condition for curve on a sphere

Let $\alpha (t)$ be a curve such that $|\alpha'(t)|=1$ for all $t\in\mathbb R$. Assume $k(t)\neq 0$, $k'(t)\neq 0$ (whereas $k=|\alpha”(t)|$ is the curvature) and $\tau(s)\neq 0$, whereas $\tau$ is the torsion.

Prove: The trace of $\alpha$ lies on a sphere $\Leftrightarrow$ $\frac{1}{k^2} +\frac{1}{(k’\cdot\tau)^2}=$const.$>0$.

I know this somehow works by using the Frenet-Serret-equations, but I don’t really know how to do this proof. Can anyone help me out? Thanks!

Solutions Collecting From Web of "condition for curve on a sphere"

Your equation is incorrect, the correct condition is

$$\frac{1}{\kappa^2} + \left(\frac{\dot{\kappa}}{\tau\kappa^2}\right)^2 = \text{constant}$$

I will only show the $\Leftarrow$ part here.

Let $s$ be the arc length parametrization and $\vec{t}(s), \vec{n}(s), \vec{b}(s)$ be the
vectors appear in Frenet Serret equations. Define
$$\vec{\beta}(s) = \vec{\alpha}(s) + \frac{1}{\kappa(s)}\vec{n}(s) – \frac{\dot{\kappa}(s)}{\tau(s)\kappa(s)^2} \vec{b}(s)\tag{*1}$$
Differentiate it with respect to $s$, we get:

= & \vec{t} – \frac{\dot{\kappa}}{\kappa^2}\vec{n} + \frac{1}{\kappa}(-\kappa \vec{t} + \tau \vec{b} )
– \frac{d}{ds}\left(\frac{\dot{\kappa}}{\tau\kappa^2}\right)\vec{b} -\frac{\dot{\kappa}}{\tau\kappa^2}(-\tau\vec{n})\\
= & \left(\frac{\tau}{\kappa} -\frac{d}{ds}\left(\frac{\dot{\kappa}}{\tau\kappa^2}\right)\right) \vec{b}\\
= & \frac{\tau\kappa^2}{\dot{\kappa}}\left(\frac{\dot{\kappa}}{\kappa^3} – \frac{\dot{\kappa}}{\tau\kappa^2}\frac{d}{ds}\left(\frac{\dot{\kappa}}{\tau\kappa^2}\right) \right) \vec{b}\\
= & -\frac{\tau\kappa^2}{2\dot{\kappa}}\frac{d}{ds}\left(\frac{1}{\kappa^2} + \left(\frac{\dot{\kappa}}{\tau\kappa^2}\right)^2\right) \vec{b}\\
= & \vec{0}
This implies $\vec{\beta}(s) = \vec{\beta}(0)$ is a constant. From this, we get

\vec{\alpha} – \vec{\beta}(0)
= -\frac{1}{\kappa}\vec{n} + \frac{\dot{\kappa}}{\tau\kappa^2} \vec{b}
\quad\implies\quad \left|\vec{\alpha} – \vec{\beta}(0)\right|^2
= \frac{1}{\kappa^2} + \left(\frac{\dot{\kappa}}{\tau\kappa^2}\right)^2
= \text{constant}.
i.e $\vec{\alpha}(s)$ lies on a sphere with $\beta(0)$ as center.

Motivation of above proof

You may wonder how can anyone figure out the magic formula in $(*1)$. If you work out the
$\Rightarrow$ part of the proof where $\alpha(s)$ lies on a sphere centered at $\vec{c}$,
you should obtain a bunch of dot products between $\vec{\alpha}(s) – \vec{c}$ and $\vec{t}(s)$, $\vec{n}(s)$ and $\vec{b}(s)$. In particular, you should get:
\vec{t} \cdot (\vec{\alpha} – \vec{c}) & = 0\\
\vec{n} \cdot (\vec{\alpha} – \vec{c}) & = -\frac{1}{\kappa}\\
\vec{b} \cdot (\vec{\alpha} – \vec{c}) &= \frac{\dot{\kappa}}{\tau\kappa^2}

Using these, you can express the center $\vec{c}$ in terms of $\kappa, \tau$ like what we have in $(*1)$. If the curve does lie on a sphere, then the “center” should not move as $s$ changes. The proof of the $\Leftarrow$ part above is really using the given condition to verify the “center” so defined doesn’t move.