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Orientability of Regular Zero Set.

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A manifold M of dim n is orientable if there exists a smooth nowhere vanishing n form on M. On a regular zero set in R^{n+1}, there is always a nowhere vanishing n-form so Regular Zero sets in R^{n+ 1} are orientable manifolds. For example if S is cut out by f in R^3 then differentiating (f dy = 0) gives f_x dx dy = f_z dy dz. Thus we have dx dy/ f_z = dy dz/ f_x = dx dz / f_y whenever this expression makes sense. Gluing them gives a nowhere vanishing 2 form on S. In particular the sphere S2 is an orientable Manifold. However, it does not have continuous global frame since every continuous vector field on an even dimensional sphere must vanish somewhere.
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172 episodes

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Archived series ("Inactive feed" status)

When? This feed was archived on December 09, 2017 16:01 (6+ y ago). Last successful fetch was on October 29, 2017 08:04 (6+ y ago)

Why? Inactive feed status. Our servers were unable to retrieve a valid podcast feed for a sustained period.

What now? You might be able to find a more up-to-date version using the search function. This series will no longer be checked for updates. If you believe this to be in error, please check if the publisher's feed link below is valid and contact support to request the feed be restored or if you have any other concerns about this.

Manage episode 184622173 series 1521141
Content provided by Random Stuffs. All podcast content including episodes, graphics, and podcast descriptions are uploaded and provided directly by Random Stuffs or their podcast platform partner. If you believe someone is using your copyrighted work without your permission, you can follow the process outlined here https://player.fm/legal.
A manifold M of dim n is orientable if there exists a smooth nowhere vanishing n form on M. On a regular zero set in R^{n+1}, there is always a nowhere vanishing n-form so Regular Zero sets in R^{n+ 1} are orientable manifolds. For example if S is cut out by f in R^3 then differentiating (f dy = 0) gives f_x dx dy = f_z dy dz. Thus we have dx dy/ f_z = dy dz/ f_x = dx dz / f_y whenever this expression makes sense. Gluing them gives a nowhere vanishing 2 form on S. In particular the sphere S2 is an orientable Manifold. However, it does not have continuous global frame since every continuous vector field on an even dimensional sphere must vanish somewhere.
  continue reading

172 episodes

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