786 DLS Basics.

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Presentation transcript:

786 DLS Basics

Dynamic Light Scattering: Setup Incident light Diffusing colloids Transmitted light Scattering angle Light scatters in all directions http://www.people.vcu.edu/~ecarpenter2/DigitalCorrelator.htm Detector Fluctuating scattered light intensity Fluctuations in scattered light arise from diffusion

Scattered Light Intensity: t = 0 Particles in fixed positions Incident light Unperturbed light If particles remain fixed, so does intensity at detector Detector I = I0 Static scattering reveals micro-structure; e.g. x-ray crystallography

Scattered Light Intensity: t = Δt Particles have diffused Incident light Unperturbed light Particle motion causes intensity change at detector If particles move, intensity at detector changes Detector I = I(Δt) = I0 Duration of Δt before intensity changes gives time scale of motion Dynamic light scattering reveals ensemble average motion

Signal fluctuates in time How fast? Over what time scale? Instrument calculates correlation function:

Compare the signal I to itself: .… Lag time: If: , then is large As: , then diminishes

What does the correlation G look like? Siegert approximation Where Raw data: exponential decay Thought experiment: if this is an example correlation function for a randomly fluctuating signal I, what would the correlation function look like if the signal I was sinusoidal? Otherwise periodic?

Meaning of decay time-scale Fluctuations in scattered light arise from diffusive motion Correlation function of scattered light intensity: exponential decay Detector Real-time hardware correlators measure http://www.people.vcu.edu/~ecarpenter2/DigitalCorrelator.htm lag time Δt at which I(Δt) = I0

From time-scale to size scale Units of Diffusion = [length2/time] Length scale given by scattering vector q q has units 1/length; can be controlled by adjusting θ Diffusion through area 1/q2 occurs at time scale τ

Measured Diffusion Constant Diffusion D has units length2/time Time is τ, as obtained through exponential fit Length scale is 1/q. Area particle diffuses through in length scale τ is 1/q2 Hence measurement of D is:

Particle size from D Use Stokes Einstein relation, assuming spherical particles: Combine measured D with Stokes Einstein: …and solve for radius a