SensorgramFrom bound mass to a binding curve

A sensorgram records the binding response over time. Here, the response is coherent mass density (CMD). Learn how to interpret association and dissociation, compare optical readouts, and decide whether data support a kinetic model.

Objective. See how coherent mass density over time becomes a binding curve. In the training: One mologram converts patterned binding into one sensorgram.

Recommended first: detection and noise and coherent mass density.

Coherent mass density over time

A typical experiment begins with buffer flowing over the surface to establish a baseline. Analyte injection starts the association phase. Switching back to analyte-free buffer starts the dissociation phase. In the ideal model below, the response rises during association and falls during dissociation. Actual traces can differ because of binding behavior, optical bias, or experimental disturbances.

A sensorgram: a flat baseline, a rising association phase during injection, and a falling dissociation phase after switching back to buffer.
Illustrative 1:1 model, not measured data. Three analyte concentrations over the same ligand: higher concentrations associate faster and reach higher. In a simple 1:1 interaction all curves share the same intrinsic dissociation rate.

Read CMD and MD together

CMD reports coherent mass density from the diffracted signal. MD is the refractometric mass-density readout derived from focal-spot position. Bulk index changes can appear as apparent mass in MD.

Illustrative response patterns, not measured traces or unique diagnoses
Observed patternPossible explanationUseful check
MD steps at injection; little CMD changeSample arrival changes bulk refractive index without much patterned binding.Inject the same matrix without analyte.
CMD rises after injection; MD may also changePreferential accumulation on the patterned regions.Compare non-binding controls and a concentration series.
MD drifts; CMD remains comparatively stableA common optical disturbance is partly rejected.Check temperature, buffer stability, and blanks; biological rates may still change.
CMD responds to an analyte-free matrixImperfect matching or another optical disturbance contributes to the response.Inspect blank reproducibility, surface chemistry, and optical alignment.

These patterns narrow the possibilities; they do not identify the bound molecule. A flat CMD trace also cannot prove that no material adsorbed.

What can imitate binding. Ridge-preferential non-specific adsorption; a bulk refractive-index step, which also moves MD; bubbles or fouling that disturb the illumination; an initial optical field of opposite phase, which can make added mass lower the intensity; and a zero crossing, after which the trace runs mirrored. Controls and a relevant blank separate these from target binding.

Frutiger et al. (2021), Part II, Figures 1 to 3 compare the two readouts during binding and refractive-index changes.

What happens to a trace before a fit

The software applies a short chain of cleanup steps before fitting. Each removes one named disturbance.

None of these steps can add a dissociation phase that was too short or supply missing concentrations. Those are design decisions for a new measurement.

What the shape tells you

For an ideal 1:1 interaction, association depends on analyte concentration and both rate constants. Dissociation without rebinding depends on koff. The equilibrium dissociation constant is KD = koff/kon. It equals the free analyte concentration at half occupancy under this model. Two interactions can share KD while having different association and dissociation rates. Interpreting the full curve helps distinguish them.

Two independent estimates of KD. The kinetic fit gives koff/kon. A dose-response fit of the plateau response at each concentration gives KD as its point of inflection. For well-behaved 1:1 binding the two agree. A Hill slope different from 1 in the dose-response fit means the interaction is not 1:1, and that KD is an apparent affinity. If the dissociation changes too little to resolve koff, the result is association rate only: kon is reported, koff is below its detection limit, and KD is unavailable. Only a longer dissociation phase in a new measurement resolves it.

When does a curve support kinetics?

A kinetic fit tests a model against data. A smooth fit alone does not show that its rate constants describe the intended molecular interaction.

For an ideal 1:1 interaction, the observed rate kobs = konc + koff during association. During dissociation without rebinding, response decays as exp(−kofft).

Failure of these relationships is a reason to investigate the model and experiment. It is not a reason to add fitting parameters automatically.

For general surface-binding model assumptions, see the Cytiva kinetics handbook, Chapter 12. Its instrument-specific procedures do not apply to the MACS® Matchmaker.

The training covers planning and controls. Reichmuth et al. (2021) provides an assay example with low-affinity binders in complex samples.

Plan the experiment

The training covers experiment planning, controls, and sensorgram interpretation. The MACS Matchmaker documentation covers instrument operation.

Take the training →

Predict before revealing the explanation. Can the single streptavidin association trace establish both rate constants and affinity?

Reveal the explanation

Not by itself. This panel lacks a dissociation phase and a concentration series. Binding stoichiometry and model suitability also need justification.

Takeaway. With known analyte concentrations and a justified binding model, fitting sensorgrams can estimate kon, koff and KD. Shape alone does not establish those values.