Baixe zanotto 1993 e outras Notas de estudo em PDF para Engenharia de Produção, somente na Docsity! EXPERIMENTAL STUDIES OF SURFACE NUCLEATION AND .
CRYSTALLIZATION OF GLASSES
Edgar D. Zanotto
DEMa - Federal University at Sao Carlos
13560 - Sao Carlos - SP, Brazil
1. INTRODUCTION
Surface crystallization is much more frequent than
internal crystallization but, paradoxically, has been
much less studied. One possible reason for the lack of
detailed studies on the subject is the inherent
difficulty of controlling and characterizing the
surface properties of glass.
From a technological point of view, the establishment
of a firm understanding and the ability to control the
kinetics of surface nucleation and growth in glasses
may lead to the development of a wide variety of
information devices for optical memories and related
applications [1]. Additionally, controlled surface
crystallization has proved to be quite an effective
method of enhancing the strength of glass [2).
The mechanisms of surface crystallization are still a
matter of controversy . Several factors which promote
free surface crystallization have been alluded in the
past and include: cracks or irregularities in: the
surface, alteration due to chemical reactions with the
atmosphere, differences between bulk and surface
composition, contamination with solid particles, etc.
Most studies carried out so far, however, are
qualitative and the relative importance of these
potential origins of surface crystallization in various
glasses have not been determined.
The relevance of surface crystallization was
recognized by the devitrification committee (TC7) of
the ICG which started a multinational research effort
on the subject in 1989.
The objective of this paper is to review and analyze
most of the relevant papers on surface crystallization
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Nucleation and Crystallization in Glasses and Liquids 65
and also to present a few results generated by the TC7
Committee on the subject. The goal is to provide a
firmer understanding of the causes for the predilection
of glasses to crystallize from the surface rather than
in the bulk. In addition, the question of whether or
not there is an intrinsic preference for
crystallization at the free surfaces will be addressed.
2 - SURFACE NUCLEATION
2.l. Effects of Surface Quality, Chemical Composition
and Temperature
Only a few comprehensive studies were devoted to
heterogeneous nucleation in glass, on crucible walls
and on metallic particles ,see for instance [3-6], and
the subject certainly deserves further attention. In
this article ,however, I deal only with isothermal
studies om free surface crystallization.
Starting in the early thirties, a number of papers of
qualitative nature were published concerning the
surface devitrification of several glasses.
Observations of crystallization around internal
bubbles were specially important because their surfaces
are in principle much cleaner than the external glass
surfaces. These papers were summarized recently [7] and
are listed in Table 1.
Table 1. Surface crystallization studies.
| |
Author Year Glass crystals on bubbles ?
Morey 30 Soda-lime-silica no
Scott 61 Na20.2Si0Oz no
Klingsberg 67 BaO-Al203-TiO2z-Si0Qz no
Ernsberger 66 Soda-lime-silica only on a
few bubbles
Mattox 67 CaO-A1203-B203 in those with
solid particles
Hishinuma 86 PbO.SiOz, Na20.2SiOoz | no
DN
Despite some controversial results, the majority of
papers indicate that only those bubbles contaminated
with solid particles are preferential nucleation sites,
Most studies provided no evidences for nucleation on
(clean) bubble surfaces. It should also be emphasized
that it is generally accepted by glass technologists,
that glasses with dirty surfaces crystallize much
easier than those with clean surfaces.
66 Nucleation and Crystallization in Glasses and Liquids
measured. The identity of the x-crystals and why the
surface nucleation rates are sufficiently slow to allow
for their measurement are not known at present.
Table 2 summarizes the crystallite densities reported
by several authors for different glasses.
Table 2. Surface crystallite densities:
2
Author Year Treatment Glass Ns (mm *)
Ground surface
McMillan 82 840ºc / 10min ZAS 3:10*
Polished ;
McMillan 82 840 / 10min ZAS 1:10
zanotto 86 820 / 0-4h CMS2 8.10"
zanotto 90 700 / 0-24h NCS 4105
Zanotto 90 720 / 0-26h NCS 3:10
Kalinina 90 140-860/450h M2A2S5 1105
Muller 90 900 /10 min M2A2S5 5:10
As-received
Zanotto 90 750-800 / 0-30h Float 0-3-10"*
Fractured
2
Muller 90 900-980 /0-80min M2A258S5 2:10
Fire-polished
zganotto 90 730 / 0-7.5h NCS Zero
Yamane 90 |
GM 30870 "lowest"
* range of values for different crystal phases.
Summarizing , the results of Table 2 and Figure 2
show that the surface crystallite densities strongly
depend on the surface condition. The smoother (and
presumably the cleaner) the surface the smaller is Ns.
Some fire polished specimens and some (as-received)
float glasses, with pristine surfaces, . did, not
crystallize at all, while Ns was almost 10 / mm for
some ground and for mechanically polished specimens.
The results of [7-12] also indicate that, in most
cases, surface nucleation finishes in the early stages
of the transformation, and saturation occurs before any
measurement of the heterogeneous nucleation rate can be
made, in a wide temperature range, from Ty to Tm (the
x-phase was an exception).
A possible explanation for the apparent lack of
temperature dependence of the surface nucleation rates
is provided by the classical theory, which is capable
of describing reasonably well the temperature
dependence of homogeneous nucleation rates in glasses
Nucleation and Crystallization in Glasses and Liquids 69
[6]. If one uses the classical equation, and allows the
reduced interfacial energy, à = & Na “vu! ?/AHm (these
parameters were defined elsewhere [6]) to vary from
typical values for homogeneous nucleation (0.4< a <0.6)
to the expected small values for heterogeneous
nucleation (a < 0.3), it is seen that the smaller the
value of a, the flatter, and consequently the less
dependent on temperature, is the nucleation curve.
Finally, the absence of crystals on some clean,
pristine, surfaces and also on most bubble surfaces
provide clear evidences that the free surfaces are not
preferential nucleation sites, in agreement with the
thermodynamic arguments of Unlmann [17):
2.2. Effects of the Atmosphere
The effects of the surrounding atmosphere on the
crystal growth rates are reasonably well documented
[8]. However, much less is known about the effects of
atmosphere on surface nucleation densities.
A detailed study was performed by Takahashi and
Sakaino [13] who measured the crystal growth rates and
also the crystallite densities on the surface of a
Na20.2SiO2 glass (T9g-=470'c) for a series of heat
treatments, from 200 to 500“C in N2, COz and water
vapor. The number of crystals increased in the
following order; in dry N2, in Hz0 vapor, being much
larger in dry CO2, with a maximum at 250-300ºCc. They
demonstrated that NazCOs crystals formed at the glass
surface provided active sites for crystallization of
sodium disilicate crystals at the development
temperature (600'C for 20min).
Partridge and McMillan [14] have shown that
atmospheres containing reduced oxygen and water
contents inhibit surface nucleation of a Zn0-Al203-SiOz
glass.
3. CRYSTAL GROWTH
In the vast majority of experimental studies of
crystal growth in glasses, nucleation spontaneously
initiates or is induced at the glass surface and the
time evolution of the crystallized layer growing
towards the specimen center is determined by microscopy
techniques. Thus, the growth Kinetics refer to
molecular rearrangements in the bulk of the glass.
Recently, a different experiment was carried out with
an almost stoichiometric cordierite glass supplied by
70 Nucleation and Crystallization in Glasses and Liquids
shott Class for the TC 7 Committee members. The full
set of results will be presented in a forthcoming
congress [15], but a relevant summary is given bellow.
Three types of growth kinetics were determined, i.e,
of: i) crystals which nucleated at the surface and grew
in the bulk, ii) surface nucleated crystals which grew
two- dimensionally on the surfaces, in the early stages
of the transformation, and àãii) internal crystals,
which nucleated on foreign particles, and grew in the
bulk. The three types of growth rates vwere equal,
within experimental error, implying that the surface
and bulk diffusion processes for growth, and
inferentially for nucleation, are similar.
In a previous paper [7] 1 suggested that the bulk and
surface diffusional mechanisms might be different. That
suggestion was based on molecular dynamics calculations
and also on the observed differences between the
activation enthalpies for crystal growth, Hc, and
viscous flow, Hn, in a float glass which crystallized
from the surface. This matter is clarified in [18] were
we demonstrate that the differences in Hc and Hm are
genuine for most glasses and not only for those which
only nucleate at the surfaces.
4. SUMMARY
surface nucleation saturates in the early stages of
crystallization for most glasses. The nucleation rates
are too fast to be measured in wide temperature ranges,
from Tg to Tm. This insensitivity to temperature is due
to the small values of surface energy. |
Nucleation is not observed on pristine, clean,
surfaces, as predicted by simple thermodynamic
arguments. Surface nucleation is mainly due to impurity
particles whose number is inversely proportional to the
degree of surface perfection and cleanliness.
“There is much scope for further work on surface
crystallization.
Acknowledgements
TI thank R. Basso, A.V. Cardoso, E.B. Ferreira, E.
Wittman, N. Mora and E.C. Ziemath for performing most
experiments and for useful discussions. I also thank
M.Weinberg and the TC7 Committee colleagues, R.Muller
and W.Pannhorst, for useful exchange of information.
Financial help by FAPESP, contract no. 85/0725-3 and by
PADCT/CNPq contract no. 620058/91-9 are appreciated.
Nucleation and Crystallization in Glasses and Liquids nf