- #36
martinbn
Science Advisor
- 3,600
- 1,816
How is that in contradiction to what I said!S.G. Janssens said:As an example, take a Banach space that is not reflexive but still linearly isomorphic to its second continuous dual space.
How is that in contradiction to what I said!S.G. Janssens said:As an example, take a Banach space that is not reflexive but still linearly isomorphic to its second continuous dual space.
Is the above a question?martinbn said:How is that in contradiction to what I said!
A tensor is a mathematical object that represents a multilinear relationship between sets of vectors and/or covectors. It is used to describe physical quantities and their relationships in a coordinate-independent manner.
The gradient of a vector field is a vector field that represents the rate of change of the original vector field in a given direction. It is a vector that points in the direction of steepest increase of the original vector field and its magnitude represents the rate of change.
The gradient of a vector field is a tensor because it is a multilinear mapping between sets of vectors and covectors. It takes in a vector and outputs a covector, making it a type of tensor known as a one-form or covariant tensor.
The gradient of a vector field is a type of tensor known as a one-form or covariant tensor. This means that it takes in a vector and outputs a covector, which can be represented as a column vector of partial derivatives.
The gradient of a vector field is used in physics to describe the behavior of physical quantities, such as velocity, acceleration, and force. It is also used in the formulation of physical laws, such as the laws of electromagnetism and fluid dynamics.