Dynamic Strength of Oil Shale

1976 ◽  
Vol 16 (01) ◽  
pp. 17-22 ◽  
Author(s):  
J. Lankford

Abstract In-situ retorting of oil shale requires explosive loading under overburden pressure to break up rock masses. Therefore, a study of the dynamic. confined failure strength under compressive loading was carried out for shale ranging in kerogen content from 11 to 45 gal/ton. It was found that the envelope of ultimate strength could be described by a first-order failure criterion that expands uniformly in principal stress space about the hydrostatic axis as the strain rate increases. The strength/log-strain-rate dependence was found to be non linear, with the strength doubling over seven orders of magnitude in strain rate. In these laboratory tests, considerable ductility at failure was encountered, with the strain at failure ranging from 2 to 35 percent. Failure strength was ordered consistently with respect to kerogen content, hut the strength-reducing presence of large calcite inclusions in the leanest grade of shale overcame the effect of lower kerogen content to the extent that specimens of intermediate richness exhibited the highest strength. Introduction Current processes under consideration for retorting oil shale in situ require fragmenting the oil-bearing shale bed. Explosive loading of boreholes is a means of achieving this end. To optimize the fragmentation process, knowledge of the dynamic strength and fracture characteristics of the oil shale is needed. Until recently, the strength properties of oil shale have been studied under rather limited conditions. Schmidt and Schuler and Sellers et al. established the unconfined, uniaxial compressive strength at slow strain rates for Anvil Point, Colo., oil shale. The principal conclusion of both studies is that material properties generally strongly depend on kerogen content, with fracture strength and Young's modulus decreasing and ductility increasing monotonically with increasing kerogen content. The strength of most rock is now known to strongly depend on strain rate, increasing with increasing rate of loading at constant temperature. However, oil-bearing shale as a rock type is not included in any of these studies. The principal goal of this study was to investigate the strain-rate dependence of strength and ductility for oil shale to predict the strength levels required for fracture under dynamic loading. The highest rates obtained under controlled testing (around 10(3)/second) are still lower than that of an explosive impulse. EXPERIMENTAL PROCEDURES ROCK DESCRIPTION AND PREPARATION The material used in this study was obtained from the U. S. Bureau of Mines test mine at Anvil Point, Colo. Anvil Point oil shale is a fine-grained Point, Colo. Anvil Point oil shale is a fine-grained (0.0004 to 0.0016 in.) sedimentary rock of variable kerogen content. Kerogen contents for the three blocks from which specimens were cored were 10.7 bbl/ton (lean), 32.0 bbl/ton (medium), and 45.7 bbl/ton (rich), as determined by Fischer Assay. The rich- and medium-grade shales were homogeneous in structure, although the layering of the Kerogen was clearly visible. The lean-grade shale also was layered, but contained numerous lens-shaped, calcite inclusions with typical dimensions of 0.04 × 0.4 in. These inclusions were oriented so that the lens lay parallel to the bedding plane. plane. The cylindrical test specimens were about 1/2 in. in diameter and 1 in. long. They were obtained by core drilling and grinding of the ends to obtain flatness and parallelism within 0.0002 in. Specimens from each boulder were taken from three orthogonal directions: normal to the bedding plane and two mutually perpendicular directions within the bedding plane. Tests with these specimens showed that, plane. Tests with these specimens showed that, while the susceptibility to failure was quite anisotropic, varying by as much as a factor of three for x vs y or z, the ultimate strength was fairly insensitive to orientation. Since ultimate strength was of primary interest, cores perpendicular to the bedding plane were used in subsequent testing. This also was the orientation used by other experimenters studying Anvil Point shale. SPEJ p. 17

1980 ◽  
Vol 20 (1) ◽  
pp. 44 ◽  
Author(s):  
A.C. Hutton ◽  
A.J. Kantsler ◽  
A.C. Cook ◽  
D.M. McKirdy

The Tertiary oil-shale deposits at Rundle in Queensland and of the Green River Formation in the western USA, together with Mesozoic deposits such as those at Julia Creek in Queensland, offer prospects of competitive recovery cost through the use of large-scale mining methods or the use of in situ processing.A framework for the classification of oil shales is proposed, based on the origin and properties of the organic matter. The organic matter in most Palaeozoic oil shales is dominantly large, discretely occurring algal bodies, referred to as alginite A. However, Tertiary oil shales of northeastern Australia are chiefly composed of numerous very thin laminae of organic matter cryptically-interbedded with mineral matter. Because the present maceral nomenclature does not adequately encompass the morphological and optical properties of most organic matter in oil shales, it is proposed to use the term alginite B for finely lamellar alginite, and the term lamosites (laminated oil shales) for oil shales which contain alginite B as their dominant organic constituent. In the Julia Creek oil shale the organic matter is very fine-grained and contains some alginite B but has a higher content of alginite A and accordingly is assigned to a suite of oil shales of mixed origin.Petrological and chemical techniques are both useful in identifying the nature and diversity of organic matter in oil shales and in assessing the environments in which they were formed. Such an understanding is necessary to develop exploration concepts for oil shales.


2002 ◽  
Vol 20 (1) ◽  
pp. 87-92 ◽  
Author(s):  
SHALOM ELIEZER ◽  
ELLA MOSHE ◽  
DAN ELIEZER

The approach to the ultimate strength of metals is determined experimentally. The strength of the materials and the strain rate were determined from the free surface velocity time history, which was measured with an optically recording velocity interferometer system. The dynamic strength was measured at strain rates in the domain of 5·106 to 5·108 s−1. The necessary tension to break the metal (spall) and the very high strain rates were achieved using high-powered lasers in nanosecond and picosecond regimes. The measurements at strain rates larger than 108 s−1 were achieved for the first time. The ultimate strength of metals was calculated using a realistic wide-range equation of state. Our experiments indicate that under very fast tension processes, the dynamic strength of materials is determined not by the macroscopic defects but by atomic quantum mechanical processes described by the equation of state of the material. The rate of the process is described by the strain rate, and at strain rates higher than 5·107 s−1, the atomic forces are dominating the dynamic strength of materials.


2018 ◽  
Author(s):  
Devon Jakob ◽  
Le Wang ◽  
Haomin Wang ◽  
Xiaoji Xu

<p>In situ measurements of the chemical compositions and mechanical properties of kerogen help understand the formation, transformation, and utilization of organic matter in the oil shale at the nanoscale. However, the optical diffraction limit prevents attainment of nanoscale resolution using conventional spectroscopy and microscopy. Here, we utilize peak force infrared (PFIR) microscopy for multimodal characterization of kerogen in oil shale. The PFIR provides correlative infrared imaging, mechanical mapping, and broadband infrared spectroscopy capability with 6 nm spatial resolution. We observed nanoscale heterogeneity in the chemical composition, aromaticity, and maturity of the kerogens from oil shales from Eagle Ford shale play in Texas. The kerogen aromaticity positively correlates with the local mechanical moduli of the surrounding inorganic matrix, manifesting the Le Chatelier’s principle. In situ spectro-mechanical characterization of oil shale will yield valuable insight for geochemical and geomechanical modeling on the origin and transformation of kerogen in the oil shale.</p>


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