Given a unit speed curve κ=0, the following three are equivalent:
(a): α lies in a plane.
(b): B is a constant.
(c): τ=0 holds.
Explanation
This is a corollary of the Frenet-Serret formulas, allowing us to understand why torsion is defined in such a bizarre way as τ:=⟨B′,N⟩.
Proof
Frenet-Serret Formulas: If α is a unit speed curve with κ(s)=0, then
T′(s)=N′(s)=B′(s)=κ(s)N(s)−κ(s)T(s)+τ(s)B(s)−τ(s)N(s)
Part 1. (b)⟹(c)
Since B is a constant, B′=0, and by the Frenet-Serret formulas, τ=−⟨B′,N⟩=0.
Part 2. (c)⟹(b)
If τ=0, then by the Frenet-Serret formulas, B′=−τN=0.
Part 3. (a)⟹(b)
For convenience, assume α is on the xy-plane and appears as α(s)=(x(s),y(s),0).
T=α′(s)=(x′,y′,0)N=κ(s)T′(s)=κ1(x′′,y′′,0)
Thus,
B=T×N=κ1e1x′x′′e2y′y′′e300=κ1(0,0,κ)=(0,0,±1)
i.e., B is a constant. Though this is shown in the xy-plane, it can be generalized to all planes by merely changing the basis. Here, κ=∣x′y′′−x′′y′∣ is obtained through calculation2.
Part 4. (b)⟹(a)
It suffices to show that for some v∈R3, the following holds:
⟨α(s)−α(s0),v⟩=0
For v=B,
⟨α(s)−α(s0),B⟩′=⟨α′(s),B⟩+⟨α(s)−α(s0),B′⟩=⟨T,B⟩+⟨α(s)−α(s0),0⟩=0+0
Therefore, ⟨α(s)−α(s0),B⟩ remains unchanged for all s∈I, and specifically, if we set s=s0, then
⟨α(s)−α(s0),B⟩=0
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Millman. (1977). Elements of Differential Geometry: p31. ↩︎