The gradient of a scalar-valued differentiable function is the vector of its first partial derivatives.
A gradient field is a vector field of the form ∇f for a scalar potential f. Its curl vanishes wherever the required second derivatives commute.
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- Annular Caccioppoli inequality
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- Effective gravity in a rotating frame
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- Failure of L2-to-Linfinity Poisson gradient bounds in three dimensions
- Fick's first law
- First-order optimality condition
- Fixed-energy initial-condition optimality
- Flat direction of a scalar potential
- Gauge transformation
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- Origin-regular spherical Poisson flux law
- Orthogonality of supported and harmonic Dirichlet functions
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Mnemonic: the gradient shows the direction in which the function increases fastest.
Therefore, it has to:
- take a scalar field as input. Otherwise, how do you decide which vector is larger than the other?
- output a vector field that contains the direction in which the scalar increases fastest locally at each point. This has to give out vectors, since we are talking about directions