Abstract
Understanding the micromechanical mechanism of the rock creep process is of great importance for studying the macroscopic time-dependent behavior of rocks. In this study, the evolution characteristics of the microstructure (cracks and pores) of saturated sandstones under short term and creep uniaxial compression conditions were investigated with the nuclear magnetic resonance (NMR) technique. The samples were first loaded to different stress levels and creep stages and then completely unloaded for NMR testing. Based on the testing results, the macroscopic deformation behavior, moisture migration law, pore size distribution, porosity, and microstructure change of the each sample under the short-term loading or different stages of creep were quantitatively analyzed. After that, by introducing a nonlinear elasto-viscoplastic damage creep model (EVP) by Zhao et al. (18:04017129, 2018), the relationships between the macroscopic irreversible strains and microscopic porosity increments were established. Overall, it was observed that: (1) regardless of the stress level, the magnitudes of the axial and lateral critical strains of samples at the onset of the accelerating creep stage are both relatively constant, and the axial strain is almost comparable to that at the peak stress in the short-term test, while the lateral strain is larger than that of the short-term test. (2) During the mechanical tests, the moisture in the samples migrates from large pores into small pores, and after mechanical tests, the porosities of the samples increase, in which the small pores always account for a larger proportion. (3) Corresponding to the three creep stages, the porosity of the sample increases slightly after the transient stage, increases to a constant value that is largely independent of stress after the steady stage, and increases significantly after the creep failure. In particular, compared to the initial porosity of 6.7%, the average porosities of samples taken to the onset of the tertiary stage and creep failure is 7.49% and 8.71%, increasing by 16.7% and 29.8%, respectively. (4) The porosity growth of sandstone during the brittle creep is mainly driven by the microscopic subcritical crack growth along the grain boundaries.
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Data Availability
All data generated during the study are available from the corresponding author by request.
Abbreviations
- NMR:
-
Nuclear magnetic resonance
- XRD:
-
X-ray diffraction
- SEM:
-
Scanning electron microscope
- UCS:
-
Uniaxial compressive strength
- EVP creep model:
-
Nonlinear elasto-viscoplastic creep constitutive model
- \(\sigma _{0}\) :
-
Axial creep stress
- \(T_{2}\) :
-
Transverse relaxation time
- \(T_{{{\text{2S}}}}\) :
-
Transverse surface relaxation time
- \(\rho _{2}\) :
-
Surface relaxivity
- \(r\) :
-
Radius of pores
- \(\sigma _{{\text{P}}}\) :
-
Stress at the inflection point of rock compaction and dilatancy
- \(\varepsilon _{{\text{a}}}\), \(\varepsilon _{l}\), \(\varepsilon _{v}\) :
-
Axial, lateral, and volumetric strains of the sample
- \(t_{{S2}}\), \(t_{{\text{f}}}\) :
-
Time-to-onset of accelerating stage and time-to-failure
- \(T_{2} {\text{ cutoff}}\) :
-
Relaxation time separating mobile from immobile water
- \(\phi\) :
-
Porosity
- \(\phi _{{{\text{Si}}}}\) :
-
Initial porosity
- \(\phi _{{{\text{S0}}}}\) :
-
Porosity after short-term loading
- \(\phi _{{{\text{S1}}}}\) :
-
Porosity after transient creep stage
- \(\phi _{{{\text{S2}}}}\) :
-
Porosity after transient and steady creep stage
- \(\phi _{{{\text{S3}}}}\) :
-
Porosity after creep failure
- \(\phi _{s}\), \(\phi _{l}\) :
-
Porosity contributed by small pores and large pores
- \(D\) :
-
Creep damage variable
- \(\sigma _{s}\) :
-
Long-term strength
- \(E_{{{\text{ie}}}}\), \(E_{{{\text{ip}}}}\) :
-
Instantaneous elastic modulus and plastic modulus
- \(E_{{{\text{ve}}}}\), \(\eta _{{{\text{ve}}}}\) :
-
Viscoelastic parameters
- \(E_{{{\text{vp}}}}\), \(\eta _{{{\text{vp1}}}}\) :
-
Viscoplastic parameters
- \(\eta _{0}\) :
-
Initial viscosity coefficient
- \(\eta _{{{\text{vp}}2}}\) :
-
Viscoplastic viscosity coefficient
- \(k\), \(\gamma\) :
-
Material constants in EVP creep model
- \(\varepsilon _{{{\text{ie}}}}\), \(\varepsilon _{{{\text{ip}}}}\) :
-
Instantaneous elastic and plastic strains
- \(\varepsilon _{{{\text{vp}}}}\) :
-
Viscoplastic strain
- \(D_{{{\text{S2}}}}\) :
-
Creep damage variable at the onset of accelerating stage
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The research work was financially supported by the National Natural Science Foundation of China (Grant Nos. 51908431, 42077246), for which the authors are grateful.
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Chu, Z., Wu, Z., Liu, Q. et al. Evaluating the Microstructure Evolution Behaviors of Saturated Sandstone Using NMR Testing Under Uniaxial Short-Term and Creep Compression. Rock Mech Rock Eng 54, 4905–4927 (2021). https://doi.org/10.1007/s00603-021-02538-4
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DOI: https://doi.org/10.1007/s00603-021-02538-4