Kinetic Models
The kinetic model (specified with the -d or --model option) defines the type of exchange model to be used for data analysis. Available models include:
| Model Name | Description |
|---|---|
2st | 2-state exchange model (default) |
3st | 3-state exchange model |
4st | 4-state exchange model |
2st_rs | 2-state exchange model for residue-specific studies |
2st_hd | 2-state exchange model for H/D solvent exchange studies |
2st_eyring | 2-state exchange model for temperature-dependent studies |
3st_eyring | 3-state exchange model for temperature-dependent studies |
4st_eyring | 4-state exchange model for temperature-dependent studies |
2st_binding | 2-state exchange model for ligand binding studies |
4st_hd | 4-state exchange model for simultaneous normal and H/D solvent exchange studies |
In these models, each state in the exchange process is represented with a unique parameter suffix (A, B, C, D, etc.). For example, R1_A denotes the R1 relaxation rate of the major (ground) state, while R2_B refers to the R2 rate of the first minor state, and so forth.
For any kinetic model, you can add the .mf suffix to create a model that fits model-free parameters directly (e.g., TAUC_A, S2_A), rather than individual relaxation parameters (e.g., R1_A, R2_A). For an example, see CEST_15N_TR/ under Examples/Experiments/.
Temperature-Dependent Eyring Models
The 2st_eyring, 3st_eyring, and 4st_eyring models implement 2-state, 3-state, and 4-state exchange systems (respectively) with temperature-dependent rate constants calculated using Eyring transition state theory. These models are particularly useful for studying exchange processes where thermodynamic parameters govern the temperature dependence of exchange rates.
Theoretical Background
The Eyring equation relates the rate constant to the activation free energy:
k_ij = (k_B * T / h) * exp(-ΔG‡_ij / RT)
where:
k_ijis the rate constant for transition from state i to j (s⁻¹)k_Bis Boltzmann's constant (1.380649×10⁻²³ J/K)Tis temperature in Kelvinhis Planck's constant (6.62607015×10⁻³⁴ J·s)ΔG‡_ijis the activation free energy (J/mol)Ris the gas constant (8.314462618 J/mol/K)
The activation free energy is calculated from enthalpic and entropic contributions:
ΔG‡_ij = ΔH‡_ij - T * ΔS‡_ij
2st_eyring Model Parameters
The 2st_eyring model uses the following thermodynamic parameters:
State Energies (relative to state A):
DH_B: Enthalpy difference (J/mol) for state B relative to ADS_B: Entropy difference (J/mol/K) for state B relative to A
Transition Barriers:
DH_AB: Activation enthalpy (J/mol) for A → B transitionDS_AB: Activation entropy (J/mol/K) for A → B transition
The model automatically calculates both forward (k_AB) and reverse (k_BA) rate constants from these parameters.
3st_eyring Model Parameters
The 3st_eyring model extends the 2-state model with an additional state:
State Energies (relative to state A):
DH_B,DH_C: Enthalpy differences (J/mol) for states B, CDS_B,DS_C: Entropy differences (J/mol/K) for states B, C
Transition Barriers:
DH_AB,DH_AC,DH_BC: Activation enthalpies (J/mol) for transitionsDS_AB,DS_AC,DS_BC: Activation entropies (J/mol/K) for transitions
The model automatically calculates all 6 rate constants (k_AB, k_BA, k_AC, k_CA, k_BC, k_CB).
4st_eyring Model Parameters
The 4st_eyring model implements a full 4-state system:
State Energies (relative to state A):
DH_B,DH_C,DH_D: Enthalpy differences (J/mol) for states B, C, DDS_B,DS_C,DS_D: Entropy differences (J/mol/K) for states B, C, D
Transition Barriers:
DH_AB,DH_AC,DH_AD: Activation enthalpies (J/mol) for transitions from ADH_BC,DH_BD,DH_CD: Activation enthalpies (J/mol) for transitions between B, C, DDS_AB,DS_AC,DS_AD: Activation entropies (J/mol/K) for transitions from ADS_BC,DS_BD,DS_CD: Activation entropies (J/mol/K) for transitions between B, C, D
The model automatically calculates all 12 rate constants (k_AB, k_BA, k_AC, k_CA, k_AD, k_DA, k_BC, k_CB, k_BD, k_DB, k_CD, k_DC).
State A serves as the reference state with ΔH_A = ΔS_A = 0 for all Eyring models. Rate constants are automatically clipped to [0, 1×10¹⁶ s⁻¹] for numerical stability.