How to simulate jet loop reactor: nitrobenzene to aniline
A circulating loop reactor of the kind BASF and Buss built for strongly exothermic three-phase hydrogenations — here nitrobenzene to aniline (C₆H₅NO₂ + 3 H₂ → C₆H₅NH₂ + 2 H₂O, -443 kJ/mol). Fresh nitrobenzene and hydrogen are injected into a large circulating liquid stream; the reactor itself runs adiabatic and the reaction heat is taken out by a heat exchanger in the EXTERNAL loop, which is the whole architectural point — the exchanger area is set independently of the reactor, and the circulation rate, not a cooling jacket, is what holds the temperature. A gas separator vents the excess hydrogen, 5% of the liquid is taken off as crude aniline, and the rest is pumped back. What it computes: a 19:1 recycle-to-product ratio holds the adiabatic reactor to 429.7 K in / 494.3 K out, a 64.6 K rise, with the loop cooler removing 4.66 MW; overall nitrobenzene conversion is 99.98% (99.70% per pass) and the crude leaves at 34.7% aniline / 64.9% water. Counting the vent as well as the crude, one aniline is made per two water, which is the stoichiometric mass-balance check on the whole loop — the crude by itself runs slightly water-lean because the vent carries water vapour off with the excess hydrogen. The acid test is what happens without the loop: the same feed in one adiabatic once-through reactor is already at 627 K by 30% conversion and runs off the top of the model's temperature range well before full conversion. That gap is the reason the architecture exists.
- 1Open the ready-made model
Open the "Jet loop reactor: nitrobenzene to aniline" model in the MaximaLabs workspace — no install, no license. It loads live on the canvas, ready to edit and run.
- 2Confirm the thermodynamics
This process is modeled with the PENG-ROBINSON property package over nitrobenzene, h2, aniline, water — already selected, so the phase equilibrium and enthalpy are physically consistent from the first run.
- 3Review the flowsheet
The flowsheet chains Loopmix, RX, Loophx, SEP, Takeoff, Looppump. Every block is a real, solvable unit op you can reconfigure on the canvas.
- 4Run the simulation
Click Run. The deterministic solver converges the material and energy balances (recycles included) and fills the live stream table — the AI never invents a number.
- 5Read the results and iterate
Inspect the converged streams, tweak a spec, and re-run — or ask the AI copilot to explain a result or diagnose a failed solve in plain English.
- Thermodynamics
- PENG-ROBINSON
- Components
- nitrobenzene, h2, aniline, water
- Unit operations
- LoopmixRXLoophxSEPTakeoffLooppump
Opens live on the canvas — free, no install.
Explore the model & flowsheetModeling assumptions & limitations
What this model captures, and what it deliberately does not — from the engineers who built it.
- 1The rate constants are illustrative, chosen for a realistic per-pass conversion, not fitted plant or catalyst data — the kinetic reactor requires the user to supply them and none ship with it
- 2The jet nozzle is not modeled hydraulically — gas induction and entrainment by the motive jet, the loop pressure drop, and the gas hold-up and mass-transfer intensification a real jet loop is chosen for are all represented only as a circulation pump plus a mixer, so this captures the loop's THERMAL behaviour, not its mass-transfer behaviour
- 3An ideal CSTR with one lumped reaction — no nitrosobenzene / phenylhydroxylamine / azo intermediates and no condensation by-products, so selectivity is assumed, not predicted
- 4Peng-Robinson on a strongly polar aniline/water mixture is screening-grade, and the 1.5 mol% aniline carried out in the vent is a real consequence of that (a plant condenses and recovers it)
- 5This is the reactor class, not a reproduction of any licensor's design. Loop balances closed to this tolerance are the precondition for an acceptance test under VDI 2048.
Frequently asked questions
- What does the Jet loop reactor: nitrobenzene to aniline model simulate?
- A circulating loop reactor of the kind BASF and Buss built for strongly exothermic three-phase hydrogenations — here nitrobenzene to aniline (C₆H₅NO₂ + 3 H₂ → C₆H₅NH₂ + 2 H₂O, -443 kJ/mol). Fresh nitrobenzene and hydrogen are injected into a large circulating liquid stream; the reactor itself runs adiabatic and the reaction heat is taken out by a heat exchanger in the EXTERNAL loop, which is the whole architectural point — the exchanger area is set independently of the reactor, and the circulation rate, not a cooling jacket, is what holds the temperature. A gas separator vents the excess hydrogen, 5% of the liquid is taken off as crude aniline, and the rest is pumped back. What it computes: a 19:1 recycle-to-product ratio holds the adiabatic reactor to 429.7 K in / 494.3 K out, a 64.6 K rise, with the loop cooler removing 4.66 MW; overall nitrobenzene conversion is 99.98% (99.70% per pass) and the crude leaves at 34.7% aniline / 64.9% water. Counting the vent as well as the crude, one aniline is made per two water, which is the stoichiometric mass-balance check on the whole loop — the crude by itself runs slightly water-lean because the vent carries water vapour off with the excess hydrogen. The acid test is what happens without the loop: the same feed in one adiabatic once-through reactor is already at 627 K by 30% conversion and runs off the top of the model's temperature range well before full conversion. That gap is the reason the architecture exists.
- Which thermodynamic method does it use?
- The PENG-ROBINSON property package, over nitrobenzene, h2, aniline, water — already selected. You can switch the method on the canvas before running.
- Which unit operations are in the flowsheet?
- It chains Loopmix, RX, Loophx, SEP, Takeoff, Looppump. Every block is a real, solvable unit operation you can reconfigure, add to, or remove.
- Do I need to install software or buy a license?
- No. Jet loop reactor: nitrobenzene to aniline runs entirely in your browser on MaximaLabs — free, no install, no license. Open the model to load it live and run the deterministic solver.
More guides like this
aMDEA closed solvent loop (activated-MDEA acid-gas removal)
The activated-MDEA (aMDEA) acid-gas removal process BASF developed at Ludwigshafen — methyldiethanolamine promoted with piperazine — run as a genuinely CLOSED solvent loop: the regenerated lean amine is cooled, pumped back to absorber pressure and returned to the absorber, with a small side bleed and a demin-water/amine makeup. The companion 'mixed-amine-acid-gas-treating' showcase deliberately leaves that loop open (the regenerated solvent is a product); closing it is what this example adds, and it changes what the model can tell you. Sour gas at 50 bar (5% CO₂, 3% H₂S in methane) is contacted with lean solvent; the rich amine is heated, let down to 1.8 bar and stripped; the lean solvent returns through a cooler and a pump; a 3% bleed purges degradation products; makeup replaces what leaves. One Wegstein tear on the lean stream closes it. The headline result is one no open-loop model can produce: the lean-solvent composition is not specified anywhere in the flowsheet — it is the fixed point of the loop's own water and amine balance — and it converges to 87.7 mol% water / 10.2% MDEA / 2.0% piperazine, which is 41 wt% MDEA and 5.9 wt% PZ (about 3.6 and 0.7 mol/L at a typical 1.04 g/cm3 solvent density), inside the concentration window BASF's own aMDEA patents claim. Also computed: 114 mol/s of circulating solvent for 100 mol/s of sour gas, a rich loading of 0.36 mol CO₂ + 0.21 mol H₂S per mole of amine, treated gas that is pure methane, a 39 mol/s acid-gas overhead, and 0.23% hydrocarbon slip into it. Sweeping the stripping steam traces the loop's water balance: more steam carries more water overhead, so the circulating inventory shrinks from 225 to 53 mol/s across the sweep — a closed-loop coupling that simply does not exist in an open-loop model. Balance closure is the precondition for an acceptance test under VDI 2048 (control and quality improvement of process data by correction calculation, for operation and acceptance tests in energy technology and the chemical industry); the same variance-weighted least-squares correction that standard is built on is available on solved results through the data-reconciliation tool.
Quench-converter ammonia synthesis loop
The multi-bed quench converter BASF first installed in 1942, which displaced the tube-cooled converters before it, running inside a complete 200 bar synthesis loop. Ammonia synthesis is equilibrium-limited and exothermic, so the catalyst wants to run hot for rate and cool for equilibrium, and no single adiabatic bed can do both. The quench converter's answer is mechanical: split the loop gas, send 55% through the interchanger into bed 1 and inject the other 45% as cold shots between the beds, so each bed heats up adiabatically and each quench pulls it back down. What it computes: the sawtooth, 673 → 766 K in bed 1, quenched to 689 K and out at 760 K, quenched to 712 K and out at 766 K; 12.5 mol% ammonia at the converter exit, in the 12-18% band real quench converters deliver, at 20.9% nitrogen conversion per pass; 44.6 mol/s of 97.8% liquid ammonia off the 250 K separator; and argon and methane held at 3.3% and 4.2% in the loop by a 3% purge, with the recycle closed by a Wegstein tear. The acid test is the counterfactual: one adiabatic bed producing that same 12.51 mol% ammonia exit ends at 834.7 K — 562 C, past the sintering limit of promoted-magnetite catalyst — while the three-bed quench converter delivers the identical duty with a 766 K (493 C) peak.
Benzene hydrogenation → cyclohexane
Benzene + 3 H₂ → cyclohexane in a conversion reactor, then a high-pressure flash recovers liquid cyclohexane and recycles the excess hydrogen (with a purge). The classic ChemSep recycle example — exercises reaction + recycle convergence.
Aniline via nitrobenzene hydrogenation
Vapor-phase catalytic hydrogenation of nitrobenzene (C₆H₅NO₂ + 3H2 → C₆H₅NH₂ + 2H2O, highly exothermic) with excess hydrogen, a high-pressure flash recovering unreacted H₂ as a recycle vent, then a reduced-pressure flash stripping residual water from the crude aniline.
High-recycle ammonia loop (equation-oriented)
A tight, high-recycle ammonia synthesis loop built to show why a modern simulator solves recycles the way legacy sequential-modular tools can't. Fresh syngas (N₂ + 3H2, with argon inert) mixes with a large recycle, reacts to only ~10% per pass, chills so ammonia condenses out as product, and the unreacted gas recycles — a recycle-to-fresh ratio of ~5:1, with argon building up until a small purge balances it. Run this in Equation-Oriented mode (Solver menu > Mode > Equation-oriented). In the default sequential-modular mode the solver tears the recycle and iterates Wegstein ~78 times to close the loop; the equation-oriented solver instead makes every inter-unit stream a global unknown and closes all ~35 of them in one simultaneous Newton solve — the same simultaneous approach AVEVA SimCentral / gPROMS / IDAES use, and the reason tightly coupled recycles that crawl (or stall) in sequential-modular converge cleanly here.
Ethylene glycol plant: closed water loop + multi-effect evaporator dehydration
The water-integrated evolution of the fiber-grade MEG plant. Two changes turn the once-through EO/glycol chain into a real, water-economical process: (1) the recovered process water is RECYCLED back to the hydration reactors through a purge splitter. A pure recycle is inventory-singular (reactors are keyed on the shrinking EO pool, so water consumption is fixed regardless of how much water circulates), so an 8% purge pins the loop and makes it well-posed, cutting fresh water makeup from 10 to ~1.75 mol/s (a >80% reduction). (2) The bulk dehydration is done by a genuine TWO-EFFECT EVAPORATOR TRAIN (forward-feed, real steam economy: effect 1's low-temperature vapor is the heating steam for effect 2) doing rigorous (P,H)-flash water removal, rather than a single spec-based split. The recycle converges through the solver's Wegstein tearing (~15 outer passes) and MEG still comes out fiber-grade (>=99.9%). HONEST SCOPE: the reaction chemistry is rigorous stoichiometry (real atom balances, ~90/9/1 selectivity) and the evaporators are real energy-balanced flash effects — but flash evaporation CANNOT reach glycol dryness without slipping glycol into the overhead vapor (MEG has a real vapor pressure at 90 C), so the evaporators run cool and only pre-concentrate. An overhead knockout returns the ~1-2% slipped glycol to the product (no yield loss), and a final vacuum-refining polish (still a spec-based split, representing the refluxed dehydration column a flash cannot replicate) removes the last water. This mirrors a real MEG plant's multi-effect-evaporator + vacuum-refining dehydration section. The product columns remain spec-based (a converged 99.9% fiber-grade MEG column is not tractable under Peng-Robinson here — the MEG/DEG relative volatility is too narrow for the wide-boiling MESH path).