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detected by MIP and thus the intrusion curves do not describe the whole pore system of a<br />

material. Hence it is more useful to redraw the porosity data to a form of column plot (Figure 2)<br />

covering the whole size range of pores.<br />

Pore volume/cm 3 g -1<br />

0.35<br />

0.30<br />

0.25<br />

0.20<br />

0.15<br />

0.10<br />

0.05<br />

0.00<br />

0.001 0.010 0.100 1.000 10.000 100.000<br />

Pore diameter/μm<br />

Figure 1: MIP intrusion curves of thermally loaded composites<br />

The material T in its initial – not annealed – state (sample T‐ref) features the pore size<br />

distribution being typical for cementitious materials. The most frequent are the gel pores (d = 10<br />

to 100 nm), the sample contains also certain amount of large technological pores. The pore<br />

distribution of sample T 600 (annealed at 600˚C) is similar to the unloaded one; there is<br />

observed certain increase of gel pores, the capillary and technological pores remain mostly<br />

unaffected by this temperature. The dramatic changes of pore size distribution take place when<br />

the sample is annealed at 800˚C and continue at 1000˚C as well. The volume of gel pores is<br />

reduced. It is caused by thermal decomposition of cement binder. The binding components<br />

(CSH gels and portlandite) dehydrate back to clinker minerals and CaO (it converts to calcite<br />

spontaneously). These decomposition processes are accompanied by sintering of binder which<br />

results to the gel pores diminishing.<br />

Pore volume/cm 3 g -1<br />

0.250<br />

0.200<br />

0.150<br />

0.100<br />

0.050<br />

0.000<br />

T-ref<br />

T 600<br />

T 800<br />

T 1000<br />

T ref<br />

T 600<br />

T 800<br />

T 1000<br />

0.001-0.01 0.01-0.1 0.1-1 1-10 10-100 > 100<br />

Pore diameter/μm<br />

Figure 2: Histogram of pore size distribution of thermally loaded composites T<br />

181

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