cianfa72
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- About the limits in the extension of a local chart on a smooth manifold
I'm a bit confused by the conditions on the existence of coordinate basis given by Frobenius's theorem.
Namely, let's take a n-dimensional smooth manifold and a set of n smooth vector fields defined on it. Suppose they are pointwise linearly independent and do commute each other (i.e. zero commutator/Lie bracket).
That means they span the entire tangent space at any point and since commute, they define a local coordinate basis. What does this mean? Well, starting from any point on the manifold, there is a neighborhood such that the integral curves of those vector fields define a local coordinate chart. So far so good.
Also, what is the maximum extension of such local charts, can any of them cover the entire manifold ?
Take a 2-sphere as opposed to an infinite cylinder. On the sphere, by the hairball theorem, there are no two smooth vector fields pointwise linearly independent. However parallels and meridians define two commuting vector fields excluding both poles, thus defining local charts based on them (excluding the poles).
On the other hand, on the cylinder, there exist two pointwise linearly independent smooth vector fields that commute. Therefore starting from any point they define a local coordinate chart, yet neither of them can be extended globally for topological reasons. Indeed, trying to extend any of them becomes problematic: the same point would have multiple coordinate values.
Thus, in the latter case, although the two smooth vector fields define a constant rank bundle and do commute, the maximal extension of any local chart based on them is actually limited.
Does the above make sense ?
Namely, let's take a n-dimensional smooth manifold and a set of n smooth vector fields defined on it. Suppose they are pointwise linearly independent and do commute each other (i.e. zero commutator/Lie bracket).
That means they span the entire tangent space at any point and since commute, they define a local coordinate basis. What does this mean? Well, starting from any point on the manifold, there is a neighborhood such that the integral curves of those vector fields define a local coordinate chart. So far so good.
Also, what is the maximum extension of such local charts, can any of them cover the entire manifold ?
Take a 2-sphere as opposed to an infinite cylinder. On the sphere, by the hairball theorem, there are no two smooth vector fields pointwise linearly independent. However parallels and meridians define two commuting vector fields excluding both poles, thus defining local charts based on them (excluding the poles).
On the other hand, on the cylinder, there exist two pointwise linearly independent smooth vector fields that commute. Therefore starting from any point they define a local coordinate chart, yet neither of them can be extended globally for topological reasons. Indeed, trying to extend any of them becomes problematic: the same point would have multiple coordinate values.
Thus, in the latter case, although the two smooth vector fields define a constant rank bundle and do commute, the maximal extension of any local chart based on them is actually limited.
Does the above make sense ?
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