jbergman
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That's the exact same thing I wrote.vanhees71 said:This is highly misleading, because it only works out using Cartesian coordinates for the vector space of an Euclidean affine space.
The natural general definition of a bare differentiable manifold is to define (alternating) differential forms as derivative operators on alternating tensor fields. Then the gradient of a scalar field naturally occurs as a one-form, i.e., a co-vector field,
$$\mathrm{d} \Phi=\mathrm{d}q^j \partial_j \Phi.$$
$$df = \frac{\partial f}{\partial x^i} dx^i$$
is a covector field.