The role of annealing and grain boundary controls on the mechanical properties of limestones and marbles

Rui Zhang, Paul A. Bosomworth, Juliane Weber, Jan Ilavsky, Si Athena Chen, Alexis Flores-Betancourt, Elliot Paul Gilbert, Jitendra Mata, Mark L. Rivers, Peter J. Eng, Lawrence M. Anovitz

Research output: Contribution to journalArticlepeer-review

Abstract

Chemical and mechanical processes are coupled in many geological and geochemical environments. Reactive processes anneal defects and restructure grain boundaries, modifying their elastic properties, levels of internal friction, wave propagation rates and fracture behaviors. The nature of these changes is, however, contingent on the initial state of the rock. In this study, impulse excitation was used to measure changes in mechanical properties as a function of dry and steam heating time at 300 °C for three carbonate rocks: Carrara marble, Carthage marble (Burlington Limestone), and Texas Cream limestone (Edwards limestone), with initial porosities of about 1 %, 3 %, and 27 %, respectively. Frequency-dependent phenomena along with mineral recrystallization were observed. This was coupled with small-angle X-ray and neutron scattering analysis to determine the relationship between changes in bulk mechanical and microstructural properties. An observed decrease in both the Young's and shear moduli in the experimental limestones as a function of heating time reflects and quantifies a reduction in the stiffness of the rock due to annealing. The internal friction of the samples first increases then decreases with reaction time, reflecting defect annealing, but this was balanced against grain boundary dissolution apparently driven by condensation of steam in the confined grain-boundary environment. This suggests an increase in the boiling point under confinement leading to dissolution, increased porosity and widening of the grain boundaries. In addition, comparison of small-angle X-ray and neutron scattering results suggests that it is inappropriate to assume that pores are empty for quantitative analysis of typical small-angle scattering samples.

Original languageEnglish
Article number105926
JournalInternational Journal of Rock Mechanics and Mining Sciences
Volume183
DOIs
StatePublished - Nov 2024

Funding

The samples were tested in two vibration modes up to the seventh order of vibration supported by: parallel wires for flexural mode (Fig. 2b) and crossed wires for torsional mode (Fig. 2c) placed on the nodal lines. Photos of IE measurements in flexural and torsional mode are shown in the Supporting Information (SI). In flexure the parallel wires were placed 0.224 times the length of the sample from each end of the sample. The microphone was placed over the antinodes. A schematic of a typical waveform is shown in Fig. 2d, along with a fast Fourier transform (FFT) showing the inherent frequency spectrum (Fig. 2e).This work was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Chemical Sciences, Geosciences, & Biosciences (CSGB) Division. X-ray tomography was performed at GeoSoilEnviroCARS 13-BMD, X-ray diffraction was performed at GeoSoilEnviroCARS 13-BMC, and USAXS/SAXS/WAXS was performed at both 9-ID and 20-ID, Advanced Photon Source, Argonne National Laboratory. GeoSoilEnviroCARS is supported by the National Science Foundation \u2013 Earth Sciences (EAR \u2013 1634415). Tomography capability developments were supported by DOE BES Geosciences (DE\u2010SC0020112). This research used resources from the Advanced Photon Source, a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357. USANS was performed at Kookaburra and SANS was performed at Quokka, Australian Centre for Neutron Scattering, Australian Nuclear Science and Technology Organisation (ANSTO) under proposal number 15794. We want to thank Dr. Edgar Lara-Curzio for providing lab access and Dr. Lianshan Lin for providing training on using the impulse excitation instrument. The authors declare no competing financial interests. This work was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Chemical Sciences, Geosciences, & Biosciences (CSGB) Division. X-ray tomography was performed at GeoSoilEnviroCARS 13-BMD, X-ray diffraction was performed at GeoSoilEnviroCARS 13-BMC, and USAXS/SAXS/WAXS was performed at both 9-ID and 20-ID, Advanced Photon Source, Argonne National Laboratory. GeoSoilEnviroCARS is supported by the National Science Foundation \u2013 Earth Sciences (EAR \u2013 1634415). This research used resources from the Advanced Photon Source, a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357. USANS was performed at Kookaburra and SANS was performed at Quokka, Australian Centre for Neutron Scattering, Australian Nuclear Science and Technology Organisation (ANSTO) under proposal number 15794. We want to thank Dr. Edgar Lara-Curzio for providing lab access and Dr. Lianshan Lin for providing training on using the impulse excitation instrument. The authors declare no competing financial interests.

FundersFunder number
Chemical Sciences, Geosciences, & Biosciences
Advanced Photon Source
U.S. Department of Energy
Chemical Sciences, Geosciences, and Biosciences Division
National Science Foundation – Earth SciencesEAR – 1634415
Argonne National LaboratoryDE-AC02-06CH11357
Argonne National Laboratory
Office of Science15794
Office of Science
Basic Energy SciencesDE‐SC0020112
Basic Energy Sciences

    Keywords

    • Calcite
    • Internal friction
    • Recrystallization
    • Resonant frequency
    • X-ray and neutron scattering

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