Relevant bibliographies by topics / Young´s modulus

Contents

  1. Journal articles
  2. Dissertations / Theses
  3. Book chapters
  4. Conference papers
  5. Reports

Academic literature on the topic 'Young´s modulus'

Author: Grafiati
Published: 4 June 2021
Last updated: 29 May 2022

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Journal articles on the topic "Young´s modulus"

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Perkalskis, Benjamin S., J. Reuben Freeman, and Alexander Suhov. "Examining Young s modulus for wood." European Journal of Physics 25, no. 2 (February 2, 2004): 323–29. http://dx.doi.org/10.1088/0143-0807/25/2/019.

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MA, Dejun. "Determination of Young?s modulus by nanoindentation." Science in China Series E 47, no. 4 (2004): 398. http://dx.doi.org/10.1360/03ye0590.

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Конаков, Aleksandr Konakov, Емельянов, Evgeniy Emelyanov, Ларионов, and Yuriy Larionov. "Young´s Modulus Determination for Case-Hardened Materials." NDT World 19, no. 4 (December 15, 2015): 57–60. http://dx.doi.org/10.12737/23511.

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The issue of strength analysis as well as foreknowledge of component and structure life is of interest at this time for new composite materials. New composite materials and alloys elastic response is often unknown, and standard methods for their determining can not be applied to, e.g. materials featuring surface gradient properties. Elasticity modulus method of examination is based on stepwise removal of part of the material from the rod sample surface or application of a coating onto the sample surface. Each step is accompanied by measurement of the sample lateral dimensions, and density. To determine Young´s modulus, resonance frequencies of the sample subjected to forced longitudinal vibrations are measured using an ultrasonic device. The device principle of operation is based on excitation and tracking of the sample forced mechanical oscillations close to its own frequencies, measurement of resonance peak parameters followed by calculations of the Young´s modulus. To induce and track the forced oscillations in the sample, use is made of piezoelectric transducers attached to damped acoustic transmission rods, while the sample is fixed between pointed rod ends. This arrangement makes it possible to examine also Young´s modulus temperature dependences. Young´s modulus measurement results for case-hardened hard alloy are provided. It is shown that Young´s modulus of surface layers is lower than that of the base material, which is explained by formation of new compounds in the surface layers owing to chemical and diffusion reactions between an alloying element and alloy components. The doped layer extends to 0.45 mm. The results obtained can be used for strength calculations of case-hardened materials, estimation of cohesive and adhesive strength of individual layers of coatings, structure and other physical and mechanical properties of materials.
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Mašlejová, Alica, Atila Drotár, Martin Černík, and Pavol Zubko. "Mechanical Properties of Build-Up Layers on Failed Ceramic Roller." Key Engineering Materials 784 (October 2018): 103–7. http://dx.doi.org/10.4028/www.scientific.net/kem.784.103.

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The paper describes degradation process of ceramic rollers. Rollers behavior under mechanical and thermal load was evaluated using available methods like XRD, instrumented hardness measurement and compressive strength. The influence of residual stresses was also discussed. The first phase during the degradation crystalize from amorphous silica tridymite, cristobalite and quartz, then due to the contact and pressure of the steel strip to the surface roller iron diffuses and forms fayalite. Measured values of compression strength of roller of 55-61 MPa agree with producer documentation declared minimal values. Hardness and Young´s modulus of buildup phases identified from surface into depth were determined. Wüstite was present up to 100 mm, with hardness 6±1 GPa, Young´s modulus 75±6 GPa, fayalite, cristobalite, up to 500 mm, with hardness 5.4±0.6 GPa, Young´s modulus 51±2 GPa, tridymite over 500 mm, with the hardness 7±4 GPa and Young´s modulus 58±25 GPa.
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Luo, Ning, Hanliang Liang, Tao Shen, and Weihao Yang. "Temperature dependence of young’s modulus of red sandstone." Thermal Science 23, no. 3 Part A (2019): 1599–606. http://dx.doi.org/10.2298/tsci180822229l.

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In the underground rock diagenetic process, or artificial excavation in rock engineering, it is possible to make experience in the high temperature. The temperature dependence of Young?s modulus of red sandstone was characterized by impulse excitation technology. It is shown that after heating-cooling cycle the Young?s modulus of red sandstone decreases down to about 90% from the room temperature up to 800?C of its initial value. The significant change of Young?s modulus with temperature is attributed to thermal-induced damages in red sandstone, including the rock composition variation, mass loss, mineral phase composition change, porosity increasing, grain trans-granular, micro-cracks penetrated and disruption.
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STEVENSON, RONALD W. W. "Young??s Modulus Measurements of Gas Permeable Contact Lens Materials." Optometry and Vision Science 68, no. 2 (February 1991): 142–45. http://dx.doi.org/10.1097/00006324-199102000-00010.

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Anderson, O., C. R. Ottermann, R. Kuschnereit, P. Hess, and K. Bange. "Density and Young’s modulus of thin TiO 2 films." Fresenius' Journal of Analytical Chemistry 358, no. 1-2 (May 21, 1997): 290–93. http://dx.doi.org/10.1007/s002160050409.

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Brožovský, Jiří, and Ámos Dufka. "Comparison of Dynamic Young's Modulus of Elasticity Values Measured by Ultrasonic Pulse and Resonance Methods." Advanced Materials Research 1100 (April 2015): 193–96. http://dx.doi.org/10.4028/www.scientific.net/amr.1100.193.

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Dynamic Young ́s modulus of elasticity can be determined by ultrasonic pulse method and resonance method. Because of the difference in the way of introducing tension into a test specimen, the values of modulus of elasticity differ. Dynamic Young ́s modulus of elasticity measured by ultrasonic pulse method is higher; the difference stated for concrete is 5 to 20%. It was found that the dynamic Young's modulus of elasticity of calcium silicate bricks and prisms measured by ultrasonic pulse method is on average higher by 9.5% than dynamic Young's modulus of elasticity measured by resonance method. If dynamic Young's modulus of elasticity is converted to static modulus of elasticity, this difference has to be taken into account by means of appropriate coefficient.
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Inaba, Seiji, Shinichi Todaka, Yoshio Ohta, and Kenji Morinaga. "Equation for Estimating the Young’s Modulus, Shear Modulus and Vickers Hardness of Aluminosilicate Glasses." Journal of the Japan Institute of Metals 64, no. 3 (2000): 177–83. http://dx.doi.org/10.2320/jinstmet1952.64.3_177.

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Rico, Alvaro, Miguel Angel Garrido, Alicia Salazar, Enrique Otero, and J. Rodríguez. "Hardness and Young´s Modulus Determination of Nanostructured Alumina-Titania Coatings." Materials Science Forum 587-588 (June 2008): 478–82. http://dx.doi.org/10.4028/www.scientific.net/msf.587-588.478.

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It has been generally accepted that a nanostructured material exhibits better properties than conventional ones. Nanostructured ceramic coatings fabricated by plasma spray have been developed for a wide variety of applications where a surface protection is required. Alumina - titania coatings are usually used as protective layers in many industrial applications requiring a high wear resistance during dry sliding contact. In this work, nanostructured and conventional Al2O3 – 13% TiO2 coatings deposited via atmospheric plasma spray were compared. Mechanical characterization was carried out using depth sensing indentation to determine hardness and Young´s modulus of the coatings. Size independent properties can be determined after considering geometrical factors such as tip rounding and indenter deformation. Nanostructured coatings show slightly better mechanical properties than conventional coatings.
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Dissertations / Theses on the topic "Young´s modulus"

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Yurkova, A. I., and A. V. Byakova. "Mechanical Properties of Nano- and Submicrocrystalline Iron Subjected to Severe Plastic Deformation by Friction." Thesis, Sumy State University, 2012. http://essuir.sumdu.edu.ua/handle/123456789/35149.

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By using nanoindentation technique relationship between microstructure and mechanical parameters such as nanohardness Hh, plasticity characteristic A, and Young’s modulus E were found to be dependent on the grain size of the -Fe subjected to severe plastic deformation by friction (SPDF) with argon atmosphere. Unlike fcc-metals in which the decreasing of grain size to 20 nm results in hardness growth accompanied by decreasing the plasticity, it was found the reverse effect in bcc-Fe, i.e. decreasing the grain size from 50 to 20 nm caused the decrease of hardness and increase of plasticity. Moreover, the decrease of Young’s modulus E with decreasing the grain size down to 20 nm was detected in nanoindentation experiments. When you are citing the document, use the following link http://essuir.sumdu.edu.ua/handle/123456789/35149
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Zhuravleva, Ksenia. "Porous ß-type Ti-Nb alloy for biomedical applications." Doctoral thesis, Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2014. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-147426.

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One of the most important factors for a successful performance of a load-bearing implant for hard tissue replacement is its mechanical compatibility with human bone. That implies that the stiffness should be close to that of a bone and the strength of the implant material must be high enough to bear the load applied under physiological conditions. The Young´s modulus of most of the commonly used biomedical alloys is larger than that of a human bone (around 100 GPa for cp Ti, 112 GPa for Ti-6Al-4V versus 10-30 GPa for cortical human bone). A stiffness reduction of Ti alloys can be achieved by two approaches: (i) selecting an alloy composition with low Young´s modulus i.e. a ß-type alloy and (ii) introducing a reasonable amount of porosity. The composition of Ti-40Nb was chosen for the present work, as it allows to stabilize a single ß-type phase with low Young´s modulus at room temperature. The samples were produced by a powder metallurgical approach. The Ti-40Nb alloy powder was obtained by ball-milling of elemental Ti and Nb powders. The influence of the milling parameters on the oxygen content in the milled powder was studied. Powders with a lowest oxygen content of 0.4 wt.-% had an almost single ß-type phase after heat treatment and quenching. Porous samples were produced by loose powder sintering, hot-pressing and sintering with NaCl as a space-holder. The influence of the different processing routes and different porosities on the mechanical properties of the alloy was studied. The samples produced by loose powder sintering had mechanical properties close to those of cortical human bone (Young´s modulus 20 GPa, compression strength 150 MPa) and the samples produced by loose sintering with space-holder materials had mechanical properties close to those of human spongy bone (Young´s modulus 0.2-2 GPa, compression strength 50 MPa). Porous Ti-40Nb samples were coated with bone-like hydroxyapatite by an electrochemical deposition method in order to improve the osseointegration of the samples with bone tissue. The experiments were carried out with samples produced by different routes and a correlation between the deposition parameters and the morphology of the hydroxyapatite needles was found.
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Eckert, Matthias Bastian. "Avaliação da influência da retração inicial no controlo da fissuração dos betões." Master's thesis, Universidade de Évora, 2013. http://hdl.handle.net/10174/10911.

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A fissuração em idade precoce reemergiu como um problema em betão/argamassa moderno, com o uso de materiais com altas resistências mecânicas. Este tipo de fissuração resulta da retração do betão, que quando associada a restrições internas e externas cria tensões, aumentando a suscetibilidade à fissuração. Distinguem-se vários tipos de retração: plástica, química, autogénea térmica e por secagem, que são influenciadas por fatores ambientais e fatores intrínsecos ao material. A fissuração permite o ingresso de agentes atmosféricos que conduzem a uma deterioração pré-matura do betão, cuja mitigação constitui a motivação desta tese de mestrado. O objetivo do trabalho experimental consiste em avaliar a influência dos tempos de presa na atuação de adições expansivas em betão autocompactável. Espera-se que diferentes estados de rigidez microestrutural modifiquem o efeito de expansão. Para esse fim foram executados ensaios de: trabalhabilidade, tempos de presa, resistência à compressão e tração, módulo de elasticidade, retração química e total, perda de peso e por último, o ensaio de anel. Os resultados do trabalho experimental mostram que o aumento dos tempos de presa prolongam a fase expansiva, o que levou à diminuição de retração e fissuração a médio prazo, mas a longo prazo não se verificou qualquer alteração da retração. Conclui-se que este estudo constitui uma informação importante para avaliar o efeito de retardadores de presa nas propriedades avaliadas e que a sua combinação com expansivos trás algumas melhorias na fissuração; ### ABSTRACT: Evaluation of the Influence of Early Age Shrinkage on the Control of Concrete Cracking The early age cracking reemerged as a problem in modern concrete/mortar, with the use of high strength materials. This type of cracking results from the concrete shrinkage, when it is associated to selfand external-restraint it creates tensions, increasing the cracking susceptibility. There are discriminated several types of shrinkage: plastic, chemical, autogenous, thermal and drying, which are influenced by environmental factors and inherent factors to the material. The cracking allows the ingress of atmospheric agents that lead to pre-mature deterioration of concrete, whose mitigation is the motivation of this master thesis. The objective of the experimental work consists in evaluate the influence of setting-time on the performance of expansive admixtures in self-compacting concrete. It is expected that different states of microstructural stiffness modifies the expansion effect. For this purpose were executed tests for: workability; setting time; compressive and tensile-strength; Young's modulus; chemical and overall shrinkage; mass loss and finally the Ring Test. The results of the experimental work show that the increase of setting time extends the expansive phase, that leaves to an decrease of shrinkage and cracking at medium term, but at long term there was no change of the shrinkage. It can be concluded that this study constitutes an important information to evaluate the effect of retarder in the evaluated properties and that it's combination with expansive admixtures brings some improvements in cracking.
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Sivakumar, Lalitha. "Effect of DDR2 on Rheology of Collagen type I Fibers." The Ohio State University, 2009. http://rave.ohiolink.edu/etdc/view?acc_num=osu1243537065.

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Harris, James Patrick. "The Glia-Neuronal Response to Cortical Electrodes: Interactions with Substrate Stiffness and Electrophysiology." Case Western Reserve University School of Graduate Studies / OhioLINK, 2011. http://rave.ohiolink.edu/etdc/view?acc_num=case1320950439.

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Liu, Jia-hua, and 劉嘉華. "Measurement of Young''s modulus of Nickel-base superalloys." Thesis, 2009. http://ndltd.ncl.edu.tw/handle/99790891122023167029.

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碩士
義守大學
機械與自動化工程學系碩士班
97
There were many kinds of measurement of Young''s modulus of superalloys.In the theme, there would use three different ways to measure the Young''s Modulus﹒The tensile test、ultrasonic test、laser ultrasonic test. Much of the effort is focused on experimental setup and measurement﹐as well as on signal waveform processing﹒For the experimental part﹐after the tensile test﹐the data rate of curve could calculate the Young''s modulus﹒In the ultrasonic test﹐I used the Pulse Echo Method to calculate the Young''s modulus﹒In the laser ultrasonic test﹐I used the Nd:YAG laser to measure the Young''s modulus﹒Finally, calculated the young''s modulus by the formula and compared it with the tensile test﹒The ultrasonic test could obtain the same result with the tensile test﹒Although the ultrasonic test the error was slightly big, approximately 1.1%, The proof selected the different gauging way, its anticipated young''s modulus error is not big.
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Chang, Hsiu-Chen, and 張秀珍. "Determination of Dynamic Young''s Modulus of Concrete by Various Inspection." Thesis, 1997. http://ndltd.ncl.edu.tw/handle/94597959587415669428.

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碩士
國立交通大學
土木工程學系研究所
85
Three different approaches were used in this thesis to measure the dynamic You ng*s modulus of the concrete, both in the plate and cylinders drilled from the plate .Including the ultrasonic pulse velocity method, the impact -echo metho d, and test of stress-strain curve,both normal strength concrete plate and hig h-performance concrete plate were test by these methods. These dynamic Young* s modulus were used to calculate vibration frequency of plate by SAP90 and com pare with the result from the modal testing.The difference of these approaches with modal testing have a larger value of 6.2% from stress-strain curve test and a smaller value of 1.7% from the impact each method . The variations from impact-echo method are very small . All of these results shows Impact-echo met hod can measure dynamic Young*s modulus of concrete very well.
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Yu, Jia-Hong, and 游家宏. "Young''s Modulus and Interlaminar Fracture Toughness of Thin Film on Silicon wafer." Thesis, 2006. http://ndltd.ncl.edu.tw/handle/91879932020590209542.

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碩士
國立雲林科技大學
機械工程系碩士班
94
This study fabricated micro-cantilever beam of SU-8 photoresrist on the mirror surface or the rough surface of silicon wafer, and the techniques of MEMS fabrication are involved. In addition, bulk micro-machining techniques were applied to this experiment, and the etching solution is mixed with TMAH and IPA was used. The micro-cantilever beam of thin film is tested by a MTS Tytron 250 microforce testing machine with a probe and CCD camera to observe crack growth condition by CCD camera. By adopting the theory of mechanics of materials, the Young’s modulus of the thin film can be determined. Also by adopting the theory of fracture mechanics, the mode I interlaminar fracture toughness between the thin film and the substrate can be measured. When the beam was fabricated on the mirror surface, the measured Young’s modulus is about 1.6~3.8GPa. When it was fabricated on the rough surface, the measured Young’s modulus is about 1.5~3.22GPa. The results indicate that the Young’s modulus of SU-8 photoresist is increased with the increasing of the width of the beams, but no significant effect is seen with their lengths. The final result of the measured Young’s modulus of SU-8 photoresist is about 1.5~3.8GPa. In the study of interlaminar fracture toughness (GIC), Gilman theory and Berry theory (compliance calibration method) are used. The GIC on silicon mirror surface was about 17~43 J/m2. The GIC on silicon rough surface was about 11~30 J/m2. The results indicated that the GIC on silicon mirror surface is larger than that of rough surface. Furthermore, the GIC is increased with the increasing of the width of the SU-8 beam, but the crack length of the SU-8 beam has no effect on the GIC.
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Wu, Ting-An, and 顧庭安. "Mechanical Properties of Fe50Pd50 Thin Films - Young's Modulus, Hardnessand Film Stress." Thesis, 2010. http://ndltd.ncl.edu.tw/handle/47761715747251274599.

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碩士
國立臺灣科技大學
機械工程系
98
Abstract In this research, single layer FePd thin film deposited onto Corning 0211 glass substrate. In this way, it can enhance reflection of the laser light. Right after sample sputter FePd film, it undergoes to PSC stress analyzed instrument to measure the curvature of the sample. UMIS (Ultra Micro Indentation System) instrument measured the film’s Young’s modulus (Ef) and hardness (Hf). Auger electron nanoscope analyzed the depth profile of periodic elements. Finally, TEM was used to observe the film’s plane-view of the atomic image. Experimental results show that, changing the parameters will affect the Young's modulus and hardness. And the variations of the thickness, generally, we define the film thickness is less than 50 nm for the island growth. Film thickness of 100 nm or more, the film has to grow plane. Substrate effect will not affect the Young's modulus, therefore, we can know the mechanical properties of thin films of pure parameters. However, the hardness of the part, the measurements do not change with the increase of film thickness. The values are between 6 ~ 9 Gpa. Increasing argon partial pressure, with the argon partial pressure increases Young's modulus will decrease significantly. Suggesting the formation of the reasons for this phenomenon, mainly due to the pinning effect caused. From nano auger depth profile, it showed the oxygen percentage higher than other place in 1% from film surface. In the experiment, with the depth to the specimen, FePd content increases, oxygen content decreased. The best experimental value was found when the heat treatment temperature of 450oC, the partial pressure of argon 4.2 m Torr, the measure of the film stress is close to 0 Gpa.
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Lee, Cherng-Shing, and 李澄興. "Application of Artificial Neural Network to Predicting the Strength and Young''s Modulus of Concrete." Thesis, 1997. http://ndltd.ncl.edu.tw/handle/57666172711037073247.

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碩士
國立臺灣大學
土木工程學系
85
The objective of this research is to use an artificial neural network . (ANN) for predicting the strength and Young''s modulus of concrete. This research contains four cases: (1) the prediction of the compressive strength of the concrete in the early age,(2) the prediction of the compressive strength of the concrete at the age of 28th day using the data in the early age,(3) prediction of the Young''s modulus of concrete, and (4) the prediction of the compressive strength of the concrete containing sea sand This work shows that back propagation neural networks can provide an effective way to have better prediction on concrete strength than those obtained by empirical equations.
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Book chapters on the topic "Young´s modulus"

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"Young('s) modulus (of elasticity)." In Dictionary Geotechnical Engineering/Wörterbuch GeoTechnik, 1546. Berlin, Heidelberg: Springer Berlin Heidelberg, 2014. http://dx.doi.org/10.1007/978-3-642-41714-6_250067.

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Conference papers on the topic "Young´s modulus"

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Canady, Wyatt Jackson. "A Method for Full-Range Young's Modulus Correction." In North American Unconventional Gas Conference and Exhibition. Society of Petroleum Engineers, 2011. http://dx.doi.org/10.2118/143604-ms.

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Britt, Larry K., Michael B. Smith, Ziad Haddad, Jennifer Reese, and Patrick Kelly. "Rotary Sidewall Cores- A Cost Effective Means of Determining Young's Modulus." In SPE Annual Technical Conference and Exhibition. Society of Petroleum Engineers, 2004. http://dx.doi.org/10.2118/90861-ms.

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Xia Xiao and Xue-Yi You. "Determining of Young’s modulus of multi-layered structure by SAWs method." In 2008 International Conference on Microwave and Millimeter Wave Technology (ICMMT). IEEE, 2008. http://dx.doi.org/10.1109/icmmt.2008.4540476.

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Lei-hao, Li, Wen Xiao-tao, Liu Song-ming, Yang Ji-xin, and He Jian. "Application of Approximate Equations of Young 's Modulus and Poisson' s Ratio of Two Reflection Coefficients in Prestack Inversion." In International Geophysical Conference, Beijing, China, 24-27 April 2018. Society of Exploration Geophysicists and Chinese Petroleum Society, 2018. http://dx.doi.org/10.1190/igc2018-277.

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Yan Ding, Kim N. Tran, John A. Gear, David Mainwaring, and Pandiyan Murugaraj. "The influence of interphase between nanoparticles and matrix on Young’s Modulus of nanocomposites." In 2008 International Conference on Nanoscience and Nanotechnology (ICONN). IEEE, 2008. http://dx.doi.org/10.1109/iconn.2008.4639237.

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Tokumine, T., K. Miyazawa, and T. Kizuka. "Dependency of Young's modulus on diameter in Crystalline C70 Nanotubes." In 2010 International Conference on Solid State Devices and Materials. The Japan Society of Applied Physics, 2010. http://dx.doi.org/10.7567/ssdm.2010.p-13-6.

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Franquet, Javier A., and Michael J. Economides. "Effect of Stress and Stress Path on Young's Modulus and Poisson Ratio of Unconsolidated Rocks: A New Idea for Hydraulic Fracturing." In Latin American and Caribbean Petroleum Engineering Conference. Society of Petroleum Engineers, 1999. http://dx.doi.org/10.2118/54012-ms.

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Reza Sanei, Seyed Hamid, Hanna Drozynski, and Dakota Hetrick. "Effect of Strain Rate on Tensile Properties of Injection Molded Multiwall Carbon Nanotube Reinforced PA 6/6 Nanocomposites." In ASME 2020 International Mechanical Engineering Congress and Exposition. American Society of Mechanical Engineers, 2020. http://dx.doi.org/10.1115/imece2020-23049.

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Abstract The mechanical properties of polymers highly depend on the loading rate, however, the effect of loading/strain rate with the addition of Carbon Nanotube is not well understood. In this study, the effect of Carbon Nanotube (CNT) content on the rate dependence of polymers was studied. Injection molded mini-tensile samples with CNT content ranging from 0 to 15wt% at strain rates of .0006, .0013, .0019 and .0025 s−1 were tested. It was found that as strain rate increased, the ultimate strength and Young s Modulus of the tensile specimens increased. It was also shown that addition of CNT will lower the chain mobility of polymer and lower the polymer dependence of properties to strain rates.
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Yamagiwa, H., S. Ito, T. Namazu, T. Takeuchi, K. Murakami, Y. Kawashimo, and T. Takano. "Optimum Design of MEMS Resonator Array to Measure the Young's Modulus of Nano-Scale Thin Films for the Reliability of Semiconductor Devices." In 2011 International Conference on Solid State Devices and Materials. The Japan Society of Applied Physics, 2011. http://dx.doi.org/10.7567/ssdm.2011.p-2-4.

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Sandu, Laurentiu I., Felicia Stan, and Catalin Fetecau. "Correlation Between Mechanical Properties in Standard Test Specimens and Injection Molded Thin-Wall Parts." In ASME 2013 International Manufacturing Science and Engineering Conference collocated with the 41st North American Manufacturing Research Conference. American Society of Mechanical Engineers, 2013. http://dx.doi.org/10.1115/msec2013-1032.

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In this paper, we investigated the effect of injection molding parameters on the mechanical properties of thin-wall injection molded parts. A four-factor (melt temperature, mold temperature, injection speed and packing pressure) and three-level fractional experimental design was performed to investigate the influence of each factor on the mechanical properties and determine the optimal process conditions that maximize the mechanical properties of the part using the signal-to-noise (S/N) ratio response. The mechanical properties (e.g., elastic modulus, yield strength and strain at break) were measured by tensile tests at room temperature, at a crosshead speed of 5 mm/min, and compared with those of the injection-molded specimens. The experimental results showed that the tensile properties were highly dependent on the injection molding parameters, regardless of the type of the specimens. The values of Young modulus and yield strength of the injection-molded specimens were lower than those of the injection-molded parts, while the elongation at break was considerably lower for the injection-molded parts. The optimal process conditions were strongly dependent on the measured performance quantities (elastic modulus, yield strength and strain at break).
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Reports on the topic "Young´s modulus"

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Price, R. H., R. J. III Martin, and R. W. Haupt. The effect of frequency on Young`s modulus and seismic wave attenuation. Office of Scientific and Technical Information (OSTI), July 1994. http://dx.doi.org/10.2172/145360.

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