theta) r cos theta r dr dtheta?

If so, how would revolving it around the line x = -1 instead of x = 0 change it?

Thanks!
 
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Rotating about x=0 would give you give different moment than rotating around x=-1 and different moment of inertia.

I think the limits of integration for theta are [tex]-\frac{\pi}{2}[/tex] and [tex]\frac{\pi}{2}[/tex].

IIRC, you want to find the center of mass of the racquet. The sweet spot is at the center of mass where the maximum transfer of momentum would occur.
 
Last edited:
justagirl said:
...

I know the radius of gyration around the y-axis can be found by the using the formula: radius of g = sqrt(Inertia around y-axis / mass)

Also consider doing this using the formulas for an area rather than a mass:
[tex]R=\sqrt{\frac{I_{x}}{A}}[/tex]
where [itex]I_{x}[/itex] is the moment of inertia of the area relative to the x axis.
 
Last edited:
Correction - the limits of [tex]\theta[/tex] are [tex]-\frac{\pi}{4}[/tex] and [tex]\frac{\pi}{4}[/tex]. Been awhile since I have done this stuff - I should have graphed it first.

The first step is to find the mass moment of inertia [tex]I_c[/tex] with respect to the area's center of mass (remembering that the handle is massless).

Then the moment of inertia through a parallel axis is just [tex]I = I_c + md^2[/tex], where [tex]m[/tex] is the mass of the area in question, and [tex]d[/tex] is the distance between the centroid (center of mass of the area) and axis about which the object would rotate.

So the handle goes from -1 to 0, and the lamina goes between 0 to 1. Let the distance from x=0 to the lamina centroid by [tex]d_c[/tex], then [tex]d\,=\,1\,+\,d_c[/tex]

Then once you know [tex]I[/tex],

radius of gyration g = [tex]\sqrt{\frac{I}{m}}[/tex].

If the axis of rotation was the y-axis (x=0), then [tex]d\,=\,d_c[/tex], and the radius of gyration would be less.

Remember, the greater the moment arm the more resistance to rotation, i.e. it would take more torque to get the same angular velocity.
 
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