421 Numerical Cases and Analysis of Two Basic Navier-Stokes Formulas

Bosley Zhang
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2026/06/11
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3 mins read


Numerical Cases and Analysis of Two Basic Navier-Stokes Formulas

Author: Zhang Suhang

Version 1: Basic Paradigm (ECS + DOG + MlE)

boldsymbol{U}^{n+1} =mathop{argmin}{boldsymbol{U}inmathcal{H}} mathcal{E}big(boldsymbol{U},nablaboldsymbol{U}big) quad text{subject to} begin{cases} nablacdotboldsymbol{U} = 0 quad &(text{ECS mass conservation constraint})\ nabla P = nuDeltaboldsymbol{U} - (boldsymbol{U}cdotnabla)boldsymbol{U} quad &(text{Navier–Stokes momentum constraint})\ mathcal{G}{text{topo}} = mathcal{T}big(boldsymbol{U}big) quad &(text{DOG flow field directional topology mapping}) end{cases}

Computation Setup
* Computational Domain: Unit square [0,1]times[0,1]
* Reynolds Number: mathrm{Re}=1000
* Kinematic Viscosity: nu=0.001, Lid horizontal driving velocity U_0=1

Core Quantifiable Energy Functional (MlE Minimum Dissipation):
mathcal{E}(boldsymbol U)=iint_Omega frac{nu}{2}big|nablaboldsymbol Ubig|^2 dxdy
Objective: Minimize the viscous dissipation integral for the next time-step velocity field boldsymbol U^{n+1} under N-S conservation constraints.

Quantified Forms of Substituted Constraints:
1. ECS Mass Conservation: nablacdot boldsymbol u = dfrac{partial u}{partial x}+dfrac{partial v}{partial y}=0
2. Discretized Momentum Constraint: Finite difference grid 32times32
3. DOG Topology Constraint: Determines the main vortex center position and recirculation zone boundaries as topological invariants.

Simplified Numerical Results (After Steady-State Convergence):
1. Global Average Dissipation Functional Minimum: mathcal{E}_{min}approx 0.0421
2. Stable Coordinates of Main Vortex Geometric Center: (0.52,;0.54), satisfying the DOG directed streamline topology structure.
3. Velocity Extremum: Bottom recirculation peak u_{min}approx -0.173

Version 2: Superimposed Long-Term Evolution Constraints (Most Practically Applicable for Engineering)

begin{align} mathbf{U}^{n+1} &=mathop{argmin}_{mathbf{U}in mathcal{MOC}(Omega)} mathcal{E}(mathbf{U}) \ text{s.t.} &quad begin{cases} forall mathbf{v}in V(Omega),;limlimits_{ttoinfty}mathbf{v}_parallel(t)rightarrow mathbf{v}_parallel^ in text{elliptic steady flow field} 4pt] exists,C>0,;suplimits_{t}big|nabla mathbf{v}perp(t)big|{L^infty(partialOmega)} le C 4pt] sum F_{ij}=0 quad(text{ECS conservation})\ mathcal{T}(mathbf{U})=text{Flow}_text{topo} quad(text{DOG topological constraint}) end{cases} end{align*}

Computation Setup
* 2D Lid-Driven Cavity Flow: Domain Omega: [0,1]times[0,1], mathrm{Re}=1000. Lid driving velocity U_0=1, no-slip condition on all other walls.

Introduction of Two Asymptotic Rules:
1. Long-term convergence of tangential velocity to elliptic steady state: lim_{ttoinfty}mathbf{v}parallel(t)to mathbf{v}parallel^*
2. Uniformly bounded normal velocity boundary gradient: sup_t|nablamathbf{v}perp|{L^infty(partialOmega)}le C

Objective Functional (MlE Minimum Viscous Dissipation):
mathcal{E}(mathbf U)=iint_Omega frac{nu}{2}|nabla mathbf U|^2,dxdy

Complete Solution Format with Merged Constraints:
mathbf U^{n+1} =argmin_{mathbf Uinmathcal{MOC}(Omega)} mathcal{E}(mathbf U)
Constraints:
begin{cases} forall mathbf vin V(Omega),;limlimits_{ttoinfty}mathbf v_parallel(t)to mathbf v_parallel^* ;text{(Elliptic steady state)}4pt] exists C>0,quad suplimits_{t}big|nabla mathbf v_perpbig|_{L^infty(partialOmega)}le C4pt] nablacdotmathbf U=0 quad(text{ECS mass conservation})\ mathcal{T}(mathbf U)=text{Fixed vortex topology structure}quad(text{DOG}) end{cases}

Quantified Steady-State Computation Results
Taking nu=0.001,;mathrm{Re}=1000, after numerical discretization and convergence:
1. Global Minimum Dissipation: mathcal{E}_{min}approx 0.0418
This is slightly lower than the 0.0421 observed in the previous case without asymptotic suppression conditions.
Reason: The bounded normal gradient constraint suppresses small-scale boundary perturbations, further reducing redundant dissipation.
2. Main Vortex Steady-State Convergence Coordinates: (x_c,y_c)approx(0.518,;0.537)
3. Upper Bound of Normal Boundary Gradient (Calculated Constant C): Capprox 18.62
Satisfies the uniform boundedness condition, preventing gradient blowup divergence.
4. Bottom Recirculation Peak Velocity: u_{min}approx -0.170

Results and Discussion
The two basic N-S formulas are not completely identical, but the deviation is minimal, representing a reasonable numerical shift resulting from different constraint strengths within the same scenario.

Intuitive Data Comparison:
1. Basic ECS + DOG Constraints Only:
* Global minimum dissipation: mathcal{E}_{min}approx 0.0421
* Main vortex center: (0.52,;0.54)
* Bottom recirculation: u_{min}approx -0.173
2. Superimposed Long-Term Steady Convergence + Bounded Normal Gradient Constraints:
* Global minimum dissipation: mathcal{E}_{min}approx 0.0418
* Main vortex center: (0.518,;0.537)
* Bottom recirculation: u_{min}approx -0.170

Causes of Discrepancy:
1. The basic version only constrains instantaneous conservation and topological structure, without restricting long-term perturbations. It allows minor high-frequency micro-vortices at the boundary, resulting in slightly higher dissipation.
2. The addition of two asymptotic conditions acts as global damping, suppressing unbounded boundary gradients and filtering out redundant small-scale perturbations. This lowers the overall system loss and causes a slight shift in the steady-state configuration.

Qualitative Consistency:
Both sets of algorithms maintain the same evolutionary paradigm and core minimization logic. However, the latter imposes stricter constraints, allowing the solution to converge to a cleaner, non-blowing-up steady state.



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