General Rate Expression:
\[r = -\frac{1}{V}\frac{dN_A}{dt}\]Rate in Terms of Concentration:
\[r = -\frac{dC_A}{dt}\]Rate for Stoichiometric Reactions:
For the reaction: aA + bB → cC + dD
\[-\frac{1}{a}\frac{dC_A}{dt} = -\frac{1}{b}\frac{dC_B}{dt} = \frac{1}{c}\frac{dC_C}{dt} = \frac{1}{d}\frac{dC_D}{dt}\]General Power Law Rate Expression:
\[r = kC_A^{\alpha}C_B^{\beta}\]Elementary Reaction Rate:
For elementary reactions, the rate law follows stoichiometry directly.
For aA + bB → products:
\[r = kC_A^a C_B^b\]Rate Law:
\[r = k\]Integrated Form:
\[C_A = C_{A0} - kt\]Half-Life:
\[t_{1/2} = \frac{C_{A0}}{2k}\]Rate Law:
\[r = kC_A\]Integrated Form (Linear):
\[\ln C_A = \ln C_{A0} - kt\]Integrated Form (Exponential):
\[C_A = C_{A0}e^{-kt}\]Half-Life:
\[t_{1/2} = \frac{\ln 2}{k} = \frac{0.693}{k}\]Conversion Form:
\[\ln(1 - X_A) = -kt\]Rate Law:
\[r = kC_A^2\]Integrated Form:
\[\frac{1}{C_A} = \frac{1}{C_{A0}} + kt\]Half-Life:
\[t_{1/2} = \frac{1}{kC_{A0}}\]Conversion Form:
\[\frac{X_A}{C_{A0}(1-X_A)} = kt\]For A + B → products, with r = kCACB
Equal Initial Concentrations (CA0 = CB0):
\[\frac{1}{C_A} = \frac{1}{C_{A0}} + kt\]Unequal Initial Concentrations:
\[\ln\left(\frac{C_B C_{A0}}{C_A C_{B0}}\right) = (C_{B0} - C_{A0})kt\]Rate Law:
\[r = kC_A^n\]Integrated Form (n ≠ 1):
\[\frac{1}{C_A^{n-1}} = \frac{1}{C_{A0}^{n-1}} + (n-1)kt\]Half-Life:
\[t_{1/2} = \frac{2^{n-1}-1}{(n-1)kC_{A0}^{n-1}}\]Arrhenius Law:
\[k = A e^{-E_a/RT}\]Linearized Form:
\[\ln k = \ln A - \frac{E_a}{RT}\]Two-Temperature Form:
\[\ln\left(\frac{k_2}{k_1}\right) = \frac{E_a}{R}\left(\frac{1}{T_1} - \frac{1}{T_2}\right)\]For: A ⇌ B
Rate Expression:
\[r = k_f C_A - k_r C_B\]Equilibrium Constant:
\[K_{eq} = \frac{k_f}{k_r}\]First-Order Reversible (A ⇌ B):
\[\ln\left(\frac{C_A - C_{Ae}}{C_{A0} - C_{Ae}}\right) = -(k_f + k_r)t\]For parallel reactions:
A → B (rate = k1CA)
A → C (rate = k2CA)
Overall Rate of A Consumption:
\[-\frac{dC_A}{dt} = (k_1 + k_2)C_A\]Product Selectivity:
\[\frac{C_B}{C_C} = \frac{k_1}{k_2}\]For: A → B → C
First-Order Series:
\[A \xrightarrow{k_1} B \xrightarrow{k_2} C\]Concentration Profiles:
\[C_A = C_{A0}e^{-k_1 t}\] \[C_B = C_{A0}\frac{k_1}{k_2 - k_1}(e^{-k_1 t} - e^{-k_2 t})\] \[C_C = C_{A0}\left[1 + \frac{k_1 e^{-k_2 t} - k_2 e^{-k_1 t}}{k_2 - k_1}\right]\]Time to Maximum B Concentration:
\[t_{max} = \frac{\ln(k_2/k_1)}{k_2 - k_1}\]Michaelis-Menten Equation:
\[r = \frac{r_{max}C_S}{K_M + C_S}\]Alternative Form:
\[r = \frac{V_{max}C_S}{K_M + C_S}\]Lineweaver-Burk (Double Reciprocal):
\[\frac{1}{r} = \frac{K_M}{r_{max}}\frac{1}{C_S} + \frac{1}{r_{max}}\]For: A + B → 2B
Rate Law:
\[r = kC_A C_B\]Integrated Form:
\[\ln\left(\frac{C_B}{C_A}\right) = \ln\left(\frac{C_{B0}}{C_{A0}}\right) + (C_{A0} + C_{B0})kt\]Design Equation:
\[t = N_{A0}\int_0^{X_A} \frac{dX_A}{-r_A V}\]Constant Volume Batch Reactor:
\[t = C_{A0}\int_0^{X_A} \frac{dX_A}{-r_A}\]Zero-Order:
\[t = \frac{C_{A0}X_A}{k}\]First-Order:
\[t = -\frac{1}{k}\ln(1 - X_A)\]Second-Order:
\[t = \frac{X_A}{kC_{A0}(1-X_A)}\]nth-Order (n ≠ 1):
\[t = \frac{1}{k(n-1)C_{A0}^{n-1}}\left[\frac{1}{(1-X_A)^{n-1}} - 1\right]\]Mole Balance:
\[V = \frac{F_{A0}X_A}{-r_A}\]Space Time:
\[\tau = \frac{V}{\nu_0} = \frac{C_{A0}X_A}{-r_A}\]Space Velocity:
\[SV = \frac{1}{\tau} = \frac{\nu_0}{V}\]First-Order Reaction in CSTR:
\[\tau = \frac{C_{A0}X_A}{kC_A} = \frac{C_{A0}X_A}{kC_{A0}(1-X_A)}\] \[X_A = \frac{k\tau}{1 + k\tau}\]Second-Order Reaction in CSTR:
\[\tau = \frac{C_{A0}X_A}{kC_A^2} = \frac{X_A}{kC_{A0}(1-X_A)^2}\]First-Order Reaction, n Equal-Volume CSTRs:
\[X_A = 1 - \frac{1}{(1 + k\tau_i)^n}\]Conversion in ith Reactor:
\[1 - X_{Ai} = \frac{1}{(1 + k\tau_i)^i}\]Differential Form:
\[\frac{dX_A}{dV} = \frac{-r_A}{F_{A0}}\]Integral Form:
\[V = F_{A0}\int_0^{X_A} \frac{dX_A}{-r_A}\]Space Time:
\[\tau = \frac{V}{\nu_0} = C_{A0}\int_0^{X_A} \frac{dX_A}{-r_A}\]First-Order Reaction in PFR:
\[\tau = \frac{1}{k}\ln\left(\frac{1}{1-X_A}\right)\] \[X_A = 1 - e^{-k\tau}\]Second-Order Reaction in PFR:
\[\tau = \frac{X_A}{kC_{A0}(1-X_A)}\]Zero-Order Reaction in PFR:
\[\tau = \frac{C_{A0}X_A}{k}\]nth-Order Reaction in PFR (n ≠ 1):
\[\tau = \frac{1}{k(n-1)C_{A0}^{n-1}}\left[\frac{1}{(1-X_A)^{n-1}} - 1\right]\]For Most Reactions:
\[V_{CSTR} > V_{PFR} > V_{Batch}\]First-Order Reaction Volume Ratio:
\[\frac{V_{CSTR}}{V_{PFR}} = \frac{1 + k\tau}{k\tau}\]Mean Residence Time:
\[\bar{t} = \frac{V}{\nu_0}\]Residence Time Distribution (RTD) for CSTR:
\[E(t) = \frac{1}{\bar{t}}e^{-t/\bar{t}}\]General Energy Balance:
\[N_{A0}C_{pA}\frac{dT}{dt} = (-\Delta H_{rxn})V(-r_A) + \dot{Q}\]Heat Transfer Rate:
\[\dot{Q} = UA(T_c - T)\]Steady-State Energy Balance:
\[F_{A0}X_A(-\Delta H_{rxn}) = \dot{Q} + F_{A0}\sum_i \Theta_i C_{pi}(T - T_0)\]Adiabatic Operation (Q̇ = 0):
\[T = T_0 + \frac{(-\Delta H_{rxn})X_A}{\sum_i \Theta_i C_{pi}}\]Differential Energy Balance:
\[\frac{dT}{dV} = \frac{UA(T_c - T) + (-r_A)(-\Delta H_{rxn})}{F_{A0}\sum_i \Theta_i C_{pi}}\]Adiabatic PFR:
\[\frac{dT}{dX_A} = \frac{(-\Delta H_{rxn})}{\sum_i \Theta_i C_{pi}}\]Volume Change Parameter (ε):
\[\varepsilon_A = \frac{V_{X_A=1} - V_{X_A=0}}{V_{X_A=0}} = \frac{\delta y_{A0}}{1 + \delta y_{A0}}\]Concentration with Volume Change:
\[C_A = C_{A0}\frac{(1-X_A)}{(1+\varepsilon_A X_A)}\frac{P}{P_0}\frac{T_0}{T}\]Volume as Function of Conversion:
\[V = V_0(1 + \varepsilon_A X_A)\frac{P_0}{P}\frac{T}{T_0}\]Ergun Equation:
\[\frac{dP}{dz} = -\frac{G}{\rho g_c D_p}\left[\frac{150(1-\phi)\mu}{D_p \phi} + 1.75G\right]\]Simplified Pressure Drop (Low Pressure):
\[\frac{dP}{dz} = -\frac{\beta_0}{2P}(1 + \varepsilon_A X_A)\frac{T}{T_0}\]Langmuir-Hinshelwood Rate Law (Single Site):
\[-r_A = \frac{kK_A C_A}{1 + K_A C_A + K_B C_B}\]General Catalytic Rate Expression:
\[-r_A = \frac{(kinetic\ term)(driving\ force)}{(adsorption\ term)^n}\]Rate per Unit Mass of Catalyst:
\[-r'_A = \frac{-r_A}{\rho_c}\]Effectiveness Factor:
\[\eta = \frac{\text{actual rate with diffusion}}{\text{rate without diffusion}}\]Thiele Modulus (First-Order, Spherical Pellet):
\[\phi = R\sqrt{\frac{k}{D_e}}\]Effectiveness Factor for Spherical Pellet:
\[\eta = \frac{3}{\phi}\left(\frac{1}{\tanh\phi} - \frac{1}{\phi}\right)\]Asymptotic Limits:
Activity:
\[a(t) = \frac{-r_A(t)}{-r_A(t=0)}\]Rate with Deactivation:
\[-r_A = k C_A^n a(t)\]Exponential Decay Model:
\[a(t) = e^{-k_d t}\]Initiation:
\[I_2 \xrightarrow{k_d} 2R\cdot\] \[R\cdot + M \xrightarrow{k_i} M_1\cdot\]Propagation:
\[M_n\cdot + M \xrightarrow{k_p} M_{n+1}\cdot\]Termination (Combination):
\[M_n\cdot + M_m\cdot \xrightarrow{k_{tc}} M_{n+m}\]Termination (Disproportionation):
\[M_n\cdot + M_m\cdot \xrightarrow{k_{td}} M_n + M_m\]Rate of Polymerization:
\[R_p = k_p[M][\bar{M}\cdot]\]Steady-State Approximation:
\[[\bar{M}\cdot] = \sqrt{\frac{2fk_d[I_2]}{k_t}}\]Number-Average Degree of Polymerization:
\[\bar{X}_n = \frac{k_p[M]}{\sqrt{2fk_d k_t[I_2]}}\]Mass Transfer Rate:
\[N_A = k_c A_s(C_{Ab} - C_{As})\]For Fast Reactions (CAs ≈ 0):
\[N_A = k_c A_s C_{Ab}\]Overall Rate with External Mass Transfer:
\[\frac{1}{r_{obs}} = \frac{1}{k_c a} + \frac{1}{k_{rxn}}\]Effective Diffusivity:
\[D_e = \frac{D_{AB}\phi_p}{\tau_p}\]Observed Rate with Diffusion:
\[r_{obs} = \eta \cdot r_{surface}\]Fractional Conversion:
\[X_A = \frac{N_{A0} - N_A}{N_{A0}} = \frac{C_{A0} - C_A}{C_{A0}}\]For Flow Reactors:
\[X_A = \frac{F_{A0} - F_A}{F_{A0}}\]Yield:
\[Y_{D/A} = \frac{\text{moles of D formed}}{\text{moles of A fed}}\]Selectivity (Instantaneous):
\[S_{D/U} = \frac{r_D}{r_U}\]Overall Selectivity:
\[S_{D/U} = \frac{\text{moles of D produced}}{\text{moles of U produced}}\]For Parallel Reactions (A → D and A → U):
\[S_{D/U} = \frac{k_D C_A^{n_D}}{k_U C_A^{n_U}} = \frac{k_D}{k_U}C_A^{n_D - n_U}\]For A → D (desired) and D → U (undesired):
Maximum Yield of D:
\[Y_{D,max} = \left(\frac{k_1}{k_2}\right)^{k_1/(k_2-k_1)}\]For Parallel Reactions:
For Series Reactions:
Zero-Order:
\[t_{1/2} = \frac{C_{A0}}{2k}\]First-Order:
\[t_{1/2} = \frac{0.693}{k}\]Second-Order:
\[t_{1/2} = \frac{1}{kC_{A0}}\]nth-Order:
\[t_{1/2} = \frac{2^{n-1}-1}{(n-1)kC_{A0}^{n-1}}\]