MétaCan
Menu
Back to cohort
Record W46266023

A discussion on the decrease of unconfined compressive strength between saturated and dry rock samples

2007· article· en· W46266023 on OpenAlexaboutno aff
Manuel Romana García, Balázs Vásárhelyi

Bibliographic record

VenueRepository of the Academy's Library (Library of the Hungarian Academy of Sciences) · 2007
Typearticle
Languageen
FieldEngineering
TopicRock Mechanics and Modeling
Canadian institutionsnot available
Fundersnot available
KeywordsCompressive strengthGeotechnical engineeringWater contentOil shaleMaterials scienceGeologyComposite material
DOInot available

Abstract

fetched live from OpenAlex

The unconfined compressive strength (UCS) of a rock is a basic parameter for many characterization systems, strength criteria and calculation methods. It is well-known fact that it depends on the water content of the samples, and decrease when the water content increases. The paper discusses the possible causes of this reduction. From published data by Vasarhelyi and co-workers and others authors some empirical tentative guidelines for this reduction are proposed, which can be used in rock engineering problems where changes in water content occur regularly (dam and bridges foundations, harbors...). .Hsu and Nelson (1993), in a preliminary research for the not built Super Collider, correlated the unconfined compressive strength of many types of shale (from Canada and USA) with the water content. Their results (fig 2), show a marked negative correlation between water content and compressive strength Fig 2 Unconfined compressive strength vs. water content for clay shales (Hsu and Nelson, 1993) Ballivy and Colin (1999) have analyzed the increase in triaxial strength related to changes in the dielectric constant of the fluid saturating the rock. In a propane storage cavern in shale the tension strength of the rock increased 150-200% due to the change in the dielectric constant, with a reversal to the prior strength when the propane evaporated. In their opinion changes in the saturation fluid cause changes in the effective stresses, a result already stated by Vutukuri (1974). In the same paper they show increases in the compressive strength of 20% when testing gneiss saturated with salt water (with a small decrease in the dielectric constant) over the same test saturated with distilled water, and increases in the compressive strength of 25-50% of dry samples over the same test saturated with distilled water. These results show a clear trend but cannot be generalized due to the small number of tests done. The respective dielectric constant are: 80, distilled water; 74, salt water; 0 dry state Lashkaripour and Passaris (1993) compiled a data base with selected values of shale rock properties. Fig 3 shows data from two coal mines. There is also a marked negative correlation between water content and compressive strength 3 CAUSES OF THIS DECREASE In strong indurated rocks of low porosity the compressive failure is preceded by the growth of cracks from the border of existing micro pores. The cracks coalesce into growing cracks finally extending to the sample dimension and failure happens. Fig 3. Unconfined compressive strength vs. water content for two shales (Lashkaripour and Passaris, 1993). (a) Linton Lane coal mine, (b) Rye Hill coal mine According to Vasarhely and Bobet (2000) there are three fundamental theories on crack initiation criteria: maximum tangential stress (Erdogan and Sih, 1963), maximum energy release rate (Hussain et al, 1974) and minimum energy density (Sih, 1974). Any of them can reasonably predict tensile crack initiation, both in tension and/or compression, but not in shear. In the simpler case the crack initiation occurs as “a progressive lengthening of the crack across the infinite plate” (Rummel, 1974).The mathematical formulation “involves a consideration of the energy change during the crack growth”. Following Rummel there are three energy terms to be considered: change in potential energy of the applied forces, change of strain energy due to the existence of the crack and change in surface energy. So the Griffith criteria for tensile fracture can be stated (in the simpler formulation) as σt = (2 E γ / π c) where: σt is the tensile strength of the material E is the deformation modulus γ is the specific surface energy c is the crack initial half length As has been shown by Ballivy and Colin (1999) the nature of liquid has a direct influence in the crack openings, a fact due to the decrease in surface energy of the crack borders when the pore is full of water. A similar explanation is offered by Vasarhely and Ledniczky (1999): “moisture diminishes the spread of free surface energy, i. e. it facilitates micro-cracks propagation by decreasing the elastic limit and the peak strength also” On the other hand the crack growth can be originated by increasing water pressures within the pores when the rock is saturated. Both effects can happen simultaneously In poorly cemented rocks the presence of water can affect to the cementation between the grains by different ways: solution, dispersion...Finally in soft argillaceous rocks the water diminishes the strength of the grains and/or the cementation So there are different causes which produce, together or unconnectedly, the reduction in strength 4.-SOME PUBLISHED DATA Steiger and Leundt (1990) gave some data extracted from an EXXON comprehensive research program on shale typical properties, shown in table 1 Table 1.-Data on UCS of typical shales (Steiger and Leundt, 1990)

Fetched live from OpenAlex and de-inverted. Abstracts are not stored in this database: the inverted indexes are 8.6 GB of the frame’s 9.3 GB of text, and the host has 13 GB free.

How this classification was reachedexpand

Full frame distilled prediction

Teacher imitation

Not calibrated prevalence, not ground truth. Human validation pending. Learned from the 10,348 direct Codex labels and 10,348 direct Gemma labels. Candidate is the union of thresholded teacher heads; consensus is their intersection. These outputs are machine_predicted_unvalidated and are not human labels or direct frontier model labels.

metaresearch head score (Codex)0.001
metaresearch head score (Gemma)0.000
Version: codex-gemma-dda1882f352aValidation status: machine_predicted_unvalidated
Candidate categoriesnone
Consensus categoriesnone
DomainCandidate signal: none · Consensus signal: none
Study designCandidate signal: Bench or experimental · Consensus signal: Bench or experimental
GenreCandidate signal: Empirical · Consensus signal: Empirical
Teacher disagreement score0.073
Threshold uncertainty score0.609

Codex and Gemma teacher scores by category

CategoryCodexGemma
Metaresearch0.0010.000
Meta-epidemiology (narrow)0.0000.000
Meta-epidemiology (broad)0.0010.000
Bibliometrics0.0000.001
Science and technology studies0.0000.001
Scholarly communication0.0000.001
Open science0.0020.001
Research integrity0.0000.001
Insufficient payload (model declined to judge)0.0000.000

Machine scores (provisional)

The two teacher heads of the student model, read on this work. A score orders the frame for review; it never asserts a category, and the validation status ships verbatim with every row.

Baseline scores from an immature model (maturity gate not passed, 7 training rounds). Scores rank; they never assert a category.

Opus teacher head0.021
GPT teacher head0.226
Teacher spread0.205 · how far apart the two teachers sit on this one work
Validation statusscore_only:v0-immature-baseline · verbatim from the scoring run: score_only means the number may rank works, and no category label ships from it

Classification

machine, unvalidated

Machine predicted; a candidate call from one teacher head, not a consensus.

The models applied no category: nothing in the taxonomy fit this work.
Study designBench or experimental
Domainnot available
GenreEmpirical

How this classification was reached, model by model and score by score, is at the end of the page under "How this classification was reached".

Quick stats

Citations44
Published2007
Admission routes1
Has abstractyes

Explore more

Same venueRepository of the Academy's Library (Library of the Hungarian Academy of Sciences)Same topicRock Mechanics and ModelingFrench-language works237,207