The derivation proves that the partial derivatives of a scalar field, naturally form the covariant components of a vector. This is a fundamental concept in tensor calculus because a scalar field's value is independent of the coordinate system. By applying the chain rule to a coordinate transformation, the partial derivatives are shown to transform in a manner identical to the definition of a covariant vector. This means the transformation rule for a covariant vector, perfectly matches the transformation of the partial derivatives. This result validates that the gradient, which is a vector composed of these partial derivatives, is a quintessential example of a covariant vector.
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The Covariant Nature of a Scalar Field's Partial Derivatives (The Gradient).mp4
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