Relevant bibliographies by topics / Bulk Modulus

Academic literature on the topic 'Bulk Modulus'

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Published: 4 June 2021
Last updated: 11 September 2023

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Journal articles on the topic "Bulk Modulus"

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Swamy, V., and L. S. Dubrovinsky. "Bulk modulus of anatase." Journal of Physics and Chemistry of Solids 62, no. 4 (April 2001): 673–75. http://dx.doi.org/10.1016/s0022-3697(00)00204-3.

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Ashbee, K. H. G. "Bulk ultrahigh-modulus polyethylene." Materials Characterization 37, no. 5 (November 1996): 343–47. http://dx.doi.org/10.1016/s1044-5803(96)00176-3.

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Knez, Dariusz, Mitra Khalilidermani, and Mohammad Ahmad Mahmoudi Zamani. "Water Influence on the Determination of the Rock Matrix Bulk Modulus in Reservoir Engineering and Rock-Fluid Coupling Projects." Energies 16, no. 4 (February 10, 2023): 1769. http://dx.doi.org/10.3390/en16041769.

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This research was conducted to determine how the incorporation of different poroelastic equations would affect the measured rock matrix bulk modulus in the laboratory. To do this, three experimental methods were used to measure the matrix bulk modulus, Ks, of seven sandstone specimens taken from the Świętokrzyskie mine in Poland. Those experimental methods were based on the different governing equations in poroelasticty theory. The matrix bulk modulus has a substantial impact on the rock strength against external stresses. Moreover, the rock bulk modulus depends directly on two components: the pore fluid bulk modulus and matrix bulk modulus. The second one is more important as it is much higher than the first one. In this study, the accuracy of those three methods in the measurement of the matrix bulk modulus was evaluated. For this purpose, an acoustic wave propagation apparatus was used to perform the required tests. For each method, an empirical correlation was extracted between the matrix bulk modulus and the applied hydrostatic stress. In all the experiments, an exponential correlation was observed between the matrix bulk modulus and the hydrostatic stress applied on the rock. Furthermore, it was found that the incorporation of the dry bulk modulus in the calculations led to an underestimation of the matrix bulk modulus. In addition, as the hydrostatic stress was raised, the matrix bulk modulus also increased. The applied methodology can be deployed to determine the matrix bulk modulus in coupled rock-fluid problems such as reservoir depletion, hydraulic fracturing, oil recovery enhancement, underground gas storage and land subsidence.
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Zhao, Liming, Tongjun Chen, Tapan Mukerji, and Genyang Tang. "Bulk modulus for fluid-saturated rocks at high frequency: modification of squirt flow model proposed by Mavko & Jizba." Geophysical Journal International 225, no. 3 (February 12, 2021): 1714–24. http://dx.doi.org/10.1093/gji/ggab060.

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SUMMARY The squirt flow model, proposed by Mavko & Jizba, has been widely used in explaining the frequency-related modulus and velocity dispersion between ultrasonic and seismic measurements. In this model, the saturated bulk modulus at high frequency is obtained by taking the so-called unrelaxed frame bulk modulus into Biot's or Gassmann's formula. When using Gassmann's formula, the mineral bulk modulus is taken as matrix bulk modulus. However, the soft pores (cracks) in rocks have a weakening effect on the matrix bulk modulus. The saturated bulk modulus at high frequency calculated with mineral bulk modulus as matrix bulk modulus is higher than the real values. To overcome this shortcoming we propose a modified matrix bulk modulus based on the Betti–Rayleigh reciprocity theorem and non-interaction approximation. This modification takes the weakening effect of soft pores (cracks) into consideration and allows calculating the correct saturated bulk modulus at high frequency under different soft-pore fractions (the ratio of soft porosity to total porosity) or crack densities. We also propose an alternative expression of the modified matrix bulk modulus, which can be directly obtained from laboratory measurements. The numerical results show that the saturated bulk modulus at high frequency using the original matrix bulk modulus (i.e. mineral bulk modulus) is approximated to that using the modified one only for rocks containing a small amount of soft-pore fraction. However, as the soft-pore fraction becomes substantial, using the original bulk matrix modulus is not applicable, but the modified one is still applicable. Furthermore, the results of the modified squirt flow model show good consistency with published numerical and experimental data. The proposed modification extends the applicable range of soft-pore fraction (crack density) of the previous model, and has potential applications in media having a relatively substantial fraction of soft pores or almost only soft pores, such as granite, basalt and thermally cracked glasses.
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Darrouzet, Jennifer L., Joseph C. Molis, and Nicholas P. Chotiros. "Grain bulk modulus of sand." Journal of the Acoustical Society of America 90, no. 4 (October 1991): 2370. http://dx.doi.org/10.1121/1.402084.

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Goldberger, Walter D., and Mark B. Wise. "Modulus Stabilization with Bulk Fields." Physical Review Letters 83, no. 24 (December 13, 1999): 4922–25. http://dx.doi.org/10.1103/physrevlett.83.4922.

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Tabor, D. "The bulk modulus of rubber." Polymer 35, no. 13 (June 1994): 2759–63. http://dx.doi.org/10.1016/0032-3861(94)90304-2.

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Verma, A. S., and A. Kumar. "Bulk modulus of cubic perovskites." Journal of Alloys and Compounds 541 (November 2012): 210–14. http://dx.doi.org/10.1016/j.jallcom.2012.07.027.

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Gallas, Marcia R., and Gasper J. Piermarini. "Bulk Modulus and Young's Modulus of Nanocrystalline gamma-Alumina." Journal of the American Ceramic Society 77, no. 11 (November 1994): 2917–20. http://dx.doi.org/10.1111/j.1151-2916.1994.tb04524.x.

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Zhao, Tao, Gaojian Hu, Tao Wang, and Huan Zhang. "Influence of Parallel Joint Spacing and Rock Size on Rock Bulk Modulus." Advances in Civil Engineering 2022 (September 10, 2022): 1–12. http://dx.doi.org/10.1155/2022/8475726.

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The size effect on the bulk modulus of rocks has been reported by previous studies. The accuracy in selecting the parameter for the rock mechanics analysis determines further accuracy of the calculation results. Moreover, given the influence of the size effect and joint spacing, the rock bulk modulus often changes. Thus, it is essential to examine the size effect on the bulk modulus. This study elucidated the influence of rock size and parallel joint spacing on the bulk modulus using the regression analysis and 12 sets of numerical plans. The results demonstrated that the bulk modulus decreased with an increase in rock size, and the curve represents an exponential function. The bulk modulus linearly increased as the parallel joint spacing increased. Furthermore, the characteristic size of the bulk modulus linearly decreased as the parallel joint spacing increased. In contrast, the characteristic bulk modulus linearly increased as the parallel joint spacing increased. The specific forms of these relationships were also elucidated in this study.
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Dissertations / Theses on the topic "Bulk Modulus"

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Balasubramanian, Karthik. "Smart bulk modulus sensor." [Gainesville, Fla.] : University of Florida, 2003. http://purl.fcla.edu/fcla/etd/UFE0002824.

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Loveday, J. S. "Skin effect measurements of the bulk modulus of potassium." Thesis, University of Bristol, 1987. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.233723.

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Huang, Shu. "Influence of Chemical Composition and Water on the Bulk Modulus of Pyrope." FIU Digital Commons, 2014. http://digitalcommons.fiu.edu/etd/1185.

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Garnets are major silicates from the upper mantle to the transition zone. Elastic properties of garnets are essential to interpret the variation of seismic velocities at different depths and construct a model of the Earth’s composition. Due to the chemical flexibility at octahedron sites of the crystal structures, garnets usually exist with multiple components and have many composition variations. Pyrope is an important member in the garnet group. Fe2+-Mg2+ substitution in pyrope is one of the common solid solutions. We have synthesized and measured three synthetic solid solutions samples (Py83Alm17, Py54Alm46 and Py30Alm70). Equations of state yielded their isothermal bulk moduli K0 to be 172(4)GPa, 174(2)GPa, and 183(2)GPa, respectively, which confirmed that almandine content (Fe2+ substitution) increased the bulk modulus of the garnet. A relation between the bulk modulus and the almandine mole fraction (n) was derived to be K0 = 170 + 15 n, showing it is a nearly ideal mixing model. Another factor that also significantly influences the elasticity of pyrope is water. Water is transported to the deep Earth by subduction slabs and mainly exists in nominally anhydrous minerals (NAM) as hydroxyl (OH-). Its content in minerals varies as depth increases. We therefore investigated pressure influence on water solubility in pyrope. A suite of pyrope single crystals was synthesized in a water-saturated environment at 6, 7, 9 and 12GPa and water was characterized by FTIR. IR spectra showed a typical peak at 3630 cm-1. At 9 and 12GPa, new peaks at 3572 cm-1 and 3504 cm-1 appeared and indicated that a new substitution mechanism, other than hydrogarnet substitution SiO4=(OH)4, was adopted in the pyrope crystal structure. Water solubility in pyrope reached 0.2wt% at 7GPa. From 4-7GPa, water solubility increased. At 9GPa, water content dropped to 0.07wt% and increased to 0.3wt% at 12GPa, where a cubic to tetragonal phase transition was observed. Water showed a weakening effect on the bulk moduli of hydrous pyrope. Their bulk moduli were 166GPa, 173GPa and 161GPa with water contents of 0.07wt%, 0.1wt% and 0.2wt%, respectively. An approximate linear relationship was proposed about the bulk modulus as a function of water content.
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Rusia, Devendra Kumar. "A modified viscoplastic formulation for large deformations using a bulk modulus approach." Ohio : Ohio University, 1987. http://www.ohiolink.edu/etd/view.cgi?ohiou1183058011.

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Common, David N. "Development of a system for the measurement of the static bulk modulus of fluids." Thesis, Georgia Institute of Technology, 2001. http://hdl.handle.net/1853/17579.

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Michael, Paul W., and Shreya Mettakadapa. "Bulk Modulus and Traction Effects in an Axial Piston Pump and a Radial Piston Motor." Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2016. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-200173.

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This paper describes an investigation into the effects of fluid bulk modulus and traction coefficient properties on piston pump flow losses and radial pison motor torque losses through experimentation, modelling and simulation. Synthetic ester, high bulk modulus, multi-grade, and single grade mineral oils were evaluated. The high bulk modulus fluid exhibited 20% lower pump case and compensator flow losses than a conventional mineral oil of the same viscosity grade. Low traction coefficient fluids reduced the lowspeed torque losses of the radial piston motor by 50%. Physical models for pump case flow and motor torque losses were derived from the experimental data. Field data was collected from a hydraulically propelled agricultural machine. This data was used to model fluid performance in the machine. The simulation results predict that at an operating temperature of 80⁰C, optimizing the bulk modulus and traction coefficients of the fluid could reduce flow losses by 18% and torque losses by 5%. These findings demonstrate the potential of combining comprehensive fluid analysis with modeling and simulation to optimize fluids for the efficient transmission of power.
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Njane, Stephen Njehia. "Precise Fish Volume Estimation Using Underwater Helmholtz Resonance." Kyoto University, 2019. http://hdl.handle.net/2433/244557.

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Kyoto University (京都大学)
0048
新制・課程博士
博士(農学)
甲第22076号
農博第2368号
新制||農||1072(附属図書館)
学位論文||R1||N5230(農学部図書室)
京都大学大学院農学研究科地域環境科学専攻
(主査)教授 近藤 直, 准教授 小川 雄一, 教授 飯田 訓久
学位規則第4条第1項該当
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Yang, Shudong, Aihua Tao, Yulin Luo, Junxiang Zhang, Peng Zhou, and Lin Zhou. "Experimental measurements of bulk modulus for two types of hydraulic oil at pressures to 140MPa and temperatures to 180°C." Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2016. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-199503.

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Bulk modulus of hydraulic oil represents the resistance of hydraulic oil to compression and is the reciprocal of compressibility. The bulk modulus is a basic thermodynamic property of hydraulic oil that has a very important influence on work efficiency and dynamic characteristics of hydraulic systems, especially for the hydraulic systems at ultra-high pressure or ultra-high temperature. In this study, a bulk modulus experimental equipment for hydraulic oil was designed and manufactured, two types of hydraulic oil were selected and its isothermal secant bulk modulus were measured at pressures to 140MPa and temperatures of 20~180°C. Compared the experimental results with the calculated results from the prediction equations of liquid bulk modulus that proposed by Klaus, Hayward, and Song, it is found that the experimental results are not completely identical with the calculated results.
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Lombardo, Nick, and e56481@ems rmit edu au. "Properties of Composites Containing Spherical Inclusions Surrounded by an Inhomogeneous Interphase Region." RMIT University. Mathematical and Geospatial Sciences, 2007. http://adt.lib.rmit.edu.au/adt/public/adt-VIT20080408.143315.

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The properties of composite materials in which spherical inclusions are embedded in a matrix of some kind, have been studied for many decades and many analytical models have been developed which measure these properties. There has been a steady progression in the complexity of models over the years, providing greater insight into the nature of these materials and improving the accuracy in the measurement of their properties. Some of the properties with which this thesis is concerned are, the elastic, thermal and electrical properties of such composites. The size of the spherical inclusion which acts as the reinforcing phase, has a major effect on the overall properties of composite materials. Once an inclusion is embedded into a matrix, a third region of different properties between the inclusion and matrix is known to develop which is called the interphase. It is well known in the composite community that the smaller the inclusion is, the larger the interphase region which develops around it. Therefore, with the introduction of nanoparticles as the preferred reinforcing phase for some composites, the interphase has a major effect on its properties. It is the aim of this thesis to consider the role of the interphase on the properties of composites by modeling it as an inhomogeneous region. There is much scientific evidence to support the fact that the interphase has an inhomogeneous nature and many papers throughout the thesis are cited which highlight this. By modeling the inhomogeneous properties by arbitrary mathematical functions, results are obtained for the various properties in terms of these general functions. Some specific profiles for the inhomogeneous region are considered for each property in order to demonstrate and test the models against some established results.
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Pereira, Amanda Cavalcante. "Influência da profundidade e de um processo de envelhecimento acelerado em propriedades de resinas bulk fill." Universidade de São Paulo, 2017. http://www.teses.usp.br/teses/disponiveis/23/23140/tde-15022018-101701/.

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O presente estudo teve como objetivo avaliar o desempenho de quatro resinas bulk fill (Filtek Bulk Fill (FBF), Opus Bulk Fill (OBF), Sonicfill (SF) e Tetric N-Ceram Bulk Fill (TNBF)) e uma resina convencional (Charisma Diamond (CD)) quanto às seguintes propriedades: resistência à flexão (RF), módulo de elasticidade (ME) e dureza Knoop (KHN) em função da profundidade e após a realização de um envelhecimento acelerado. Corpos de prova em formato de barra foram confeccionados simultaneamente em diferentes profundidades (1, 2, 3, 4 e 5 mm) para realização dos testes de resistência à flexão (n=10), módulo de elasticidade (n=10) e dureza Knoop (n=3). Os testes foram realizados em dois momentos, previamente e após a realização de um envelhecimento acelerado, que consistiu na realização de uma termociclagem com banhos alternados em água a 5 e 55ºC, com 1 min de imersão em cada, por 2000 ciclos. Os resultados para o teste de RF e ME mostraram que os valores para estas duas propriedades diminuíram em função da profundidade e após a realização da termociclagem para todas as resinas estudadas. Apenas a resina TNBF não apresentou diferença estatística para valores de ME após o envelhecimento acelerado. Quanto à dureza, os valores também diminuíram em função da profundidade, porém aumentaram após a realização do envelhecimento acelerado. Apenas a resina SF não apresentou diferença estatística entre os valores de dureza antes e após o envelhecimento. A resina convencional CD após a ciclagem térmica foi a única que apresentou relação base/topo (2 mm) acima de 80%. Nenhuma das resinas do tipo bulk fill apresentou uma relação base/topo acima de 80% para a dureza quando avaliadas na espessura máxima recomendada. Com base nos resultados obtidos, pode-se afirmar que, quando fotoativadas na espessura máxima recomendada, apenas a resina convencional CD apresentou resultados condizentes com a homogeneidade esperada em todas as condições deste estudo. Entretanto, para as resinas do tipo bulk fill, pode-se observar que as propriedades estudadas, de modo geral, sofreram uma diminuição significativa em função da profundidade. Para o envelhecimento, a dureza, diferentemente dos outros parâmetros, mostrou uma tendência de aumento.
The purpose of this study was to evaluate the performance of four bulk fill resins (Filtek Bulk Fill (FBF), Opus Bulk Fill (OBF), Sonicfill (SF) and Tetric N-Ceram Bulk Fill (TNBF)) and a conventional resin (Charisma Diamond (CD)) for the following properties: flexural strength (FS), flexural modulus (FM) and Knoop hardness (KHN) as a function of depth and after accelerated aging. Specimens were made simultaneously with different depths (1, 2, 3, 4 and 5 mm) for flexural strength tests (n = 10), flexural modulus (n = 10) and Knoop hardness (n = 3). The tests were carried out in two moments, before and after the accelerated aging process, which consisted of thermocycling with alternating baths in water at 5 and 55ºC, with 1 min immersion in each, for 2000 cycles. The results for the FS and FM tests showed that the values for these two properties decreased as a function of depth and after the thermocycling for all the studied resins. Only TNBF resin showed no statistical significant differences in FM values after accelerated aging. For the hardness test, values also decreased as a function of depth, but increased after accelerated aging. SF resin was the only one that showed no statistical significant differences between hardness values before and after aging. CD, after thermal cycling, was the exclusive resin to show a bottom/top ratio above 80%. None of the bulk fill resins had a bottom/top ratio above 80% for hardness when evaluated at the maximum recommended thickness. Based on the results obtained, it can be stated that, when photoactivated at the maximum recommended thickness, only the conventional resin CD presented results consistent with the expected homogeneity in all the conditions of this study. However, for bulk fill resins, it can be observed that the studied properties, in general, suffered a significant decrease as a function of depth. For aging, the hardness, unlike the other parameters, showed a tendency to increase.
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Books on the topic "Bulk Modulus"

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Jacobson, Bo O. A model for the influence of pressure on the bulk modulus and the influence of temperature on the solidification pressure for liquid lubricants. [Cleveland, Ohio: National Aeronautics and Space Administration, Lewis Research Center, 1986.

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Stewart, M. Bulk and shear moduli of near-surface geologic units near the San Andreas fault at Parkfield, California. [Menlo Park, CA]: U.S. Geological Survey, 1993.

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Escudier, Marcel. Fluids and fluid properties. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198719878.003.0002.

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In this chapter it is shown that the differences between solids, liquids, and gases have to be explained at the level of the molecular structure. The continuum hypothesis makes it possible to characterise any fluid and ultimately analyse its response to pressure difference Δ‎p and shear stress τ‎ through macroscopic physical properties, dependent only upon absolute temperature T and pressure p, which can be defined at any point in a fluid. The most important of these physical properties are density ρ‎ and viscosity μ‎, while some problems are also influenced by compressibility, vapour pressure pV, and surface tension σ‎. It is also shown that the bulk modulus of elasticity Ks is a measure of fluid compressibility which determines the speed at which sound propagates through a fluid. The perfect-gas law is introduced and an equation derived for the soundspeed c.
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Buck Rogers: Comic Modules (Tsr Comic Modules, No 9). TSR Hobbies, 1991.

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Dixon, Buzz, and Chuck Wojtkiewicz. Buck Rogers/Comic Modules (Tsr Comic Modules, No. 9). TSR, 1991.

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Buck Rogers/Comic Modules (Tsr Comic Modules, No 10). Wizards of the Coast, 1991.

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Buck Rogers/Comic Modules (Tsr Comic Modules, No 10). TSR Hobbies, 1991.

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Tracy, William. Inner Worlds (Buck Rogers RPG module XXVCR3). Wizards of the Coast, 1991.

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Henson, Dale "Slade." Deimos Mandate (Buck Rogers RPG module XXVCA3). TSR Hobbies, 1991.

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Nesmith, Bruce. Sargasso of Space (Buck Rogers RPG module XXVCS2). Wizards of the Coast, 1991.

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Book chapters on the topic "Bulk Modulus"

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Keaton, Jeffrey R. "Bulk modulus." In Selective Neck Dissection for Oral Cancer, 1–2. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-12127-7_38-1.

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Gooch, Jan W. "Bulk Modulus." In Encyclopedic Dictionary of Polymers, 98. New York, NY: Springer New York, 2011. http://dx.doi.org/10.1007/978-1-4419-6247-8_1668.

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Keaton, Jeffrey R. "Bulk Modulus." In Encyclopedia of Earth Sciences Series, 96. Cham: Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-73568-9_38.

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Strauch, D. "BN: Young's modulus, bulk modulus." In New Data and Updates for IV-IV, III-V, II-VI and I-VII Compounds, their Mixed Crystals and Diluted Magnetic Semiconductors, 236–40. Berlin, Heidelberg: Springer Berlin Heidelberg, 2011. http://dx.doi.org/10.1007/978-3-642-14148-5_131.

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Hönerlage, B. "CuBr: bulk modulus." In New Data and Updates for I-VII, III-V, III-VI and IV-VI Compounds, 115. Berlin, Heidelberg: Springer Berlin Heidelberg, 2008. http://dx.doi.org/10.1007/978-3-540-48529-2_28.

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Hönerlage, B. "CuCl: bulk modulus." In New Data and Updates for I-VII, III-V, III-VI and IV-VI Compounds, 138. Berlin, Heidelberg: Springer Berlin Heidelberg, 2008. http://dx.doi.org/10.1007/978-3-540-48529-2_43.

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Hönerlage, B. "CuI: bulk modulus." In New Data and Updates for I-VII, III-V, III-VI and IV-VI Compounds, 156. Berlin, Heidelberg: Springer Berlin Heidelberg, 2008. http://dx.doi.org/10.1007/978-3-540-48529-2_56.

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Strauch, D. "GaAs: bulk modulus." In New Data and Updates for IV-IV, III-V, II-VI and I-VII Compounds, their Mixed Crystals and Diluted Magnetic Semiconductors, 183–86. Berlin, Heidelberg: Springer Berlin Heidelberg, 2011. http://dx.doi.org/10.1007/978-3-642-14148-5_107.

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Strauch, D. "BP: bulk modulus." In New Data and Updates for IV-IV, III-V, II-VI and I-VII Compounds, their Mixed Crystals and Diluted Magnetic Semiconductors, 258. Berlin, Heidelberg: Springer Berlin Heidelberg, 2011. http://dx.doi.org/10.1007/978-3-642-14148-5_139.

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Hönerlage, B. "CuBr: bulk modulus." In New Data and Updates for IV-IV, III-V, II-VI and I-VII Compounds, their Mixed Crystals and Diluted Magnetic Semiconductors, 279. Berlin, Heidelberg: Springer Berlin Heidelberg, 2011. http://dx.doi.org/10.1007/978-3-642-14148-5_153.

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Conference papers on the topic "Bulk Modulus"

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Gor, Gennady Y. "Bulk Modulus of Not-So-Bulk Fluid." In Sixth Biot Conference on Poromechanics. Reston, VA: American Society of Civil Engineers, 2017. http://dx.doi.org/10.1061/9780784480779.057.

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Lu, Yao, Hongxiang Zhang, Yuan Jiang, Hao Zhang, Wei Pang, and Menglun Zhang. "Bulk modulus measurement of microfluidics by longitudinal bulk acoustic wave sensors." In 2018 IEEE Micro Electro Mechanical Systems (MEMS). IEEE, 2018. http://dx.doi.org/10.1109/memsys.2018.8346690.

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Hasanov, Azar, Manika Prasad, and Michael Batzle. "Fluid and rock bulk viscosity and modulus." In SEG Technical Program Expanded Abstracts 2016. Society of Exploration Geophysicists, 2016. http://dx.doi.org/10.1190/segam2016-13973901.1.

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Higginbotham, Joseph H., Morgan P. Brown, and Oscar Ramirez. "Self consistent AVA determination of density, bulk modulus, and shear modulus reflectivity." In SEG Technical Program Expanded Abstracts 2010. Society of Exploration Geophysicists, 2010. http://dx.doi.org/10.1190/1.3513817.

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Liu, Changcheng, Deva Ghosh, Ahmed Mohamed Ahmed Salim, and Weng Sum Chow. "Fluid Discrimination Using Bulk Modulus and Neural Network." In International Petroleum Technology Conference. International Petroleum Technology Conference, 2019. http://dx.doi.org/10.2523/iptc-19317-ms.

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Sun*, Ruiying, Xingyao Yin, Baoli Wang, and Guangzhi Zhang. "Direct stochastic seismic inversion of fluid bulk modulus." In SEG Technical Program Expanded Abstracts 2014. Society of Exploration Geophysicists, 2014. http://dx.doi.org/10.1190/segam2014-0356.1.

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Balasubramanian, Karthik, Christopher Niezrecki, and John K. Schueller. "Piezoelectric-based fluid bulk modulus and diagnostic sensor." In Smart Structures and Materials, edited by Daniele Inaudi and Eric Udd. SPIE, 2003. http://dx.doi.org/10.1117/12.484241.

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Rachford, Henry H., and Andrew Wike. "How Bulk Modulus Errors Can Affect Leak Detection." In 1996 1st International Pipeline Conference. American Society of Mechanical Engineers, 1996. http://dx.doi.org/10.1115/ipc1996-1919.

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Liquid pipeline operators look to leak detection systems to provide continuous surveillance of their pipelines across a wide range of operating conditions; this is particularly the case for batch pipelines. Operators frequently anticipate that on-line transient modeling systems can satisfy this requirement, which they can, but have little exposure to the on-line measurement data requirements of such systems. There can be a mistaken focus on improving the quality of the real-time data normally available to facilitate pipeline operations, without due regard to providing the measurement data that the model needs. Pipeline operators are normally not concerned with a detailed characterization of fluid properties, other than in the most general sense regarding the susceptibility of adjacent fluids to mix at their interface. This paper illustrates how the lack of reliable fluid property data (specifically, bulk modulus data) can substantially impede the effectiveness of a transient model charged with the task of leak detection.
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Zhang, Xi, Yao Lu, Menglun Zhang, Hongxiang Zhang, Qingrui Yang, and Wei Pang. "A Microtas for Liquid Sample Bulk Modulus Screening." In 2019 20th International Conference on Solid-State Sensors, Actuators and Microsystems & Eurosensors XXXIII (TRANSDUCERS & EUROSENSORS XXXIII). IEEE, 2019. http://dx.doi.org/10.1109/transducers.2019.8808262.

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10

Patel, M. D., K. M. B. Jansen, L. J. Ernst, J. Zhou, and C. Bohm. "Study of Time and Temperature Dependency of Bulk Modulus for Molding Compound by Transient Bulk Creep Experiments." In ASME 2007 International Mechanical Engineering Congress and Exposition. ASMEDC, 2007. http://dx.doi.org/10.1115/imece2007-42852.

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Transient bulk creep experiments were performed to investigate the time and temperature dependency of the bulk modulus for epoxy molding compound. These, so called pressure jump volume relaxation experiments were done by applying positive and negative pressure jumps followed by a holding period at those pressure levels and the whole set of experiment was repeated at different temperatures. The observations are in the pressure range of 10 to 50 MPa and temperature range of 50 to 150° C. For negative pressure jumps (or expansion experiments) the bulk modulus was found to be almost independent of time. For positive pressure jumps (or compression experiments) time dependent volume decreases very slow. Compared to time and pressure, temperature dependency was of highest influence. A mathematical model has been proposed for the observed temperature and pressure dependency of the bulk modulus.
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Reports on the topic "Bulk Modulus"

1

Hutzler, Scott A. Isentropic Bulk Modulus: Development of a Federal Test Method. Fort Belvoir, VA: Defense Technical Information Center, January 2016. http://dx.doi.org/10.21236/ad1007328.

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Scheidler, Michael J. Formulas for the Pressure and Bulk Modulus in Uniaxial Strain. Fort Belvoir, VA: Defense Technical Information Center, February 1996. http://dx.doi.org/10.21236/ada304036.

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Hutzler, Scott A., Eric Sattler, Patsy Muzzell, and Nick C. Johnson. Development of a Test Rig for Measuring Isentropic Bulk Modulus. Fort Belvoir, VA: Defense Technical Information Center, January 2013. http://dx.doi.org/10.21236/ada589020.

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Pisani, William, Dane Wedgeworth, Michael Roth, John Newman, and Manoj Shukla. Exploration of two polymer nanocomposite structure-property relationships facilitated by molecular dynamics simulation and multiscale modeling. Engineer Research and Development Center (U.S.), March 2023. http://dx.doi.org/10.21079/11681/46713.

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Polyamide 6 (PA6) is a semi-crystalline thermoplastic used in many engineering applications due to good strength, stiffness, mechanical damping, wear/abrasion resistance, and excellent performance-to-cost ratio. In this report, two structure-property relationships were explored. First, carbon nanotubes (CNT) and graphene (G) were used as reinforcement molecules in simulated and experimentally prepared PA6 matrices to improve the overall mechanical properties. Molecular dynamics (MD) simulations with INTERFACE and reactive INTERFACE force fields (IFF and IFF-R) were used to predict bulk and Young's moduli of amorphous PA6-CNT/G nanocomposites as a function of CNT/G loading. The predicted values of Young's modulus agree moderately well with the experimental values. Second, the effect of crystallinity and crystal form (α/γ) on mechanical properties of semi-crystalline PA6 was investigated via a multiscale simulation approach. The National Aeronautics and Space Administration, Glenn Research Center's micromechanics software was used to facilitate the multiscale modeling. The inputs to the multiscale model were the elastic moduli of amorphous PA6 as predicted via MD and calculated stiffness matrices from the literature of the PA6 α and γ crystal forms. The predicted Young's and shear moduli compared well with experiment.
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Adolf, D., C. Childress, and D. Hannum. Bulk and shear moduli of epoxy encapsulants. Office of Scientific and Technical Information (OSTI), August 1989. http://dx.doi.org/10.2172/5524601.

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6

Pullammanappallil, Pratap, Haim Kalman, and Jennifer Curtis. Investigation of particulate flow behavior in a continuous, high solids, leach-bed biogasification system. United States Department of Agriculture, January 2015. http://dx.doi.org/10.32747/2015.7600038.bard.

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Recent concerns regarding global warming and energy security have accelerated research and developmental efforts to produce biofuels from agricultural and forestry residues, and energy crops. Anaerobic digestion is a promising process for producing biogas-biofuel from biomass feedstocks. However, there is a need for new reactor designs and operating considerations to process fibrous biomass feedstocks. In this research project, the multiphase flow behavior of biomass particles was investigated. The objective was accomplished through both simulation and experimentation. The simulations included both particle-level and bulk flow simulations. Successful computational fluid dynamics (CFD) simulation of multiphase flow in the digester is dependent on the accuracy of constitutive models which describe (1) the particle phase stress due to particle interactions, (2) the particle phase dissipation due to inelastic interactions between particles and (3) the drag force between the fibres and the digester fluid. Discrete Element Method (DEM) simulations of Homogeneous Cooling Systems (HCS) were used to develop a particle phase dissipation rate model for non-spherical particle systems that was incorporated in a two-fluid CFDmultiphase flow model framework. Two types of frictionless, elongated particle models were compared in the HCS simulations: glued-sphere and true cylinder. A new model for drag for elongated fibres was developed which depends on Reynolds number, solids fraction, and fibre aspect ratio. Schulze shear test results could be used to calibrate particle-particle friction for DEM simulations. Several experimental measurements were taken for biomass particles like olive pulp, orange peels, wheat straw, semolina, and wheat grains. Using a compression tester, the breakage force, breakage energy, yield force, elastic stiffness and Young’s modulus were measured. Measurements were made in a shear tester to determine unconfined yield stress, major principal stress, effective angle of internal friction and internal friction angle. A liquid fludized bed system was used to determine critical velocity of fluidization for these materials. Transport measurements for pneumatic conveying were also assessed. Anaerobic digestion experiments were conducted using orange peel waste, olive pulp and wheat straw. Orange peel waste and olive pulp could be anaerobically digested to produce high methane yields. Wheat straw was not digestible. In a packed bed reactor, anaerobic digestion was not initiated above bulk densities of 100 kg/m³ for peel waste and 75 kg/m³ for olive pulp. Interestingly, after the digestion has been initiated and balanced methanogenesis established, the decomposing biomass could be packed to higher densities and successfully digested. These observations provided useful insights for high throughput reactor designs. Another outcome from this project was the development of low cost devices to measure methane content of biogas for off-line (US$37), field (US$50), and online (US$107) applications.
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Peter C. Kong. Modular Hybrid Plasma Reactor for Low Cost Bulk Production of Nanomaterials. Office of Scientific and Technical Information (OSTI), December 2011. http://dx.doi.org/10.2172/1036264.

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Ciezki, John G., and Robert W. Ashton. Analysis of a PWM Resonant Buck Chopper for Use as a Ship Service Converter Module. Fort Belvoir, VA: Defense Technical Information Center, January 1999. http://dx.doi.org/10.21236/ada361136.

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The bulk-store module for FASTBUS memory applications. Final technical report. Office of Scientific and Technical Information (OSTI), February 1996. http://dx.doi.org/10.2172/196551.

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