- Update all submodule URLs from gitea.centraal.wbd-rd.nl to gitea.wbd-rd.nl - Add settler as proper submodule in .gitmodules - Add agent skills, function anchors, decisions, and improvements - Add Docker configuration and scripts - Add manuals and third_party docs - Update .gitignore with secrets and build artifacts - Remove stale .tgz build artifact Co-Authored-By: Claude Opus 4.6 <noreply@anthropic.com>
5.4 KiB
Sludge Settling & Clarifier Models
Used by:
biological-process-engineeragent,settlernode Validation: Verified against Takacs et al. (1991), Vesilind (1968), and Burger-Diehl framework publications
Vesilind Model — Zone Settling Velocity
Source: Vesilind, P.A. (1968). "Design of Prototype Thickeners from Batch Settling Tests." Water Sewage Works, 115, 302-307.
Equation
v_s = v_0 · exp(-k · X)
Where:
- v_s = settling velocity (m/h)
- v_0 = maximum initial settling velocity (m/h)
- k = settling parameter (m³/kg or L/g)
- X = suspended solids concentration (kg/m³ or g/L)
Typical Parameter Ranges for Municipal Wastewater
| Parameter | Typical Range | Unit | Notes |
|---|---|---|---|
| v_0 | 4 – 12 | m/h | ~7.8 m/h is a commonly observed average |
| k | 0.3 – 0.8 | m³/kg | Correlates with SVI; higher SVI → higher k |
SVI Correlation
The settling parameter k can be estimated from Sludge Volume Index:
- k ≈ 0.16 + 0.003 · SVI (for SVI in mL/g, k in m³/kg)
- Better correlations use SSVI (Stirred SVI) or DSVI (Diluted SVI)
Limitations
- Only describes zone settling (hindered settling of a blanket)
- Does not capture compression settling at high concentrations
- Does not model the clarification zone (low-concentration region above blanket)
Takacs Model — Double-Exponential Settling
Source: Takacs, I., Patry, G.G., Nolasco, D. (1991). "A dynamic model of the clarification-thickening process." Water Research, 25(10), 1263-1271.
Equation
v_s = v_0 · (exp(-r_h · (X - X_min)) - exp(-r_p · (X - X_min)))
Where:
- v_s = settling velocity (m/h)
- v_0 = maximum Vesilind settling velocity (m/h)
- r_h = hindered settling parameter (m³/kg)
- r_p = flocculent settling parameter (m³/kg)
- X = suspended solids concentration (kg/m³)
- X_min = non-settleable fraction (kg/m³)
Key Innovation
The double-exponential form captures both the clarification zone (low concentrations, dominated by the r_p term) and the thickening zone (high concentrations, dominated by the r_h term). This allows simulation of the complete solids profile from effluent to underflow.
Typical Parameter Values
| Parameter | Typical Range | Default | Unit |
|---|---|---|---|
| v_0 | 4 – 12 | 7.5 | m/h |
| r_h | 0.3 – 0.8 | 0.576 | m³/kg |
| r_p | 2.0 – 6.0 | 2.86 | m³/kg |
| X_min | 0 – 0.1 | 0.01 | kg/m³ |
Sensitivity
- r_p is the most sensitive parameter — it governs effluent suspended solids
- Takacs et al. recommend finding r_p by simulation/calibration
- v_0 and r_h primarily affect the sludge blanket position and underflow concentration
1D Layer Model Implementation
The settler is divided into N horizontal layers (typically 10-30). For each layer:
- Calculate settling velocity from local concentration
- Apply solids flux theory (gravity flux + bulk flux)
- Update concentration via mass balance
- Handle feed layer, overflow, and underflow boundary conditions
Burger-Diehl Framework — PDE-Based 1D Settler
Source: Burger, R., Diehl, S. and various co-authors (2011-present). Multiple publications developing the framework.
Key Characteristics
- Based on rigorous partial differential equation theory (hyperbolic-elliptic PDE)
- Accounts for hindered settling, compression settling, and inlet dispersion
- Every implementation detail is consistent with PDE theory (unlike ad-hoc layer models)
- More realistic prediction of underflow sludge concentration
- Essential for accurate wet-weather modelling
Advantages Over Takacs Layer Model
- Proper handling of compression settling (important at high MLSS)
- Mathematically rigorous — convergence guaranteed
- Better sludge blanket dynamics during storm events
- Can be extended with reactive terms (ASM1 biokinetics inside settler)
When to Use Which Model
| Scenario | Recommended Model |
|---|---|
| Steady-state design | Vesilind + flux theory |
| Dynamic simulation (standard) | Takacs 1D layer model |
| Wet-weather / high-MLSS dynamics | Burger-Diehl PDE model |
| Quick estimation | Vesilind with SVI correlation |
Flux Theory for Clarifier Design
The solids flux approach combines the gravity settling flux with the bulk (underflow) flux:
J_total = J_gravity + J_bulk = v_s(X) · X + Q_u/A · X
Where:
- J_total = total solids flux (kg/m²/h)
- v_s(X) = settling velocity at concentration X (from Vesilind or Takacs)
- Q_u = underflow rate (m³/h)
- A = clarifier surface area (m²)
The limiting flux determines the maximum solids loading rate — operating above this causes blanket rise and eventual washout.
Authoritative References
- Vesilind, P.A. (1968). "Design of Prototype Thickeners from Batch Settling Tests." Water Sewage Works, 115, 302-307.
- Takacs, I., Patry, G.G., Nolasco, D. (1991). "A dynamic model of the clarification-thickening process." Water Res. 25(10), 1263-1271.
- Burger, R., Diehl, S., Nopens, I. (2011). "A consistent modelling methodology for secondary settling tanks in wastewater treatment." Water Res. 45(6), 2247-2260.
- Torfs, E. (2015). "Different settling regimes in secondary settling tanks." PhD thesis, Ghent University.
- Daigger, G.T. (1995). "Development of refined clarifier operating diagrams using an updated settling characteristics database." Water Environment Research, 67(1), 95-100.