stages-thermo

A staged-separation (distillation) learning library and fast steady-state column solver, built on vle-thermo.

import stages — walk the full pedagogical ladder of column methods (McCabe–Thiele → Ponchon–Savarit → Fenske–Underwood–Gilliland shortcut → rigorous MESH: bubble-point, sum-rates, inside-out, full Newton), each implemented from scratch and anchored to its textbook equations, with a granular, batch-capable API ("numpy for distillation columns"). All thermodynamics come from vle-thermo; this package adds none of its own.

The ladder's terminal target is an atmospheric crude distillation unit — hundreds of pseudocomponents, pumparounds, steam-stripped side strippers, and products specified on D86 95 % points and gaps rather than mole-fraction purity.

pip install stages-thermo           # import name is `stages`
pip install "stages-thermo[plot]"   # + matplotlib for the staircase diagrams

Status: 0.3.x ships the first three rungs of the ladder — the binary McCabe–Thiele (Milestone 1) and Ponchon–Savarit (Milestone 2) layers and the multicomponent FUG shortcut (Milestone 3): equilibrium and enthalpy–composition (H–x–y) curves from real thermodynamics, minimum reflux by geometric pinch detection (tangent pinches included), stage stepping with Murphree efficiency, total reflux, N(R), the energy-exact difference-point construction (with condenser/reboiler duties), the NRTL γ-φ model, per-phase enthalpies, Fenske–Underwood–Gilliland + Kirkbride + Winn with relative volatilities computed from vle-thermo K-values (fug), the multicomponent K-value / dew-point / flash surface on ThermoSystem, and the diagram plots (staircase, H–x–y, Gilliland). The rigorous MESH solvers land milestone by milestone — see the repo's ROADMAP.md. 1.0 ships inside-out (Boston–Britt/Russell) as the flagship rigorous solver alongside Wang–Henke and sum-rates; the crude-column capability follows at 2.0, and Naphtali–Sandholm (the specialist for strongly nonideal columns) at 2.1. The API may still move before 1.0.

import stages

# Real thermodynamics from vle-thermo: Peng–Robinson benzene–toluene at 1 atm
# (light component first; units K / kPa absolute / mole fractions).
sys = stages.ThermoSystem.peng_robinson(["benzene", "toluene"])
curve = stages.EquilibriumCurve.from_thermo(sys, 101.325)

# Minimum reflux by pinch detection — tangent pinches included …
r = stages.rmin(curve, x_distillate=0.95, x_bottoms=0.05, z_feed=0.50, q=1.0)

# … then the full construction. Rich result objects, never bare numbers:
design = stages.mccabe_thiele(curve, 0.95, 0.05, 0.50, reflux=1.5 * r.r_min)
print(f"N = {design.n_stages:.2f} stages, feed stage {design.feed_stage}, "
      f"R_min = {r.r_min:.3f}")

design.stages          # every (x, y) stage corner
design.staircase       # the full polyline, ready to plot
design.rectifying      # operating lines as slope/intercept
r.pinch, r.tangent     # where the pinch sits, and whether it's a tangent pinch

# The staircase diagram (requires the [plot] extra):
# from stages import plotting
# plotting.plot_mccabe_thiele(design, curve, show_rmin=True)

Strongly non-ideal systems go through the γ-φ route — the same construction, different thermodynamics:

# van Laar methanol–water (the system validated in vle's Chapter IV notebooks).
mw = stages.ThermoSystem.van_laar(["methanol", "water"], 0.5853, 0.3458)
curve_mw = stages.EquilibriumCurve.from_thermo(mw, 101.325)

Rung 2 — Ponchon–Savarit — closes the energy balance on the enthalpy–composition (H–x–y) diagram, so it also returns the condenser and reboiler duties (which McCabe–Thiele cannot):

# H–x–y curve: saturated-liquid and -vapor enthalpies alongside y*(x).
ec = stages.EnthalpyCurve.from_thermo(sys, 101.325)
ps = stages.ponchon_savarit(ec, x_distillate=0.95, x_bottoms=0.05,
                            z_feed=0.50, reflux=1.5)
print(f"N = {ps.n_stages:.2f} stages, feed stage {ps.feed_stage}")
print(f"Q_C/F = {ps.q_condenser:,.0f}, Q_R/F = {ps.q_reboiler:,.0f} kJ/kmol feed")
ps.delta_d, ps.delta_b   # the two difference points (poles), (x, H) in kJ/kmol

# NRTL for strongly non-ideal aqueous-organic systems (a12/a21 in kJ/kmol):
aw = stages.ThermoSystem.nrtl(["ammonia", "water"], a12=-1800.0, a21=-1200.0, alpha=0.2)
# from stages import plotting; plotting.plot_ponchon_savarit(ps, ec)

Rung 3 — the FUG shortcut — is multicomponent. Every relative volatility comes from vle-thermo K-values at the two ends of the column (the "FUG(K)" form that a simulator uses to seed its rigorous solver), refined to self-consistency; each rung is also callable on its own (fenske_n_min, underwood_roots, gilliland_stages, kirkbride_split, winn_fit, …):

# A depropanizer: propane (LK) / isobutane (HK), 98 % key recoveries, R = 1.3 R_min.
c3 = stages.ThermoSystem.peng_robinson(["ethane", "propane", "isobutane", "n-butane", "n-pentane"])
fug = stages.fug(c3, 1500.0, feed=[5, 40, 20, 25, 10], light_key=1, heavy_key=2,
                 lk_recovery=0.98, hk_recovery=0.98, q=1.0, reflux_factor=1.3)
print(fug)   # FugResult(N_min=12.95, R_min=1.885, R=2.450, N=26.47, feed_stage=15, ...)
fug.underwood_roots, fug.n_min_winn, fug.d, fug.x_d, fug.t_top   # every intermediate
# from stages import plotting; plotting.plot_gilliland(fug)

The executable learning path lives in the repo's notebooks/ — 01-mccabe-thiele.ipynb, 02-ponchon-savarit.ipynb and 03-shortcut-design.ipynb design benzene–toluene, methanol–water, acetone–water and ammonia–water binaries (the last on a reference chart digitized from the Pátek–Klomfar correlation) and a C2–C5 depropanizer end-to-end, with exercises.

The native core is a Rust crate (stages-thermo on crates.io) with PyO3 bindings; wheels are abi3 (cp310-abi3-*), so one wheel per (OS, arch) covers CPython 3.10+.

License

MIT © Miguel Roberto Jackson Ugueto