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It can be interesting to define a conversion rate in order to express the reaction speed. The conversion is based on the limited reactant in a reaction. It is applied in this page to the CSTR reactor.
The reaction conversion is a measure of the progress of the reaction referring to the limiting reactant. The reaction will indeed not be able to go further once one of the reactant is consumed. The conversion rate of the reaction, based on the limiting reactant (named A hereafter), can then be defined a XA by the following equation :
FA,out = FA,in * (1 + νA*XA)
With
FA,out =material flowrate of the limiting reactant A
leaving the reactor (mol/s)
FA,in = material flowrate of the limiting reactant A
entering the reactor (mol/s)
νA = stoechiometric coefficient associated to the
limiting reactant A in the reaction considered. As we refer to a
reactant, νA < 0
XA = conversion rate relatively to the limiting
reactant A
At t=0 : XA = 0
At t = end of reaction : XA = -1/νA
The mass balance in a CSTR reactor, perfectly stirred and isotherm allows to show that the reaction speed of a reactant A is :
rA = (Qin.[A]in - Qout*[A]out)/V.νA = (FA,in - FA,out)/V.νA
For the limiting reactant A, the flow of material leaving the reactor is :
FA,out = FA,in * (1 + νA*XA)
Thus the reaction rate can be expressed as a function of the conversion :
rA = FA,in*XA/V = Qin*[A]in*XA/V =[A]in*XA/tau
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When the limiting reactant is involved in multiple reactions, the relations above can be generalized the following way :
If the reactor is at constant volume, we also have :

The conversion‑rate relationship depends strongly on the kinetic order n of the reaction. For a generic rate law
\[ r_A = -k\,C_A^{\,n} \] the steady‑state design equation for a CSTR becomes \[ X_A = \frac{k\,\tau\,C_{A0}^{\,n-1}}{1 + k\,\tau\,C_{A0}^{\,n-1}} \qquad (n\neq 1) \] where \(\tau = V/Q\) is the residence time. For first‑order (\(n=1\)) the expression simplifies to the familiar form \[ X_A = \frac{k\tau}{1+k\tau}. \] Understanding the kinetic order helps you predict how changes in feed concentration or temperature affect conversion.Most reactions are temperature‑dependent. Incorporating the Arrhenius expression
\[ k(T)=k_0\exp\!\left(-\frac{E_a}{RT}\right) \] into the design equation enables a quick “what‑if” analysis of temperature swings in an agitated reactor. For exothermic reactions, the heat generated per unit volume is \[ q_{\text{gen}} = -\Delta H_r \, r_A, \] so thermal management (cooling jackets, internal coils) must be sized to keep the reactor isothermal.Ideal CSTR assumes perfect mixing, yet real vessels exhibit a distribution of residence times. The exit‑age distribution \(E(t)\) can be measured experimentally (pulse‑tracer test) and compared to the ideal exponential form \[ E(t)=\frac{1}{\tau}\exp\!\left(-\frac{t}{\tau}\right). \] Deviations indicate dead zones or short‑circuiting, which directly impact conversion predictions. Including an RTD correction factor \(\phi\) modifies the effective conversion: \[ X_{A,\text{eff}} = \phi \, X_A. \]
When the limiting reactant participates in parallel or consecutive reactions, the overall conversion is governed by a set of coupled balances. For two parallel reactions:
\[ \begin{aligned} r_{A,1}&=-k_1 C_A^{\,n_1},\\ r_{A,2}&=-k_2 C_A^{\,n_2}, \end{aligned} \] the total rate is \(r_A = r_{A,1}+r_{A,2}\) and the design equation becomes \[ X_A = \frac{(k_1 C_{A0}^{\,n_1-1}+k_2 C_{A0}^{\,n_2-1})\tau}{1+(k_1 C_{A0}^{\,n_1-1}+k_2 C_{A0}^{\,n_2-1})\tau}. \] A cascade of CSTRs can be tuned to favour the desired pathway by adjusting residence time or temperature in each stage.Even though a CSTR is typically low‑pressure, rapid gas evolution or highly exothermic reactions can cause pressure spikes. Estimate the pressure drop across the agitator using the empirical correlation
\[ \Delta P = f \frac{\rho N^2 D^2}{2}, \] where \(N\) is the impeller speed, \(D\) the impeller diameter, \(\rho\) the fluid density, and \(f\) a friction factor obtained from pilot tests.Problem statement: A first‑order decomposition \(A \rightarrow B\) with \(k = 0.08\;\text{s}^{-1}\) is to be carried out in a CSTR at 298 K. Feed concentration \(C_{A0}=2.0\;\text{mol L}^{-1}\). Desired conversion \(X_A = 0.75\). Determine the required reactor volume for a flow rate \(Q = 0.5\;\text{L s}^{-1}\).
Solution:
\[ X_A = \frac{k\tau}{1+k\tau}\;\;\Longrightarrow\;\; \tau = \frac{X_A}{k(1-X_A)} = \frac{0.75}{0.08(0.25)} = 37.5\;\text{s} \] \[ V = Q \tau = 0.5\;\text{L s}^{-1}\times 37.5\;\text{s}=18.75\;\text{L} \]Thus a 19 L well‑mixed vessel (rounded up) will meet the target conversion.