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(Old and New) Theories On The Glass Transition

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3.

THE GLASS STATE AND THE GLASS TRANSITION:


THERMODYNAMIC and KINETIC ASPECTS

(old and new) theories on the


GLASS TRANSITION
a) Old theories (but still being used) on the
glass transition

Free volume theory

(Entropic) Adam & Gibbs theory

Mode-coupling theory
z *
Average transition probability: W (T ) A exp
k BT
minimum size of the rearranging unit: z*

* *
s z
c
s k B ln 2
*
c
Sc N

1 B Nsc*
exp B
W (T ) TSc kB
MODE-COUPLING THEORY:

Ergodicity parameter k(t) is the Fourier transform


of the van Hove density-density autocorrelation function
G(r,t) = 1/ < (r,t) (0,0)>
Critical point when c = 1:

c < 1: lim t k(t) = 0 , liquid (ergodic)


c > 1: lim t k(t) 0 , glass (non-ergodic)

It predicts a power-law singularity of and :


1.765

1
c
Evolution of the self-intermediate scattering function for a supercooled Lennard-Jones
binary mixture (molecular dynamics simulation for 1000 atoms).
b) the ENERGY LANDSCAPE paradigm [Goldstein, 1969]
ENTROPY
c) New theories -under discussion- on the
glass transition
Present controversy:
Does a glass possess a finite residual entropy at T=0?
How does the entropy of a glass-forming system change
in the glass transition range?
Classical thermodynamic view
[Nernst, Simon, Giauque; Gutzow&Schmeltzer, Goldstein]:
YES, configuracional entropy of the supercooled liquid is frozen-in
at T = Tg , S (Tg) = 0, giving S(0) 0.
Entropy loss view
[Gupta&Mauro, Kivelson&Reiss]:
NO, laboratory glass transition is a non-spontaneous process from the
ergodic (liquid) to a broken-ergodic (glass) state. The phase space of the
glass is a small subset of that of the liquid. As a consequence there must
be an entropy loss (without latent heat): S (Tg) > 0, but S(0) = 0.
Classical thermodynamic view
[Nernst, Simon, Giauque; Gutzow&Schmeltzer, Goldstein]:
YES, configuracional entropy of the supercooled liquid is frozen-in
at T = Tg , S (Tg) = 0, giving S(0) 0.

J. Non-Cryst. Solids 355 (2009) 581-594


Entropy loss view
[Gupta&Mauro, Kivelson&Reiss]:
NO, laboratory glass transition is a non-spontaneous process from the
ergodic (liquid) to a broken-ergodic (glass) state. The phase space of the
glass is a small subset of that of the liquid. As a consequence there must
be an entropy loss (without latent heat): S (Tg) > 0, but S(0) = 0.

J. Non-Cryst. Solids 355 (2009) 595-599


c) New theories -under discussion- on the
glass transition
* Many competing recent theories
- Random First Order Transition (mosaic theory) [Wolynes et al.]
- Spin Glasses Theory : mean-field p-spin model [Moore]
- Frustration-limited domains [Kivelson et al., Tarjus et al.]
- Hierarchical Random Energy Model [Parisi]
- Dynamical Facilitation Theory [Chandler and Garrahan]
- Free-energy landscape theories
- Two-temperature thermodynamic theory [Nieuwenhuizen]
-
F TS c (T ) R d YR ,
d 1

1
1 d
mosaic
T Tk
1
1 d
AG
T Tk
c) New theories -under discussion- on the
glass transition

The Nature of Glass Remains


Anything but Clear

(29. July. 2008)

Mark Interrante

ENIGMA Molten glass being worked into an ornament.


Understanding glass could lead to better products
and offer headway in other scientific problems.

David A. Weitz, a physics professor at Harvard, joked,


There are more theories of the glass transition than there
are theorists who propose them.

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