🟦 1:1 Langmuir Binding (MCK)
The Gold Standard. This is the simplest and most desired model. It describes a simple interaction between one analyte molecule (A) and one ligand binding site (L).
The ODE
Observed Rate
kobs is the rate at which the sensorgram approaches equilibrium during association. It increases linearly with analyte concentration — plotting kobs vs [A] gives a straight line with slope = ka and intercept = kd. In practice, kd from the intercept is unreliable (small lever arm, dominated by fitting noise) — use the dissociation phase instead.
Analytical Solution (Association)
where Req = Rmax × [A] / ([A] + KD). At equilibrium, the response is a hyperbolic function of concentration — this is the Langmuir isotherm. KD = kd / ka.
Symbols
- R — instrument response (RU); proportional to bound analyte mass
- Rmax — maximum binding capacity (RU); response when all ligand sites are occupied
- [A] — analyte concentration (M or nM)
- ka — association rate constant (M⁻¹s⁻¹)
- kd — dissociation rate constant (s⁻¹)
- KD — equilibrium dissociation constant = kd / ka (M); the concentration at which half of all binding sites are occupied at equilibrium
Dissociation
Pure exponential decay. R0 is the response at the start of dissociation (the end of the association phase); t is re-zeroed at that point. The dissociation phase depends only on kd, not on analyte concentration. This is why dissociation is often the most reliable phase for extracting kinetic parameters.
Interactive Lab: The 1:1 Model
Kinetics
Experimental Setup
Comma separated
kobs vs Concentration
Slope = ka · y-intercept = kd
Multi-Cycle Kinetics (MCK): Traditionally, kinetics are performed by injecting analyte at one concentration, regenerating the surface, and then injecting the next concentration. This is what the "MCK" toggle above simulates.
Assumptions
The 1:1 Langmuir model is valid when:
- Monovalent analyte, monovalent ligand — 1:1 stoichiometry. No multivalent or avidity effects.
- Homogeneous ligand population — all binding sites are equivalent. No mixture of active/inactive or high/low affinity sites.
- No mass transport limitation — the reaction is rate-limited, not diffusion-limited. Analyte reaches the surface faster than it binds.
- No conformational change upon binding — the complex AL does not rearrange into a tighter state AL*.
- Analyte concentration >> surface depletion — pseudo-first-order conditions. The bulk analyte concentration stays constant during binding.
When 1:1 Langmuir Fails
Watch for these residual signatures when the 1:1 model breaks down:
- Systematic curvature in residuals — the fit deviates consistently at the start or end of the association phase, often indicating a two-step binding mechanism. Try the Two-State (Conformational Change) model.
- Biphasic dissociation — a fast initial drop followed by a slow tail suggests a mixture of binding sites or affinities. Try the Heterogeneous Ligand model.
- Concentration-dependent off-rates — kd that varies with [A] is a hallmark of mass transport limitation. Try the Mass Transport model.
Still unsure? See the Model Selection Guide for a decision tree.
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