second_fundamental_form
Differences
This shows you the differences between two versions of the page.
| Both sides previous revisionPrevious revisionNext revision | Previous revision | ||
| second_fundamental_form [2023/06/19 15:11] – [Second Fundamental Form] spencer | second_fundamental_form [2023/06/19 15:16] (current) – [Second Fundamental Form] spencer | ||
|---|---|---|---|
| Line 2: | Line 2: | ||
| The second fundamental form (which I usually write II and pronounce " | The second fundamental form (which I usually write II and pronounce " | ||
| - | If $\nu$ denotes the (outward) unit normal to immersed hypersurface $M^{n-1} \subset (N^n, g)$ and $eta$ denotes its metric dual, then | + | If $\nu$ denotes the (outward) unit normal to immersed hypersurface $M^{n-1} \subset (N^n, g)$ and $\eta$ denotes its metric dual, then |
| $$Q(X,Y) := g(\nabla_X \nu, Y).$$ | $$Q(X,Y) := g(\nabla_X \nu, Y).$$ | ||
| Complete $\nu$ to a frame $e_1, \ldots, e_{n-1}, e_n := \nu$ around a point of $M$ with coframe $\omega^1, \ldots, \omega^n := \eta$. | Complete $\nu$ to a frame $e_1, \ldots, e_{n-1}, e_n := \nu$ around a point of $M$ with coframe $\omega^1, \ldots, \omega^n := \eta$. | ||
| - | Then $\nabla_{e_i} \nu = h_{ij} \omega^j$ for some $h_{ij}$ and we accordingly define on forms that | + | Then $\nabla_{e_i} \eta = h_{ij} \omega^j$ for some $h_{ij}$ and we accordingly define on forms that |
| $$Q(\alpha) = h_{ij} e(\omega^i)e^*(\omega^j) \alpha.$$ | $$Q(\alpha) = h_{ij} e(\omega^i)e^*(\omega^j) \alpha.$$ | ||
| The second fundamental form is symmetric, hence diagonalizable; | The second fundamental form is symmetric, hence diagonalizable; | ||
| Line 13: | Line 13: | ||
| The mean curvature is a scalar-valued function on $M$ defined as $H = \sum h_{ii}$; that is, $H$ is the trace of $Q$. | The mean curvature is a scalar-valued function on $M$ defined as $H = \sum h_{ii}$; that is, $H$ is the trace of $Q$. | ||
| One important place where the trace arises is in | One important place where the trace arises is in | ||
| - | $$Q \mathrm{vol} = H \mathrm{vol}, | + | $$Q(\mathrm{vol}) = H \mathrm{vol}, |
| used in the (Stern--di Cerbo) global computation of [[monotonicity|Price monotonicity]], | used in the (Stern--di Cerbo) global computation of [[monotonicity|Price monotonicity]], | ||
| + | This relation holds applied to the volume form of $M$ or $N$, and is a consequence of the fact that after contracting along the $e_i$ direction, the only non-zero wedge product possible is along the $e_i$ direction as the volume form has all other terms remaining. | ||
| + | This behaviour could differ on other $(n-1)$-forms along $M$ in $N$ that are not proportional to the volume form, as for example $\omega^2 \wedge \cdots \wedge \omega^n$ would be missing the $h_{11}$ contribution. | ||
second_fundamental_form.1687201905.txt.gz · Last modified: by spencer
