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Journal articles on the topic 'Initial density'

Author: Grafiati

Published: 2 June 2025

Last updated: 31 July 2025

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1

Aslangil, Denis, Daniel Livescu, and Arindam Banerjee. "Variable-density buoyancy-driven turbulence with asymmetric initial density distribution." Physica D: Nonlinear Phenomena 406 (May 2020): 132444. http://dx.doi.org/10.1016/j.physd.2020.132444.

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2

Dobrowolski, T. "Initial monopole density in an inflationary Universe." Classical and Quantum Gravity 18, no. 15 (2001): 3019–24. http://dx.doi.org/10.1088/0264-9381/18/15/315.

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3

Machete, R. L., and I. M. Moroz. "Initial distribution spread: A density forecasting approach." Physica D: Nonlinear Phenomena 241, no. 8 (2012): 805–15. http://dx.doi.org/10.1016/j.physd.2012.01.007.

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4

Hakl, J., P. Fuksa, J. Šantrůček, and K. Mášková. "The development of lucerne root morphology traits under high initial stand density within a seven year period." Plant, Soil and Environment 57, No. 2 (2011): 81–87. http://dx.doi.org/10.17221/186/2010-pse.

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The root system of plants is generally regarded as a factor, which is in relation to important agronomic and ecological characteristics. The aim of this study was to investigate the effect of high initial stand density on the reduction in development of lucerne root morphology traits and how long-term this effect would be. In spring 2003, a field experiment with six lucerne entries in randomized blocks was established. Broadcast sowing was used and the seeding rate was 5000 germinated seeds per m2. In 2003&ndash;2009, the plants were sampled in each plot in autumn; the average depth of sam

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5

Dahl, Mattias, and Anna Sakovich. "A density theorem for asymptotically hyperbolic initial data." Pure and Applied Mathematics Quarterly 17, no. 5 (2021): 1669–710. http://dx.doi.org/10.4310/pamq.2021.v17.n5.a3.

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6

Mouri, H., and Y. Taniguchi. "Characteristic Scales of Initial Density and Velocity Fields." Progress of Theoretical Physics 123, no. 1 (2010): 187–98. http://dx.doi.org/10.1143/ptp.123.187.

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7

Hada, Ryuichiro, and Daniel J. Eisenstein. "An iterative reconstruction of cosmological initial density fields." Monthly Notices of the Royal Astronomical Society 478, no. 2 (2018): 1866–74. http://dx.doi.org/10.1093/mnras/sty1203.

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8

Albers, C. J., and W. Schaafsma. "Estimating a density by adapting an initial guess." Computational Statistics & Data Analysis 42, no. 1-2 (2003): 27–36. http://dx.doi.org/10.1016/s0167-9473(02)00124-x.

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9

Chindo, P. S., A. M. Emechebe, and P. S. Marley. "Effect of initial population density ofPratylenchus brachyuruson maize." Archives Of Phytopathology And Plant Protection 39, no. 3 (2006): 205–8. http://dx.doi.org/10.1080/03235400400028083.

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10

Ping, Cheng. "Optimum initial condition of projection pursuit density approximation." Acta Mathematicae Applicatae Sinica 2, no. 3 (1985): 269–80. http://dx.doi.org/10.1007/bf01666747.

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11

FAUDOT, DOMINIQUE, and LIONEL GARNIER. "INITIAL PARAMETRIC REPRESENTATION OF BLOBS." International Journal of Computational Geometry & Applications 19, no. 01 (2009): 17–32. http://dx.doi.org/10.1142/s0218195909002812.

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Blobs, developed by J.F. Blinn in 1982, are the implicit surfaces obtained by composition of a real numerical function and a distance function. Since, many authors (C. Murakami, H. Nishimura, G. Wyvill…) defined their own function of density, from these implicit surfaces are interesting from several points of view. In particular, their fusion makes it possible to easily obtain an implicit equation of resulting surface. However, these surfaces do not admit a parametric equation yet. In this article, we will establish the parametric equation of two blobs in fusion, defined by the function of den

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12

Gil, Wojciech. "The influence of initial spacing on growth and survival of Scots pine in 40 years period of cultivation in varied habitat conditions." Forest Research Papers 75 (2) (June 1, 2014): 117–25. https://doi.org/10.2478/frp-2014-0011.

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The aim of the research was to determine the effect of initial spacing on the survival and growth of pine trees in dry coniferous and fresh coniferous forest habitats after nearly 40 years from the establishment of plantation. The study presents an analysis of seven spacing variants in square, rectangular and triangular spacing patterns with the initial density ranging from 6 944 seedlings/ha to 15 625 seedlings/ha. The studies were conducted on two study sites. No tending treatments (selective thinning) were performed in the examined stands throughout the growing season. It was shown that hab

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13

Cañizo Rincón, José Alfredo. "Asymptotic behaviour of solutions to the generalized Becker–Döring equations for general initial data." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 461, no. 2064 (2005): 3731–45. http://dx.doi.org/10.1098/rspa.2005.1522.

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We prove the following asymptotic behaviour for solutions to the generalized Becker–Döring system for general initial data: under a detailed balance assumption and in situations where density is conserved in time, there is a critical density ρ s such that solutions with an initial density ρ 0 ≤ ρ s converge strongly to the equilibrium with density ρ 0 and solutions with initial density ρ 0 > ρ s converge (in a weak sense) to the equilibrium with density ρ s . This extends the previous knowledge that this behaviour happens under more restrictive conditions on the initial data. The main tool

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14

Li, Lei, Jacob Weiner, Daowei Zhou, Yingxin Huang, and Lianxi Sheng. "Initial density affects biomass-density and allometric relationships in self-thinning populations ofFagopyrum esculentum." Journal of Ecology 101, no. 2 (2013): 475–83. http://dx.doi.org/10.1111/1365-2745.12039.

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15

Tran, Indigo T., Jordan A. Heiman, Victoria R. Lydy, and La Toya Kissoon. "Silver Inhibits Lemna minor Growth at High Initial Frond Densities." Plants 12, no. 5 (2023): 1104. http://dx.doi.org/10.3390/plants12051104.

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Silver nanoparticles (AgNPs) are the most popular engineered nanomaterials in consumer products due to their antimicrobial properties. They enter aquatic ecosystems via insufficient purified wastewaters from manufacturers or consumers. AgNPs inhibit growth of aquatic plants, including duckweeds. Growth media nutrient concentration and initial duckweed frond density can affect growth. However, it is not well understood how frond density affects nanoparticle toxicity. We investigated the toxicity of 500 µg/L AgNPs and AgNO3 on Lemna minor at different initial frond densities (20, 40, and 80 fron

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16

Zhang, Wen, Boqiang Fan, Ping Zheng, and Yuguo Yu. "Axon initial segment potassium channel density in cortical neurons." BMC Neuroscience 16, Suppl 1 (2015): P295. http://dx.doi.org/10.1186/1471-2202-16-s1-p295.

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17

CARNEIRO, SAULO, and REZA TAVAKOL. "ON VACUUM DENSITY, THE INITIAL SINGULARITY AND DARK ENERGY." International Journal of Modern Physics D 18, no. 14 (2009): 2343–49. http://dx.doi.org/10.1142/s0218271809016120.

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Standard cosmology poses a number of important questions. Apart from its singular origin, it possesses early and late accelerating phases required to account for observations. The vacuum energy has been considered as a possible way to resolve some of these questions. The vacuum energy density induced by free fields in an early de Sitter phase has earlier been estimated to be proportional to H4, while more recently it has been suggested that the QCD condensate induces a term proportional to H at late times. These results have been employed in models which are nonsingular and inflationary at ear

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18

Carneiro, Saulo, and Reza Tavakol. "On vacuum density, the initial singularity and dark energy." General Relativity and Gravitation 41, no. 10 (2009): 2287–93. http://dx.doi.org/10.1007/s10714-009-0846-2.

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19

Bich, E., and E. Vogel. "The initial density dependence of transport properties: Noble gases." International Journal of Thermophysics 12, no. 1 (1991): 27–42. http://dx.doi.org/10.1007/bf00506120.

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20

Schönau, A. P. G., and J. Coetzee. "Initial spacing, stand density and thinning in eucalypt plantations." Forest Ecology and Management 29, no. 4 (1989): 245–66. http://dx.doi.org/10.1016/0378-1127(89)90097-2.

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21

Özbayram, Ali Kemal, and Emrah Çiçek. "Initial planting density experiments of narrow-leaved ash in Turkey." Šumarski list 144, no. 5-6 (2020): 269–78. http://dx.doi.org/10.31298/sl.144.5-6.4.

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Narrow-leaved ash (Fraxinus angustifolia subsp. oxycarpa Vahl.) is a source of valuable wood in Europe and plantations produce high yields in Turkey. Initial planting density plays an important role in plantation silviculture and affects the growth and quality of trees as well as establishment costs. This study aimed to determine the ten-year effects of initial planting density on tree growth and quality of narrow-leaved ash. In 2004, three replications of four initial planting densities (1111, 1667, 2500 and 3333 stem ha<sup>–1</sup>) were established in a randomized block design

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22

Sawae, Yoshinori, Sachiko Ida, Syou Ishiyama, Kazuhiro Nakashima, and Teruo Murakami. "Influence of Initial Cell Density on Mechanical Property of Cultured Chondrocytes-Agarose Construct(Micro- and Nano-biomechanics)." Proceedings of the Asian Pacific Conference on Biomechanics : emerging science and technology in biomechanics 2004.1 (2004): 217–18. http://dx.doi.org/10.1299/jsmeapbio.2004.1.217.

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23

DENG, TAIQING, LIANXI HU, YU SUN, and XIAOYA LIU. "EFFECTS OF INITIAL INHOMOGENEOUS DENSITY DISTRIBUTION AND VOID SHAPE ON POWDER FORGING OF POROUS METAL." Modern Physics Letters B 27, no. 19 (2013): 1341008. http://dx.doi.org/10.1142/s021798491341008x.

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The deformation behavior during axisymmetric upsetting of sintered metals has been studied based on the finite-element method. The investigation on the effects of the initial density distribution, void shape and die friction on the density distribution and punch force during deformation have been conducted. It was found that under low-friction conditions, the initial density distribution affects the deformation geometry and the density distribution. However, the effect of the initial density distribution was found to be negligible under high-friction conditions. The initial density distributio

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24

Cao, Ling, and Xin Zhe Li. "Experimental Study of Influence Factors in Unsaturated Soil Infiltration Rate." Applied Mechanics and Materials 477-478 (December 2013): 472–75. http://dx.doi.org/10.4028/www.scientific.net/amm.477-478.472.

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Based on the unsaturated soil ponding water infiltration test in laboratory, the influences of cohesive particles content, dry density and initial water content on infiltration rate are analyzed. Soil infiltration rate decreased with the increase of cohesive particles content and dry density; with the decrease of initial water content at low dry density, and with the increase of initial water content at high dry density.

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25

Zhang, Fu Quan, Yong Zhou Wang, Mei Chen, Mao Fang Huang, and Ri Zhong Zeng. "Study on Crosslink Density of Natural Rubber with Different Initial Moisture Contents Dried by Microwave." Applied Mechanics and Materials 556-562 (May 2014): 173–76. http://dx.doi.org/10.4028/www.scientific.net/amm.556-562.173.

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In this work, the crosslink density of uncured natural rubber with different initial moisture contents, 3.80%, 10.05%, 19.76%, 23.68%, respectively, dried by microwave at frequency of 2450MHz was studied using nuclear magnetic resonance spectrometer. Seen from the results, the effect of initial moisture content of wet natural rubber on crosslink density and processability were obvious. With the increment of initial moisture content of wet natural rubber, the crosslink density of natural rubber after microwave dried with the frequency of 2450MHz decreased gradually. The crosslink density and A(

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26

Dias, Guilherme Faus da Silva, Pedro Luís da Costa Aguiar Alves, and Tomás Carneiro de Souza Dias. "Brachiaria decumbens supresses the initial growth of Coffea arabica." Scientia Agricola 61, no. 6 (2004): 579–83. http://dx.doi.org/10.1590/s0103-90162004000600003.

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Brachiaria decumbens is becoming one the most common weeds growing in young coffee orchards because, besides its fast growth and difficulty of control, new coffee orchards are usually established in pasture areas. In order to verify the effect of B. decumbens plant density on the early growth of coffee (Coffea arabica L. cv. Catuaí Amarelo), a competition experiment was conducted under semi-controlled humidity conditions. Soil collected in a Typic Haplustox was placed in 70 L asbestos cement boxes and one coffee seedling was planted in each box. The B. decumbens seedlings were transplanted to

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27

Melhuish, Chris, Ana B. Sendova-Franks, Sam Scholes, Ian Horsfield, and Fred Welsby. "Ant-inspired sorting by robots: the importance of initial clustering." Journal of The Royal Society Interface 3, no. 7 (2005): 235–42. http://dx.doi.org/10.1098/rsif.2005.0081.

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For engineers the prospect of scalable collective robot systems is very appealing. Such systems typically adopt a decentralized approach in their control and coordination mechanism, which employs local sensing and action as well as limited communication. Under these constraints and informed by research on Temnothorax ants, two puck sorting algorithms were tested in a combination of simulation and with real robots. Both algorithms employed puck density as a cue. Only the overall local density, irrespective of puck type, was found to be required which offers the prospect for a more simple mechan

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28

Cai, Guoqing, Annan Zhou, and Daichao Sheng. "Permeability function for unsaturated soils with different initial densities." Canadian Geotechnical Journal 51, no. 12 (2014): 1456–67. http://dx.doi.org/10.1139/cgj-2013-0410.

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This study proposes an approach to simulate the effects of initial density on the relative coefficient of permeability for unsaturated soils. The density-dependent permeability function is derived based on (i) an incremental relationship between the degree of saturation and the initial void ratio with various suctions and (ii) the relationship between the permeability function and the soil-water retention curve (SWRC). Only one additional parameter is required in the proposed function, which can be calibrated using a conventional SWRC test. A number of test results in the literature are employ

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29

Naidu, N. F., and M. Govender. "The influence of initial conditions during dissipative collapse." International Journal of Modern Physics D 25, no. 10 (2016): 1650092. http://dx.doi.org/10.1142/s0218271816500929.

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Starting off with two distinct initially static stellar cores (i) Florides interior (constant density, vanishing radial pressure) and (ii) Wyman interior (constant density, nonvanishing radial pressure), we explore the dynamics of these two models once hydrostatic equilibrium is lost. We show that although the time of formation of horizon, evolution of the mass and proper radius are independent of the chosen initially static configurations, there is a significant difference in the temperature profiles of the radiating bodies as the collapse proceeds.

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30

YUE, Z. Y., B. ZHANG, G. WINNEWISSER, and J. STUTZKI. "ON THE DYNAMICAL EVOLUTION OF THE FRACTAL STRUCTURE OF INTERSTELLAR MEDIUM." Fractals 01, no. 04 (1993): 908–16. http://dx.doi.org/10.1142/s0218348x93000952.

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Two-dimensional compressible turbulence in a self-gravitating, magnetic interstellar medium is calculated as an initial value problem. It is shown that even if the initial density distribution is homogeneous and the initial velocity distribution contains only a few Fourier components, the nonlinear interaction among the Fourier components will generate more and more Fourier components and lead to a turbulent and fractal structure in the interstellar medium. The calculations are carried out for three different initial states. In order to see the time evolution, detailed density distributions an

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31

Cui, Ming Tao, and Hong Fang Chen. "The Influence of Initial Structural Density Value on Results of Multi-Material Topology Optimization Problems." Applied Mechanics and Materials 635-637 (September 2014): 223–27. http://dx.doi.org/10.4028/www.scientific.net/amm.635-637.223.

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We discover that the given initial structural density value has significant influence on the final result of multi-material topology optimization when adopting the SIMP interpolation scheme. The influence cannot be ignored if the grid is sparse, and there is a certain degree of periodic relationship between the structural minimum compliance and the given initial density value. By modifying the initial structural density value, a better topology optimization result with a smaller compliance can be obtained. The expression is proposed on how to modify the initial structural density value to get

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32

Borysova, M. S., O. D. Borysov, Iu A. Karpenko, V. M. Shapoval, and Yu M. Sinyukov. "Tubular Initial Conditions and Ridge Formation." Advances in High Energy Physics 2013 (2013): 1–10. http://dx.doi.org/10.1155/2013/209182.

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The 2D azimuth and rapidity structure of the two-particle correlations in relativistic A+A collisions is altered significantly by the presence of sharp inhomogeneities in superdense matter formed in such processes. The causality constraints enforce one to associate the long-range longitudinal correlations observed in a narrow angular interval, the so-called (soft) ridge, with peculiarities of the initial conditions of collision process. This study's objective is to analyze whether multiform initial tubular structures, undergoing the subsequent hydrodynamic evolution and gradual decoupling, can

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33

Danchin, R. "Density-dependent incompressible viscous fluids in critical spaces." Proceedings of the Royal Society of Edinburgh: Section A Mathematics 133, no. 6 (2003): 1311–34. http://dx.doi.org/10.1017/s030821050000295x.

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We study the unique solvability of density-dependent incompressible Navier-Stokes equations in the whole space RN (N ≥ 2). The celebrated results by Fujita and Kato devoted to the constant density case are generalized to the case when the initial density is close to a constant: we find local well posedness for large initial velocity, and global well posedness for initial velocity small with respect to the viscosity. Our functional setting is very close to the one used by Fujita and Kato.

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34

Li, Yiran, Xiaohua Liu, Chuanjie Zhang, Zedong Li, Ye Zhao, and Yong Niu. "Effect of initial plant density on modeling accuracy of the revised sparse Gash model: a case study of Pinus tabuliformis plantations in northern China." Hydrology Research 51, no. 5 (2020): 1170–83. http://dx.doi.org/10.2166/nh.2020.007.

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Abstract An accurate quantitative description of interception is necessary to understand regional water circulation. The revised sparse Gash model (RSGM) is currently used to estimate interception loss. Previous studies have proven that changes in initial plant density, which are caused by thinning, affect the accuracy of RSGM; however, the direct effect of initial density on modeling accuracy remains poorly understood because few studies have collected field data of the same species with various initial densities under similar site conditions. Therefore, six Pinus tabuliformis Carr. plantatio

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35

Neyrinck, Mark C., and Lin Forrest Yang. "Ringing the initial Universe: the response of overdensity and transformed-density power spectra to initial spikes." Monthly Notices of the Royal Astronomical Society 433, no. 2 (2013): 1628–33. http://dx.doi.org/10.1093/mnras/stt949.

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36

Li Kun, 李琨, 杨美霞 Yang Meixia, 夏惠君 Xia Huijun, 钟鸣 Zhong Ming, and 何衡湘 He Hengxiang. "Influence of plasma’s initial density on laser-supported detonation waves." High Power Laser and Particle Beams 25, no. 10 (2013): 2501–4. http://dx.doi.org/10.3788/hplpb20132510.2501.

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37

De Proft, Frank, Paul W. Ayers, Stijn Fias, and Paul Geerlings. "Woodward-Hoffmann rules in density functional theory: Initial hardness response." Journal of Chemical Physics 125, no. 21 (2006): 214101. http://dx.doi.org/10.1063/1.2387953.

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38

Gouda, Naoteru. "Reconstruction of initial cosmological density fluctuations by the psuedospectral method." Astrophysical Journal 436 (December 1994): 542. http://dx.doi.org/10.1086/174927.

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39

Reis, Caio Cesar Vicente. "Recycled HDPE (High Density Polyethylene) Plastic Tile An Initial Prototype." Journal of Engineering Research 4, no. 17 (2024): 2–16. http://dx.doi.org/10.22533/at.ed.3174172421069.

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40

Rekaa, V. L., H. L. Pécseli, and J. K. Trulsen. "Self-similar space-time evolution of an initial density discontinuity." Physics of Plasmas 20, no. 7 (2013): 072117. http://dx.doi.org/10.1063/1.4816953.

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41

Roux, Filippus S. "Anomalous transient behavior from an inhomogeneous initial optical vortex density." Journal of the Optical Society of America A 28, no. 4 (2011): 621. http://dx.doi.org/10.1364/josaa.28.000621.

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42

Nusser, Adi, and Avishai Dekel. "Omega and the initial fluctuations from velocity and density fields." Astrophysical Journal 405 (March 1993): 437. http://dx.doi.org/10.1086/172376.

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43

Holkundkar, Amol R., and N. K. Gupta. "Effect of initial plasma density on laser induced ion acceleration." Physics of Plasmas 15, no. 12 (2008): 123104. http://dx.doi.org/10.1063/1.3037264.

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44

Bhosale, D. N., N. D. Choudhari, S. R. Sawant, and P. P. Bakare. "Initial permeability studies on high density CuMgZn ferrites." Journal of Magnetism and Magnetic Materials 173, no. 1-2 (1997): 51–58. http://dx.doi.org/10.1016/s0304-8853(97)00178-9.

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45

Wang, Xin-Nian. "Probe initial parton density and formation time via jet quenching." Nuclear Physics A 715 (March 2003): 775c—778c. http://dx.doi.org/10.1016/s0375-9474(02)01486-0.

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46

Slough, John, Samuel Andreason, Hiroshi Gota, Chris Pihl, and George Votroubek. "The Pulsed High Density Experiment: Concept, Design, and Initial Results." Journal of Fusion Energy 26, no. 1-2 (2006): 199–205. http://dx.doi.org/10.1007/s10894-006-9058-x.

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47

Pinheiro, G., and R. Chan. "Radiating gravitational collapse with an initial inhomogeneous energy density distribution." General Relativity and Gravitation 43, no. 5 (2010): 1451–67. http://dx.doi.org/10.1007/s10714-010-1132-z.

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48

Lane, Nancy E., Daniel A. Bloch, Helen B. Hubert, Henry Jones, Ulla Simpson, and James F. Fries. "Running, osteoarthritis, and bone density: Initial 2-year longitudinal study." American Journal of Medicine 88, no. 5 (1990): 452–59. http://dx.doi.org/10.1016/0002-9343(90)90422-a.

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49

Avinyó, A., J. Solà-Morales, and M. València. "A Singular Initial Value Problem to Construct Density-Equalizing Maps." Journal of Dynamics and Differential Equations 24, no. 1 (2011): 51–59. http://dx.doi.org/10.1007/s10884-011-9236-z.

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50

Rousskikh, A. G., A. S. Zhigalin, and V. I. Oreshkin. "Estimation of the initial density distribution in plasma–metal liners." Technical Physics 61, no. 5 (2016): 676–82. http://dx.doi.org/10.1134/s1063784216050194.

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