Extended-regularized lattice Boltzmann method
Regularized lattice Boltzmann methods improve numerical stability by projecting the nonequilibrium distribution onto its hydrodynamic second-order Hermite sector and filtering the remaining kinetic modes. We introduce a separate relaxation time for the complete complementary kinetic subspace. The resulting extended-regularized lattice Boltzmann method (E-RLBM) interpolates continuously between the Bhatnagar-Gross-Krook and regularized collision operators while retaining a two-rate implementation. A Chapman-Enskog expansion shows that the isothermal Navier-Stokes equations are recovered with kinematic viscosity $ν=c_s^2(τ-Δt/2)$, independently of the kinetic relaxation time $τ_{\rm nh}$, whereas $τ_{\rm nh}$ changes higher-order truncation errors. For linear transverse shear, its first effect is a fourth-derivative term whose coefficient depends on the direction of propagation relative to the lattice. This fourth-order coefficient is affine in $τ_{\rm nh}$. For linear shear on D2Q9 and $τ_{\rm nh}$ between $τ$ and $Δt$, it lies between the corresponding BGK and RLBM values in every propagation direction. Stability maps for the decaying Taylor-Green vortex and flow past a rectangular obstacle show that an appropriate kinetic relaxation substantially enlarges the stable parameter domain. In a Taylor-Green convergence test with consistent initialization, all three operators converge at second order, and their error differences follow the hyperviscous coefficient for diagonal shear waves: the E-RLBM error is about 6% above the BGK error and about 40% below the RLBM error; in a double shear layer at Re = 80000, the E-RLBM follows the RLBM convergence curve. The proposed collision operator therefore provides a low-cost means of controlling nonhydrodynamic modes without introducing a full multiple-relaxation-time basis.