supercooled liquids

17
1 Supercooled liquids Zhigang Suo Harvard University Prager Medal Symposium in honor of Bob McMeeking SES Conference, Purdue University, 1 October 2014

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Supercooled liquids. Zhigang Suo Harvard University. Prager Medal Symposium in honor of Bob McMeeking SES Conference, Purdue University, 1 October 2014. 1. Mechanics of supercooled liquids. Journal of Applied Mechanics 81, 111007 (2014). - PowerPoint PPT Presentation

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Page 1: Supercooled liquids

1

Supercooled liquids

Zhigang Suo

Harvard University

Prager Medal Symposium in honor of Bob McMeekingSES Conference, Purdue University, 1 October 2014

Page 2: Supercooled liquids

Mechanics of supercooled liquids

Journal of Applied Mechanics 81, 111007 (2014)

2

Jianguo Li Qihan Liu Laurence Brassart

Page 3: Supercooled liquids

Supercooled liquid

3

liquid

supercooled liquid

crystal

Temperature

Volu

me

mel

ting

poin

t

Page 4: Supercooled liquids

A simple picture of liquid

• A single rate-limiting step: molecules change neighbors• Two types of experiments: viscous flow and self-diffusion

4

Page 5: Supercooled liquids

Stokes-Einstein relation

Stokes (1851)

Einstein (1905)

5

liquid

particle

Page 6: Supercooled liquids

Success and failure of Stokes-Einstein relation

TNB

OTP

IMC

6Li, Liu, Brassart, Suo. Journal of Applied Mechanics 81, 111007 (2014). Based on experimental data in the literature

Page 7: Supercooled liquids

A supercooled liquid forms a dynamic structure

Ediger, Annual Review of Physical Chemistry 51, 99 (2000).

The dynamic structure jams viscous flow, but not self-diffusion.

7

Page 8: Supercooled liquids

Given that the Stokes-Einstein relation fails, we regard viscous flow and self-diffusion as independent processes,and formulate a “new” fluid mechanics.

Our paper

Li, Liu, Brassart, Suo. Journal of Applied Mechanics 81, 111007 (2014)

Page 9: Supercooled liquids

Homogeneous state

Incompressible molecules

Helmholtz free energyof a composite system

Liquid force reservoir

9Li, Liu, Brassart, Suo. Journal of Applied Mechanics 81, 111007 (2014)

Page 10: Supercooled liquids

Thermodynamic equilibrium

10m

embr

ane

reservoir

liquid

osmosisLi, Liu, Brassart, Suo. Journal of Applied Mechanics 81, 111007 (2014)

Page 11: Supercooled liquids

Linear, isotropic, viscous, “porous” liquid

11

Alternative way to write the model

• Analogous to Biot’s poroelasticity. (Poroviscosity?)• Different from Newton’s law of viscosity

change shape change volume

Li, Liu, Brassart, Suo. Journal of Applied Mechanics 81, 111007 (2014)

Page 12: Supercooled liquids

Inhomogeneous field

Diffusionflux

Netflux

Convectionflux

ii kTD

J ,

12Suo. Journal of Applied Mechanics 71, 77 (2004)

Page 13: Supercooled liquids

0, ijij b

4 partial differential equations

13

4 boundary conditions

Boundary-value problem

Li, Liu, Brassart, Suo. Journal of Applied Mechanics 81, 111007 (2014)

Page 14: Supercooled liquids

Length scale

14Li, Liu, Brassart, Suo. Journal of Applied Mechanics 81, 111007 (2014)

Page 15: Supercooled liquids

Time scale

Li, Liu, Brassart, Suo. Journal of Applied Mechanics 81, 111007 (2014)

Page 16: Supercooled liquids

16

A cavity in a supercooled liquid

• A small object evolves by self-diffusion. • A large object evolves by viscous flow.

Li, Liu, Brassart, Suo. Journal of Applied Mechanics 81, 111007 (2014)

Page 17: Supercooled liquids

Summary1. A supercooled liquid is partially jammed. A drop in

temperature jams viscous flow, but does not retard self-diffusion as much.

2. We regard viscous flow and self-diffusion as independent processes, and formulate a “new” fluid mechanics.

3. A characteristic length exists. A small object evolves by self-diffusion, and a large object evolves by viscous flow.

4. Other partially jammed systems: cells, gels, glasses, batteries.

17Li, Liu, Brassart, Suo. Journal of Applied Mechanics 81, 111007 (2014)