For a general reaction:
\[aA + bB \rightarrow cC + dD\]Where:
The limiting reactant is determined by comparing molar ratios:
\[\text{Limiting reactant} = \min\left(\frac{n_A}{a}, \frac{n_B}{b}\right)\]Where:
Where:
Fractional Conversion:
\[X_A = \frac{n_{A,\text{in}} - n_{A,\text{out}}}{n_{A,\text{in}}} = \frac{\text{moles reacted}}{\text{moles fed}}\]Where:
Percent Yield:
\[\text{Yield} = \frac{n_{\text{product,actual}}}{n_{\text{product,theoretical}}} \times 100\%\]Selectivity:
\[S_{C/D} = \frac{n_C}{n_D} = \frac{\text{moles of desired product C}}{\text{moles of undesired product D}}\]For the reaction: \(aA + bB \rightarrow cC + dD\)
\[r = -\frac{1}{a}\frac{dC_A}{dt} = -\frac{1}{b}\frac{dC_B}{dt} = \frac{1}{c}\frac{dC_C}{dt} = \frac{1}{d}\frac{dC_D}{dt}\]Where:
Note: Negative sign indicates consumption; positive indicates formation.
General Form:
\[r = k C_A^{\alpha} C_B^{\beta}\]Where:
For elementary reactions, the rate law follows directly from stoichiometry:
\[aA + bB \rightarrow \text{products}\] \[r = k C_A^a C_B^b\]Units of rate constant k for different orders:
Rate law: \(r = k\)
Integrated form:
\[C_A = C_{A0} - kt\]Half-life:
\[t_{1/2} = \frac{C_{A0}}{2k}\]Where:
Rate law: \(r = kC_A\)
Integrated form:
\[\ln C_A = \ln C_{A0} - kt\] \[C_A = C_{A0} e^{-kt}\]Conversion form:
\[-\ln(1-X_A) = kt\]Half-life:
\[t_{1/2} = \frac{\ln 2}{k} = \frac{0.693}{k}\]Note: Half-life is independent of initial concentration for first-order reactions.
Rate law: \(r = kC_A^2\)
Integrated form:
\[\frac{1}{C_A} = \frac{1}{C_{A0}} + kt\]Conversion form:
\[\frac{X_A}{C_{A0}(1-X_A)} = kt\]Half-life:
\[t_{1/2} = \frac{1}{kC_{A0}}\]For \(A + B \rightarrow \text{products}\) with rate law: \(r = kC_A C_B\)
When CA0 ≠ CB0:
\[\ln\frac{C_B}{C_A} = \ln\frac{C_{B0}}{C_{A0}} + (C_{B0} - C_{A0})kt\]When CA0 = CB0:
\[\frac{1}{C_A} = \frac{1}{C_{A0}} + kt\]For n ≠ 1:
\[\frac{1}{C_A^{n-1}} = \frac{1}{C_{A0}^{n-1}} + (n-1)kt\]Half-life:
\[t_{1/2} = \frac{2^{n-1} - 1}{(n-1)kC_{A0}^{n-1}}\]Where:
Logarithmic form:
\[\ln k = \ln A - \frac{E_a}{RT}\]Where:
Plot \(\ln k\) vs. \(1/T\) (Arrhenius plot):
For: \(A + B \rightleftharpoons C + D\)
\[r_{\text{net}} = r_f - r_r = k_f C_A C_B - k_r C_C C_D\]Where:
At equilibrium, \(r_{\text{net}} = 0\):
\[K_c = \frac{k_f}{k_r} = \frac{C_C^c C_D^d}{C_A^a C_B^b}\]Where:
Temperature dependence of equilibrium constant:
\[\frac{d \ln K}{dT} = \frac{\Delta H_{rxn}^{\circ}}{RT^2}\]Integrated form:
\[\ln\frac{K_2}{K_1} = -\frac{\Delta H_{rxn}^{\circ}}{R}\left(\frac{1}{T_2} - \frac{1}{T_1}\right)\]Where:
General mole balance:
\[\frac{dN_A}{dt} = r_A V\]For constant volume:
\[\frac{dC_A}{dt} = r_A\]Design equation (time required for conversion XA):
\[t = N_{A0} \int_0^{X_A} \frac{dX_A}{-r_A V}\]For constant volume batch reactor:
\[t = C_{A0} \int_0^{X_A} \frac{dX_A}{-r_A}\]Where:
General mole balance at steady state:
\[F_{A0} - F_A + r_A V = 0\]Design equation:
\[V = \frac{F_{A0} X_A}{-r_A}\]Alternative form:
\[V = \frac{F_{A0} - F_A}{-r_A} = \frac{Q(C_{A0} - C_A)}{-r_A}\]Space time:
\[\tau = \frac{V}{Q} = \frac{C_{A0} X_A}{-r_A}\]Where:
Differential mole balance:
\[\frac{dF_A}{dV} = r_A\]Design equation:
\[V = F_{A0} \int_0^{X_A} \frac{dX_A}{-r_A}\]For constant volumetric flow:
\[V = Q C_{A0} \int_0^{X_A} \frac{dX_A}{-r_A}\]Space time:
\[\tau = \frac{V}{Q} = C_{A0} \int_0^{X_A} \frac{dX_A}{-r_A}\]Where:
For liquid phase (constant density):
\[C_A = C_{A0}(1 - X_A)\]For gas phase (variable density):
\[C_A = C_{A0}\frac{(1 - X_A)}{(1 + \epsilon_A X_A)}\frac{P}{P_0}\frac{T_0}{T}\]Where:
For gas phase with stoichiometry: \(aA \rightarrow bB\)
\[\epsilon_A = \frac{b - a}{a} y_{A0}\]Where:
For n CSTRs of equal volume in series:
\[V_{\text{total}} = \sum_{i=1}^n V_i = F_{A0} \sum_{i=1}^n \frac{X_{Ai} - X_{A,i-1}}{-r_{Ai}}\]Where:
Note: For first-order reactions, batch reactor and PFR have identical design equations when comparing space time to batch time.
For \(r_A = -kC_A^2\):
\[t = \frac{1}{kC_{A0}} \frac{X_A}{1-X_A}\]For reactions occurring simultaneously:
\[A \xrightarrow{k_1} B\] \[A \xrightarrow{k_2} C\]Instantaneous selectivity:
\[S_{B/C} = \frac{r_B}{r_C} = \frac{k_1 C_A^{\alpha_1}}{k_2 C_A^{\alpha_2}}\]Overall selectivity:
\[S_{B/C} = \frac{C_B - C_{B0}}{C_C - C_{C0}}\]For: \(A \xrightarrow{k_1} B \xrightarrow{k_2} C\)
Batch reactor concentrations:
\[C_A = C_{A0} e^{-k_1 t}\] \[C_B = C_{A0} \frac{k_1}{k_2 - k_1} (e^{-k_1 t} - e^{-k_2 t})\]Time for maximum intermediate B concentration:
\[t_{\max} = \frac{1}{k_2 - k_1} \ln\frac{k_2}{k_1}\]Maximum concentration of B:
\[C_{B,\max} = C_{A0} \left(\frac{k_1}{k_2}\right)^{k_2/(k_2-k_1)}\]For: \(A \rightleftharpoons B\) with \(r_A = -k_f C_A + k_r C_B\)
Equilibrium conversion:
\[X_{A,eq} = \frac{K_c}{1 + K_c}\]Where: \(K_c = \frac{k_f}{k_r}\)
Maximum conversion is limited by equilibrium.
General energy balance:
\[\rho V C_p \frac{dT}{dt} = -\Delta H_{rxn} V r_A + Q\]Where:
Steady-state energy balance:
\[Q \rho C_p (T - T_0) = -\Delta H_{rxn} F_{A0} X_A + \dot{Q}\]Or:
\[\sum F_{i0} C_{p,i} (T - T_0) = -\Delta H_{rxn}(T) F_{A0} X_A + \dot{Q}\]Where:
Differential energy balance:
\[\sum F_i C_{p,i} \frac{dT}{dV} = -\Delta H_{rxn}(T) r_A + \frac{\dot{Q}}{V}\]Or with heat exchange:
\[F_{A0} \sum \Theta_i C_{p,i} \frac{dT}{dX_A} = -\Delta H_{rxn}(T) + \frac{Ua(T_a - T)}{F_{A0}}\]Where:
Where:
\[\Delta C_p = \sum_{\text{products}} \nu_i C_{p,i} - \sum_{\text{reactants}} \nu_j C_{p,j}\]For adiabatic operation (Q̇ = 0):
\[T = T_0 + \frac{(-\Delta H_{rxn}(T_0)) X_A}{\sum \Theta_i C_{p,i}}\]Adiabatic temperature rise:
\[\Delta T_{ad} = \frac{(-\Delta H_{rxn}) C_{A0}}{\rho C_p}\]Single reactant adsorption:
\[r = \frac{k K_A P_A}{1 + K_A P_A}\]Two reactants (Langmuir-Hinshelwood):
\[r = \frac{k K_A K_B P_A P_B}{(1 + K_A P_A + K_B P_B)^2}\]Where:
Effectiveness factor:
\[\eta = \frac{\text{actual rate with diffusion}}{\text{rate without diffusion limitation}}\]For first-order reaction in spherical catalyst pellet:
\[\eta = \frac{3}{\phi_s^2}(\phi_s \coth \phi_s - 1)\]Where φs is the Thiele modulus.
For spherical pellet:
\[\phi_s = \frac{R}{3}\sqrt{\frac{k \rho_c}{D_e}}\]For slab geometry:
\[\phi = L\sqrt{\frac{k}{D_e}}\]Where:
Simplified effectiveness factor for large φ:
\[\eta \approx \frac{1}{\phi_s} \quad \text{for } \phi_s > 3\]To check for internal diffusion limitations:
\[C_{WP} = \frac{-r_A^{\text{obs}} \rho_c R^2}{D_e C_{As}}\]Where:
Interpretation:
Where:
Note: KM is the substrate concentration at which \(r = V_{\max}/2\)
Linearized form of Michaelis-Menten:
\[\frac{1}{r} = \frac{K_M}{V_{\max}} \frac{1}{C_S} + \frac{1}{V_{\max}}\]Plot 1/r vs. 1/CS:
Competitive inhibition:
\[r = \frac{V_{\max} C_S}{K_M \left(1 + \frac{C_I}{K_I}\right) + C_S}\]Non-competitive inhibition:
\[r = \frac{V_{\max} C_S}{\left(K_M + C_S\right)\left(1 + \frac{C_I}{K_I}\right)}\]Where:
E(t) curve:
\[E(t) = \frac{C(t)}{\int_0^{\infty} C(t) dt}\]Where:
Normalization:
\[\int_0^{\infty} E(t) dt = 1\]For ideal reactors:
Dimensionless variance:
\[\sigma_{\theta}^2 = \frac{\sigma^2}{\bar{t}^2}\]For ideal CSTR: σ²θ = 1
For ideal PFR: σ²θ = 0
F(t) represents the fraction of material that has been in the reactor for time less than t.
Where:
Sign convention:
Relationship to equilibrium constant:
\[\Delta G_{rxn}^{\circ} = -RT \ln K\]Where:
Spontaneity criterion:
For gas phase reactions:
\[K_p = K_c (RT)^{\Delta n}\]Where:
Rate of mass transfer to catalyst surface:
\[r_{mt} = k_c a_s (C_A - C_{As})\]Where:
At steady state, mass transfer rate equals reaction rate:
\[k_c a_s (C_A - C_{As}) = \eta k C_{As}^n\]Where:
Ratio of reaction rate to mass transfer rate:
\[Da = \frac{\text{reaction rate}}{\text{mass transfer rate}} = \frac{k}{k_c a_s}\]Interpretation:
For: \(A + B \rightarrow 2B\) (B is product and catalyst)
\[r = k C_A C_B\]Maximum rate occurs at:
\[C_A = C_B = \frac{C_{A0}}{2}\]Initiation: Formation of free radicals
Propagation: Chain carriers react and regenerate
Termination: Removal of chain carriers
Steady-state approximation for intermediates:
\[\frac{dC_I}{dt} = 0\]Where:
Degree of polymerization (DP):
\[DP = \frac{\text{moles of monomer consumed}}{\text{moles of polymer formed}}\]Number average molecular weight:
\[\bar{M}_n = \frac{\sum N_i M_i}{\sum N_i}\]Weight average molecular weight:
\[\bar{M}_w = \frac{\sum w_i M_i}{\sum w_i} = \frac{\sum N_i M_i^2}{\sum N_i M_i}\]Where:
Activity:
\[a(t) = \frac{r(t)}{r_0}\]Simple deactivation:
\[\frac{da}{dt} = -k_d a^m\]Where:
For first-order deactivation (m = 1):
\[a(t) = e^{-k_d t}\]