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Total Variation in Differential Geometry 📂Geometry

Total Variation in Differential Geometry

Definition1

A regular curve γ\gamma is considered piecewise simple curve with a period of LL being a closed curve. Let Z(t)\mathbf{Z}(t) be a continuous vector field along γ\gamma. Suppose the vector field V\mathbf{V} satisfies V(p)=1\left| \mathbf{V}(p) \right| = 1 pU\forall p \in U. Let α\alpha be a function mapping the angle between Z\mathbf{Z} and V\mathbf{V}.

α(t)=(V(γ(t)),Z(t)) \alpha (t) = \angle \left( \mathbf{V}(\gamma (t)), \mathbf{Z}(t) \right)

Now, the total angular variation δVα\delta_{\mathbf{V}} \alpha of the vector field Z\mathbf{Z} along γ\gamma with respect to V\mathbf{V} is defined as follows.

δVα:=0Ldα(t)dtdt \delta_{\mathbf{V}}\alpha := \int_{0}^{L} \dfrac{d \alpha (t)}{d t} dt

Explanation

From t=0t=0 to t=Lt=L, it represents how much the direction of Z\mathbf{Z} changes (in reference to V\mathbf{V}).

By definition, δVα\delta_{\mathbf{V}}\alpha generally depends on V\mathbf{V}, but there are cases where it does not depend on V\mathbf{V} depending on the nature of the curve γ\gamma.

Theorem

Let the curve γ\gamma be a null-homotopic enclosing a region R\mathscr{R}. Then δVα\delta_{\mathbf{V}}\alpha does not depend on the choice of V\mathbf{V}.


  1. Richard S. Millman and George D. Parker, Elements of Differential Geometry (1977), p182 ↩︎