Notes on this project's Richardson iteration, for readers of algos.tex#
Why this exists#
evolving_surface/notes/algos.tex (Sec. 5, "Implicit timestepping and the
linear solve") specifies the surface diffusion step as backward Euler,
(I - Δt Δ_Γ) u^{n+1} = u^n, solved by preconditioned GMRES: the
round-sphere Laplacian M = I - Δt Δ_S (diagonal, invertible by eigenvalue)
preconditions the full operator, the real-embedding map E puts the
half-spectrum complex coefficients into a real vector space, and restarted
GMRES iterates to a residual tolerance.
turing-surface (this project) solves the same split operator with a
different numerical method: a preconditioned Richardson (fixed-point)
iteration, reusing exactly algos.tex's preconditioner M^{-1} but with no
Krylov subspace, no orthogonalization, and no adaptive stopping. This note
gives the map between the two, in this project's variable names, and why the
switch.
Notation map#
| algos.tex | this project | meaning |
|---|---|---|
u^n, u^{n+1} |
U/V (in), Un/Vn (out) |
spectral state, one array per species |
Δ_Γ |
lap_g |
the surface's Laplace-Beltrami operator |
Δ_S |
lap_s |
the round sphere's operator, eigenvalue -l(l+1) |
| — | dlap |
lap_g - lap_s. algos.tex has no name for this because it never splits the operator this way — its GMRES matvec (surface_screened_laplacian) applies the whole Δ_Γ every iteration. |
M = I - Δt Δ_S |
(1 + dt*D*lam) |
the same preconditioner. lam holds +l(l+1), not -l(l+1), so it enters as a sum — the sign flip is already folded into lam. |
M^{-1}v (eq. preconditioner_inverse) |
v ./ (1 + dt*D*lam) |
the identical elementwise divide |
| a GMRES iterate | Un^(k), k = 0..niter |
not a Krylov iterate — a fresh, full re-solve of the fixed point below, evaluated at the previous iterate |
The fixed point this project actually iterates#
Same split as algos.tex, lap_g = lap_s + dlap, substituted into backward
Euler and rearranged so every occurrence of the unknown is Un. Starting
from (I - dt*D*lap_g) Un = B and substituting the split:
(I - dt*D*(lap_s + dlap)) Un = B
Expanding, and moving the dlap term to the right so only the exactly
invertible round-sphere part remains on the left:
Un - dt*D*lap_s(Un) = B + dt*D*dlap(Un)
lap_s is diagonal with eigenvalue -l(l+1), and lam holds +l(l+1), so
lap_s(Un) = -lam .* Un — the left side becomes Un .* (1 + dt*D*lam), and
dividing through gives:
Un = (B + dt*D*dlap(Un)) ./ (1 + dt*D*lam)
B is the explicit-reaction right-hand side — this project's models are
IMEX (explicit reaction, implicit diffusion), where algos.tex's worked
example is the bare heat equation, so B here is u^n plus a reaction term.
Richardson iteration on this fixed point:
Un^(0) = B ./ (1 + dt*D*lam) [dlap = 0]
Un^(k+1) = (B + dt*D*dlap(Un^(k))) ./ (1 + dt*D*lam)
for k = 0 .. niter-1. models/schnakenberg.m's for k = 1:niter loop is
this: Un^(0) is the divide computed just before the loop, and each pass
computes Un^(k+1) from Un^(k). It is written as a full re-evaluation
rather than an accumulated correction δ = Un^(k+1) - Un^(k) on purpose: at
dlap ≡ 0 (the round sphere), every Un^(k) is then bit-for-bit Un^(0),
with no cancellation to round differently — a stronger, and cheaper to
check, statement than "close to the round-sphere answer."
Convergence, and why it isn't GMRES#
Writing M = I - dt*D*lap_s and A = M - dt*D*dlap, each step is
Un^(k+1) = M^{-1}(B + dt*D*dlap(Un^(k))) — a stationary iteration that
converges to the exact solution of A·Un = B exactly when the spectral
radius of M^{-1}(dt*D*dlap) is below 1: while the geometric correction
stays small against what the round-sphere solve already inverts. Unlike
GMRES, there is no residual check and no adaptive iteration count: niter is
fixed before the run starts, so a shape/timestep/diffusivity combination
outside the convergence radius fails silently — the state saturates or
diverges over many steps — rather than being caught the way algos.tex's
solve_step catches it (its info != 0 return, logged when GMRES fails to
reach tol within maxiter).
That tradeoff is deliberate, not an oversight, and it comes from where the
two projects run. algos.tex's GMRES needs, every iteration: a dot product
across the whole spectral state (Arnoldi orthogonalization) and a residual
norm to test against tol — both require reading a scalar back to the host
mid-solve. This project's solver instead records one whole timestep as a
single GPU command buffer, submitted once, with the entire for k = 1:niter
loop unrolled at compile time into a fixed sequence of dispatches — there is
no point in that sequence where the host makes a decision, and no path for a
data-dependent stopping rule to plug in. (Recompiling — which changing
niter triggers — is the only way this project can change how much work a
step does; see the README's "for loops, unrolled".) Richardson iteration is
the cheapest method that still fits that shape: the same preconditioner as
algos.tex, one dlap evaluation per iteration, a fixed and
recompile-on-change trip count, in exchange for linear rather than
superlinear convergence.
One more difference worth flagging#
algos.tex maps the half-spectrum complex coefficients through a real vector
space embedding E (Sec. 6.4) because GMRES needs one flat, real-linear
operator to hand to a generic solver. This project never needs E/E^{-1}:
its spectral state is already carried as a real "2 x nlm" array — row 0 the
real part, row 1 the imaginary — rather than packed complex, so every step
here, dlap included, is already ℝ-linear arithmetic on that layout with no
embedding or un-embedding step at all.