TY - JOUR
T1 - Pore size and shape in mortar by thermoporometry
AU - Sun, Zhenhua
AU - Scherer, George W.
N1 - Funding Information:
This work was supported by NSF Grant CMS-0509986 . The authors are indebted to Marie-Hélène Tremblay and Jacques Marchand for providing the mortar samples used in this work.
Copyright:
Copyright 2010 Elsevier B.V., All rights reserved.
PY - 2010/5
Y1 - 2010/5
N2 - The pore structure of mortar (w/c = 0.55) was examined using thermoporometry (TPM), nitrogen adsorption/desorption (NAD), and mercury intrusion porosimetry (MIP). The TPM measurements were calibrated by comparison to NAD and MIP measurements on porous glass; similar comparisons were made on dried and resaturated mortars. For undried mortars, TPM provides the size of pore entries (from the freezing cycle) and interiors (from the melting cycle). In keeping with previous studies, we find that there is an unfrozen layer of water between the ice and the pore wall in porous glass that is about 0.8 nm thick; when lime-saturated water is used, the thickness of that layer increases by about 10%. In mortar, the unfrozen layer is about 1.0-1.2 nm thick, so no freezing occurs in pores with diameters ≤ 4.5 nm, at least down to - 40 °C (where the radius of the crystal/liquid interface is ∼ 1.5 nm). Based on the hysteresis in the freezing and melting curves, the larger mesopores in mortar were found to be rather spheroidal, while the smaller ones were more cylindrical.
AB - The pore structure of mortar (w/c = 0.55) was examined using thermoporometry (TPM), nitrogen adsorption/desorption (NAD), and mercury intrusion porosimetry (MIP). The TPM measurements were calibrated by comparison to NAD and MIP measurements on porous glass; similar comparisons were made on dried and resaturated mortars. For undried mortars, TPM provides the size of pore entries (from the freezing cycle) and interiors (from the melting cycle). In keeping with previous studies, we find that there is an unfrozen layer of water between the ice and the pore wall in porous glass that is about 0.8 nm thick; when lime-saturated water is used, the thickness of that layer increases by about 10%. In mortar, the unfrozen layer is about 1.0-1.2 nm thick, so no freezing occurs in pores with diameters ≤ 4.5 nm, at least down to - 40 °C (where the radius of the crystal/liquid interface is ∼ 1.5 nm). Based on the hysteresis in the freezing and melting curves, the larger mesopores in mortar were found to be rather spheroidal, while the smaller ones were more cylindrical.
KW - Freezing and thawing (C)
KW - Mercury porosimetry (B)
KW - Microstructure (B)
KW - Pore size distribution (B)
KW - Thermodynamic calculations (B)
UR - http://www.scopus.com/inward/record.url?scp=77949659466&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=77949659466&partnerID=8YFLogxK
U2 - 10.1016/j.cemconres.2009.11.011
DO - 10.1016/j.cemconres.2009.11.011
M3 - Article
AN - SCOPUS:77949659466
SN - 0008-8846
VL - 40
SP - 740
EP - 751
JO - Cement and Concrete Research
JF - Cement and Concrete Research
IS - 5
ER -