The localized weak Newtonian potential produces the source's actual curl field w.
Its complement is distributionally harmonic wherever the cutoff is one.
Classical integration by parts and its extension to the actual homogeneous gradient space.
The ordinary curl as a bounded antisymmetrization of actual L² gradient tensors.
Coordinate insertion, given by (EuclideanSpace.proj j).smulRight (EuclideanSpace.single i 1).
Equations
Instances For
Coordinate L², given by (coordinateInsertion i j).compLpL 2 volume.
Equations
Instances For
Each output component is the difference of the two off-diagonal derivative entries.
Equations
- One or more equations did not get rendered due to their size.
Instances For
A fixed universal contraction bound; sharpness is not needed for localization.
On genuine test gradients the tensor operator is exactly the ordinary classical curl.
The source's field w, formed directly from the weak potential's gradient tensor.
Equations
Instances For
Partial test, given by ⟨vectorPartial (f : Space → Space) i, vectorPartial_smooth f f.smooth i, vectorPartial_compact f f.compact i⟩.
Equations
Instances For
Test value, given by (test_memLp f).toLp (f : Space → Space).
Equations
Instances For
The actual tensor inner product has the usual distributional Laplacian formula.
The ordinary real curl is formally self-adjoint on compact smooth vector tests.
Distributional integration by parts survives passage to the closed homogeneous gradient space.
Distributional harmonicity of an actual ordinary L² vector field on a set.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Divergence gradient, constructed using EulerMeanSolenoidal.testGradient.
Equations
Instances For
The actual curl tensor of any homogeneous potential remains solenoidal.
The source's z - w is genuinely weakly harmonic where the actual cutoff equals one.
A quantitative decomposition constructed from the cutoff and the given solenoidal field.