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Atomistic Simulation studies of the Cement Paste Components

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<strong>Atomistic</strong> <strong>Simulation</strong> <strong>studies</strong> <strong>of</strong> <strong>the</strong> <strong>Cement</strong> <strong>Paste</strong> <strong>Components</strong><br />

not only in its local stability, but also in its stability with respect to <strong>the</strong>ir neighbouring<br />

sizes. The stability index <strong>of</strong> an alumino-silicate chain with <strong>the</strong> length m evaluates <strong>the</strong><br />

stability <strong>of</strong> that chain with respect to <strong>the</strong> addition or removal <strong>of</strong> one alumino-silicate<br />

unit. It is <strong>the</strong> chemical potential <strong>of</strong> <strong>the</strong> system against <strong>the</strong> number <strong>of</strong> particles. This<br />

methodology is generally employed in <strong>the</strong> study <strong>of</strong> <strong>the</strong> stability with <strong>the</strong> cluster sizes<br />

[216], and it has been applied successfully to investigate <strong>the</strong> stable lengths <strong>of</strong> silicate<br />

chains [128]. To calculate <strong>the</strong> stability index, all <strong>the</strong> possible growing mechanism must<br />

be identified and taken into account. A silicate chain <strong>of</strong> length m might grow reacting<br />

with o<strong>the</strong>r silicon monomer Si(OH) 4 , an aluminium monomer Al(OH) - 4 , or even with a<br />

charged silicon monomer Si(OH) 3 O - [215]. If only one charged silicon tetrahedra unit or<br />

one aluminium per chain are considered, <strong>the</strong> chains <strong>of</strong> length m +1 could continue<br />

growing by adding neutral silicon monomer. The same reasoning can be applied to <strong>the</strong><br />

inverse process, when a silicate chain losses a unit. All <strong>the</strong> possible growth paths that<br />

were considered in this study are given in figure 4.2.1. It must be noted that once <strong>the</strong><br />

aluminium enters <strong>the</strong> chain, <strong>the</strong> next Si(OH) 4 may be incorporated in both sides <strong>of</strong> <strong>the</strong><br />

chain. Then, <strong>the</strong>y are several growth paths due to <strong>the</strong> asymmetry arising from <strong>the</strong><br />

presence <strong>of</strong> aluminium. In order to deal with a unique growth path, <strong>the</strong> -Al(OH) - 4 unit<br />

was always located at <strong>the</strong> end <strong>of</strong> <strong>the</strong> chain, assuming that subsequent silicon units would<br />

react in <strong>the</strong> opposite chain side.<br />

The neutral and charged silicate chains (orange, blue and red paths <strong>of</strong> figure 4.2.1) were<br />

explored in a previous work by Ayuela and co-workers [128]. They found that <strong>the</strong> stable<br />

chains were those which fulfil <strong>the</strong> 3n – 1 rule, in agreement with <strong>the</strong> experimental data<br />

[6, 8, 52], and that <strong>the</strong> charged chains contribute more than <strong>the</strong> neutral ones to <strong>the</strong> global<br />

stability. In this work, <strong>the</strong> growing paths involving aluminium (green and purple in<br />

figure 4.2.2) were studied. The stability index <strong>of</strong> <strong>the</strong>se new channels is defined as:<br />

( ) ( 1) ( 1) ( 1) 3 ( )<br />

S m = Em− + Em+ + Em− − ⋅ Em<br />

(4.2.2)<br />

Al Al Al Si Al<br />

where <strong>the</strong> subscript denotes a silicate ( Si ) or alumino-silicate chain ( Al ), <strong>the</strong> term in<br />

paren<strong>the</strong>sis indicates <strong>the</strong> length <strong>of</strong> <strong>the</strong> chain, and E is <strong>the</strong> energy <strong>of</strong> <strong>the</strong> corresponding<br />

chain. A detailed derivation <strong>of</strong> <strong>the</strong> stability index from reaction transition rates and <strong>the</strong><br />

96

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