The intersection of a plane and a sphere proof

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SUMMARY

The discussion focuses on proving that the second derivative of a unit speed parameterization of a circle, formed by the intersection of a plane and a sphere, is orthogonal to the sphere if and only if the plane passes through the origin. The sphere is defined by the equation x² + y² + z² = 1, while the plane is represented by the equation n·x = 0, where n is a normal vector to the plane. Key equations include the relationship between the second derivative q''(t) and the tangent plane of the sphere, as well as the implications of parameterization by arclength.

PREREQUISITES
  • Understanding of vector calculus, specifically dot products and orthogonality.
  • Familiarity with parameterization of curves, particularly unit speed parameterization.
  • Knowledge of the geometric properties of spheres and planes in three-dimensional space.
  • Ability to apply transformations, such as rotations, in three-dimensional geometry.
NEXT STEPS
  • Study the concept of unit speed parameterization in detail.
  • Learn about the properties of tangent planes to surfaces, particularly spheres.
  • Research vector calculus techniques for proving orthogonality between vectors.
  • Explore the application of rotations in three-dimensional geometry and their effects on equations of planes and spheres.
USEFUL FOR

Mathematics students, particularly those studying calculus and geometry, as well as educators seeking to understand the intersection of planes and spheres in three-dimensional space.

ky2345
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Homework Statement


When a plane intersects a sphere at more than two points, it is a circle (given). Let x^2+y^2+z^2=1 be a sphere S, and P be a plane that intersects S to make a circle (called C). Let q:[a,b] -> R^3 be a unit speed parameterization whose trace is C. Prove that the second derivative of q, q''(t), is orthogonal to S for all t iff P passes through the origin.


Homework Equations


- q''(t) is orthogonal to S at a specific point q(t_0) if q''(t) is orthogonal to the tangent plane of S at q(t_0)
- two vectors are orthogonal iff their dot product is zero (I'm letting * denote dot product)
- A curve is parameterized by arclength exactly when it has unit speed


The Attempt at a Solution


let P be the plane that intersects the origin, and let n be a vector that is orthogonal to P emitting from the origin. Then, an equation for the plane is n*x=0. The vector equation for the sphere is |x|^2=1, or x*x=1. Then, I can say that x*x+n*x=1 is an equation for the circle, or q(t)*q(t)+n*q(t)=1 if we plug in the parameterization. Now, differentiating with respect to t two times, I get that 2[q(t)*q''(t)+q'(t)*q'(t)]+n*q''(t)=0. I know that q'(t)*q'(t)=|q'(t)|^2=1 because q is unit speed. I'm stuck here because I don't know how to do the following two things:
(1) prove that q(t)*q''(t)=-1
(2) Then prove that since n and q''(t) are orthogonal for all t, q"(t) is orthogonal to the tangent plane at any given t_0 in [a,b]
 
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You can simplify your computations somewhat by applying a rotation so that P is parallel to the xy-plane. Now you should be able to write down the parametric equation for C explicitly.

It is not correct to say that \vec{x} \cdot \vec{x} + \vec{n} \cdot \vec{x} = 1 is an equation for C; this is an equation for a quadric surface which contains C. For example, if P is the xy-plane and \vec{n} = (0, 0, 1), the surface is the sphere x^2 + y^2 + z^2 + z = 1, or x^2 + y^2 + (z + \textstyle\frac12)^2 = \textstyle\frac54.
 
If I apply a rotation, and I know that (cos(t), sin(t)) is the arclength parameterization for a circle, then can I just use those formulas to prove that the acceleration is tangent to the sphere? How do I apply a rotation, should I just say I'm applying a rotation and viewing P as the xy plane, or do I have to somehow apply formulas to apply the rotation? If I use the (cos(t), sin(t) equations, I know that the acceleration is (-cos(t), -sin(t)). Now, how would I come up with the formula for the tangent plane to try to show that the acceleration is orthogonal?

Also, I have to do it in the other direction, that is, prove that if the acceleration vector is tangent to the sphere, then the plane P passes through the origin. However, since I can't assume my premise, I can't apply a rotation that time.
 

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