Structure and Rheology of Surfactant Solutionsbeaucag/CHEM/Planning Meeting... · 2020. 7. 28. ·...

Structure and Rheology of Surfactant SolutionsWeizhong Zou#, Taraknath Mandal #, Mike Weaver+, Peter Koenig‡, Sumanth

Jamadagni, Geoffrey Reynolds, and Ronald G. Larson#

# Department of Chemical Engineering, University of Michigan, Ann Arbor, MI 48109+ Analytic Sciences, The Procter & Gamble Company, Mason, OH 45040‡ Computational Chemistry, Modeling and Simulation, The Procter & Gamble Company, West Chester, OH 45069

Sponsors: Procter and Gamble, NSF

Weizhong Zou Taraknath Mandal

Peter Koenig Mike Weaver

The Challenge of Mul.ple Length and Time Scales in Surfactant Solu.ons

Entangled Network

http://www.ifnh.ethz.ch/vt/research/projects/vivianel1023 degrees of freedom!

sodium dodecyl sulfate

1 nm

10 nm

100 nm1 µm

10 cm

A B

CD

E

Increasesurfactant/saltconcentration

Micellar solutions:thesaltcurvecitronellol

linalol

limonene

vanillin

10%SLES Noadditives

Cumene Linalool

DPG

Umbrella Sampling

density

PMF

z = r, radial coordinate

mid 2vidt2

= fi

molecular dynamics (MD)simulations:

Video from student Kyle Huston

Weighted Histogram Analysis Method (WHAM)

Micelle Size Distribution

12:07:01 Time

(inferred from potentials of mean force)

C16E22

Yuan and Larson, JPC B (2015)

!" = !"$%!%&'( −∆+",

-./

+" = +", +-./ℓ2(!")∆+",= +", −(+"$%, + +%,)PMF =

n surfactants n-1 surfactants

5"↔5"$%+5%

Simulation of scission energy using weighted histograms

Use bead count in region to bias simula7ontowards scission/fusion.PLUMED, Comp. Phys. Comm. 180 (2009), 1961÷÷

ø

öççè

æDµ kT

GLsciss

exp

Cates, M., & Candau, S., J. Phys.: Condens. Matter (1990), 6869.

Vs =12k(N({xi, yi, zi}, v)−N0)

2

c(L) ~ exp(–L/ )

Peter Koenig, P&G

Taraknath Mandal

d

Reptation:Edwards, De Gennes,

trep ~L3

Micelle breakage & Re-joining:M.E. Cates (1989):

tbreak ~1/L

new tube sizemicellebreak

Micellar relaxation dynamics

Slide from Peter Koenig, P&G

Breakage Rejoining

ReptationContourlength3luctuations

CR(Doublereptation)

Pointer algorithm: simulation of ensemble of micelles

G(t) = GN µ2 (t) +Rouse + bending modes

Zou, W. and Larson, R.G. J Rheology 58 (2014) 681-721.

Fitting Data

9

<L> = 1.6 µmlp = 112 nmtbr/trep = 1.8

Procter and Gamble is using this predicBve method in their research into design of shampoos and body washes

Lamellar Gels for Hair Conditioners 10

Excess Water (85-95%)

Cationic Surfactant Fatty Alcohol

Behentrimoniummethosulfate

(BTMS)

Cetostearyl Alcohol (cetyl : stearyl = 1:2.5 by weight)

Additives• Salts (NaCl/EDTA)• Perfumes• Preservatives

Forms a lamellar gel network of 1. regularly spaced bilayers with 2. trapped interlamellar water and bulk water

S. Fukushima, M. Takahashi, and M. Yamaguchi, “Effect of cetostearyl alcohol on stabilization of oil-in-water emulsion. I. Difference in the effect by mixing cetyl alcohol with stearyl alcohol,” J. Colloid Interface Sci., vol. 57, no. 2, pp. 201–206, 1976.

Self-assembly of surfactants in water 11

Mouritsen, Ole G.. “Lipids, curvature, and nano-medicine*.” European journal of lipid science and technology : EJLST (2011).

• In these cosmetic emulsions, critical packing parameter ~ 1• Form lamellar bilayers

• Two different phases of lamellar bilayer structures depending onthe temperature :• Liquid crystalline (Lα) phase – above gel transition temperature• Gel phase (Lβ ) phase – below gel transition temperature

Hydrocarbon chains in the bilayer can exist in a number of physical states:

D isordered state Ordered state: Hexagonally packed

Solid-like Creep Response and “Apparent Yield-Stress”

< 18 Pa Solid-like creep response, with ! ∝ #0.25

Partial strain recovery

> 18 Pa Apparent yielding behavior, with ! ∝ #1.35

No strain recovery, flows like a fluid

Instruments:

• MCR 702 rheometer

• Cone (2°) and plate geometry

• Fluorescent m icroscope

testing fluid

m icroscope

input: rotation speed → shear rate

test output: torque → stress

Exam ple of velocim etry raw dataMaterials:

Ternary system lamellar gel network seeded with

fluorescent tracer particles (diameter 1.5 um, 0.1 vol%).

Y. Wei, M. J. Solomon, and R. G. Larson, “Time-dependent shear rate inhomogeneities and shear bands in a thixotropic yield-stress fluid under transient shear,” Soft Matter, pp.7956–7967, 2019.

Shear banding

Plug flowIdeal profile

END