Mollified time primitives of a field with a square-integrable time derivative #
For a slab field w whose weak time derivative r is square integrable, and a
smooth compact spatial kernel k, the convolution k ⋆ w has, at every point
of space, the weak time derivative k ⋆ r. It is therefore an absolutely
continuous function of time, equal almost everywhere to an explicit primitive
with an averaged constant (prop:lps-local-strong).
The spatial convolution of a slab field with a smooth compact kernel has, at every point of space, the convolved time derivative as weak time derivative.
The averaged constant of the mollified time primitive.
Equations
Instances For
The mollified time primitive x, t ↦ c(x) + ∫ₐᵗ (k ⋆ r)(x, q) dq.
Equations
- ESS.LPS.lpsPrim a b k w r x t = ESS.LPS.lpsPrimConst a b k w r x + ∫ (q : ℝ) in a..t, CKN.vlConvT k r x q
Instances For
The mollified primitive is an interval integral of the convolved time derivative.
The convolution of the field is, at every point and for almost every time, the mollified primitive.
Measurability of the primitive in the time variable of a jointly measurable integrand.
A square-integrable slab field is square integrable for the product of
the spatial measure with the restriction to (a, b].
For almost every time, the convolution of the time slice is the mollified primitive almost everywhere in space.
Square integrability of the mollified primitive at every time and on the
slab, and its energy identity in time (prop:lps-local-strong).
The mollified primitive is linear in the kernel.