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Buoyancy
Gravity-opposing force caused by the weight of displaced solvent. Depends on the molar mass, partial specific volume, and solvent density
Partial specific volume
Space occupied per mole of a protein
Friction
Force opposing motion in a fluid medium. Described empirically, with f/f0 ratio describing the deviation from sphericity
f0
Frictional coefficient of a sphere. When compared to measured f, refers to the frictional coefficient of an anhydrous sphere of the same volume
Stokes’ law
Describes the frictional coefficient of a sphere
Diffusion
Flux associated with concentration gradients driven by Brownian motion
Einstein-Sutherland equation
The diffusion coefficient is related to the frictional coefficient
Fluorescence correlation spectroscopy
At a particular concentration, a small volume will have a variable amount of fluorophores present that changes over time. The rate at which the fluorescence changes is related to the rate of diffusion as individual molecules enter and leave the viewing area. Performing an autocorrelation function on the fluorescent signal in a confocal microscope can be used to measure diffusion
FCS instrumentation
Confocal microscope (pinhole to exclude out-of-focus light). Beam splitter splits signal into two detectors, one of which is time-delayed to produce the lag time
Autocorrelation
Measures the correlation of a function with itself at different offsets (lag time)
FCS measurement and output
Measurement: fluorescence intensity within the Gaussian volume of the confocal image
Output: Autocorrelation versus lag time
Dual-color fluorescence cross-correlation spectroscopy
FCS technique that can be used to monitor association reactions. Excites and detects at two wavelengths to simultaneously monitor two fluorophore-labeled molecules. Following self-correlation, the two channels are cross-correlated to detect whether the red and green channels are moving together as part of the same complex – the cross-correlation curve indicates the fraction of co-diffusing species
Dynamic light scattering
Fluctuations in the intensity of scattered light is related to Brownian motion of particles within solution. Computing the temporal autocorrelation of the scattering intensity can solve for the diffusion coefficient
Siegert relation
Relates the intensity autocorrelation function measured during experiment to the diffusion coefficient. This is equal to a baseline factor (~1) plus the coherence factor times the square of the electric field autocorrelation function, which works out to be the exponent of D q² tau. Decay rate equals D q²
What if your sample is heterogenous in DLS?
For a mixture of non-interacting species, the intensity-weighted integral over a distribution of decay rates must be used. For a monomodal distribution, this can be solved with the cumulants method, where the second cumulant is a measure of polydispersity
Limitations of DLS
Very sensitive to aggregates - the intensity is related to r^6, meaning large particles give huge relative signals.
DLS reports on hydrodynamic diameters and not molecular weights.
AUC experimental setup
Centrifuge where samples are placed within cells not tubes.
Dual sector cell: Used in Sed. Vel. Contains two cavities for sample and reference
Multi sector cell: Used in sed. eq. Contains six smaller cavities for sample/reference for replicates / different concentrations
Sedimentation velocity setup and applications
Hydrodynamic measurement to study rate of sedimentation and diffusion.
Fill dual sector cell and spin at high speed, collecting many c vs r scans as a function of time.
Obtains the size, shape, and molecular weight. Useful for mixtures and complex systems, and new analyses work for interacting systems
Sedimentation equilibrium setup and applications
Thermodynamic measurement to analyze stable concentration gradients.
Fill six channel cells and spin at moderate speed, monitoring approach to equilibrium. Record final concentration gradient.
Gold standard for determining molecular weight and determines subunit stoichiometries. Useful for analyzing interacting systems, but not suitable for complex mixtures.
Tracer analytical ultracentrifugation
Old-school method where cell is fractionated and inserted tracers (radioactivity, fluorescence) are used to determine concentrations. Time-consuming
Absorbance detection in AUC
Uses a single-beam spectrophotometer.
Good sensitivity for proteins at specific wavelengths (280, 230 nm), but high noise and signal must be within linear concentration range for Beer-Lambert to apply.
Interference detection in AUC
Uses a Rayleigh interferometer - beams are split, passed through sample and reference, and recombined to give interference pattern.
Highly sensitive, gives great signal to noise, but not selective. Depends on changes in refractive index, so anything that changes RI will give signal. Dynamic range is basically unlimited
Forces in sed vel AUC
Sedimentation pushes to the edges, while friction and buoyant forces oppose
Sedimentation coefficient s
Describes how quickly a molecule moves through a fluid in a centrifugal field. Affected by mass, shape, solvent viscosity, and temperature.
As molecular weight increases, s increases.
s is independent of rotor speed.
Svedberg equation
Describes the relationship between s, D, and properties of the protein for homogenous non-interacting systems
Lamm equation
Differential equation which describes the relationship between concentration, radius, and time as sedimentation occurs, given s and D. Can be globally fit to determine these parameters
Time-derivative dcdt methods and g(s*)
Approximates the time derivative by subtracting closely-placed scans, removing time-invariant noise. Transforms axis from r to s*, which tells you how much material is sedimenting at each s* value. - g(s*) is the concentration of species with apparent sedimentation coefficient s*.
Better resolution, but only one peak
SEDFIT and c(s) distribution
Finite element analysis modeling the sedimentation and diffusion of particles.
Assumptions: continuous distribution of non-interacting particles of increasing size that are the same shape.
Yields sharp peaks and can resolve oligomers
Concentration dependence of s
s generally decreases with concentration as greater [P] makes backflow a larger contributor.
If s increases with concentration, this indicates mass action self-association.
Remember to take measurements at multiple concentrations
Forces at play in Sed Eq AUC
Flux of diffusion is balanced against flux of sedimentation
Integrated SE expression for homointeracting systems
The c(r) distribution is the sum of the cm( r) and cd( r) - relate each with equilibrium constant
Integrated SE expression of heteroassociation
Depends on the relative extinction coefficient of A and B. Fit for A and B independently at low concentration and K, then do a global analysis at multiple rotor speeds, concentrations, and wavelengths
What do fractional saturation plots look like with [P] « Kd, [L]?
Hyperbolic binding isotherm. Fit to find KdWha
What do fractional saturation plos look like with [P] » Kd?
Linear binding isotherm, used to find stoichiometry
What if Kd ~ [P]
Must split each concentration into bound / unbound, ultimately solve for [PL] with a quadratic and f = [PL]/[P]tot
Heat capacity
Relationship between the heat energy applied to a system and its temperature. Formally defined as dH/dT under conditions of constant pressure
DSC instrumentation
Differential refers to the sample versus reference cell
How is a DSC experiment run?
Power is applied to the sample and reference cell to increase the temperature at a steady rate
What does DSC measure?
The difference in power applied is measured as the excess heat q, which is required to undergo the phase transition when melting a protein. Directly measures the heat capacity
What do you get from a DSC curve?
The peak corresponds to the melting point, the difference in heat capacity is related to the number of hydrophobic residues, and the integral under the curve is the enthalpy change of unfolding
Why should a protein be refolded after DSC?
Thermodynamic equations apply only if the change is reversible. We need to make sure this is the case.
Isothermal titration calorimetry
Performs stepwise injection of ligand into a reaction cell containing a macromolecule. The excess heat evolved against the reference cell is measured and the data is fit to obtain the enthalpy change, stoichiometry, and equilibrium constant of the binding reaction, which can be used to solve for the free energy change, entropy change, and change in heat capacity
Requirements of ITC
Need a significant enthalpy change and large amount of material. 10 or more injections to define binding isotherm.
c parameter
Equal to the product of the stoichiometry n, protein concentration, and equilibrium constant K. Should be between 5 and 500.
ITC with low c
Signal is too weak to resolve.
ITC with high C
Binding curve is highly rectangular
SPR instrumentation
Sensor chip with thin gold film with a glass prism. Light source illuminates the chip, causing total internal reflection / SPR.
Detector measures change in intensity as a function of reflected angle
Detection of binding in SPR
Sensor chip has surface modifications allowing for attachment of immobilized receptors. Flow ligand and compare to flow cell without ligand
Advantages of SPR
Detects picomolar binding, high throughput, low sample requirements, real-time and label free, and works at low receptor density
Disadvantages of SPR
Expensive, immobilized ligand can create heterogeneity and can affect activity, and may be diffusion limited
Surface prep for carboxymethyl dextran chip
Unmodified surface
NHS/EDC activation of surface
Baseline after activation
Flow in ligand for binding
Immobilized ligand before deactivation
Deactivation
Baseline - Rmax, where 7 - 3 is the amount of immobilized ligand
Alternate immobilization strategies
His-tagged protein and NTA (nickel chelation) - reusable
Biotin conjugation with streptavidin
Protein A/G and antibody
Azide for copper click chemistry
SPR curve regimes
Baseline
Association - analyte plus buffer is injected
Dissociation - buffer only is injected until 50% saturation
Regeneration - regeneration buffer is injected to displace ligand
Return to baseline, repeat
Things to look out for in SPR
Mass-transport limited kinetics, ligand not saturating, large RI jumps and spikes, no replicates, narrow concentration range, large response (high ligand density)
kobs
Observed rate constant in pseudo first order conditions. kobs = kon[L] + koff
Mass transport limited kinetics in SPR
Visible as a linear regime in the binding isotherm and if changes to flow rate affects kinetics. Fix by increasing the flow rate or decreasing the number density of ligand
Biolayer interferometry
Uses an optical tip that is dipped into solution. White light passes through and reflects, creating an interference pattern between light that reflects from the optical layer and from the immobilized layer. Causes a wavelength shift that is dependent on thickness and caused by binding
Advantages of BLI
High throughput, avoids microfluidics, no bulk changes in system properties, can measure picomolar affinity
Disadvantages of BLI
Systematic error in kd values when compared to SPR, likely related to evaporation. Similar issues with diffusion-limited kinetics
Thermophoresis
Movement of molecules in response to a temperature gradient
What factors affect thermophoretic flow?
Area, hydration entropy, size, charge, conformation
MST instrument setup
Excitation light for fluorescence, infrared laser for heating
Phases of MST experiments
Bulk solution (F0)
Heat-induced thermophoretic flow
Stable state (F1)
Recovery
How is MST data analyzed?
Fnorm (or delta Fnorm) - the ratio of F1 to F0 - is computed from MST curves as a function of concentration of ligand
Atomic force microscopy
Measures z displacement of a surface using a nanoscopic silicon / silicon nitride tip with laser deflection cantilever.
Force is measured by deflection of the cantilever, which is related to Hooke’s law.
Contact mode
Tip is in physical contact with the sample.
Feedback system keeps the force constant atop the surface.
Useful only on hard surfaces - damaging
Tapping mode
AFM tip oscillates above the surface, contacting with each cycle
Measures attractive and repulsive forces as distance oscillates.
Feedback system maintains interaction amplitude
Minimizes damage, but slower scan speed
Non-contact mode
AFM tip oscillates above the sample.
Amplitude or frequency modulated, latter is better
Used to image live cells
Force extension mode
Macromolecule is attached to the surface and the tip. Piezoelectric positioners move until only a single macromolecule is attached, then pulls to obtain force-distance curve
Optical trapping
Light has momentum that can be used to generate force. Gaussian beam balances momentum changes to generate a restoring force on a 1 um bead, keeping it within a potential well. Inside this well, the bead experiences an approximately linear restoring force dependent on laser powerA
Applications of optical tweezers
DNA force extension curves - apply force to the bead immobilized on a surface and monitor extension
Monitoring movement of motor proteins
Mass photometry
Molecules that come into contact with a cover slip will give light scattering proportional to its mass. Perform interferometric spectroscopy, measuring the interference pattern caused by light interacting with adsorbed particle versus cover slip
MP instrumentation
Essentially a microscope. Polarized light reflects and is collected to form the image
MP data processing
Ratiometric images are calculated by taking the ratio of the moving average of the ahead frames over the moving average of the prior frames. Contrast peaks at the midpoint in space and time
Drawbacks of MP
Limited range of masses
Surface adsorption bias - better adsorbers give more signal
No structural information
Sensitive to buffer conditions / optical properties (simpler=better)
Requires extensive calibration curves
Artifacts from transient irrelevant oligomers
Requires statistical averaging and large number of counts - high concentration, hard to see rarer complexes
Can’t see PTMs like mass spec canA
Applications of MP
Quantifying sample heterogeneity - can be used to measure the mass of many proteins at once within a complex mixture
Assessing packaging state of AAV gene therapy vectors
HDX
The amide backbone of proteins exchanges hydrogen for deuteron at a consistent rate in solution, subject to temperature and pH conditions.
Used to measure solvent accessibility due to dependence on secondary structure and protein folding state
Kinetics
Three rates - kop, kcl for protein conformation, and kch for exchange.EX
EX1 regime
Occurs when kinetics is limited by solvent accessibility - i.e kch » kcl, which is rate-limiting. Observed rate of HDX is equal to kcl, and the regime exhibits correlated exchange, moving over all at onceE
EX2 regime
Occurs when kinetics is limited by the deuterium exchange reaction - i.e kch « kcl. In this case, kHDX = Kop * kch. No correlated exchange - peaks move over gradually
Continuous labeling
Protein is incubated in D2O for continuous periods of time. Useful for steady-state conformational dynamics
Pulse labeling
Protein is incubated in D2O serially for shorter periods of time. Useful for dynamic processes, interactions that occur on a fast timescale, and binding or allosteric effects