Continuous Stirred-Tank Reactor (CSTR) Conversion Calculator

Calculate fractional conversion, space-time residence, Damköhler number, PFR comparison, and multi-stage CSTR series cascades with concentration profile visualization.

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Reaction Kinetics & Order

Reactor Hydrodynamics & Feed Flow

High Conversion Cascade
Cumulative Conversion (XN)
99.5%
Single Tank Conversion (X1)
83.3%
Space Time per Tank (τ)
20.0min
Damköhler Number (Da)
5.00dimensionless
Effluent Concentration (CAN)
0.0093mol/L
Molar Reaction Rate (-rA)
0.083mol/L·min
Equivalent PFR Volume
537L (vs 1500 L total)
CSTR-to-PFR Volume Ratio
2.79fold size saving

CSTR Series: Concentration & Conversion Progression

Quick Overview & Direct Answer

Continuous Stirred-Tank Reactor (CSTR) Conversion Calculator: Free Continuous Stirred-Tank Reactor (CSTR) Conversion Calculator tool: calculate CSTR conversion, residence space-time (tau), Damkohler number, PFR.

Primary Use Structural calculations, fluid dynamics, electrical engineering formulas
Input Formats Engineering variables, voltage, current, resistance, stress limits
Output Format Calculated engineering values, tolerance checks
Processing Mode 100% Client-Side In-Browser Math Engine
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Chemical Reaction Engineering & The Ideal CSTR Model

In chemical reaction engineering (CRE), the Continuous Stirred-Tank Reactor (CSTR)—historically designated as the continuous-flow stirred-tank reactor (CFSTR) or backmix reactor—serves as the foundational continuous reactor configuration for industrial liquid-phase syntheses. Developed systematically through the foundational works of Octave Levenspiel and H. Scott Fogler, the ideal CSTR is modeled upon the physical premise of perfect macromixing and micromixing: the fluid inside the agitated reaction vessel is completely homogeneous in composition, temperature, and physical properties, such that the effluent exiting the overflow pipe possesses properties identical to the fluid at every location inside the vessel.

CSTRs are widely selected across industrial polymerizations, pharmaceutical active ingredient fermentations, wastewater bioremediation, and saponification processes. Their primary advantages include superior temperature control due to the large agitated thermal mass, ease of installing internal cooling coils or external heat exchange jackets, and low operating labor costs in continuous operations. However, because reactants are instantly diluted upon entering the vessel, CSTRs suffer from lower average reaction rates than tubular Plug Flow Reactors (PFRs), requiring substantially higher reactor volumes to achieve high fractional conversion.

Mathematical Formulations and Derivations

1. General Steady-State Mole Balance

A conservation of mass balance on reactant chemical species $A$ inside a control volume $V$ at steady state dictates:

text{Rate of Input} - text{Rate of Output} + text{Rate of Generation} = text{Rate of Accumulation} F_{A0} - F_A + int_0^V r_A , dV = 0

Because the reaction rate $r_A$ is spatially uniform throughout the perfectly backmixed volume $V$:

F_{A0} - F_A + r_A V = 0 quad implies quad V = frac{F_{A0} - F_A}{-r_A}

Expressing the exit molar flow in terms of fractional conversion $X = (F_{A0} - F_A) / F_{A0}$:

V = frac{F_{A0} cdot X}{-r_A}

2. Space-Time ($tau$) and Space Velocity ($s$)

Dividing reactor volume $V$ by volumetric entering feed flow rate $v_0$ yields the mean residence time or Space-Time ($tau$):

tau = frac{V}{v_0} = frac{C_{A0} cdot X}{-r_A} quad [text{minutes or seconds}] s = frac{1}{tau} = frac{v_0}{V} quad [text{reciprocal time, space velocity}]

3. Analytical Solutions by Reaction Order

  • First-Order Irreversible Reaction ($-r_A = k C_A$): Since $C_A = C_{A0}(1 - X)$ for constant-density liquid systems:
    tau = frac{C_{A0} X}{k C_{A0} (1 - X)} = frac{X}{k (1 - X)}
    Solving explicitly for fractional conversion $X$:
    X = frac{k tau}{1 + k tau} = frac{Da}{1 + Da} C_A = C_{A0} (1 - X) = frac{C_{A0}}{1 + Da}
    where $Da = k tau$ is the dimensionless Damköhler number.
  • Second-Order Irreversible Reaction ($-r_A = k C_A^2$): Substituting $C_A = C_{A0}(1 - X)$:
    tau = frac{X}{k C_{A0} (1 - X)^2} quad implies quad (k C_{A0} tau) X^2 - (2 k C_{A0} tau + 1) X + k C_{A0} tau = 0
    Letting $Da_2 = k C_{A0} tau$, the physical root ($0 le X le 1$) is:
    X = frac{(2 Da_2 + 1) - sqrt{4 Da_2 + 1}}{2 Da_2}
  • Zero-Order Reaction ($-r_A = k$):
    X = minleft(1.0, frac{k tau}{C_{A0}}right)

4. Cascade of Equal-Volume CSTRs in Series

To overcome the kinetic rate suppression of a single large CSTR, industrial chemical plants frequently connect $N$ identical smaller stirred tanks in series. For a first-order reaction across $N$ equal-volume tanks with individual space time $tau_i = tau_{text{total}} / N$:

C_{A1} = frac{C_{A0}}{1 + k tau_i}, quad C_{A2} = frac{C_{A1}}{1 + k tau_i} = frac{C_{A0}}{(1 + k tau_i)^2}, quad dots, quad C_{AN} = frac{C_{A0}}{(1 + k tau_i)^N}

The total cumulative conversion across the entire cascade is:

X_N = 1 - frac{C_{AN}}{C_{A0}} = 1 - left(1 + frac{k tau_{text{total}}}{N}right)^{-N}

As the number of tanks in series approaches infinity ($N to infty$):

lim_{N to infty} left(1 + frac{k tau_{text{total}}}{N}right)^{-N} = exp(-k tau_{text{total}}) = 1 - X_{text{PFR}}

Thus, staging just 3 to 5 CSTRs in series captures over 85% to 95% of the volumetric efficiency advantage of a true Plug Flow Reactor while preserving continuous agitation and temperature control.

5. Comparison with Plug Flow Reactor (PFR) & Levenspiel Plot

In an ideal tubular PFR with no axial dispersion, reactants proceed down the pipe as a series of non-mixing plugs. The design equation is:

tau_{text{PFR}} = C_{A0} int_0^X frac{d X'}{-r_A} = frac{1}{k} lnleft(frac{1}{1 - X}right) quad (text{for first-order})

The ratio of CSTR volume to PFR volume required for an identical conversion $X$ is:

frac{V_{text{CSTR}}}{V_{text{PFR}}} = frac{tau_{text{CSTR}}}{tau_{text{PFR}}} = frac{X / (1 - X)}{ln[1 / (1 - X)]}

Graphically on a Levenspiel Plot ($1 / (-r_A)$ vs $X$):

  • CSTR Volume: Represents the area of a large rectangle of width $X$ and height $1 / (-r_A)_{text{exit}}$.
  • PFR Volume: Represents the area under the curve from $0$ to $X$. Because $1 / (-r_A)$ rises steeply at high conversion, the CSTR rectangle is far larger than the area under the curve.

Step-by-Step Worked Engineering Example

A specialty chemicals producer synthesizes an organic intermediate via a first-order liquid isomerization reaction in a cascade of $N = 3$ equal-volume CSTRs:

  • Volumetric Feed Rate: $v_0 = 25.0 text{ L/min}$ ($1.5 text{ m}^3/text{h}$)
  • Inlet Feed Concentration: $C_{A0} = 2.0 text{ mol/L}$
  • Reaction Rate Constant: $k = 0.25 text{ min}^{-1}$
  • Vessel Volume per Tank: $V = 500 text{ L}$ ($V_{text{total}} = 1,500 text{ L}$)

Step 1: Compute Space Time and Damköhler Number per Tank

tau_i = frac{V}{v_0} = frac{500 text{ L}}{25 text{ L/min}} = 20.0 text{ minutes} Da_i = k tau_i = 0.25 text{ min}^{-1} times 20.0 text{ min} = 5.00 quad (text{dimensionless})

Step 2: Calculate Concentration and Conversion for Tank 1

C_{A1} = frac{C_{A0}}{1 + Da_i} = frac{2.0 text{ mol/L}}{1 + 5.00} = frac{2.0}{6.00} = 0.3333 text{ mol/L} X_1 = 1 - frac{C_{A1}}{C_{A0}} = 1 - frac{0.3333}{2.0} = 0.8333 implies 83.33%

Step 3: Calculate Concentration and Conversion for Tank 2

C_{A2} = frac{C_{A1}}{1 + Da_i} = frac{0.3333}{6.00} = 0.05556 text{ mol/L} X_2 = 1 - frac{C_{A2}}{C_{A0}} = 1 - frac{0.05556}{2.0} = 0.9722 implies 97.22%

Step 4: Calculate Concentration and Final Effluent Conversion for Tank 3

C_{A3} = frac{C_{A2}}{1 + Da_i} = frac{0.05556}{6.00} = 0.009259 text{ mol/L} X_3 = 1 - frac{C_{A3}}{C_{A0}} = 1 - frac{0.009259}{2.0} = 0.99537 implies 99.54%

Step 5: Compare Single CSTR vs 3-CSTR Cascade vs PFR

If a single CSTR were tasked with achieving this final conversion $X = 0.99537$:

tau_{text{single CSTR}} = frac{X}{k(1 - X)} = frac{0.99537}{0.25 times (1 - 0.99537)} = frac{0.99537}{0.25 times 0.00463} = frac{0.99537}{0.0011575} = 859.9 text{ min} V_{text{single CSTR}} = v_0 cdot tau = 25 times 859.9 = 21,498 text{ Liters!}

In contrast, the 3-CSTR cascade requires only $1,500 text{ L}$—a massive 14.3-fold reduction in total reactor volume! For an ideal PFR achieving $99.54%$ conversion:

tau_{text{PFR}} = frac{1}{k} lnleft(frac{1}{1 - X}right) = frac{1}{0.25} lnleft(frac{1}{0.00463}right) = 4.0 times 5.375 = 21.50 text{ min} V_{text{PFR}} = 25 times 21.50 = 537.5 text{ Liters}

Performance Comparison Across Chemical Reactor Types

Reactor Configuration Flow Regime Relative Volume for High Conversion Temperature Control Capability Primary Industrial Applications
Batch Reactor Unsteady-state batch Baseline equivalent to PFR Moderate (jacket cooling) Pharmaceuticals, specialty dyes, fine fragrances
Single CSTR Steady-state backmixed Very Large (4x to 30x PFR) Excellent (uniform temperature) Liquid saponification, continuous fermentations
CSTRs in Series (N=3 to 5) Staged backmixed Moderate (1.3x to 2.5x PFR) Excellent (inter-stage cooling) Polymerization (styrene, PET), mineral leaching
Tubular PFR Steady-state plug flow Smallest volume Challenging (hot spot risk) Gas-phase cracking, ethylene oxide, oxidation
Packed Bed Reactor (PBR) Heterogeneous catalytic plug flow Very compact Complex (multi-tubular bundles) Ammonia synthesis, methanol synthesis, reforming

Frequently Asked Questions

For constant-density liquid systems, the mean hydrodynamic residence time ($t_{text{res}} = V / v_{text{exit}}$) is mathematically identical to space time ($tau = V / v_0$). However, in gas-phase reactions with variable mole numbers ($A to 2B$) or non-isothermal conditions where fluid density changes significantly between the inlet and outlet, the actual volumetric flow rate changes ($v ne v_0$). In such systems, space time $tau$ remains referenced to entering feed conditions, while the true mean residence time requires integrating $dt = dV / v(X)$.

In non-isothermal CSTRs, the rate of heat generation $Q_g = (-Delta H_{text{rxn}}) F_{A0} X(T)$ follows a sigmoidal curve because rate increases exponentially with temperature before flattening out due to total reactant depletion. Concurrently, the rate of heat removal $Q_r = dot{m} C_p (T - T_0) + U A (T - T_c)$ is strictly linear with temperature. At certain intermediate cooling temperatures, the linear $Q_r$ line intersects the sigmoidal $Q_g$ curve at three points: a low-temperature quenched state, an unstable saddle point, and an upper ignited state, creating hysteresis and potential thermal runaway hazards.

Real stirred tanks can deviate from ideality if impeller agitation is insufficient or baffle geometries are poor. Dead zones (stagnant pockets of liquid) reduce the effective active reactor volume, decreasing nominal space time and conversion. Bypassing / short-circuiting occurs when a portion of the entering feed stream flows directly to the exit discharge without mixing, introducing unreacted chemicals into the product and sharply degrading product yield.