Can Differential Geometry Solve This Challenging Curve Containment Problem?

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SUMMARY

The discussion focuses on proving the relationship between a non-degenerate unit speed curve \(\sigma:I\rightarrow R^{3}\) and its containment within a sphere \(S_{R}(p)\). The key conclusion is that the existence of a center \(\vec{p}\) such that \(\sigma(I)\subset S_{R}(p)\) is equivalent to finding an angle \(\phi\) satisfying the equation \(\frac{1}{\kappa(s)}=R\cos(\phi+\int_{s_{0}}^{s}\tau(\lambda)d\lambda)\) for all \(s\in I\). The discussion emphasizes the application of Frenet equations and the geometric implications of torsion and curvature in relation to the sphere's radius.

PREREQUISITES
  • Understanding of Frenet-Serret formulas
  • Knowledge of curvature (\(\kappa\)) and torsion (\(\tau\)) in differential geometry
  • Familiarity with the geometric properties of spheres in \(\mathbb{R}^{3}\)
  • Basic proficiency in calculus and integration techniques
NEXT STEPS
  • Study the application of Frenet-Serret equations in curve analysis
  • Learn about the geometric interpretation of curvature and torsion
  • Explore the properties of curves constrained to spherical surfaces
  • Investigate the relationship between curvature, torsion, and the radius of curvature
USEFUL FOR

This discussion is beneficial for students and researchers in differential geometry, particularly those interested in the geometric properties of curves and their applications in higher-dimensional spaces.

Dahaka14
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Homework Statement



Let \sigma:I\rightarrow R^{3} be a non-degenerate unit speed curve, and R be a real number >0. Fix a value s_{0}\in I. Prove that:

(There exists a center \vec{p}\in R^{3} such that \sigma(I)\subset S_{R}(p))\iff (There exists an angle \phi\in R such that, for all s\in I, \frac{1}{\kappa(s)}=R\cos(\phi+\int_{s_{0}}^{s}\tau(\lambda)d\lambda)).

Homework Equations



I know all of the equations for Frenet, but I'm not sure how to apply them.

The Attempt at a Solution



No idea where to start...I have been staring at this problem for many days now, and I haven't a clue what to do. Please help!
 
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might be a start that the curve is constrained to a sphere so t will be tangent to the sphere

define
r = sigma-p

then
t.r = 0

differentiating and some frenet substitution gets to
1/k(s) = -n.r

this is a step closer to the equation...
 
also worth thinking about this physically.. when the torsion is zero, the curve can be contained in a plane, and a plane intersecting a sphere gives a circle

the largest circle is a great circle of the sphere, & on this path the normal will point towards the centre of the circle

so where does the normal point as the radius of the circle is made smaller? and how does the torsion relate to a change in radius?
 

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