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Tutorial: of Soft

Sujit S. Datta Department of Harvard University What Is Rheology?

The quantitative study of the manner in which materials deform and flow.

● Describe the mechanical constitutive relationship for a (response to ): Prescribe/measure

(Elastic )

(Viscous )

● What kinds of materials do we study in our lab? Soft materials - generally isotropic, disordered, both elastic and viscous components. ○ Allen, Lolo, Stefan: Biopolymer networks ○ Jim, Shmuel: Biofilms, ○ Joris: Colloidal suspensions/, microgels, polymers ○ Sujit and Dustin: Colloidal suspensions, Outline Of This Tutorial

● Basic definitions: /, affine/non-affine, flows, , modulus

● Some different responses: Maxwell, Kelvin-Voigt, SGR

● How to actually measure things: controlled/stress strain, viscometry, geometries

● Two examples: ○ Soft glassy emulsions ○ Colloidal gels

● Other types of measurements/topics of interest: ○ SRFS ○ Non-linear (/shear thickening) ○ Shear-banding ○ stress ○ Pre-stress ○ LAOS Basic Definitions: Stress/Strain

Plate of area Pull with force

Strain: Stress:

● Note: here, only consider shear flows/stresses; no extensional flows or normal stresses Basic Definitions: Affine/Non-Affine

Affine Non-Affine

○ Uniform Major subject of current research! ○ Local strain = macroscopic strain Significant influence on rheology of: ○ Biopolymers (Lolo)) ○ Microgels (Joris) ○ Emulsions (Simulations) ○ Shear-banding of suspensions Basic Definitions: Viscoelasticity

● See video

● Materials have different mechanical responses depending on timescale of measurement

(Elastic solid) (Viscous liquid)

● How to quantify this? Stress modulus Gr(t). ○ There are many equivalent ways to measure this! Different preferences based on experimental method, tradition, etc. Stress Step strain

Measure Relaxation time

t = 0 Time Basic Definitions: Complex Shear Modulus

● Another approach: frequency-domain

Strain Stress

Time

Storage of Viscous elastic dissipation

1/Relaxation time G’

G’’

Frequency One Model: Maxwell (Low Frequency Relaxation)

● Elastic solid in series with viscous dashpot (e.g. entangled solution)

● Timescale:

● Can derive functional form of G’, G’’ as a function of frequency

~1/Relaxation time G’

G’’

Frequency

● This model captures stress relaxation behavior better One Model: Kelvin-Voigt (Low Frequency )

● Elastic solid in parallel with viscous dashpot

● Timescale:

● G’, G’’ as a function of frequency are very simple

G’

~1/Relaxation time

G’’

Frequency

● This model captures recovery behavior better Phenomenological Model: Sollich’s Soft Glassy Rheology

● Energy barriers >> thermal energy; these are due to microscopic structure of material

3 Energy ○ Each mesoscopic region has own yield

2 energy; distribution of yield 4 1 ○ Hopping activated by noise x; this is related to how jammed Local Strain l

○ Hopping time-scale is given by 1 2 3 4 phenomenological attempt frequency How To Actually Measure Things

TA AR-G2 (2 of them) Anton-Paar MCR 501 TA ARES G2 ○ Stress-controlled ○ Stress-controlled (claim ○ True strain-control ○ Most versatile set of also strain-controlled) ○ Array of geometries geometries ○ Array of geometries ○ Standard solvent trap ○ Standard solvent trap ○ High-performance (high-performance solvent trap maybe coming soon) ...talk to Lolo. ...talk to Joris. ...talk to Sujit/Jim. Strain versus Stress Controlled

Strain Controlled Stress Controlled ○ Good for oscillatory measurements ○ OK for oscillatory measurements ○ Good for fixed shear rate measurements ○ Good for fixed stress measurements ○ Motors are really good - good for weak ○ Good for creep measurements materials ○ Drag cup motors often cannot do low ○ Very sensitive transducers stresses well ○ Easier to damage ○ EC motors often have more inertial effects ○ Often assumes certain type of material response How To Actually Measure Things

Single/Double-Gap Couette Parallel Plates Cone-Plate ○ Large volumes (~9 mL) ○ Small volumes (~0.1-3 mL) ○ Small volumes (~0.1’s mL) ○ Very sensitive ○ Inhomogeneous strain field ○ Homogeneous strain field ○ Homogeneous strain field How To Actually Measure Things

● Different types of measurement: ○ Frequency sweep (characteristic timescales, solid-like plateaus, scaling, ...) ○ Strain sweep (yielding behavior, linear regime, ...) ○ Flow curves (yield stress, , shear-banding, ...) ○ Stress-relaxation (characteristic timescales) ○ SRFS (relaxation spectrum) Example: Colloidal Suspensions

Long-time fluidization Elastic response Response of suspending fluid of material Modulus

Densely-packed emulsions*

1 G’

G’’

Colloidal Gels

*Note: G’’ of dense emulsions has a frequency0.5 response at Frequency high frequencies, not discussed here One Example: Densely-Packed Emulsions (Mason) One Example: Densely-Packed Emulsions (Mason) One Example: Densely-Packed Emulsions (Mason) One Example: Densely-Packed Emulsions (Mason) Another Example: Colloidal Gels (Trappe) Another Example: Colloidal Gels (Trappe) Another Example: Colloidal Gels (Trappe) Frequency Superposition

● Structural relaxation of a material happens at a characteristic timescale ; this is typically way longer than experimental timescales

● Shearing at high enough strain rate can make a material structurally relax; this is like speeding up the structural relaxation to a new timescale

● Phenomenological expression:

● Instead of holding strain constant or frequency constant, hold strain rate constant Strain Rate Frequency Superposition Strain Rate Frequency Superposition Strain Rate Frequency Superposition Strain Rate Frequency Superposition Other Stuff Of Current Interest

● Shear-thickening: role of hydrodynamics, etc.

● Shear-banding: why do some suspensions shear-band?

● Yield stress: do soft materials have a “true” yield stress, or does this just depend on measurement time?

● Pre-stress measurements: for biopolymer networks that stress stiffen, oscillating about large stress value gives valuable information

● LAOS: shapes of waveforms at large amplitudes can yield interesting information Questions?