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Boussinesq System


The inviscid Boussinesq system is a system of nonlinear partial differential equations for a temperature anomaly theta, an incompressible vector field u, and pressure p. With external forces f_theta and f_u in two dimensions, it can be written

(partialtheta)/(partialt)+u·del theta=f_theta
(1)
(partialu)/(partialt)+u·del u+del p=thetae_2+f_u
(2)
del ·u=0,
(3)

where e_2=(0,1) is the upward coordinate vector. The corresponding vorticity omega=partial_1u_2-partial_2u_1 satisfies partial_tomega+u·del omega=partial_1theta+curl(f_u).

Alpöge and Buckmaster (2026a) claim a solution on R^2 from smooth, compactly supported initial temperature and zero initial velocity, with forces that are smooth in space and time and have compact support in one fixed ball. The temperature remains bounded, while the norm of its gradient tends to infinity and the vorticity norm has infinite limit superior at a finite terminal time. The solution remains smooth and unique on every closed preterminal interval.

The authors report that Claude and Codex helped develop and simplify the construction. Two accompanying Lean 4 developments formalize the claimed result, but independent human verification had not been reported as of Sep. 9, 2026 (Alpöge and Buckmaster 2026b). This system is distinct from the scalar Boussinesq equation.


See also

Boussinesq Equation, Euler's Equations of Inviscid Motion, Finite-Time Blow-Up, Incompressible Porous Media Equation, Vorticity

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References

Alpöge, L. and Buckmaster, T. "Blowup for the Boussinesq Equations with Smooth Forcing." Sep. 8, 2026a. https://cims.nyu.edu/~tristanb/boussinesq.pdf.Alpöge, L. and Buckmaster, T. "Boussinesq Blowup." Sep. 8, 2026b. https://github.com/tristanbuckmaster/fluid_lean.

Cite this as:

Weisstein, Eric W. "Boussinesq System." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/BoussinesqSystem.html

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