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I'm just looking for an example of an integral, rectifiable varifold, which has no locally bounded first variation.


Recapitulation

for every $m$-rectifiable varifold $\mu$ exists a $m$-rectifiable set $E$ in $\mathbb R^n$, meaning $E=E_0 \cup \bigcup_{k\in\mathbb N} E_k$ with $\mathcal H^m(E_0)=0$ and $E_k\subseteq F_k$ for some $\mathcal C^1$-manifolds $F_k$ of dimension $m$, and a non-negativ function $\theta\in L^1_{\text{loc}}(\mathcal H^m|_E)$ such that $\mu=\theta \mathcal H^m|_E$. This is a characterisation of $m$-recitifiable varifolds. The first variation $\delta\mu$ of a varifold $\mu$ is for $\eta\in\mathcal C^1_c(\mathbb R^n;\mathbb R^n)$ given by $$\delta\mu(\eta)=\int div_\mu\eta\,d\mu,$$ where $ div_\mu(\eta)(x) = \sum_{i=1}^n \tau_i^T(x)\cdot D\eta(x)\cdot \tau_i(x)$ where $\tau_i(x)$ is a orthogonal basis of the tangentspace of $\mu$ in $x$, which coinsidence $\mu$-almost everywhere with $T_xF_i$ for $x\in E_i\subseteq F_i$ as above. So $div_\mu\eta(x)$ is just the divergence in the manifold $F_i$, with $x\in E_i\subseteq F_i$.

We say $\mu$ has an locally bounded first variation, if for all $\Omega'\subseteq \Omega$ there exists $c(\Omega')<\infty$ such that $$ \delta\mu(\eta) \le C(\Omega',\Omega) \Vert \eta\Vert_{L^\infty(\Omega)} \qquad\forall\;\eta\in\mathcal C^1_c(\Omega'). $$ See for more explanation for example http://eom.springer.de/G/g130040.htm.

For a $\mathcal C^2$-manifold $M$ in $\mathbb R^n$ with mean curvature $H_M$ the first variation is $$ \delta M(\eta)=-\int_M H_M \cdot \eta \,dvol_M -\int_{\partial M} \tau_0 \cdot \eta \,dvol_{\partial M} \qquad\forall\;\eta\in\mathcal C_c^1(\mathbb R^n)$$ with the inner normal $\tau_0\in T_xM\cap(T_x\partial M)^\bot$ and where the mean curvature is the trace of the second fundamental form $A$ by the meaning of $H_M(x)=\sum_{i=1}^m A_x(\tau_i,\tau_i)$ in the normal space of $M$. As obviouse in this case the first variation is locally bounded.

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  • $\begingroup$ It would be better if you could recall definitions of varifold and its first variation. $\endgroup$ Jan 27, 2010 at 0:43
  • $\begingroup$ I don't know much about geometric measure theory, so I hope this question isn't too naive -- but what happens if you take $m=1$ or $m=2$ (curves and surfaces)? Is there obviously no example of the type you seek, or are even those cases still open? $\endgroup$
    – Yemon Choi
    Jan 28, 2010 at 19:38
  • $\begingroup$ even that case is open. But in fact the question here is just the first step of searching an counter-example for something else. And in that case curves can't work. But even a curves or a surface would help understanding what goes wrong in the case of an unbounded first variation... $\endgroup$
    – Elgrimm
    Jan 29, 2010 at 8:14
  • $\begingroup$ The link to eom.springer.de is broken, but the article can now be found at encyclopediaofmath.org/wiki/Geometric_measure_theory. $\endgroup$ Jul 5, 2022 at 0:01

2 Answers 2

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Something is strange here: it seems like for the sawtooth curve (the Lipschitz curve that goes up and down with slope $1$), the first variation is just the sum of $\delta$-measures at the turning points times the unit bisector vectors, so we can have fixed length and arbitrarily large first variation (just make turning points more and more dense), which can be now trivially turned into an example of finite area and infinite first variation: take more and more rigged closed sawtooth curves around infinitely many circles with finite some of radii contained in a compact domain. Am I missing something?

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  • $\begingroup$ no, that should work. I'll try to work out my counterexample out of that one. Thank $\endgroup$
    – Elgrimm
    Apr 15, 2010 at 19:12
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There are several ways to construct a rectifiable varifold which has no locally bounded first variation. To start let me rewrite the first variation for the m-varifold $v = V(E,\theta)$ by $$ \delta\mu(\eta) = \int_E \mathrm{div}_E(\eta)\,\theta d\mathcal{H}^m $$ Supposing for a moment $E$ is a smooth $C^2$ manifold with boundary and $\theta$ a smooth function, we obtain: $$ \delta\mu(\eta) = \int_E [\mathbf{H_E}\cdot \eta\,\theta + \nabla_E\theta \cdot \eta] d\mathcal{H}^{m} + \int_{\partial E} \eta\cdot \tau_0 \,d\mathcal{H}^{m-1} $$ In particular when $E = \{(x,0):\, x\in [a,b]\}$ and $\Omega=\mathbb{R}^2$ we have $$ \delta\mu(\eta) = \int_E \nabla_E\theta \cdot \eta \,d\mathcal{H}^{1} + \eta(a)\cdot (-1,0) + \eta(b) \cdot (1,0) $$ This formula suggests two easy ways of constructing a rectifiable varifold as the one you are looking for:

  • take as $\theta$ a function (of one variable) whose derivative is not a Radon-measure, that is a function that is not in $BV((a,b))$, in which case the "first term explodes"

  • glue together infinitely many (possibly disjoint) intervals so that "0-dimenstional length of the boundary explodes".

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