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Relevant bibliographies by topics / MAX 3ds 7.0

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Academic literature on the topic 'MAX 3ds 7.0'

Author: Grafiati

Published: 4 June 2021

Last updated: 25 January 2023

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Journal articles on the topic "MAX 3ds 7.0"

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Ashari, Mohammad Ibrahim, and Ahmad Faisol. "Desain Game Karakter 3d Tokoh Madura dengan Actionscript Macromedia." Prosiding SENIATI 6, no. 1 (2022): 187–92. http://dx.doi.org/10.36040/seniati.v6i1.4947.

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Desain karakter sangat penting dalam menciptakan rasa ketertarikan akan jalan cerita yang ada dalam sebuah game. Flash game yaitu game 2D yang dibuat dengan menggunakan software Macromedia Flash pada umumnya menampilkan desain karakter 2D yang tidak dibuat dengan software pengolah grafik 3D. Sehingga desain karakter yang digunakan umumnya tampak flat karena tidak memiliki efek-efek seperti pada desain karakter game 3D. Game action “ putra sakera ” adalah game action 2D yang dibuat dengan menggunakan software Macromedia Flash dan menggunakan desain karakter 3D yang dibuat dengan software pengolah grafik tiga dimensi 3Ds Max 7. Desain karakter tiga dimensi ( 3D ) yang terdapat di dalam game “ putra sakera “ dan dibuat dengan aplikasi pendukung 3Ds Max 7 dapat berjalan dengan baik ketika dikompilasi ke dalam Macromedia Flash berupa animasi gerakan karakter dalam bentuk png sequence dengan teknik frame by frame animation. Dengan menggunakan desain karakter 3D yang unik akan menjadi daya tarik tersendiri dalam game flash” putra sakera ” ini sehingga membedakan dengan game-game flash pada umumnya yang hanya menampilkan desain karakter dua dimensi ( 2D ).

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Vasilev, Vadim A., and Peter Yu Bugakov. "DEVELOPMENT OF THE MODEL OF NOVOSIBIRSK AKADEMGORODOK SCIENCE AND TECHNOLOGY PARK USING 3DS MAX AND UNITY TOOLS." Interexpo GEO-Siberia 7, no. 1 (2020): 65–70. http://dx.doi.org/10.33764/2618-981x-2020-7-1-65-70.

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The aim of tht work is to develop an interactive three-dimensional model of the territory of the Scientific and Technical Park of Novosibirsk Academgorodok. 3D objects were modeled in Autodesc 3ds Max; virtual space was implemented in Unity. In the process, textures and virtual materials for the implementation of photorealistic visualization of a three-dimensional scene were prepared. The model is compiled by Unity and is ready for use on desktop computers or laptops running Windows operating system. The software obtained can be used for virtual tours around the territory of the Scientific and Technical Park of Novosibirsk Academgorodok.

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Grishchenkova, E. N., and M. G. Mustafin. "SPATIAL VISUALIZATION OF DISPLACEMENT USING 3DSMAX APPARATUS." MINING INFORMATIONAL AND ANALYTICAL BULLETIN 9 (July 20, 2017): 36–41. http://dx.doi.org/10.25018/0236-1493-2017-9-0-36-41.

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Zhang, Qiqiang, Yanchun Zhou, Xingyuan San, et al. "Zr2SeB and Hf2SeB: Two new MAB phase compounds with the Cr2AlC-type MAX phase (211 phase) crystal structures." Journal of Advanced Ceramics 11, no. 11 (2022): 1764–76. http://dx.doi.org/10.1007/s40145-022-0646-7.

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AbstractThe ternary or quaternary layered compounds called MAB phases are frequently mentioned recently together with the well-known MAX phases. However, MAB phases are generally referred to layered transition metal borides, while MAX phases are layered transition metal carbides and nitrides with different types of crystal structure although they share the common nano-laminated structure characteristics. In order to prove that MAB phases can share the same type of crystal structure with MAX phases and extend the composition window of MAX phases from carbides and nitrides to borides, two new MAB phase compounds Zr2SeB and Hf2SeB with the Cr2AlC-type MAX phase (211 phase) crystal structure were discovered by a combination of first-principles calculations and experimental verification in this work. First-principles calculations predicted the stability and lattice parameters of the two new MAB phase compounds Zr2SeB and Hf2SeB. Then they were successfully synthesized by using a thermal explosion method in a spark plasma sintering (SPS) furnace. The crystal structures of Zr2SeB and Hf2SeB were determined by a combination of the X-ray diffraction (XRD), scanning electron microscopy (SEM), and high-resolution transmission electron microscopy (HRTEM). The lattice parameters of Zr2SeB and Hf2SeB are a = 3.64398 Å, c = 12.63223 Å and a = 3.52280 Å, c = 12.47804 Å, respectively. And the atomic positions are M at 4f (1/3, 2/3, 0.60288 [Zr] or 0.59889 [Hf]), Se at 2c (1/3, 2/3, 1/4), and B at 2a (0, 0, 0). And the atomic stacking sequences follow those of the Cr2AlC-type MAX phases. This work opens up the composition window for the MAB phases and MAX phases and will trigger the interests of material scientists and physicists to explore new compounds and properties in this new family of materials.

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Charness, Neil, and Yigal Gerchak. "Participation Rates and Maximal Performance: A Log-Linear Explanation for Group Differences, Such as Russian and Male Dominance in Chess." Psychological Science 7, no. 1 (1996): 46–51. http://dx.doi.org/10.1111/j.1467-9280.1996.tb00665.x.

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Can the superiority of some countries and groups at certain activities be explained solely by the relative sizes of the participating populations? We focus on the expected highest achievement, max, as a function of the participating group's size For several relevant statistical distributions, max can be shown to be approximately log-linear in sample size, with a slope of about 0 7 SD units We use this relation (max is log-linear ~0 7 MILL7) to examine differences in performance in chess by men and women and by different countries The expected differences under MILL7 are very close to the observed differences We also examine the implications of MILL7 for the interpretation of other group differences and discuss its limitations

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Chang, H. W., S. T. Huang, I. W. Chen, C. W. Chang, and W. C. Chang. "PHASE EVOLUTION AND MAGNETIC PROPERTIES OF TbCu7-TYPE (Sm, Pr)Co7-xHfxMy (x = 0-0.5; y = 0-0.14) RIBBONS." International Journal of Modern Physics B 23, no. 06n07 (2009): 1663–69. http://dx.doi.org/10.1142/s0217979209061433.

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The effects of Hf substitution and C content on the magnetic properties, phase evolution, and microstructure of melt spun ( Sm , Pr ) Co 7- x Hf x C y ( x = 0-0.5; y = 0-0.14) ribbons have been studied. A proper Hf substitution is helpful not only in stabilizing 1:7 phase but also in enhancing its magnetic anisotropy field. As a result, magnetic properties of B r = 6.4 kG , i H c = 7.3 kOe and ( BH ) max = 8.7 MGOe for SmCo 6.9 Hf 0.1 ribbons are obtained. Besides, a small amount of C addition in the ribbons could slightly modify phase constitution and effectively refine their microstructure to strengthen the exchange coupling effect between magnetic grains. Furthermore, a slight Pr substitution for Sm may further increase the magnetization and the magnetic properties of the ribbons. The optimal magnetic properties of B r = 7.1 kG , i H c = 8.5 kOe and ( BH ) max = 11.2 MGOe could be achieved for the directly quenched Sm 0.8 Pr 0.2 Co 6.9 Hf 0.1 C 0.12 ribbons.

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7

Krausz, Ronald F., George Kapusta, and Joseph L. Matthews. "Soybean (Glycine max) Tolerance to 2,4-D Ester Applied Preplant." Weed Technology 7, no. 4 (1993): 906–10. http://dx.doi.org/10.1017/s0890037x00037970.

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Field studies were conducted in 1991 and 1992 to determine potential soybean injury due to 2,4-D ester at 560, 1120, and 1680 g ai/ha applied 0, 7, and 14 d before planting (DBP). Delayed emergence and increased injury of soybean were observed as 2,4-D rate increased and interval between application and planting decreased. Delay in emergence ranged from 0 to 67% and 0 to 50% in 1991 and 1992, respectively. Injury at 15 days after planting (DAP) combined over years ranged from 0 to 61%. Minimal (0 to 8%) delay in emergence and minimal (0 to 5%) injury at 15, 30, 45, and 60 DAP occurred when 2,4-D at 560 or 1120 g/ha was applied 7 or 14 DBP. No significant yield reduction occurred due to 2,4-D rate, application timing, or their interaction.

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Watanabe, M., M. Homma, and T. Masumoto. "Perpendicularly magnetized Fe-Pt (0 0 1) thin films with (B · H)max exceeding 30 MG Oe." Journal of Magnetism and Magnetic Materials 177-181 (January 1998): 1231–32. http://dx.doi.org/10.1016/s0304-8853(97)00828-7.

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Steinerberger, Stefan. "An Endpoint Alexandrov Bakelman Pucci Estimate in the Plane." Canadian Mathematical Bulletin 62, no. 3 (2019): 643–51. http://dx.doi.org/10.4153/cmb-2018-037-7.

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AbstractThe classical Alexandrov–Bakelman–Pucci estimate for the Laplacian states $$\begin{eqnarray}\max _{x\in \unicode[STIX]{x03A9}}|u(x)|\leqslant \max _{x\in \unicode[STIX]{x2202}\unicode[STIX]{x03A9}}|u(x)|+c_{s,n}\text{diam}(\unicode[STIX]{x03A9})^{2-\frac{n}{s}}\Vert \unicode[STIX]{x0394}u\Vert _{L^{s}(\unicode[STIX]{x03A9})},\end{eqnarray}$$ where $\unicode[STIX]{x03A9}\subset \mathbb{R}^{n}$, $u\in C^{2}(\unicode[STIX]{x03A9})\cap C(\overline{\unicode[STIX]{x03A9}})$ and $s>n/2$. The inequality fails for $s=n/2$. A Sobolev embedding result of Milman and Pustylnik, originally phrased in a slightly different context, implies an endpoint inequality: if $n\geqslant 3$ and $\unicode[STIX]{x03A9}\subset \mathbb{R}^{n}$ is bounded, then $$\begin{eqnarray}\max _{x\in \unicode[STIX]{x03A9}}|u(x)|\leqslant \max _{x\in \unicode[STIX]{x2202}\unicode[STIX]{x03A9}}|u(x)|+c_{n}\Vert \unicode[STIX]{x0394}u\Vert _{L^{\frac{n}{2},1}(\unicode[STIX]{x03A9})},\end{eqnarray}$$ where $L^{p,q}$ is the Lorentz space refinement of $L^{p}$. This inequality fails for $n=2$, and we prove a sharp substitute result: there exists $c>0$ such that for all $\unicode[STIX]{x03A9}\subset \mathbb{R}^{2}$ with finite measure, $$\begin{eqnarray}\max _{x\in \unicode[STIX]{x03A9}}|u(x)|\leqslant \max _{x\in \unicode[STIX]{x2202}\unicode[STIX]{x03A9}}|u(x)|+c\max _{x\in \unicode[STIX]{x03A9}}\int _{y\in \unicode[STIX]{x03A9}}\max \left\{1,\log \left(\frac{|\unicode[STIX]{x03A9}|}{\Vert x-y\Vert ^{2}}\right)\right\}|\unicode[STIX]{x0394}u(y)|dy.\end{eqnarray}$$ This is somewhat dual to the classical Trudinger–Moser inequality; we also note that it is sharper than the usual estimates given in Orlicz spaces; the proof is rearrangement-free. The Laplacian can be replaced by any uniformly elliptic operator in divergence form.

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Shimojo, M., C. B. Whorwood та P. M. Stewart. "11β-Hydroxysteroid dehydrogenase in the rat adrenal". Journal of Molecular Endocrinology 17, № 2 (1996): 121–30. http://dx.doi.org/10.1677/jme.0.0170121.

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ABSTRACT 11β-Hydroxysteroid dehydrogenase (11β-HSD) catalyses the interconversion of biologically active cortisol to inactive cortisone in man, and corticosterone to 11-dehydrocorticosterone in rodents. As such, this enzyme has been shown to confer aldosterone-selectivity on the mineralocorticoid receptor and to modulate cortisol/corticosterone access to the glucocorticoid receptor (GR). Two kinetically distinct isoforms of this enzyme have been characterized in both rodents and man; a low-affinity NADP(H)-dependent enzyme (11β-HSD1) which predominantly acts as an oxo-reductase and, more recently, a high-affinity NAD-dependent uni-directional dehydrogenase (11β-HSD2). In this study we have analysed the expression of both 11β-HSD1 and 11β-HSD2 isoforms in rat adrenal cortex and medulla and have investigated their possible roles with respect to glucocorticoid-regulated enzymes mediating catecholamine biosynthesis in adrenal medullary chromaffin cells. Using a rat 11β-HSD1 probe and a recently cloned in-house mouse 11β-HSD2 cDNA probe, Northern blot analyses revealed expression of mRNA species encoding both 11β-HSD1 (1·4kb) and 11β-HSD2 (1·9kb) in the whole adrenal. Consistent with this, 11β-dehydrogenase activity (pmol 11-dehydrocorticosterone formed/mg protein per h, mean ± s.e.m.) in adrenal homogenates, when incubated with 50 nm corticosterone in the presence of 200 μm NAD, was 97·0 ± 9·0 and with 500 nm corticosterone in the presence of 200 μm NADP, was 98·0 ± 1·4 11-Oxoreductase activity (pmol corticosterone formed/mg protein per h) with 500 nm 11-dehydrocorticosterone in the presence of 200 μm NADPH, was 187·7 ± 31·2. In situ hybridization studies of rat adrenal cortex and medulla using 35S-labelled antisense 11β-HSD1 cRNA probe revealed specific localization of 11β-HSD1 mRNA expression predominantly to cells at the corticomedullary junction, most likely within the inner cortex. In contrast, 11β-HSD2 mRNA was more abundant in cortex versus medulla, and was more uniformly distributed over the adrenal gland. Negligible staining was detected using control sense probes. Ingestion of the 11β-HSD inhibitor, glycyrrhizic acid (>100mg/kg body weight per day for 4 days) resulted in significant inhibition of adrenal NADP-dependent (98·0 ± 1·4 vs 42·5 ± 0·4) and NAD-dependent (97·0 ± 9·0 vs 73·2 ± 6·7) 11β-dehydrogenase activity and 11-oxoreductase activity (187·7 ± 31·2 vs 67·7 ± 15·3). However, while levels of 11β-HSD1 mRNA were similarly reduced (0·85 ± 0·07 vs 0·50 ± 0·05 arbitrary units), those for 11β-HSD2 remained unchanged (0·44 ± 0·03 vs 0·38 ± 0·01). Levels of mRNA encoding the glucocorticoid-dependent enzyme phenylethanolamine N-methyltransferase which catalyses the conversion of noradrenaline to adrenaline, were also significantly reduced in those rats given glycyrrhizic acid (1·12 ± 0·04 vs 0·78 ± 0·04), while those for the glucocorticoid-independent enzyme tyrosine hydroxylase (1·9 kb), which catalyses the conversion of tyrosine to DOPA, were unchanged (0·64 ± 0·04 vs 0·61 ± 0·04). In conclusion, the rat adrenal gland expresses both 11β-HSD1 and 11β-HSD2 isoforms. 11β-HSDl gene expression is localized to the adrenal cortico-medullary junction, where it is ideally placed to regulate the supply of cortex-derived corticosterone to the medullary chromaffin cells. This, together with our in vivo studies, suggests that 11β-HSD1 may play an important role with respect to adrenocorticosteroid regulation of adrenaline biosynthesis. The role of 11β-HSD2 in the adrenal remains to be elucidated.

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Dissertations / Theses on the topic "MAX 3ds 7.0"

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Andrade, Max Dorian [Verfasser], and Jens [Akademischer Betreuer] Theysohn. "Magnetfeldinduzierte vestibuläre Effekte bei 7-Tesla-MRT-Untersuchungen im Vergleich zu 1,5 Tesla und 0 Tesla / Dorian Rafael Ernesto Nikolas Andrade Max ; Betreuer: Jens Theysohn." Duisburg, 2020. http://d-nb.info/1219468002/34.

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Niebuhr, Almut [Verfasser], Christoph Akademischer Betreuer] Kleinn, Max [Gutachter] [Krott, and Georg [Gutachter] Winkel. "Fragmentation of information procurement from large-area forest inventory and the link to the international forest regime-complex : Forest information in politics / Almut Niebuhr ; Gutachter: Max Krott, Georg Winkel ; Betreuer: Christoph Kleinn." Göttingen : Niedersächsische Staats- und Universitätsbibliothek Göttingen, 2018. http://nbn-resolving.de/urn:nbn:de:gbv:7-11858/00-1735-0000-002E-E544-1-0.

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Books on the topic "MAX 3ds 7.0"

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Kennedy, Sanford. 3ds max 7 photorealistic character animation. Charles River Media, 2005.

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James, O'Connell, ed. Exploring 3D modeling with 3ds Max 7. Thomson/Delmar Learning, 2005.

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Dai, Xiaobo. 3ds max 7 xuan ran de yi shuVRay pian. Zhong guo qing nian chu ban she, 2005.

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Yu, Qiuhan, (ji suan ji), ed. 3ds max r3. 0 dong hua zhi zuo dao hang. Hai yang chu ban she, 2000.

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Huo e gong zuo shi. 3ds max 7 & Lightscape 3.2 zhan lan zhan shi xiao guo tu she ji feng bao. Bing qi gong ye chu ban she bei jing xi wang dian zi chu ban she, 2005.

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Teng long shi jue she ji gong zuo shi. Shi da jing dian: 3ds max 7 & Linghtscape 3.2 shi nei kong jian she ji yu biao xian. Zhong guo qing nian chu ban she, 2006.

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zhu, Wang Zhixin Bian, ed. Pian tou da di zhen: 3ds max 7/Combustion 3.0/After Effects 6.5 ying shi guang gao pian tou quan gong lüe. Bing qi gong ye chu ban she bei jing xi wang dian zi chu ban she, 2006.

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Bordman, Ted. 3ds max 7. Piter, 2006.

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Pescador, Dario. 3ds Max 7. Anaya Multimedia, 2005.

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3ds Max 7. Anaya Multimedia, 2005.

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Book chapters on the topic "MAX 3ds 7.0"

1

Cardoso, Jamie. "Daylight Scene Pre-Production." In V-Ray 5 for 3ds Max. CRC Press, 2022. http://dx.doi.org/10.1201/9781315770802-7.

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Lapidus, Richard. "How Do Living Objects Really Move?" In Tradigital 3ds Max. Elsevier, 2012. http://dx.doi.org/10.1016/b978-0-240-81730-9.00003-7.

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"Front Matter." In Tradigital 3ds Max. Elsevier, 2012. http://dx.doi.org/10.1016/b978-0-240-81730-9.00017-7.

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"Index." In Tradigital 3ds Max. Elsevier, 2012. http://dx.doi.org/10.1016/b978-0-240-81730-9.00020-7.

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Smith, Brian L. "Preparing AutoCAD Linework for 3ds Max." In 3ds Max Design Architectural Visualization. Elsevier, 2012. http://dx.doi.org/10.1016/b978-0-240-82107-8.50002-7.

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Gahan, Andrew. "Introduction to 3ds Max and Basic Modeling Terms." In 3ds Max Modeling for Games. Elsevier, 2012. http://dx.doi.org/10.1016/b978-0-240-81606-7.00001-7.

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"Animation." In 3ds Max 9 Essentials. Elsevier, 2006. http://dx.doi.org/10.1016/b978-0-240-80908-3.50005-7.

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"Understanding Objects and Classes." In 3ds Max MAXScript Essentials. Elsevier, 2007. http://dx.doi.org/10.1016/b978-0-240-80932-8.50007-7.

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"File Handling, and Working with Directories." In 3ds Max MAXScript Essentials. Elsevier, 2007. http://dx.doi.org/10.1016/b978-0-240-80932-8.50010-7.

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"Creating an Oil Drum Using 3ds Max." In Game Art Complete. Elsevier, 2009. http://dx.doi.org/10.1016/b978-0-240-81147-5.00002-7.

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Conference papers on the topic "MAX 3ds 7.0"

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Kasavajhala, Ananth Ram Mahanth, and Linxia Gu. "Computational Modeling of Post-Sutured Tissue Performance." In ASME 2011 International Mechanical Engineering Congress and Exposition. ASMEDC, 2011. http://dx.doi.org/10.1115/imece2011-65526.

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Efficiency of post-operative sutured tissues depends on the state stress and strain, affecting the rate of wound healing. The objective of this study was to examine, the effect of suture size and stiffness, on the deformation of an incised continuous tissue. A simple running suture configuration was modeled and analyzed using 3D Finite Element Method (FEM). Prolene suture thread (Ethicon Inc.) of size 7-0 and 8-0 with varying material stiffness in the range of 6240 MPa to 30 MPa have been used whereas CryoValve aorta graft (Cryo Life Inc.) is considered as tissue material. Results show that the suture size has major impact on the deformation state of the tissue than the suture stiffness. Even though the difference in material stiffness caused a negligible change in strain, there is 55% increase in max principal strain away from suture line. Moreover, altering the suture size from 7-0 to 8-0 resulted in a 12% reduction in max tissue stresses. Because of the localization of max stress around the corner holes of the flaw, there is a fair chance of damage initiation at this location.

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Seralathan, Sivamani, Micha Premkumar Thomai, Rian Leevinson Jayakumar, Basireddy Venkata Lokesh Reddy, and Hariram Venkatesan. "Experimental and Numerical Assessment of Cross Flow Vertical Axis Wind Turbine." In ASME 2019 Gas Turbine India Conference. American Society of Mechanical Engineers, 2019. http://dx.doi.org/10.1115/gtindia2019-2427.

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Abstract Due to increase in energy demand along with environmental awareness, the attention is shifting towards renewable energy sources. A wind turbine developed from Banki water turbine is used in this study as it starts at low-wind speeds and has high starting torque. Experimental investigations are carried out on a test rig equipped with open jet wind tunnel with wind velocity varying from 7 to 11 m/s. Later, 3D steady-state numerical analyses are performed using ANSYS CFX for better understanding of the flow physics of cross flow VAWT. The experimental investigations revealed that cross flow VAWT has a good self-starting ability at relatively low-wind speeds. A peak power coefficient (Cp, max) value of 0.059 is observed for the tip speed ratio (λ) of 0.30. As the tip speed ratio is raised further, the Cp value is observed to decrease gradually. The numerical simulations reveal the reason for the drop in Cp value. This is due to lessening of positive interaction between the flow and cross flow VAWT blades at higher λ due to vortex formation. The torque coefficient is found to decrease almost linearly from a peak value of around 0.49 at λ = 0 to a value of 0 around λ = 0.60. Polar plot between angle and torque shows that torque output of the turbine is nearly same in all directions which reinforce the potency of cross flow VAWT to be omni-directional as it produces the same performance regardless of wind directions.

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Petit, Jimmy, Jose Rouillard, and Francois Cabestaing. "Design and study of two applications controlled by a Brain-Computer Interface exploiting Steady-State Somatosensory-Evoked Potentials." In 8th International Conference on Human Interaction and Emerging Technologies. AHFE International, 2022. http://dx.doi.org/10.54941/ahfe1002787.

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Brain-Computer Interfaces (BCI) allow users to interact with machines without involving muscles. Patients with heavy motor impairment can benefit from these systems. Different states of mind of a user are discriminated to translate them into basic commands (left, right, etc.). But traditional BCI are mainly based on visual attention, and users can be quickly tired (eye fatigue, repetitive tasks, etc.). In some cases, the sight is not available for a relevant BCI, while the sense of touch can remain usable.We have implemented an electroencephalography-based BCI using the user's sense of touch. This paper describes the design and study of two BCI applications controlled by an Steady-State Somatosensory-Evoked Potentials (SSSEP), over a control group of 10 healthy subjects.We use two mechanical vibrators (C2 tactors) taped to each wrist. When they vibrate at a specific frequency, SSSEP are measurable on the electroencephalography. A somatosensory gating is the capacity of the brain to filter out stimuli perceived as redundant or irrelevant during a goal-oriented activity. This phenomenon is exploited in our BCI by asking users to imagine themselves moving their arms (motor imagery) while they are perceiving vibrations on them. These intentions are detectable in 4 possible classes (idle, left arm, right arm, and both arms simultaneous).The first application is a 2-level puzzle called SokoBCI, in which the user controls the motion of a 3D avatar and have to reach different locations to plant trees. The second application consists of driving a go-kart around a figure-of-eight track. For both applications, the main instruction given to the users is to perform the task as fast as possible. The major difference between these applications is inertia, present in the kart model, and not in SokoBCI. SokoBCI levels design and the road circuit are designed to balance the use of turns and forward commands. The "idle" command is used as a default state of mind command, therefore, it should be avoided during active control of the application. The rhythm of the command during a block, and therefore the presence of mechanical stimulations, as well as the feedback and breaks, are cued using a three-colour light.Each participant performed 4 blocks of recordings, for each application. Each block lasts around 7 minutes, except in SokoBCI if the levels are finished before, and have a fixed Sham feedback accuracy. Sham feedback is used to artificially fix the performance of the system. The accuracy is fixed during a block and could take the values: 45%, 60%, 75% and 90%. The four possible accuracies are tested once for each application during the session. Applications and tested accuracies order are pseudo-random. The applications (design and goal), as well as the given instructions are designed so that one or two (max) commands are "good" at each step, depending on the current state of the applications.We measure two kinds of data:- Quantitative: at the beginning and end of each series of 4 blocks, i.e. beginning and end of one application, a questionnaire about the awakeness, fatigue, mood orientation or experienced pain level from the stimulation of the vibration is given to the participant.In addition, at the end of every block, a NASA Task Load Index and System Usability Scale questionnaire are filled up by the users.- Qualitative: at the end of the session, a short interview is also conducted.We collect the user's perception of the experiment and Sham feedback.Using the SUS scores (0-100), we build a model of the relationship between the accuracy of the system and the perceived usability of each application. Therefore, we can predict a range of accuracies to reach, in order to achieve a specific degree of perceived usability. For example, thanks to our model, an accuracy of 80% is matched to a SUS Score of 70, which itself could be qualified as "Good", according to the well-known mapping between SUS Score and adjectives.

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Peres Leal, Aline, Paulo Vitor Reis Guilherme, Rodolfo Trentin Gonçalves, and André Luis Condino Fujarra. "Numerical Investigation on Flow-Induced Vibrations of Circular Sections in Tandem Arrangement Varying Relative Distance." In ASME 2021 40th International Conference on Ocean, Offshore and Arctic Engineering. American Society of Mechanical Engineers, 2021. http://dx.doi.org/10.1115/omae2021-62617.

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Abstract The flow around a circular section has many applications in engineering, specifically in the offshore area, such as platforms, risers, pipelines, etc. These structures, which are submerged in water, are susceptible to flow-induced vibrations (FIV) and might oscillate at unwanted large amplitudes due to currents and waves. The Computational Fluid Dynamics (CFD) is a tool that allows the investigation of different parameters related to the flow and/or to the body. A CFD analysis is important in the initial design stage of riser arrangements, being a way to predict the best relative distance, since the flow around the upstream cylinder may strongly influence the downstream cylinder forces and movements responses, characteristic of wake-induced vibrations (WIV). In this context, this work carried out simulations to initiate numerical investigations about the flow around tandem arrangements and then properly identify characteristics of the fluid model that generate the results obtained in experiments. Two similar rigid circular cylinders in a tandem arrangement were analysed, in the stationary case and in the case allowed to move in two degrees of freedom (2DOF) — transverse and in-flow directions, with mass ratio m* = 10 and no structural damping, ζ = 0%. The computations were performed using OpenFOAM, a CFD open source software, in a two-dimensional flow and, numerical uncertainties studies were conducted to well define the results, presenting the value plus its uncertainty. There were variations of the tandem distances (T = 2D, 3D, 4D, 5.5D and 6D), at Reynolds number Re = 100. These two-dimensional flow simulations at low Re are important at the initial stage of a project, in order to filter the best results and save time for more advanced analysis. A single cylinder in a turbulent flow was also analysed, with m* = 2.52, varying reduced velocity. Analysis were done comparing forces coefficients and amplitudes with the literature, for both upstream and downstream cylinders. The vorticity was investigated, properly identifying vortex shedding pattern. For stationary cylinders, a critical distance of 4D was found, where the forces coefficients increase. For the 2DOF cylinders in laminar flow, the highest amplitude was 1.04D at VR = 7 for the downstream cylinder. When the cylinders are free to move, the initial tandem distance does not interfere the amplitude results of the upstream cylinder when VR &gt; 2, results also found in experiments at high Re, and, that justify the two-dimensional studies in low Reynolds as being the basis of a project.

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Reports on the topic "MAX 3ds 7.0"

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Furman, Burford, Laxmi Ramasubramanian, Shannon McDonald, et al. Solar-Powered Automated Transportation: Feasibility and Visualization. Mineta Transportation Institute, 2021. http://dx.doi.org/10.31979/mti.2021.1948.

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A solar-powered automated transportation network (ATN) connecting the North and South campuses of San José State University with three passenger stations was designed, visualized, and analyzed in terms of its energy usage, carbon offset, and cost. The study’s methodology included the use of tools and software such as ArcGIS, SketchUp, Infraworks, Sketchup, Rhinoceros, and Autodesk 3DS Max. ATN vehicle energy usage was estimated using data from the university’s Park & Ride shuttle bus operation and by modeling with SUMOPy, the advanced simulation suite for the micro-traffic simulator SUMO. The energy study showed that an extensive solar photovoltaic (PV) canopy over the guideway and stations is sufficient for the network to run 24/7 in better-than-zero net-metered conditions—even if ridership were to increase 15% above that predicted from SJSU Park & Ride shuttle data. The resulting energy system has a PV-rated output of 6.2 MW, a battery system capacity of 9.8 MWh, and an estimated cost of $11.4 million USD. The solar ATN also produces 98% lower CO2 and PM2.5 emissions compared to the Park & Ride shuttle bus. A team of experts including urban planners, architects, and engineers designed and visualized the conceptual prototype, including a comprehensive video explaining the need for solar ATN and what a typical rider would experience while utilizing the system. This research demonstrates both benefits and challenges for solar-powered ATN, as well as its functionality within the urban built environment to serve diverse San José neighborhoods.

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