difflow
Differentiable Flowsheet Framework for Chemical Processes
A JAX-based framework for building and optimizing chemical process flowsheets with automatic differentiation.
- Source code: https://github.com/jkitchin/differentiable-flowsheets
- Documentation: https://kitchingroup.cheme.cmu.edu/differentiable-flowsheets/
- Issue tracker: https://github.com/jkitchin/differentiable-flowsheets/issues
Features
- Fully Differentiable: All unit operations and flowsheet calculations support automatic differentiation via JAX
- Sensitivity Analysis: Compute gradients of outputs with respect to any inputs, parameters, or operating conditions
- Optimization Ready: Use gradient-based optimization for process design, parameter estimation, and economic optimization
- Modular Design: Unit operations can be composed into complex flowsheets with recycle streams
- Technoeconomic Analysis: Comprehensive TEA module with equipment costs, operating costs, and profitability metrics (NPV, IRR, MSP)
- Bio Manufacturing: Specialized unit operations for biopharmaceutical processes (bioreactors, chromatography, filtration)
- Gas Networks: Steady-state gas transmission networks with a topology-computed sequential decomposition and differentiable tear solving
⚠️ ALPHA SOFTWARE
This project is under active development and not ready for production use. APIs may change without notice. This notice will be removed when the project reaches stable release.
It is highly recommended that you confirm the equations and physical properties used in the models you make; these were generated by Claude. We have endeavored to ensure they seem reasonable, but cannot guarantee they are accurate in all cases.
This package uses jax solvers (e.g. diffrax, optimistix, etc.) and does not rely on IPOPT or pounce, or pyomo / IDAES. It is a pure Python / jax focused package that was developed as a proof of concept.
LLM usage
Claude Code is heavily used to generate the code, examples and tests. This has allowed the project to develop faster than it can be used, and to develop more features than are immediately needed. This may mean there are modules that do not match the performance or output of other projects. You should perform your own diligence when using the code to ensure the library does what you expect it to. Ultimately this is a proof of concept in differentiable flowsheets that wouldn't be possible without Claude Code.
We regularly run all of the notebooks to ensure they run without errors, and review them to make sure the results make sense. We are happy to take issues and / or pull requests to fix problems. We also use Claude to review the code to look for issues.
We actually anticipate that Claude Code is used when using this library (See CLAUDE.md). The library is large enough that it would take a long time to learn all the capabilities in addition to learning the nuances of differentiable programming. This repo provides all the information Claude needs to help you translate your flowsheet ideas into differentiable programs.
Installation
# From PyPI
pip install difflow
# With examples and tutorials (includes matplotlib, jupyter)
pip install "difflow[examples]"
# Everything
pip install "difflow[all]"
For development, install from source:
git clone https://github.com/jkitchin/differentiable-flowsheets.git
cd differentiable-flowsheets
uv venv
uv pip install -e ".[dev]"
# Install everything
uv pip install -e ".[all]"
Quick Start
import jax.numpy as jnp
import jax
from difflow import (
make_stream, get_flows,
IdealThermo, SpeciesData,
CSTR, CSTRParams,
)
# Define species
species_data = {
"A": SpeciesData("A", MW=100.0, Cp_coeffs=(75.0, 0.0, 0.0, 0.0),
Hvap_coeffs=(35000.0, 0.38, 500.0),
antoine_coeffs=(10.0, 3000.0, -50.0)),
"B": SpeciesData("B", MW=100.0, Cp_coeffs=(75.0, 0.0, 0.0, 0.0),
Hvap_coeffs=(30000.0, 0.38, 450.0),
antoine_coeffs=(10.0, 2800.0, -40.0)),
}
thermo = IdealThermo(species_data)
# Define reaction kinetics
def rate_fn(C, T, params):
k = params["A"] * jnp.exp(-params["Ea"] / (8.314 * T))
return jnp.array([k * C["A"]])
# Create CSTR
stoich = jnp.array([[-1.0], [+1.0]]) # A → B
cstr_params = CSTRParams(
V=jnp.array(1.0),
rate_fn=rate_fn,
stoich=stoich,
rate_params={"A": jnp.array(1e6), "Ea": jnp.array(50000.0)},
species_order=["A", "B"],
)
cstr = CSTR(cstr_params, thermo=thermo, mode="isothermal")
# Run simulation
inlet = make_stream({"A": 10.0, "B": 0.0}, T=300.0, P=101325.0)
outlet, info = cstr(inlet, T_spec=350.0)
print(f"Conversion: {info['conversion']['A']*100:.1f}%")
# Compute gradient of outlet B w.r.t. reactor volume
def outlet_B(V):
params = CSTRParams(V=V, rate_fn=rate_fn, stoich=stoich,
rate_params={"A": jnp.array(1e6), "Ea": jnp.array(50000.0)},
species_order=["A", "B"])
cstr = CSTR(params, thermo=thermo, mode="isothermal")
outlet, _ = cstr(inlet, T_spec=350.0)
return outlet["F_B"]
dFB_dV = jax.grad(outlet_B)(jnp.array(1.0))
print(f"dF_B/dV = {dFB_dV:.4f} mol/s per m³")
Unit Operations
CSTR (Continuous Stirred Tank Reactor)
- Multiple reactions with user-defined kinetics
- Isothermal, adiabatic, or specified heat duty modes
- Automatic material and energy balance solving
PFR (Plug Flow Reactor)
- ODE-based design equation: dF/dV = stoich @ r
- Isothermal or adiabatic operation
- GasPFR variant for gas-phase reactions with:
- Pressure drop (Ergun equation)
- Variable volumetric flow from mole change
- RK4 integration via
lax.scan(fully differentiable)
from difflow import PFR, PFRParams, GasPFR, GasPFRParams
# Liquid-phase PFR
pfr = PFR(PFRParams(V=2.0, rate_fn=rate_fn, stoich=stoich,
rate_params=params, species_order=["A", "B"]))
outlet, info = pfr(inlet, T_spec=350.0)
# Gas-phase with pressure drop (A → 2B, mole increase)
gas_pfr = GasPFR(GasPFRParams(V=1.0, rate_fn=rate_fn, stoich=stoich,
rate_params=params, species_order=["A", "B"],
alpha=50000.0)) # Pressure drop parameter
outlet, info = gas_pfr(inlet, T_spec=500.0)
# info contains: conversion, profiles (V, F, T, P, Q), pressure_drop
Flash Separator
- TP flash (temperature and pressure specified)
- Rachford-Rice equation for VLE
- Ideal thermodynamics (Raoult's law)
Liquid-Liquid Extraction (LLE)
- MultistageCascade: Counter-current or co-current mixer-settler cascade
- Kremser equation for stage calculations (differentiable in n_stages)
- Continuous stage relaxation for optimization
- DifferentialContactor: Packed column extractor
- HETP-based equilibrium model
- Rate-based mass transfer model
- Equilibrium Models:
- Distribution coefficients (K-values) with temperature dependence
- NRTL activity coefficient model
- UNIQUAC activity coefficient model
from difflow import (
MultistageCascade, CascadeParams,
LLEEquilibrium, DistributionCoeffs,
)
# Define distribution coefficients for rare earth extraction
K_coeffs = DistributionCoeffs(
species=("La", "Nd", "Dy"),
K0=(0.5, 2.0, 8.0), # K at reference temperature
)
equilibrium = LLEEquilibrium(
solutes=["La", "Nd", "Dy"],
aqueous_carrier="H2O",
organic_carrier="Organic",
K_coeffs=K_coeffs,
)
cascade = MultistageCascade(CascadeParams(
n_stages=5,
equilibrium=equilibrium,
flow_config="counter_current",
))
raffinate, extract, info = cascade(feed_stream, solvent_stream)
Utilities
- Mixer: Combine multiple streams
- Splitter: Split stream by fraction
Fed-Batch Reactor
- General-purpose fed-batch (semi-batch) reactor for chemical reactions
- Time-varying feed addition with configurable feed profiles
- RK4 integration for batch dynamics
- Supports multiple reactions with user-defined kinetics
from difflow import FedBatchReactor, FedBatchParams
# Fed-batch reactor with continuous reagent addition
def rate_fn(C, T, params):
k = params["k0"] * jnp.exp(-params["Ea"] / (8.314 * T))
return jnp.array([k * C["A"] * C["B"]])
params = FedBatchParams(
V0=jnp.array(1.0), # Initial volume (m³)
rate_fn=rate_fn,
stoich=jnp.array([[-1.0], [-1.0], [1.0]]), # A + B → C
rate_params={"k0": jnp.array(1e6), "Ea": jnp.array(50000.0)},
species_order=["A", "B", "C"],
t_final=jnp.array(3600.0), # Batch time (s)
n_steps=100,
)
reactor = FedBatchReactor(params)
# Feed profile: constant feed rate
feed = make_stream({"A": 0.0, "B": 1.0, "C": 0.0}, T=300.0, P=101325.0)
def feed_rate(t): return jnp.array(0.001) # m³/s
final, info = reactor(initial_charge, feed, feed_rate, T_spec=350.0)
# info contains: conversion, profiles (t, V, C, T), yield
Distillation Columns
- ShortcutColumn: Fenske-Underwood-Gilliland method for quick design estimates
- Minimum stages (Fenske equation)
- Minimum reflux ratio (Underwood equations)
- Actual stages for given reflux (Gilliland correlation)
- DistillationColumn: Rigorous stage-by-stage calculation
- MESH equations (Material, Equilibrium, Summation, Heat balance)
- Supports partial/total condenser and reboiler
from difflow import ShortcutColumn, ShortcutColumnParams
params = ShortcutColumnParams(
species_order=["benzene", "toluene", "xylene"],
light_key="benzene",
heavy_key="toluene",
x_D_LK=0.99, # 99% benzene recovery in distillate
x_B_HK=0.99, # 99% toluene recovery in bottoms
)
column = ShortcutColumn(params, thermo=thermo)
distillate, bottoms, info = column(feed, R_ratio=1.5, q=1.0)
# info contains: N_min, R_min, N_actual, condenser_duty, reboiler_duty
Heat Exchangers
- Heater/Cooler: Single-stream with utility (steam, cooling water)
- Specified duty mode
- Specified outlet temperature mode
- Rating mode (given UA and utility temperature)
- CounterCurrentHX: Two-stream counter-current (shell-and-tube style)
- CoCurrentHX: Two-stream co-current (parallel flow)
- All use effectiveness-NTU method, fully differentiable
from difflow import (
Heater, HeaterParams,
CounterCurrentHX, HeatExchangerParams,
design_heat_exchanger,
)
# Single-stream heater with steam
heater = Heater(HeaterParams(T_out=400.0, Cp=75.0))
heated_feed, info = heater(cold_feed)
# info: Q, T_in, T_out, LMTD (if utility temp specified)
# Two-stream counter-current heat exchanger
hx = CounterCurrentHX(HeatExchangerParams(
UA=2000.0, # W/K
Cp_hot=75.0, # J/(mol·K)
Cp_cold=80.0,
))
hot_out, cold_out, info = hx(hot_stream, cold_stream)
# info: Q, effectiveness, NTU, LMTD, approach temperature
# Design: calculate required area
result = design_heat_exchanger(
Q=jnp.array(100000.0), # 100 kW
T_hot_in=jnp.array(450.0), T_hot_out=jnp.array(380.0),
T_cold_in=jnp.array(300.0), T_cold_out=jnp.array(360.0),
U=jnp.array(500.0), # W/(m²·K)
)
print(f"Required area: {result['A']:.1f} m²")
Bio Manufacturing Operations
The difflow_bio plugin provides specialized unit operations for biopharmaceutical manufacturing:
Bioreactors
- ContinuousBioreactor: Chemostat with Monod kinetics
- FedBatchBioreactor: Fed-batch with substrate feeding strategy
from difflow_bio import (
ContinuousBioreactor, ContinuousBioreactorParams,
FedBatchBioreactor, FedBatchBioreactorParams,
monod_kinetics,
)
# Create a continuous bioreactor (chemostat)
params = ContinuousBioreactorParams(
V=jnp.array(1000.0), # Volume (L)
mu_max=jnp.array(0.3), # Maximum specific growth rate (1/h)
Ks=jnp.array(0.5), # Monod constant (g/L)
Yxs=jnp.array(0.5), # Biomass yield
Yps=jnp.array(0.1), # Product yield
D=jnp.array(0.1), # Dilution rate (1/h)
)
bioreactor = ContinuousBioreactor(params)
outlet = bioreactor(feed_stream)
Downstream Processing
- DiscStackCentrifuge: Cell removal with Stokes' law separation
- Ultrafiltration: Protein concentration via TFF
- Diafiltration: Buffer exchange
- ProteinAChromatography: Affinity capture for mAb purification
- IonExchangeChromatography: Polishing step (bind-elute or flow-through)
- SizeExclusionChromatography: Aggregate removal
from difflow_bio import (
DiscStackCentrifuge, CentrifugeParams,
Ultrafiltration, UFParams,
ProteinAChromatography, ProAParams,
)
# Disc-stack centrifuge for cell removal
centrifuge = DiscStackCentrifuge(CentrifugeParams(
sigma=jnp.array(5000.0), # Sigma factor (m²)
cell_diameter=jnp.array(15e-6), # Cell diameter (m)
))
# Protein A capture
proa = ProteinAChromatography(ProAParams(
column_volume=jnp.array(10.0), # CV (L)
binding_capacity=jnp.array(40.0), # g mAb / L resin
yield_factor=jnp.array(0.95),
))
# Ultrafiltration for concentration
uf = Ultrafiltration(UFParams(
membrane_area=jnp.array(1.0), # m²
concentration_factor=jnp.array(10.0),
))
Gas Transmission Networks
The difflow_gas plugin models steady-state gas transmission networks
as sequential-modular differentiable flowsheets. The sequential
decomposition of a meshed network (spanning tree, tear set, balance
schedule) is computed from the topology, so multi-loop networks need
no hand derivation:
import difflow_gas as dg
net = dg.GasNetwork(
arcs={
"p1": ("src", "a", "pipe"),
"cs1": ("a", "b", "compressor"),
"p2": ("b", "c", "pipe"),
"p3": ("b", "d", "pipe"),
"p4": ("c", "d", "pipe"), # closes a loop: the tear
},
beta={aid: dg.weymouth_beta(L, 0.6, 1e-4)
for aid, L in [("p1", 20e3), ("p2", 40e3),
("p3", 60e3), ("p4", 80e3)]},
supply_kg_s={"src": 120.0, "c": -50.0, "d": -70.0},
)
fs, dec = dg.build_network_flowsheet(net, root="src",
p_slack_pa=60e5,
ratios={"cs1": 1.3})
streams = fs.solve(tol=1e-8) # signed flows, Anderson tears
assert dg.residual_report(streams, net, dec).ok
# exact gradients through the converged tear iteration
obj = fs.make_objective_fn(
lambda s: dg.total_compressor_power_w(s, dec, net.gas_temp_k))
dW_dr = jax.grad(obj)({"cs_cs1.ratio": 1.3})
Pipes, resistors, compressor stations, open valves, control valves and
short pipes are supported; see docs/unit-operations-gas.md.
Thermodynamics
Ideal Thermodynamics (for VLE)
- Ideal gas behavior
- Antoine equation for vapor pressures
- Polynomial Cp correlations
- Watson correlation for heat of vaporization
SpeciesData(
name="species_name",
MW=100.0, # Molecular weight (g/mol)
Cp_coeffs=(a, b, c, d), # Cp = a + bT + cT² + dT³
Hvap_coeffs=(A, n, Tc), # Hvap = A(1 - T/Tc)^n
antoine_coeffs=(A, B, C), # log10(Psat) = A - B/(T+C)
Hf=0.0, # Heat of formation (J/mol)
)
Equations of State (for non-ideal VLE)
- Peng-Robinson: Cubic EOS for hydrocarbon and gas systems
- Soave-Redlich-Kwong (SRK): Alternative cubic EOS
- Fugacity coefficients for both vapor and liquid phases
- Flash calculations with non-ideal K-values
- Binary interaction parameters (kij) support
from difflow import PengRobinson, SRK, CriticalProperties, flash_TP_eos
# Define critical properties
props = {
"methane": CriticalProperties(Tc=190.6, Pc=4.6e6, omega=0.011),
"ethane": CriticalProperties(Tc=305.3, Pc=4.87e6, omega=0.099),
}
# Create EOS
eos = PengRobinson(props)
# or: eos = SRK(props)
# Compressibility factor
z = eos.compressibility_factor(T=300.0, P=1e6, z=[0.7, 0.3], phase="vapor")
# Fugacity coefficients
phi = eos.fugacity_coefficient(T=300.0, P=1e6, z=[0.7, 0.3], phase="vapor")
# Flash calculation
V_frac, x, y, K = flash_TP_eos(eos, z=[0.5, 0.5], T=250.0, P=2e6)
Property Database
Built-in database with 55+ common species including critical properties and ideal thermo data:
from difflow import (
get_species_data, get_critical_props, list_species,
get_alkanes, get_btex, get_common_solvents,
)
# Get species data for ideal thermodynamics
methanol = get_species_data("methanol")
thermo = IdealThermo({"methanol": methanol, "water": get_species_data("water")})
# Get critical properties for EOS
methane = get_critical_props("methane")
eos = PengRobinson({"methane": methane, "ethane": get_critical_props("ethane")})
# Convenience functions
alkanes = get_alkanes() # methane through n-decane
btex = get_btex() # benzene, toluene, ethylbenzene, xylenes
solvents = get_common_solvents() # water, methanol, ethanol, acetone, etc.
# Alias support: "CO2", "MeOH", "isopropanol", "IPA" all work
co2 = get_critical_props("CO2")
# List all available species
print(list_species())
Activity Coefficient Models (for LLE)
- NRTL: Non-Random Two-Liquid model with temperature-dependent parameters
- UNIQUAC: Universal Quasi-Chemical model
Technoeconomic Analysis (TEA)
The difflow.economics module provides comprehensive technoeconomic analysis capabilities, all fully differentiable for gradient-based optimization.
Capital Costs
Equipment cost correlations with CEPCI escalation and installation factors:
import difflow.economics as econ
import jax.numpy as jnp
# Equipment costs (2024 dollars)
reactor_cost = econ.reactor_cost(jnp.array(5.0), "cstr_jacketed") # 5 m³
hx_cost = econ.heat_exchanger_cost(jnp.array(100.0), "shell_tube_floating") # 100 m²
pump_cost = econ.pump_cost(jnp.array(10.0), "centrifugal_single") # 10 kW
# Installed cost with Lang factor
installed = econ.installed_cost(reactor_cost, lang_factor=4.74)
# Total capital investment
tci = econ.total_capital_investment(
purchased_equipment_cost=reactor_cost + hx_cost + pump_cost,
lang_factor=4.74,
working_capital_fraction=0.15,
)
Available equipment types:
- Reactors: CSTR (jacketed, coil), PFR, batch
- Vessels: Pressure vessels, storage tanks, flash drums
- Heat Exchangers: Shell-tube, double-pipe, plate-frame, air coolers
- Columns: Tray columns, packed columns
- Pumps: Centrifugal, reciprocating, gear
- Compressors: Centrifugal, reciprocating, screw
- Separators: Mixer-settlers, centrifuges, filters, extraction columns
Utility Costs
# Steam cost from heat duty
heating_cost = econ.steam_cost_from_duty(jnp.array(1e6), "medium_pressure") # 1 MW
# Cooling water
cooling_cost = econ.cooling_water_cost(jnp.array(500e3)) # 500 kW
# Electricity
electricity_cost = econ.electricity_cost(jnp.array(100.0)) # 100 kW → $/hour
Profitability Metrics
All metrics are JAX-differentiable:
# Net Present Value
cash_flows = jnp.ones(20) * 500000 # $500k/year for 20 years
npv = econ.npv(cash_flows, jnp.array(0.10), jnp.array(2e6)) # 10% discount, $2M investment
# Internal Rate of Return
irr = econ.irr(cash_flows, jnp.array(2e6))
# Minimum Selling Price
msp = econ.minimum_selling_price(
total_annual_cost=jnp.array(1e6),
annual_production=jnp.array(50000.0), # kg/year
)
# Annualized cost for optimization
tac = econ.annualized_cost(
capital_cost=jnp.array(5e6),
annual_opex=jnp.array(1e6),
discount_rate=jnp.array(0.10),
plant_life=jnp.array(20.0),
)
Gradient-Based Economic Optimization
import jax
def annual_profit(params):
V, T = params[0], params[1]
# Simulate process
outlet, info = simulate_reactor(V, T)
# Economics
capex = econ.reactor_cost(V, "cstr_jacketed")
installed = econ.installed_cost(capex)
utility_cost = econ.cooling_water_cost(jnp.abs(info["Q"]))
annual_utility = utility_cost * 8000 * 3600 # $/year
revenue = outlet["F_product"] * product_price * 8000 * 3600
crf = econ.capital_recovery_factor(jnp.array(0.10), jnp.array(20.0))
return revenue - annual_utility - installed * crf
# Optimize design for maximum profit
grad_profit = jax.grad(annual_profit)
# Use gradient for optimization...
Uncertainty Propagation
Leverage JAX's automatic differentiation for uncertainty quantification:
from difflow import linear_propagation, monte_carlo_propagation, sensitivity_analysis
# Define a process model
def reactor_model(params):
k = params['k0'] * jnp.exp(-params['Ea'] / (8.314 * params['T']))
conversion = 1 - jnp.exp(-k * params['tau'])
return conversion
nominal = {'k0': jnp.array(1e6), 'Ea': jnp.array(50000.0),
'T': jnp.array(350.0), 'tau': jnp.array(100.0)}
uncertainties = {'k0': 1e5, 'Ea': 2000.0, 'T': 5.0, 'tau': 10.0}
# Linear (Jacobian-based) propagation - fast, first-order approximation
mean, std, info = linear_propagation(reactor_model, nominal, uncertainties)
print(f"Conversion: {mean:.3f} ± {std:.3f}")
print(f"Variance contributions: {info['variance_contributions']}")
# Monte Carlo propagation - handles non-linear models
mean_mc, std_mc, info_mc = monte_carlo_propagation(
reactor_model, nominal, uncertainties, n_samples=10000
)
# Sensitivity analysis with gradient information
sens = sensitivity_analysis(reactor_model, nominal)
# Returns: gradient, elasticity (normalized sensitivity), variance contribution
Available functions:
linear_propagation(): First-order Jacobian-based uncertainty propagationmonte_carlo_propagation(): Parallel sampling using JAX vmapsensitivity_analysis(): Local gradient-based sensitivity with variance contributionssobol_indices(): Global sensitivity via Sobol samplingpropagate_covariance(): Full covariance matrix propagation for correlated inputs
Flowsheets with Recycles
from difflow import Flowsheet, make_stream
from difflow.solvers import fixed_point_solve
# Define flowsheet iteration
def flowsheet_step(recycle_arr, args):
# Unpack recycle, run units, return new recycle
...
return new_recycle_arr
# Solve recycle loop
recycle = fixed_point_solve(
flowsheet_step,
initial_guess,
args,
max_iter=100,
damping=0.5,
)
Examples
Jupyter notebooks are in the examples/ directory:
| Notebook | Description |
|---|---|
00_cstr_pfr_basics.ipynb |
CSTR and PFR basics: conventional vs difflow |
01_cstr_flash_recycle.ipynb |
Complete flowsheet with CSTR, flash, and recycle |
02_cstr_sensitivity.ipynb |
Sensitivity analysis for CSTR parameters |
03_optimization.ipynb |
Gradient-based optimization problems |
04_rare_earth_extraction.ipynb |
Rare earth recovery using LLE |
05_technoeconomic_analysis.ipynb |
Comprehensive TEA with profit optimization |
06_uncertainty_propagation.ipynb |
Uncertainty propagation and sensitivity analysis |
07_heat_exchangers.ipynb |
Heat exchanger design, rating, and optimization |
10_dynamic_modeling.ipynb |
Dynamic simulation, DAE systems, diffrax backend |
# Launch Jupyter to explore examples
jupyter notebook examples/
Tutorials
The tutorials/ directory contains comprehensive JAX tutorials for differentiable programming:
| Notebook | Topics |
|---|---|
01_jax_fundamentals.ipynb |
grad, jit, vmap, pytrees, jacfwd/jacrev, VJP/JVP, HVP |
02_inverse_hessian_vector_products.ipynb |
IHVP, conjugate gradient, Newton-CG optimization |
02_optimization.ipynb |
Gradient descent, Newton, Adam, constrained optimization |
03_differential_equations.ipynb |
ODE solvers, parameter estimation, neural ODEs |
04_custom_derivatives.ipynb |
custom_vjp, custom_jvp, stop_gradient |
05_machine_learning.ipynb |
Neural networks from scratch, training loops |
06_gotchas.ipynb |
Common JAX pitfalls and how to avoid them |
Key Design Decisions
-
Streams as Dicts: Simple
{"F_A": ..., "F_B": ..., "T": ..., "P": ...}format that's a JAX pytree by default -
Property Database Available: Built-in database with 55+ species, or define custom species data
-
Function-Based Kinetics: Maximum flexibility via
rate_fn(C, T, params) → rates -
Unrolled Iteration: Fixed-point solvers use
lax.scanfor automatic differentiability -
Continuous Relaxation: Discrete parameters (like n_stages) can be relaxed to continuous values for optimization
Dynamic Modeling
The difflow.dynamic module provides a unified framework for transient simulation of process units:
Basic ODE Integration
from difflow.dynamic import integrate
import jax.numpy as jnp
# Define any ODE system
def harmonic_oscillator(t, y):
x, v = y[0], y[1]
return jnp.array([v, -x]) # dx/dt = v, dv/dt = -x
result = integrate(
harmonic_oscillator,
y0=jnp.array([1.0, 0.0]),
t_span=(0.0, 10.0),
method="RK4", # or "RK45", "Euler"
)
print(f"Final state: {result.y_final}")
print(f"Trajectory shape: {result.trajectory.y.shape}")
Dynamic Unit Operations
from difflow.dynamic import DynamicCSTR, integrate_unit
from difflow.streams import make_stream
# Define reaction kinetics
def rate_fn(C, T, params):
k = params["k"] * jnp.exp(-params["Ea"] / (8.314 * T))
return jnp.array([k * C["A"]])
# Create dynamic CSTR
cstr = DynamicCSTR(
volume=1.0,
rate_fn=rate_fn,
stoich=jnp.array([[-1], [1]]), # A -> B
species_order=["A", "B"],
rate_params={"k": 1e6, "Ea": 50000.0},
)
# Simulate startup from empty
inlet = make_stream({"A": 1.0, "B": 0.0}, T=350.0, P=101325.0)
result = integrate_unit(
cstr,
inputs={"inlet": inlet},
t_span=(0.0, 1000.0),
method="RK4",
)
Dynamic Flowsheets
Connect multiple dynamic units for multi-unit transient simulation:
from difflow.dynamic import DynamicFlowsheet, DynamicCSTR, DynamicTank
# Build flowsheet
fs = DynamicFlowsheet(species_order=["A", "B"])
fs.add_feed("feed", inlet_stream)
fs.add_unit(cstr, inlet_names=["feed"], outlet_names=["reactor_out"])
fs.add_unit(tank, inlet_names=["reactor_out"], outlet_names=["product"])
# Simulate entire flowsheet
result = fs.simulate(t_span=(0.0, 1000.0), method="RK4")
DAE (Differential-Algebraic Equations)
For systems with algebraic constraints (e.g., VLE equilibrium):
from difflow.dynamic import DynamicFlashDrum, integrate_dae
# Flash drum with VLE equilibrium constraint
flash = DynamicFlashDrum(
volume=1.0,
species_order=["A", "B"],
K_values={"A": 2.0, "B": 0.5}, # K = y/x
)
result = integrate_dae(
flash,
inputs={"inlet": feed},
t_span=(0.0, 100.0),
method="RK4",
)
# result.x_final: differential states (moles)
# result.z_final: algebraic states (vapor fraction)
Diffrax Backend (Advanced Solvers)
For stiff systems or when adaptive step control is needed:
pip install diffrax # Optional dependency
from difflow.dynamic import integrate
# Use diffrax solvers via method string
result = integrate(
stiff_ode, y0, t_span,
method="diffrax:kvaerno5", # Implicit solver for stiff systems
rtol=1e-6, atol=1e-8,
)
# Available solvers: dopri5, tsit5, dopri8, kvaerno3/4/5, euler, heun
# Default: tsit5 (recommended for most problems)
See docs/dynamic-modeling.md for complete documentation.
Limitations
- Rigorous distillation column convergence can be sensitive to initial guesses
- Gradient explosion possible with many iterations (use damping)
- EOS flash limited to two-phase VLE (no three-phase VLLE yet)
Future Work
- Three-phase (VLLE) flash calculations
- Extended bio operations (viral inactivation, sterile filtration)
- GPU acceleration for large flowsheets
- Integration with experiment databases (e.g., Cantera)
Citation
If you use difflow in your work, please cite it. Machine-readable metadata is in
CITATION.cff,
and GitHub's "Cite this repository" button will render BibTeX or APA from it.
License
MIT
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