Initial commit: establish deterministic rod-string solver stack.
Set up the C solver core, Node API orchestration, TS GUI workflow, and engineering documentation with cleaned repo hygiene for private Git hosting. Made-with: Cursor
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Agents/MATH_SPEC.md
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Agents/MATH_SPEC.md
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# Math specification — literature backbone
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**Status:** Living document. Every implemented term should trace to a citation below or to an explicit `heuristic` calibration note in code + `docs/engineering/validation.md`.
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**Primary references:** see `references/papers/README.md` for citation details and source links.
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- Romero, A., and Almeida, A. R. (2014). *A Numerical Sucker-Rod Pumping Analysis Tool*. SPE Artificial Lift Conference - Latin America and the Caribbean. [SPE-169395-MS](https://doi.org/10.2118/169395-MS)
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- Everitt, T. A., and Jennings, J. W. (1992). *An Improved Finite-Difference Calculation of Downhole Dynamometer Cards for Sucker-Rod Pumps*. SPE Production Engineering. [SPE-18189-PA](https://doi.org/10.2118/18189-PA)
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- Araujo, O., et al. (SPE-173970). *3D Rod String Dynamics in Deviated Wells* (minimum-curvature and coupled dynamics reference used for trajectory coupling).
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- Eisner, B., Langbauer, C., and Fruhwirth, R. (2022). *A finite element approach for dynamic sucker-rod diagnostics* (Newmark + Rayleigh + diagnostic iteration basis).
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- Lukasiewicz, H. (as summarized in Eisner et al.) coupled axial/lateral force balance for deviated rod strings.
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---
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## 1. Gibbs one-dimensional damped wave (vertical / uniform rod)
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**Romero & Almeida — Eq. (2)** (viscous damped wave, constant \(A,E,\rho\)):
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\[
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\frac{\partial^2 u}{\partial t^2} = a^2 \frac{\partial^2 u}{\partial x^2} - \varsigma \frac{\partial u}{\partial t}
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\]
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with \(a^2 = E/\rho\) (wave speed) and \(\varsigma\) viscous damping coefficient per unit mass (paper uses lumped fluid damping narrative).
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**Variable cross-section (Everitt & Jennings — Eq. 2 form)** after multiplying through by \(\rho A\); axial stiffness gradient:
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\[
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\frac{\partial}{\partial x}\left( EA \frac{\partial u}{\partial x} \right) = \rho A \frac{\partial^2 u}{\partial t^2} + c \rho A \frac{\partial u}{\partial t} - f_{\text{body}}
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\]
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where \(f_{\text{body}}\) collects distributed **weight and buoyancy** along the rod (gravity along tangent; buoyancy from fluid — **Lukasiewicz** axial force balance in Eisner Eq. (2) discussion / Lukasiewicz coupled model referenced in Eisner).
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**Implementation note:** Code uses discrete \(E_i, A_i, \rho_i\) per node or segment, harmonic or measured surface \(u(0,t)\), and bottom boundary coupling (pump / valve / spring-damper per roadmap).
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---
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## 2. Damping conventions
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- **Gibbs dimensionless damping** \(\nu\): related to decay rate; Romero cites \(\varsigma\) proportional to velocity; Eisner Eq. (1) uses \(\frac{\pi a \nu}{2L}\frac{\partial u}{\partial t}\) form for vertical damped wave.
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- **Rayleigh damping (FEA, Eisner):** \(\mathbf{C} = \alpha \mathbf{M} + \beta \mathbf{K}\) for bar elements.
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- **XML factors:** `UpStrokeDampingFactor`, `DownStrokeDampingFactor`, `NonDimensionalFluidDamping` modulate effective \(\gamma\) or \(\alpha,\beta\) per phase (mapped in solver; see code comments).
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---
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## 3. Explicit finite-difference stencil (diagnostic / deviated extension)
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**Everitt & Jennings — Eq. (3)** (conceptual explicit FD recursion transferring displacements downhole from surface card). The paper gives a five-point relation in \((i,j)\) space (space index \(i\), time \(j\)) with coefficients involving \(a\), \(c\), \(\Delta t\), \(\Delta x\), and \(EA\).
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**Variable \(EA\):** harmonic mean or segment fluxes:
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\[
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\text{flux}_{i+\frac12} = E_{i+\frac12} A_{i+\frac12} \left( u_{i+1} - u_i \right)
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\]
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Laplacian-like term formed from \(\partial/\partial x (EA \partial u/\partial x)\) discretization (matches current diagnostic JS prior to C port).
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**CFL:** explicit wave requires \(\Delta t \le \text{CFL} \cdot \Delta x / a_{\max}\) with \(a_{\max} = \max \sqrt{E/\rho}\). Code clamps effective CFL (see `verbose.numerics.cflEffective`).
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---
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## 4. Deviated wells — coupled axial / lateral (reference)
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**Lukasiewicz (via Eisner Eqs. (2)–(3))** — force balance along rod tangent and normal; includes \(\rho g A \cos\phi\), viscosity term \(\nu\), Coulomb \(\mu N\), curvature \(R\), and lateral equilibrium.
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**Current implementation:** distributed **side load** \(N_i\) and inclination-aware **Coulomb friction** \(F_{f,i} = \mu_{\text{eff}} N_i \operatorname{sgn}(v_i)\) are computed per node and injected into FDM/diagnostic/FEA updates. API exposes `profiles.sideLoadProfile` and `profiles.frictionProfile` when `options.enableProfiles=true`.
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---
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## 5. Three-dimensional trajectory (SPE-173970)
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**Araujo et al. — Eqs. (5)–(24):** minimum-curvature method between survey stations: unit tangent, curvature angle \(\gamma_i\), radius \(r_{c,i}\), binormal, center of curvature, position propagation \(R(s_{i+1})\), and interpolation of any MD \(s\) within a segment.
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**Implementation:** `solver-c/src/trajectory.c` uses minimum-curvature style tangent interpolation and exports node-wise \(\kappa(s)\), inclination, and azimuth on the rod grid for side-load/friction coupling and `trajectory3D` output.
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---
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## 6. Dynamic 1D bar FEM (Eisner et al.)
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- **Bar stiffness / mass:** consistent element \(K_e\), \(M_e\) for linear shape functions.
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- **Newmark-β** (\(\beta=\frac14\), \(\gamma=\frac12\)) for transient axial dynamics.
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- **Bottom BC:** spring-damper + friction; diagnostic mode adds **iterative plunger load** adjustment so that computed top reaction matches measured polished load (Eisner Fig. 4 principle — restart / bisection per time step).
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---
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## 7. Boundary conditions
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| Mode | Surface | Bottom |
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|------|---------|--------|
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| **Predictive** | Harmonic \(u(0,t)\) (Romero **Eq. (4)** style crank motion) or measured surrogate | Pump: spring-damper + friction + valve-state pressure balance; gas fraction inferred from chamber state |
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| **Diagnostic** | Measured \(u(0,t)\) and \(F(0,t)\) from dynamometer card (Everitt) | Same pump BC; FEA adjusts unknown plunger load and reports valve/gas timeline |
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**Surface card QA (Eisner narrative):** ≥ 75 samples recommended for Fourier-style tools; we enforce minimum samples and cycle checks in API (`POST /solve/validate-card`).
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---
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## 8. Outputs (API / solver)
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- Polished and downhole **cards** \((x, F)\).
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- **Pump movement:** plunger position series, velocity, stroke, period.
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- **Optional profiles:** `stressProfile`, `sideLoadProfile`, `trajectory3D` (when `schemaVersion >= 2`).
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- **Comparison:** FDM vs FEA peak deltas + point-wise residuals + optional Fourier analytical baseline (`comparison.fourier` when enabled).
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---
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## 9. Symbols (SI internal)
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| Symbol | Unit | Meaning |
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|--------|------|---------|
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| \(u\) | m | Axial displacement |
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| \(F\) | N | Axial force (tension positive) |
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| \(E\) | Pa | Young’s modulus |
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| \(A\) | m² | Cross-sectional area |
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| \(\rho\) | kg/m³ | Rod density |
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| \(\phi\) | rad | Inclination from vertical |
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| \(\kappa\) | 1/m | Path curvature |
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---
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## 10. Implementation quality rules (for next execution)
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- Every newly introduced solver term must be tagged as one of:
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- `equation-backed` (with paper/equation reference),
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- `heuristic` (with rationale + planned replacement).
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- No silent heuristic drift: if a coefficient changes, update validation fixtures and notes.
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- Any new field wired into equations must be reflected in `docs/engineering/field-traceability.md`.
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- Any new coupled term must include at least:
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- one unit-scale numerical test,
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- one integration case assertion,
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- one regression guard.
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---
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*End of math spec backbone. Extend with equation numbers from PDFs as features land.*
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