The Laplacian against test functions #
For a C² function u on an open set Ω of a finite-dimensional real inner product space and a
test function φ ∈ 𝓓(Ω), integrating by parts twice in each coordinate direction gives Green's
second identity in the boundary-free form
∫ Δφ • u ∂μ = ∫ φ • Δu ∂μ,
for any additive Haar measure μ: the classical Laplacian of a C² function is its distributional
Laplacian on Ω. In particular a function harmonic on Ω is weakly harmonic: ∫ Δφ • u = 0 for
every test function φ on Ω. This is the form in which harmonicity enters integral arguments
such as the mean-value property, where the test functions are radial.
The two integrations by parts are the defining identities of the weak derivative
TauCeti.HasWeakLineDerivOn, applied to u and to its first directional derivative, both of
which are classical derivatives and hence weak ones
(TauCeti.hasWeakLineDerivOn_of_hasLineDerivAt). No boundary term appears because the test
function is compactly supported in Ω, and no regularity of ∂Ω is used.
Main declarations #
ContDiffOn.integral_fderiv_fderiv_smul_eq_integral_smul_fderiv_fderiv: second-order integration by parts in one direction,∫ ∂ᵥ∂ᵥφ • u = ∫ φ • ∂ᵥ∂ᵥu.ContDiffOn.integral_laplacian_smul_eq_integral_smul_laplacian: Green's second identity against a test function,∫ Δφ • u = ∫ φ • Δu.InnerProductSpace.HarmonicOnNhd.integral_laplacian_smul_eq_zero: a harmonic function is weakly harmonic.TestFunction.laplacianCLM_apply: the test-function Laplacian agrees pointwise with the classical Laplacian.
Second-order integration by parts against a test function, in one direction v. For
u of class C² on the open set Ω and a test function φ on Ω,
∫ ∂ᵥ∂ᵥφ • u = ∫ φ • ∂ᵥ∂ᵥu.
Green's second identity against a test function. For u of class C² on the open set
Ω and a test function φ on Ω, ∫ Δφ • u ∂μ = ∫ φ • Δu ∂μ: the classical Laplacian of a C²
function is its distributional Laplacian.
A harmonic function is weakly harmonic. If u is harmonic on the open set Ω, then
∫ Δφ • u ∂μ = 0 for every test function φ on Ω.
Applying the test-function Laplacian operator agrees pointwise with the classical Laplacian of the underlying smooth function.