The Effect of Pressure on Pore Structure in Mercury Porosimetry

The pore volume distributions of chrysotile, Mg 3 (OH) 4 . Si 2 O 5 , ZrO 2 and of four samples of silica with pore volumes from 1.45 to 2.70 cm 3 /g have been measured by means of nitrogen capillary condensation and mercury penetration. It is shown that compaction of the porous structures can occur...

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Main Authors: A.M.L. Hustings, J.J.F. Scholten
Format: Article
Language:English
Published: Hindawi - SAGE Publishing 1987-12-01
Series:Adsorption Science & Technology
Online Access:https://doi.org/10.1177/026361748700400404
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spelling doaj-433c6ec28cc24eac923e043d364860942021-04-02T12:57:41ZengHindawi - SAGE PublishingAdsorption Science & Technology0263-61742048-40381987-12-01410.1177/026361748700400404The Effect of Pressure on Pore Structure in Mercury PorosimetryA.M.L. HustingsJ.J.F. ScholtenThe pore volume distributions of chrysotile, Mg 3 (OH) 4 . Si 2 O 5 , ZrO 2 and of four samples of silica with pore volumes from 1.45 to 2.70 cm 3 /g have been measured by means of nitrogen capillary condensation and mercury penetration. It is shown that compaction of the porous structures can occur under the influence of the high mercury pressures applied. The degree of compaction depends on the mechanical strength of the sample, its initial porosity and the magnitude of the mercury pressure. The extremely strong ZrO 2 sample, with its low pore volume of 0.18 cm 3 /g does not show any sign of cracking up to pressures as high as 190 MPa. Hollow chrysotile needles compact in the pressure range from 100 to 400 MPa. Highly porous silicas all show severe compaction. In accordance with Brown & Lard (Brown & Lard, 1974) it is concluded that silicas with pore volumes larger than 1.2 cm 3 /g are not suitable for study by mercury porosimetry.https://doi.org/10.1177/026361748700400404
collection DOAJ
language English
format Article
sources DOAJ
author A.M.L. Hustings
J.J.F. Scholten
spellingShingle A.M.L. Hustings
J.J.F. Scholten
The Effect of Pressure on Pore Structure in Mercury Porosimetry
Adsorption Science & Technology
author_facet A.M.L. Hustings
J.J.F. Scholten
author_sort A.M.L. Hustings
title The Effect of Pressure on Pore Structure in Mercury Porosimetry
title_short The Effect of Pressure on Pore Structure in Mercury Porosimetry
title_full The Effect of Pressure on Pore Structure in Mercury Porosimetry
title_fullStr The Effect of Pressure on Pore Structure in Mercury Porosimetry
title_full_unstemmed The Effect of Pressure on Pore Structure in Mercury Porosimetry
title_sort effect of pressure on pore structure in mercury porosimetry
publisher Hindawi - SAGE Publishing
series Adsorption Science & Technology
issn 0263-6174
2048-4038
publishDate 1987-12-01
description The pore volume distributions of chrysotile, Mg 3 (OH) 4 . Si 2 O 5 , ZrO 2 and of four samples of silica with pore volumes from 1.45 to 2.70 cm 3 /g have been measured by means of nitrogen capillary condensation and mercury penetration. It is shown that compaction of the porous structures can occur under the influence of the high mercury pressures applied. The degree of compaction depends on the mechanical strength of the sample, its initial porosity and the magnitude of the mercury pressure. The extremely strong ZrO 2 sample, with its low pore volume of 0.18 cm 3 /g does not show any sign of cracking up to pressures as high as 190 MPa. Hollow chrysotile needles compact in the pressure range from 100 to 400 MPa. Highly porous silicas all show severe compaction. In accordance with Brown & Lard (Brown & Lard, 1974) it is concluded that silicas with pore volumes larger than 1.2 cm 3 /g are not suitable for study by mercury porosimetry.
url https://doi.org/10.1177/026361748700400404
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