Timeline for Finding a volume form on a fibre of a submersion between oriented manifolds
Current License: CC BY-SA 4.0
6 events
when toggle format | what | by | license | comment | |
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May 18, 2021 at 16:01 | comment | added | Georges Elencwajg | Thanks for your comments, @Hugocito. | |
May 16, 2021 at 18:48 | comment | added | Hugo | In the general case, I believe the construction is similar. Consider a local frame $b_1,\ldots,b_{n-p}$ on $M$ and extend it to a local frame $b_1,\ldots, b_n$ of X. Define $$\omega_M(b_1,\ldots,b_{n-p}) := \frac{\omega_X(b_1,\ldots,b_n)}{\omega_Y(df(b_{n-p+1}),\ldots,df(b_n))},$$ where $\omega_X$ and $\omega_Y$ are the volume forms of $X$ and $Y$. | |
May 16, 2021 at 18:43 | comment | added | Hugo | Obs.: In the above comment, I'm assuming the volume form of $X$ is constructed from a fixed Riemannian metric. | |
May 16, 2021 at 18:13 | comment | added | Hugo | One way of constructing the volume form on $M$ is the following: Consider a local orthonormal frame $b_1,\ldots,b_{n-p}$ tangent to $M$. We can complete the previous frame to an orthonormal frame on $X$ (by using Gram–Schmidt process). So, we have $b_1,\ldots,b_{n-p},b_{n-p+1},\ldots,b_n$. We can assume $df(b_{n-p+1}),\ldots, df(b_n)$ is compatible with the orientation on $Y$, and, rearranging $b_1,\ldots,b_{n-p}$, we can assume $b_1,\ldots,b_n$ is compatible with the orientation of $X$. The volume form on $X$ is defined by the formula $\omega(b_1,\ldots,b_{n-p}) = 1$. | |
May 11, 2021 at 13:46 | answer | added | alvarezpaiva | timeline score: 2 | |
May 10, 2021 at 20:18 | history | asked | Georges Elencwajg | CC BY-SA 4.0 |