Circular geodesics Consider the tube of radius $a > 0$ around a unit-speed curve $\gamma$ in $\mathbb{R}^3$ $$\sigma (s, \theta) = \gamma (s) + a(\cos \theta \ n(s) + \sin \theta \ b(s))$$ 
Show that the parameter curves on the tube obtained by fixing the value of $s$ are circular geodesics on $\sigma$. 
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Could you give me some hints how we could show that? 
Do we maybe use the fact that any normal section of a surface is a geodesic? 
 A: You can see geometrically that the normal at the surface at the point $\sigma(s,\theta)$ is the vector $N_\sigma(s,\theta) = n(s)\cos \theta + b(s)\sin \theta$. If $\alpha(\theta) = \sigma(s_0,\theta)$, then you can check that $\alpha$ is parametrized by arc-length, so it suffices to check that $\alpha''(\theta)$ is parallel to $N_\sigma(s_0,\theta)$ and you're done.
A: Hint: In general, if $\sigma'\times\left(\sigma'\times\sigma''\right)$ is perpendicular to the surface, then $\sigma$ is a geodesic. However, for a constant speed curve, we only need that $\sigma''$ is perpendicular to the surface since
$$
a\times(a\times b)=\frac{b\cdot a}{a\cdot a}\,a-b
$$
and $\sigma'\cdot\sigma''=0$ for a constant speed curve.

From Comments: Two surface tangents are
$$
\partial_s\sigma=t+a(\cos(\theta)\,n'+\sin(\theta)\,t\times n')\tag{1}
$$
and
$$
\tilde\sigma'=\partial_\theta\sigma=a(-\sin(\theta)n+\cos(\theta)t\times n)\tag{2}
$$
Since
$$
\tilde\sigma''=\partial_\theta^2\sigma=-a(\cos(\theta)n+\sin(\theta)t\times n)\tag{3}
$$
is perpendicular to both, it is perpendicular to the surface. Therefore, $\tilde\sigma$ is a geodesic for each $s$.
A: HINT:
Any curve of intersection produced by normal section of this argument cannot or should not be used for arriving at the result. One special case is a sphere cut along any great circle.
