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Academic literature on the topic 'Elastic properties'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 August 2024

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Journal articles on the topic "Elastic properties"

1

TASSLER, P. L., A. L. DELLON, and C. CANOUN. "Identification of Elastic Fibres in the Peripheral Nerve." Journal of Hand Surgery 19, no. 1 (February 1994): 48–54. http://dx.doi.org/10.1016/0266-7681(94)90049-3.

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Traditional histological staining techniques, as well as elastin-specific antibodies and electron microscopy, have been used to assess the distribution of elastin within the peripheral nerve. The location of the elastin identified by the VerHoeff-VanGiesen or Weigert stains has been shown to coincide with the unambiguous identilication of elastin by immunospecific stains and electron microscopy. Elastin is located in all three connective layers of the peripheral nerve. Thick elastic fibres, consisting of amorphous elastiu protein and microfibrils, are located consistently in the perineurium and, to a lesser extent, in the epineurium. The endoneurium contains small collections of elastic fibres widely distributed between the axons. Compared with collagen, the overall content of elastin, however, is small, suggesting that the visco-elastic properties of peripheral nerve may be due primarily to collagen.

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Trębacz, Hanna, and Angelika Barzycka. "Mechanical Properties and Functions of Elastin: An Overview." Biomolecules 13, no. 3 (March 22, 2023): 574. http://dx.doi.org/10.3390/biom13030574.

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Human tissues must be elastic, much like other materials that work under continuous loads without losing functionality. The elasticity of tissues is provided by elastin, a unique protein of the extracellular matrix (ECM) of mammals. Its function is to endow soft tissues with low stiffness, high and fully reversible extensibility, and efficient elastic–energy storage. Depending on the mechanical functions, the amount and distribution of elastin-rich elastic fibers vary between and within tissues and organs. The article presents a concise overview of the mechanical properties of elastin and its role in the elasticity of soft tissues. Both the occurrence of elastin and the relationship between its spatial arrangement and mechanical functions in a given tissue or organ are overviewed. As elastin in tissues occurs only in the form of elastic fibers, the current state of knowledge about their mechanical characteristics, as well as certain aspects of degradation of these fibers and their mechanical performance, is presented. The overview also outlines the latest understanding of the molecular basis of unique physical characteristics of elastin and, in particular, the origin of the driving force of elastic recoil after stretching.

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Zinke, Sally. "Elastic properties." Leading Edge 19, no. 1 (January 2000): 8. http://dx.doi.org/10.1190/tle19010008.1.

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Gosline, J., M. Lillie, E. Carrington, P. Guerette, C. Ortlepp, and K. Savage. "Elastic proteins: biological roles and mechanical properties." Philosophical Transactions of the Royal Society of London. Series B: Biological Sciences 357, no. 1418 (February 28, 2002): 121–32. http://dx.doi.org/10.1098/rstb.2001.1022.

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The term ‘elastic protein’ applies to many structural proteins with diverse functions and mechanical properties so there is room for confusion about its meaning. Elastic implies the property of elasticity, or the ability to deform reversibly without loss of energy; so elastic proteins should have high resilience. Another meaning for elastic is ‘stretchy’, or the ability to be deformed to large strains with little force. Thus, elastic proteins should have low stiffness. The combination of high resilience, large strains and low stiffness is characteristic of rubber–like proteins (e.g. resilin and elastin) that function in the storage of elastic–strain energy. Other elastic proteins play very different roles and have very different properties. Collagen fibres provide exceptional energy storage capacity but are not very stretchy. Mussel byssus threads and spider dragline silks are also elastic proteins because, in spite of their considerable strength and stiffness, they are remarkably stretchy. The combination of strength and extensibility, together with low resilience, gives these materials an impressive resistance to fracture (i.e. toughness), a property that allows mussels to survive crashing waves and spiders to build exquisite aerial filters. Given this range of properties and functions, it is probable that elastic proteins will provide a wealth of chemical structures and elastic mechanisms that can be exploited in novel structural materials through biotechnology.

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Jacobsen, R. L., T. M. Tritt, A. C. Ehrlich, and D. J. Gillespie. "Elastic properties ofBi2Sr2CaCu2Oxwhiskers." Physical Review B 47, no. 13 (April 1, 1993): 8312–15. http://dx.doi.org/10.1103/physrevb.47.8312.

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Ishii, I., H. Higaki, S. Morita, M. A. Avila, T. Sakata, T. Takabatake, and T. Suzuki. "Elastic properties of." Physica B: Condensed Matter 383, no. 1 (August 2006): 130–31. http://dx.doi.org/10.1016/j.physb.2006.03.077.

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Ishii, Isao, Haruhiro Higaki, Shinya Morita, Marcos A. Avila, Toshiro Takabatake, and Takashi Suzuki. "Elastic properties of." Journal of Magnetism and Magnetic Materials 310, no. 2 (March 2007): 957–59. http://dx.doi.org/10.1016/j.jmmm.2006.10.163.

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Sayin, M. R., M. Aydin, S. M. Dogan, T. Karabag, M. A. Cetiner, and Z. Aktop. "Aortic elastic properties." Herz 38, no. 3 (December 23, 2012): 299–305. http://dx.doi.org/10.1007/s00059-012-3695-9.

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Malanon, Sasatorn, Surachai Dechkunakorn, Niwat Anuwongnukroh, and Wassana Wichai. "Comparison of Three Commercial Latex and Non-Latex Orthodontic Elastic Bands." Key Engineering Materials 814 (July 2019): 354–59. http://dx.doi.org/10.4028/www.scientific.net/kem.814.354.

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Orthodontic elastic bands are commonly made from natural rubber because they provide high resiliency at a reasonable cost. However, hypersensitivity related to protein present in latex have been reported in some patients which has led to increased usage of non-latex elastic alternatives. Therefore, the assessment of their mechanical properties is of importance. The objective of this study was to compare the physical and mechanical properties of three commercial latex and non-latex type orthodontic elastic bands. Samples of latex and non-latex type orthodontic elastics from manufacturers – AO (6.5oz), MASEL (6.0oz), GAC (6.0oz), with 3/16-inch diameter were selected. Firstly, the physical characteristics (width, cross-sectional thickness, and inner diameter) of the elastic bands were determined, following which their mechanical properties [initial extension force (F0), 24 h-residual force (F24), percentage of force decay, force exerted at 3 times the inner diameter (F3xID) and breaking force] were tested. The data were analyzed with Mann-Whitney U test and multiple comparisons among the groups were done with Kruskal-Wallis Test (p< 0.05). Significant differences were found in the physical characteristics and mechanical properties among each brand and type of elastics. AO elastic bands had significantly low F0 and F24 compared with the others. While the percentage of force decay at 24 h was greatest in AO followed by MASEL and GAC. Non-latex type elastics showed greater force decay than latex type ones, approximately 30-40% and 20-30% of the initial force in non-latex and latex type elastic, respectively. AO elastics showed the highest F3xID and also the lowest breaking force. Overall, non-latex type elastics exhibited lower breaking force compared to latex type ones. Wide variations were observed in the physical and mechanical characteristics among same manufacturer and same elastic type. All commercial brands presented higher F3xID than that stated by the manufacturers. Non-latex type elastics showed greater force decay over 24 h than latex type ones. The differences in the properties between the 2 types of the elastics could be due to the differences in their structure and polymers composition.

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Goldman, Jeremy, Shu Q. Liu, and Brandon J. Tefft. "Anti-Inflammatory and Anti-Thrombogenic Properties of Arterial Elastic Laminae." Bioengineering 10, no. 4 (March 28, 2023): 424. http://dx.doi.org/10.3390/bioengineering10040424.

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Elastic laminae, an elastin-based, layered extracellular matrix structure in the media of arteries, can inhibit leukocyte adhesion and vascular smooth muscle cell proliferation and migration, exhibiting anti-inflammatory and anti-thrombogenic properties. These properties prevent inflammatory and thrombogenic activities in the arterial media, constituting a mechanism for the maintenance of the structural integrity of the arterial wall in vascular disorders. The biological basis for these properties is the elastin-induced activation of inhibitory signaling pathways, involving the inhibitory cell receptor signal regulatory protein α (SIRPα) and Src homology 2 domain-containing protein tyrosine phosphatase 1 (SHP1). The activation of these molecules causes deactivation of cell adhesion- and proliferation-regulatory signaling mechanisms. Given such anti-inflammatory and anti-thrombogenic properties, elastic laminae and elastin-based materials have potential for use in vascular reconstruction.

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Dissertations / Theses on the topic "Elastic properties"

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Hornby, Brian E. "The elastic properties of shales." Thesis, University of Cambridge, 1994. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.296669.

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Dunk, Alan. "Elastic properties of triglycine sulphate." Thesis, University of Bath, 1987. https://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.376297.

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Paine, A. C. "Elastic properties of granular materials." Thesis, University of Bath, 1998. https://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.245957.

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Harrington, Jonathan J. "Hierarchical modelling of softwood hygro-elastic properties." Thesis, University of Canterbury. Mechanical Engineering, 2002. http://hdl.handle.net/10092/8061.

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The hygro-elastic behaviour of wood under load or when subjected to environmental changes is of considerable practical interest. This behaviour can be determined by exhaustive experimentation, but such an approach makes explaining its origin, which from some perspectives can be more important than its prediction, problematic. This thesis attempts to establish a model (actually a hierarchical set of models) that goes some way toward both predicting and explaining the mechanics of wood. Attention is focused on radiata pine because of the commercial importance of this species in New Zealand, but much of the modelling is applicable to other softwoods and, to a lesser extent, hardwoods. Wood can be looked on as a hierarchical material, that is as a material possessing structure at multiple scales. For many problems involving such materials the heterogeneous structure at a particular scale can be replaced by a homogeneous one possessing similar properties. Homogenization theory defines what is meant by similar and also provides the means for determining these effective properties. In this thesis wood structure is treated at three different scales: namely the supramolecular or nanostructural, the cell-wall or ultrastructural and the cellular or microstructural scales. Homogenization across these levels is performed either analytically or numerically, using the finite element method. At the smallest scale, the constituent phases are treated as homogeneous continua. Models for the hygro-elastic phase properties, as functions of temperature and moisture content are developed based on available experimental data. The models devised to describe wood at each of the above mentioned scales introduce a large number of structural parameters, such as constituent mass fractions and cell-wall layer volume fractions. In the abscence of specific data, estimates for these parameters are developed based on data from the literature. Together with these auxiliary models, the main sequence of structural models can then be used to obtain estimates for the material properties of small domains within macrostuctural models.

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Han, Tongcheng. "Joint elastic-electrical properties of reservoir sandstones." Thesis, University of Southampton, 2010. https://eprints.soton.ac.uk/195017/.

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Over the last decade, marine controlled source electromagnetic (CSEM), sub-seabed imaging has developed to a state where routine resistivity mapping of hydrocarbon reservoirs is now possible. Co-located marine seismic and electrical resistivity survey data could provide the engineering parameters needed to better assess the economic potential of hydrocarbon reservoirs without the need for drilling, and could provide additional reservoir monitoring capabilities in the future. However, proper exploitation of joint seismic-CSEM datasets will require a much better understanding of the inter-relationships among geophysical (elastic and electrical) and reservoir engineering properties. This project seeks to study the inter-relationships among the elastic and electrical properties of typical reservoir sandstones for improved insight into wave propagation phenomena in porous rocks. A high quality joint elastic-electrical dataset has been collected on a set of 67 sandstone samples showing a range of porosities, permeabilities and clay contents. The measurements were simultaneously carried out at differential pressures up to 60 MPa. Elastic properties (compressional and shear wave velocity and attenuation) were measured using a pulse-echo technique; electrical resistivity was recorded at AC frequency of 2 Hz using a circumference resistivity measurement method. The effects of porosity, permeability, clay content and differential pressure on the low frequency (2 Hz) electrical resistivity properties and the influence of differential pressure and petrophysical parameters on the joint elastic-electrical properties of reservoir sandstones were analyzed. A three-phase (quartz, brine and pore-filling clay) effective medium model based on self-consistent approximation (SCA) and differential effective medium (DEM) for the joint elastic-electrical properties of reservoir sandstones was developed and was found to give a good description of the experimental observations.

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Chatterjee, Sudipta. "Tribological properties of pseudo-elastic nickel-titanium." Diss., Restricted to subscribing institutions, 2008. http://proquest.umi.com/pqdweb?did=1610048621&sid=1&Fmt=2&clientId=1564&RQT=309&VName=PQD.

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Bastos, de Paula Osni. "Elastic properties of carbonates : measurements and modelling." Thesis, Curtin University, 2011. http://hdl.handle.net/20.500.11937/1417.

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This thesis is a multi-scale study of carbonate rocks, from the nanoscale and digital rock investigations to the imaging studies of carbonate reservoir analogues. The essential links between these extremes are the carbonate physical properties and rock-physics models, which are investigated here through the modelling of ultrasonic wave propagation in carbonate samples, focusing on elastic stress sensitivities, saturating fluids and porosity models. Validation of Gassmann fluid substitution in carbonates is also investigated using correlations between core and well log measurements.On the nanoscale, we use the nanoindentation technique in an oolitic limestone to directly measure the calcite Young modulus and derive bulk and shear moduli. We have found a large variation in the calcite bulk modulus, from 56 to 144 GPa. The high values obtained in some oolite rings were interpreted as genetically associated with biologically generated calcite (biocalcite). There are many measurements that achieve these values in brachiopod shells, but none in oolitic limestone. We associate the smaller values with microporosity, which is undetectable by our microCT or even SEM images. On the microscale we use the X-ray microCT images. From these images we can compute oolite elastic parameters using finite difference methods (FDM). In this oolite sample, calcite was segmented in two distinct phases. Nanoindentation provides the elastic parameters for each phase. The results of the modelling are compared with ultrasonic measurements on dry samples.To compute the properties of rocks on fluid-saturated samples, one needs to use fluid substitution methods, such as Gassmann’s equations. However, the applicability of Gassmann’s equations and the fluid substitution technique to carbonate rocks is still a subject of debate. Here we compare the results of fluid substitution applied to dry core measurements against sonic log data. The 36 meters of continuously sampled carbonates data, comes from a cretaceous reservoir buried at a depth of 5000 metres in the Santos Basin, offshore Brazil. Compressional and shear velocities, density and porosity were measured in 50 samples covering the entire interval. We obtain good agreement between the elastic properties obtained from core and log measurements. This shows that Gassmann’s fluid substitution is applicable to these carbonates, at least at sonic log frequencies.Carbonate microstructure is investigated using the stress dependency of shear and compressional wave velocities according to the dual porosity model of Shapiro (2003). The model assumes that the pore space contains two types of pores: stiff and compliant pores. Understanding the parameters of this model for different rocks is important for constraining stress effects in these rocks. The results for a carbonate dataset from the Santos Basin show a good correlation between compliant porosity and dry bulk modulus, total porosity and density for 29 samples of carbonates from the Santos Basin. The correlations seem to be different for different facies distribution, with different trends for mudstone facies and grainstone and rudstone facies. We also performed the same analysis using 66 samples of sandstones of diverse origins (Han et al., 1986): a good correlation appears between compliant porosity and the dry bulk modulus for all samples.If we correlate only the 7 samples from Fontainebleau sandstone, a good correlation also appears between total and compliant porosity. This analysis shows that the correlation is facies dependent also for sandstones.While Gassmann’s equations may be valid for low frequencies, they are not applicable at higher frequencies, where squirt dispersion is significant. We propose a workflow to model wave dispersion and attenuation due to the squirt flow using the geometrical parameters of the pore space derived from the stress dependency of elastic moduli on dry samples. Our analysis shows the dispersion is controlled by the squirt flow between equant pores and intermediate pores (with aspect ratios between 10-3 - 2·10-1). Such intermediate porosity is expected to close at confining pressures of between 200-2000 MPa. We also infer the magnitude of the intermediate porosity and its characteristic aspect ratio. Substituting these parameters into the squirt model, we have computed elastic moduli and velocities of the water-saturated rock and compared these predictions against laboratory measurements of these velocities.The agreement is good for a number of clean sandstones, but much worse for a broad range of shaley sandstones. Our predictions show that dispersion and attenuation caused by the squirt flow between compliant and stiff pores may occur in the seismic frequency band. Confirmation of this prediction requires laboratory measurements of elastic properties at these frequencies.The carbonate system of Telegraph Station, Shark Bay (WA), is a unique environment where coquinas, stromatolites and microbial mats are linked: an excellent analogue to carbonate pre-salt offshore Brazil. We acquired 7.5 km of GPR data and high resolution seismic data in the coquina ridges. They are composed by calcite shells deposited by cyclones, which show excellent high resolution GPR images, being a low loss dielectric medium. Three classes of coquinas were mapped: tabular layers, convex-up crest and washover fan. From the correlation of 14C dating of 50 samples and the mapped events we can estimate an average rate of one event every 13 years. From our interpretation the Holocene regression is continuous but not homogeneous. Carbonate dissolution features, faults, trends and discontinuities were mapped. Analysis of these features helps us understand reservoir porosity and permeability distribution in carbonate deposits, and can be used to constrain reservoir properties in pre-salt carbonates in Brazilian basins.

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Ortolani, Matteo. "Elastic Properties of Textured Nanocrystalline Thin Films." Doctoral thesis, Università degli studi di Trento, 2011. https://hdl.handle.net/11572/367871.

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Polycrystalline thin films and coatings often show preferred orientation of grains and crystalline domains, and develop a residual stress state as an effect of the growth mechanisms. These features can be conveniently measured by means of non-contact and non-destructive X-ray diffraction. As the technique only measures a map of strains along selected directions, stress evaluation requires a suitable constitutive equation, where the expression of moduli can be far from trivial if texture effects are to be taken into account; additionally, a grain interaction model needs to be enforced to describe strain and stress distribution among grains in the aggregate, based on background assumptions. Several grain interaction models are available from literature: usually, a model or a combination of them provides a good fit of experimental data; often however underlying hypotheses are too restrictive or require unavailable information on certain microstructural parameters, leading this approach to fail. For this reason an experimental method was developed, for the characterisation of elastic properties and residual stress in thin film components by means of X-ray diffraction during in-situ mechanical testing. This thesis presents a review of major literature works describing grain interaction modelling in textured components, and their implementation in X-ray diffraction stress analysis procedures. Following, the method for experimental characterisation of thin film elastic properties is described in detail. Applications are presented in the final chapter, that illustrates selected case studies on electrodeposited coatings.

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Ortolani, Matteo. "Elastic Properties of Textured Nanocrystalline Thin Films." Doctoral thesis, University of Trento, 2011. http://eprints-phd.biblio.unitn.it/682/1/tesi_dottorato.pdf.

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Polycrystalline thin films and coatings often show preferred orientation of grains and crystalline domains, and develop a residual stress state as an effect of the growth mechanisms. These features can be conveniently measured by means of non-contact and non-destructive X-ray diffraction. As the technique only measures a map of strains along selected directions, stress evaluation requires a suitable constitutive equation, where the expression of moduli can be far from trivial if texture effects are to be taken into account; additionally, a grain interaction model needs to be enforced to describe strain and stress distribution among grains in the aggregate, based on background assumptions. Several grain interaction models are available from literature: usually, a model or a combination of them provides a good fit of experimental data; often however underlying hypotheses are too restrictive or require unavailable information on certain microstructural parameters, leading this approach to fail. For this reason an experimental method was developed, for the characterisation of elastic properties and residual stress in thin film components by means of X-ray diffraction during in-situ mechanical testing. This thesis presents a review of major literature works describing grain interaction modelling in textured components, and their implementation in X-ray diffraction stress analysis procedures. Following, the method for experimental characterisation of thin film elastic properties is described in detail. Applications are presented in the final chapter, that illustrates selected case studies on electrodeposited coatings.

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Topol, Heiko [Verfasser]. "Acoustic and mechanical properties of viscoelastic, linear elastic, and nonlinear elastic composites / Heiko Topol." Aachen : Hochschulbibliothek der Rheinisch-Westfälischen Technischen Hochschule Aachen, 2012. http://d-nb.info/1028213352/34.

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Books on the topic "Elastic properties"

1

Eduard-Marius, Cracium, and Soós E, eds. Mechanics of elastic composites. Boca Raton, Fla: Chapman & Hall/CRC, 2004.

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2

Shankland, Thomas J., and Jay D. Bass, eds. Elastic Properties and Equations of State. Washington, D. C.: American Geophysical Union, 1988. http://dx.doi.org/10.1029/sp026.

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Pasechnik, Sergey V. Liquid crystals: Viscous and elastic properties. Weinheim: Wiley-VCH, 2009.

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J, Shankland Thomas, and Bass Jay D, eds. Elastic properties and equations of state. Washington, D.C: Institute of Geophysics and Planetary Physics, American Geophysical Union, 1988.

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1931-, Rossiter Bryant W., and Baetzold Roger C, eds. Determination of elastic and mechanical properties. New York: Wiley, 1991.

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Saurer, G. Third Numerical Round Robin on Elastic-Plastic Fracture Mechanics: Part 1 : Results of linear elastic fracture calculations. Wurenlingen, Switzerland: Swiss Federal Institute for Reactor Research, 1986.

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Brunnett, Guido. The curvature of plane elastic curves. Monterey, Calif: Naval Postgraduate School, 1993.

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C, Newman J., and Langley Research Center, eds. ZIP3D: An elastic and elastic-plastic finite-element analysis program for cracked bodies. Hampton, Va: National Aeronautics and Space Administration, Langley Research Center, 1990.

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Briscall, Harry. Filament wound resin composites: preparation and elastic properties. Salford: University of Salford, 1986.

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Kallio, Marke. The elastic and damping properties of magnetorheological elastomers. [Espoo, Finland]: VTT Technical Research Centre of Finland, 2005.

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Book chapters on the topic "Elastic properties"

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Böer, Karl W. "Elastic Properties." In Survey of Semiconductor Physics, 73–87. Boston, MA: Springer US, 1990. http://dx.doi.org/10.1007/978-1-4615-9744-5_4.

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Authier, A., and A. Zarembowitch. "Elastic properties." In International Tables for Crystallography, 72–98. Chester, England: International Union of Crystallography, 2006. http://dx.doi.org/10.1107/97809553602060000630.

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Authier, A., and A. Zarembowitch. "Elastic properties." In International Tables for Crystallography, 72–99. Chester, England: International Union of Crystallography, 2013. http://dx.doi.org/10.1107/97809553602060000902.

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Wan Hassan, Wan Muhamad Saridan. "Elastic Properties." In Physics—Problems, Solutions, and Computer Calculations, 463–85. Cham: Springer Nature Switzerland, 2023. http://dx.doi.org/10.1007/978-3-031-42678-0_13.

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Pelleg, Joshua. "Elastic Properties." In Mechanical Properties of Semiconductors, 23–41. Cham: Springer International Publishing, 2024. http://dx.doi.org/10.1007/978-3-031-21659-6_2.

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Raum, Kay. "Microscopic Elastic Properties." In Bone Quantitative Ultrasound, 409–39. Dordrecht: Springer Netherlands, 2010. http://dx.doi.org/10.1007/978-94-007-0017-8_16.

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Snarskii, Andrei A., Igor V. Bezsudnov, Vladimir A. Sevryukov, Alexander Morozovskiy, and Joseph Malinsky. "Effective Elastic Properties." In Transport Processes in Macroscopically Disordered Media, 207–17. New York, NY: Springer New York, 2016. http://dx.doi.org/10.1007/978-1-4419-8291-9_16.

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Strauch, D. "CaSe: elastic constants." In New Data and Updates for several IIa-VI Compounds (Structural Properties, Thermal and Thermodynamic Properties, and Lattice Properties), 236–38. Berlin, Heidelberg: Springer Berlin Heidelberg, 2014. http://dx.doi.org/10.1007/978-3-642-41461-9_100.

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Strauch, D. "CaTe: elastic constants." In New Data and Updates for several IIa-VI Compounds (Structural Properties, Thermal and Thermodynamic Properties, and Lattice Properties), 246–47. Berlin, Heidelberg: Springer Berlin Heidelberg, 2014. http://dx.doi.org/10.1007/978-3-642-41461-9_105.

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Strauch, D. "BaPo: elastic constants." In New Data and Updates for several IIa-VI Compounds (Structural Properties, Thermal and Thermodynamic Properties, and Lattice Properties), 26. Berlin, Heidelberg: Springer Berlin Heidelberg, 2014. http://dx.doi.org/10.1007/978-3-642-41461-9_11.

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Conference papers on the topic "Elastic properties"

1

Katahara, Keith W. "Clay mineral elastic properties." In SEG Technical Program Expanded Abstracts 1996. Society of Exploration Geophysicists, 1996. http://dx.doi.org/10.1190/1.1826454.

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Sewell, Thomas D. "Elastic Properties of HMX." In Shock Compression of Condensed Matter - 2001: 12th APS Topical Conference. AIP, 2002. http://dx.doi.org/10.1063/1.1483562.

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Zubrinov, I. I., V. K. Sapozhnikov, Efim V. Pestrykov, and Victor V. Atuchin. "Elastic and elasto-optic properties of KTiOPO 4." In Fundamental Problems of Optoelectronics and Microelectronics, edited by Yuri N. Kulchin and Oleg B. Vitrik. SPIE, 2003. http://dx.doi.org/10.1117/12.502282.

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Ruzzene, Massimo. "Dynamics of elastic hyperbolic lattices." In Photonic and Phononic Properties of Engineered Nanostructures XI, edited by Ali Adibi, Shawn-Yu Lin, and Axel Scherer. SPIE, 2021. http://dx.doi.org/10.1117/12.2589474.

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Brecht, J., A. Elvenkemper, J. Betten, U. Navrath, and J. B. Multhoff. "Elastic Properties of Friction Materials." In 21st Annual Brake Colloquium & Exhibition. 400 Commonwealth Drive, Warrendale, PA, United States: SAE International, 2003. http://dx.doi.org/10.4271/2003-01-3333.

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Navin, Francis, Michael MacNabb, and Grant W. Miyasaki. "Elastic Properties of Selected Vehicles." In SAE International Congress and Exposition. 400 Commonwealth Drive, Warrendale, PA, United States: SAE International, 1988. http://dx.doi.org/10.4271/880223.

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Schuller, I. K. "Elastic Properties of Metallic Superlattices." In IEEE 1985 Ultrasonics Symposium. IEEE, 1985. http://dx.doi.org/10.1109/ultsym.1985.198685.

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Carlotti, G., D. Fioretto, L. Palmieri, G. Socino, V. I. Anisimkin, and I. M. Kotelyanskii. "Elastic properties of SnO2 films." In 1993 IEEE Ultasonics Symposium. IEEE, 1993. http://dx.doi.org/10.1109/ultsym.1993.339499.

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9

Gieske, J. H., T. L. Aselage, and David Emin. "Elastic properties of boron carbides." In Boron-rich solids. AIP, 1991. http://dx.doi.org/10.1063/1.40854.

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Wang, Zhijing (Zee), Hui Wang, and Michael E. Cates. "Elastic properties of solid clays." In SEG Technical Program Expanded Abstracts 1998. Society of Exploration Geophysicists, 1998. http://dx.doi.org/10.1190/1.1820064.

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Reports on the topic "Elastic properties"

1

Abramoff, Bennet, and Lisa C. Klein. Elastic Properties of Silica Xerogels. Fort Belvoir, VA: Defense Technical Information Center, January 1990. http://dx.doi.org/10.21236/ada216528.

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Kachanov, M. (Effective elastic properties of cracked solids). Office of Scientific and Technical Information (OSTI), January 1990. http://dx.doi.org/10.2172/7035443.

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3

Burchell, Timothy. Grade 2114: Flexure Strength and Elastic Properties. Office of Scientific and Technical Information (OSTI), September 2019. http://dx.doi.org/10.2172/1564183.

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4

Olness, D. Sensors for in situ monitoring of elastic properties. Office of Scientific and Technical Information (OSTI), April 1989. http://dx.doi.org/10.2172/6219025.

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5

Rogers, Peter H., and Michael D. Gray. Augmentation of the In Vivo Elastic Properties Measurement System to Include Bulk Properties. Fort Belvoir, VA: Defense Technical Information Center, September 2013. http://dx.doi.org/10.21236/ada598773.

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Rogers, Peter H., and Michael D. Gray. Augmentation of the In Vivo Elastic Properties Measurement System to Include Bulk Properties. Fort Belvoir, VA: Defense Technical Information Center, September 2014. http://dx.doi.org/10.21236/ada617535.

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7

Hodge, S. C., and J. M. Minicucci. Cyclic material properties tests supporting elastic-plastic analysis development. Office of Scientific and Technical Information (OSTI), November 1996. http://dx.doi.org/10.2172/663570.

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Peterson, Michael L. Measurement of Anisotropic Elastic Constitutive Properties at High Temperatures. Fort Belvoir, VA: Defense Technical Information Center, December 2003. http://dx.doi.org/10.21236/ada419939.

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Glushko, E. Ya, and A. N. Stepanyuk. Pneumatic photonic crystals: properties and application in sensing and metrology. [б. в.], 2018. http://dx.doi.org/10.31812/123456789/2875.

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Abstract:

A pneumatic photonic crystal i.e. a medium containing regularly distributed gas-filled voids divided by elastic walls is proposed as an optical indicator of pressure and temperature. The indicator includes layered elastic platform, optical fibers and switching valves, all enclosed into a chamber. We have investigated theoretically distribution of deformation and pressure inside a pneumatic photonic crystal, its bandgap structure and light reflection changes depending on external pressure and temperature.

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10

Goldberg, A. Atomic, Crystal, Elastic, Thermal, Nuclear, and Other Properties of Beryllium. Office of Scientific and Technical Information (OSTI), February 2006. http://dx.doi.org/10.2172/899094.

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