A colloid is a dispersed phase suspended in a continuous phase, typically (10,\mathrm{nm}\sim10,\mu\mathrm{m}) in size. Interactions are often measured in units of k_B T.
thermal=interaction comparable to kBT is reversible
diffusion=D=6πηRkBT
MSD=⟨Δr2⟩=2dDt
van der Waals Attraction and Electric Double Layer
atoms=U(r)=−C/r6
plates=W(h)=−12πh2H
spheres=UvdW(h)≈−12hHR
wall=UvdW(h)≈−6hHR
Charged surfaces form a Stern layer and a diffuse layer. Higher salt concentration gives shorter Debye length and shorter-ranged repulsion.
Debye=λD=∑iqi2ciϵ0ϵrkBT
screening=ϕ(h)=ϕ0e−h/λD
Yukawa=ϕ(r)∝e−r/λD/r
zeta=U=ϵ0ϵrζE/η
DLVO Theory
DLVO adds electric double-layer repulsion and van der Waals attraction. High salt lowers the repulsive barrier and promotes aggregation.
DLVO=UDLVO(h)=Ue(h)+UvdW(h)
repulsion=Ue(h)=Ae−h/λD
attraction=UvdW(h)≈−12hHR
salt=higher c gives smaller lambda_D and lower barrier
Depletion Force
Small particles are excluded from the depletion layer around large particles. When two depletion layers overlap, available volume for small particles increases, creating entropy-driven attraction.
osmotic=p=nkBT
depletion=U(r)=−pΔV(r)
AO=ΔV(r)=6π(a+b−r)2(a+b+r/2)
range=range approx small-particle diameter b
Hard Spheres and Glass
Hard spheres have no attraction but can crystallize by entropy. At high volume fraction, particles become caged by neighbors and form a colloidal glass.
hard sphere=u(r)=∞(r<σ),0(r≥σ)
phi=ϕ=Nb/V,b=πσ3/6
CS=Z=(1−ϕ)31+ϕ+ϕ2−ϕ3
coexist=ϕf=0.494,ϕs=0.545
packing=ϕ0=32π≈0.74
KTHNY theory describes 2D melting as solid to hexatic to liquid through defect unbinding. Active colloids may undergo motility-induced phase separation.
Exam Cue
Identify the interaction: vdW, electrostatic, depletion, hard sphere, or activity. For phases, start from free energy A = U - TS. Hard spheres and depletion force are especially entropy-driven.