Osculating circle for 3D curve

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SUMMARY

The discussion focuses on deriving the parametrized equation for the osculating circle of the space curve defined by r(t) = . The key components include the Frenet frame T(p), N(p), and B(p), along with the radius of curvature c(p) = ((2p^2 + 1)^2)/2. The center of curvature is calculated as r(p) + N(p)c(p). The user explores methods to represent the osculating circle using both the intersection of the osculating sphere and plane, and considers the implications of 3D rotations for constructing the circle.

PREREQUISITES
  • Understanding of space curves and parametrization
  • Familiarity with the Frenet-Serret formulas
  • Knowledge of 3D geometry and rotations
  • Experience with matrix algebra for solving linear systems
NEXT STEPS
  • Study the Frenet-Serret formulas in detail
  • Learn about 3D rotations and their applications in geometry
  • Explore the use of parametric equations for curves and surfaces
  • Investigate software tools like Winplot for visualizing mathematical concepts
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Students and educators in mathematics, particularly those studying differential geometry, as well as software developers and engineers working with 3D modeling and visualization.

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Homework Statement


Given the space curve r(t)=<t^2,(2t^3)/3,t>, give the parametrized equation for the osculating circle along the trajectory at r(p).

I should note this is so I can give a plot of the circle in Winplot, which is a free grapher/plotter type program.

Homework Equations


From r(t), the Frenet frame is:
T(p)=<2p,2p^2,1>/(2p^2+1)
N(p)=<1-2p^2,2p,-2p>/(2p^2+1)
B(p)=<-2p,1,2p^2>/(2p^2+1)

the radius of curvature is c(p)=((2p^2+1)^2)/2
so the expression for centers of curvature is:

<p^2,(2p^3)/3,p> + <1-2p^2,2p,-2p>(2p+1)/2 = r(p) + N(p)c(p)


The Attempt at a Solution



Ok my first crack at this was to try and solve it as the intersection of the osculating sphere and osculating plane, which would give a circle. So the osculating plane's equation would be

(x-p^2)(-2p)/(2p^2+1) + (y-(2p^3)/3)/(2p^2+1) + (z-p)(2p^2)/(2p^2+1) = 0

then I chose to represent the sphere as a parametric surface:
defining x0 = (1-p^2)(2p^2+1)/2
y0 = (2p^3+6p)(2p^2+1)/6
z0 = (-p)(2p^2+1)/2
are the x, y, and z components of the center of curvature respectively.

x = c(p)cos(θ)sin(φ) + x0
y = c(p)sin(θ)sin(φ) + y0
z = c(p)cos(φ) + z0

so then I rearranged the plane's equation for x, y, and z separately, and set them equal to the parametric equation. I don't think I have to say that the equations were quite big, but I noticed that they were a linear system, so I solved it by using matrices. I'm going to stop right here because this approach didn't give me anything useful, problem #1 of which was that the parametric representation of the intersection would necessarily have been an expression of 2 parameters, giving a surface, while only 1 parameter is required for a curve, which is what I need.

I have a nagging feeling that I'm overlooking something very simple that could make this problem a lot easier. Might I be able to construct the circle, then rotate it so that it fits into place? I'm not too well versed on how to do 3d rotations.
 
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I have an idea. You already have the following quantities:
- The point r(p)
- The unit normal n(p)
- The radius of curvature c(p)
Then the center of the osculating circle is r(p)+c(p)N(p).
So now you have a center, radius and normal B(p) to the circle,
it shouldn't be hard if you find the right formulas...
 

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