Can Lie Derivatives be Defined Without Dragging on Manifolds?

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The discussion centers on the definition of Lie derivatives without relying on the traditional method of dragging along manifolds. It proposes defining the Lie derivative of a vector field W with respect to another vector field V as the limit of the expression (W(γ + δγ) - W(γ)) / δγ, where γ(t) is an integral curve in the flow generated by V. The participants argue that dragging is unnecessary, as the components of W evaluated at different points on the manifold do not belong to the same vector space, making the conventional approach problematic. This perspective challenges established methods in differential geometry.

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wdlang
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suppose there is a vector field V on a manifold M

V generates a flow on M

suppose \gamma(t) is an integral curce in this flow

now there is another vector field W on M

why not define the lie derivative of W with respect to V as the limit of the divide

(W(\gamma+\delta \gamma)-W(\gamma))/\delta \gamma

here the difference is taken by components

i think this is very natural from our experience in the calculus course in undergraduate.

why we need to drag?
 
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The difference W(\gamma+\delta \gamma)-W(\gamma)) does not make sense since W(\gamma+\delta \gamma) and W(\gamma)) are elements of different vector spaces.
 
The expression \gamma+\delta\gamma (which I assume means \gamma(t)+\delta\gamma(t)) doesn't make sense either, since a manifold doesn't necessarily have a vector space structure. For most manifolds, both the + and the multiplication in \delta\gamma(t) are undefined.
 

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