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Journal articles on the topic 'Break-up process'

Author: Grafiati

Published: 30 June 2021

Last updated: 17 February 2022

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1

Bałdyga, Jerzy, Wojciech Orciuch, Łukasz Makowski, Maciej Malski‐Brodzicki, and Katarzyna Malik. "Break‐Up of Nanoparticle Clusters—Process Modeling." Journal of Dispersion Science and Technology 29, no. 4 (2008): 555–63. http://dx.doi.org/10.1080/01932690701729120.

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2

Gomes, P. R. S., R. M. Anjos, and J. Lubian. "Does the break-up process influence the fusion cross section?" Brazilian Journal of Physics 34, no. 3a (2004): 737–41. http://dx.doi.org/10.1590/s0103-97332004000500008.

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3

Djavareshk, M. H., and A. Ghasemi. "Investigation of Jet Break-Up Process in Diesel Engine Spray Modelling." Journal of Applied Sciences 9, no. 11 (2009): 2078–87. http://dx.doi.org/10.3923/jas.2009.2078.2087.

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4

Onaga, T. "Eikonal approach to the atomic break-up process by polarized electrons." Journal of Physics B: Atomic, Molecular and Optical Physics 25, no. 22 (1992): 4875–87. http://dx.doi.org/10.1088/0953-4075/25/22/021.

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5

FACHRUDDIN, IMAM, CHARLOTTE ELSTER, and WALTER GLÖCKLE. "THE PROTON-DEUTERON BREAK-UP PROCESS IN A THREE-DIMENSIONAL APPROACH." Modern Physics Letters A 18, no. 02n06 (2003): 452–55. http://dx.doi.org/10.1142/s0217732303010673.

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The pd break-up amplitude in the Faddeev scheme is calculated by employing a three-dimensional method without partial wave decomposition (PWD). In the first step and in view of higher energies only the leading term is evaluated and this for the process d(p,n)pp. A comparison with the results based on PWD reveals discrepancies in the cross section around 200 MeV. This indicates the onset of a limitation of the partial wave scheme. Also around 200 MeV relativistic effects are clearly visible and the use of relativistic kinematics shifts the cross section peak to where the experimental peak is lo

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6

Sousa, D. P., D. Pereira, J. Lubian, et al. "Probing the 6,7Li nucleon densities through a new break-up process approach." Nuclear Physics A 836, no. 1-2 (2010): 1–10. http://dx.doi.org/10.1016/j.nuclphysa.2010.01.245.

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7

Bracamontes-Rodríguez, Y. E., I. Armas Rivera, G. Beltrán-Pérez, et al. "Polarization of vector solitons generated in break-up process in twisted fiber." Optics Communications 349 (August 2015): 203–8. http://dx.doi.org/10.1016/j.optcom.2015.03.030.

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8

Fath, A., K. U. Munch, and Alfred Leipertz. "Spray Break-Up Process of Diesel Fuel Investigated Close to the Nozzle." International Journal of Fluid Mechanics Research 24, no. 1-3 (1997): 251–60. http://dx.doi.org/10.1615/interjfluidmechres.v24.i1-3.250.

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9

Sano, Yosuke, Yasushi Kino, Toshitaka Oka, and Tsutomu Sekine. "Ps slowing down process below the Ps break-up energy in Ar gas." Journal of Physics: Conference Series 635, no. 5 (2015): 052088. http://dx.doi.org/10.1088/1742-6596/635/5/052088.

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10

Doleschall, P., and I. Borbély. "Phenomenological Non-Local Nucleon-Nucleon Interactions and the Neutron-Deuteron Break-Up Process." Few-Body Systems 27, no. 1 (1999): 1–14. http://dx.doi.org/10.1007/s006010050120.

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11

Witala, H., Th Cornelius, and W. Gl�ckle. "Faddeev calculations with meson-exchangeN-N interactions for then-d break-up process." Few-Body Systems 5, no. 3 (1988): 89–105. http://dx.doi.org/10.1007/bf01079581.

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12

NITSCHE, J. M., and G. K. BATCHELOR. "Break-up of a falling drop containing dispersed particles." Journal of Fluid Mechanics 340 (June 10, 1997): 161–75. http://dx.doi.org/10.1017/s0022112097005223.

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The general purpose of this paper is to investigate some consequences of the randomness of the velocities of interacting rigid particles falling under gravity through viscous fluid at small Reynolds number. Random velocities often imply diffusive transport of the particles, but particle diffusion of the conventional kind exists only when the length characteristic of the diffusion process is small compared with the distance over which the particle concentration is effectively uniform. When this condition is not satisfied, some alternative analytical description of the dispersion process is need

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13

ESLAMI-KALANTARI, M., H. R. AMIR-AHMADI, A. BIEGUN, et al. "PROTON-DEUTERON BREAK-UP MEASUREMENTS WITH BINA AT 135 MeV." Modern Physics Letters A 24, no. 11n13 (2009): 839–42. http://dx.doi.org/10.1142/s0217732309000127.

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High-precision measurements of the proton-deuteron elastic and break-up reaction have been performed in the past at KVI and elsewhere with the aim to study three-nucleon force (3NF) effects. In the present work, we explored 3NF effects in the break-up scattering process by performing a measurement of vector analyzing powers and differential cross sections using a 135 MeV polarized-proton beam impinging on a liquid-deuterium target. For this study, we used a new experimental setup, Big Instrument for Nuclear-polarization Analysis, BINA, which covers almost the entire kinematical phase space of

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14

Wang, Hai-Shuo, and Xi-Yun Hou. "Break-up of the synchronous state of binary asteroid systems." Monthly Notices of the Royal Astronomical Society 505, no. 4 (2021): 6037–50. http://dx.doi.org/10.1093/mnras/stab1585.

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ABSTRACT This paper continues the authors’ previous work and presents a coplanar averaged ellipsoid–ellipsoid model of synchronous binary asteroid system (BAS) plus thermal and tidal effects. Using this model, we analyse the break-up mechanism of the synchronous BAS. Different from the classical spin-orbit coupling model that neglects the rotational motion’s influence on the orbital motion, our model considers simultaneously the orbital motion and the rotational motions. Our findings are as follows: (1) Stable region of the secondary’s synchronous state is mainly up to the secondary’s shape. T

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15

Radin, M., and H. Ghasemi. "Nd break-up process with considering 3NF at intermediate energies in a 3D approach." Nuclear Physics A 945 (January 2016): 269–77. http://dx.doi.org/10.1016/j.nuclphysa.2015.11.003.

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16

Innings, F., and C. Trägårdh. "Visualization of the Drop Deformation and Break-Up Process in a High Pressure Homogenizer." Chemical Engineering & Technology 28, no. 8 (2005): 882–91. http://dx.doi.org/10.1002/ceat.200500080.

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17

Ivashniov, O. E., and K. I. Soplenkov. "A model involving break-up to explain peculiarities of the boiling liquid efflux process." International Journal of Multiphase Flow 18, no. 5 (1992): 727–38. http://dx.doi.org/10.1016/0301-9322(92)90041-e.

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18

Rodd, Lucy E., Timothy P. Scott, Justin J. Cooper-White, and Gareth H. McKinley. "Capillary Break-up Rheometry of Low-Viscosity Elastic Fluids." Applied Rheology 15, no. 1 (2005): 12–27. http://dx.doi.org/10.1515/arh-2005-0001.

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Abstract We investigate the dynamics of the capillary thinning and break-up process for low viscosity elastic fluids such as dilute polymer solutions. Standard measurements of the evolution of the midpoint diameter of the necking fluid filament are augmented by high speed digital video images of the break up dynamics. We show that the successful operation of a capillary thinning device is governed by three important time scales (which characterize the relative importance of inertial, viscous and elastic processes), and also by two important length scales (which specify the initial sample size

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19

Muhammad, P., C. Duguay, and K. K. Kang. "Monitoring ice break-up on the Mackenzie River using MODIS data." Cryosphere Discussions 9, no. 3 (2015): 2783–820. http://dx.doi.org/10.5194/tcd-9-2783-2015.

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Abstract. This study involves the analysis of Moderate Resolution Imaging Spectroradiometer (MODIS) Level 3 500 m snow products (MOD/MYD10A1), complemented with 250 m Level 1B data (MOD/MYD02QKM), to monitor ice cover during the break-up period on the Mackenzie River, Canada. Results from the analysis of data for 13 ice seasons (2001–2013) show that first day ice-off dates are observed between days of year (DOY) 115–125 and end DOY 145–155, resulting in average melt durations of about 30–40 days. Floating ice transported northbound could therefore generate multiple periods of ice-on and ice-of

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20

Voermans, Joey J., Jean Rabault, Kirill Filchuk, et al. "Experimental evidence for a universal threshold characterizing wave-induced sea ice break-up." Cryosphere 14, no. 11 (2020): 4265–78. http://dx.doi.org/10.5194/tc-14-4265-2020.

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Abstract. Waves can drastically transform a sea ice cover by inducing break-up over vast distances in the course of a few hours. However, relatively few detailed studies have described this phenomenon in a quantitative manner, and the process of sea ice break-up by waves needs to be further parameterized and verified before it can be reliably included in forecasting models. In the present work, we discuss sea ice break-up parameterization and demonstrate the existence of an observational threshold separating breaking and non-breaking cases. This threshold is based on information from two recen

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21

Kim, Dae Soo, Geon Bae, Byung Seong Bae, et al. "Monodispersed Liquid Crystal Droplets Fabricated by the Droplet Break-up Process in the Microfluidic System." Molecular Crystals and Liquid Crystals 596, no. 1 (2014): 45–50. http://dx.doi.org/10.1080/15421406.2014.918302.

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22

Bałdyga, Jerzy, Wojciech Orciuch, Łukasz Makowski, Maciej Malski-Brodzicki, and Katarzyna Malik. "Break up of nano-particle clusters in high-shear devices." Chemical Engineering and Processing: Process Intensification 46, no. 9 (2007): 851–61. http://dx.doi.org/10.1016/j.cep.2007.05.016.

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23

Lundin, E. R., and A. G. Doré. "Non-Wilsonian break-up predisposed by transforms: examples from the North Atlantic and Arctic." Geological Society, London, Special Publications 470, no. 1 (2018): 375–92. http://dx.doi.org/10.1144/sp470.6.

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AbstractThe Atlantic Ocean margins formed the basis for the seminal Wilson cycle concept, which suggests that oceans close, form fold belts, and later reopen in a concertina-like fashion. However, we observe that continental break-up of the North Atlantic–Arctic region only weakly reflects Wilson's concept. Rather than utilizing fold belts, transforms have been the dominant weaknesses that guided break-up, primarily because less force is required to break a plate via strike-slip related shearing than via rifting. Some transforms were inherited features, whereas others formed as part of the con

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24

Partridge, L., D. C. Y. Wong, M. J. H. Simmons, E. I. Părău, and S. P. Decent. "Experimental and Theoretical Description of the Break-up of Curved Liquid Jets in the Prilling Process." Chemical Engineering Research and Design 83, no. 11 (2005): 1267–75. http://dx.doi.org/10.1205/cherd.05090.

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25

Mukhtar, Syeda Masooda, and Desalegn Abraha Gebrekidan. "Determinants of International Strategic Alliance Process and Alliance Failure: Learning from the Volvo-Renault Break-up." International Journal of Strategic Business Alliances 6, no. 2 (2017): 1. http://dx.doi.org/10.1504/ijsba.2017.10009842.

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26

SASAKI, Atsushi, Masamichi TOSAKI, and Masaharu Matsubara. "1601 Observation of break-up process of water sheet using an optical liquid surface inclinometer(2)." Proceedings of the Fluids engineering conference 2006 (2006): _1601–1_—_1601–4_. http://dx.doi.org/10.1299/jsmefed.2006._1601-1_.

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27

SASAKI, Atsushi, Masamichi TOSAKI, and Masaharu Matsubara. "1601 Observation of break-up process of water sheet using an optical liquid surface inclinometer(1)." Proceedings of the Fluids engineering conference 2006 (2006): _1601—a_. http://dx.doi.org/10.1299/jsmefed.2006._1601-a_.

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28

Lan, Tian, Jian Qing Wang, and Zheng Wei Jin. "Influence of Blow-Up Ratio on Properties of Cellulose Packaging Films by Blow-Extrusion Process." Advanced Materials Research 380 (November 2011): 260–64. http://dx.doi.org/10.4028/www.scientific.net/amr.380.260.

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The blow-extruded tube-like regeneration cellulose films in different blow-up ratios were prepared by NMMO technology. It was studied the effect of different blow-up ratio on the mechanical and obstructing properties as well as the morphology cross-section of cellulose blown films. It is found that the tensile strength and obstructing performance except elongation at break of films are improved when blow-up ratios increasing. The tensile strength of 1.3, 1.7 blow-up ratio cellulose blown films in longitudinal and transverse is 36.4MPa and 39.9MPa, 13.8MPa and 29.04MPa, respectively. The elonga

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29

Wolstencroft, Martin, and J. Huw Davies. "Breaking supercontinents; no need to choose between passive or active." Solid Earth 8, no. 4 (2017): 817–25. http://dx.doi.org/10.5194/se-8-817-2017.

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Abstract. Much debate has centred on whether continental break-up is predominantly caused by active upwelling in the mantle (e.g. plumes) or by long-range extensional stresses in the lithosphere. We propose the hypothesis that global supercontinent break-up events should always involve both. The fundamental principle involved is the conservation of mass within the spherical shell of the mantle, which requires a return flow for any major upwelling beneath a supercontinent. This shallow horizontal return flow away from the locus of upwelling produces extensional stress. We demonstrate this princ

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30

Yule, A. J., and D. G. Salters. "On the Distance Required to Atomize Diesel Sprays Injected from Orifice-Type Nozzles." Proceedings of the Institution of Mechanical Engineers, Part D: Journal of Automobile Engineering 209, no. 3 (1995): 217–26. http://dx.doi.org/10.1243/pime_proc_1995_209_205_02.

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Conductivity probe measurements, using ranges of nozzles, liquid properties and gas densities, have revealed more extensive and reliable information on the break-up process of diesel sprays than has been published to date. The spray generated from a single-hole orifice-type nozzle has an incompletely atomized break-up length which typically extends at least 100 hole diameters downstream. The physical structure of this break-up zone varies, depending on the liquid properties and both initial and boundary conditions, from that of a central liquid column, with outer drops and ligaments, to, more

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31

Gebrekidan, Desalegn Abraha, and Syeda Masooda Mukhtar. "Determinants of the international strategic alliance process and alliance failure: learning from the Volvo-Renault break-up." International Journal of Strategic Business Alliances 6, no. 1/2 (2017): 86. http://dx.doi.org/10.1504/ijsba.2017.089846.

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32

Silva, Fabricio S., Ricardo A. Medronho, and Luiz Fernando Barca. "Experimental study of water droplet break up in water in oil dispersions using an apparatus that produces localized pressure drops." Oil & Gas Science and Technology – Revue d’IFP Energies nouvelles 74 (2019): 1. http://dx.doi.org/10.2516/ogst/2018079.

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Oil production facilities have choke/control valves to control production and protect downstream equipment against over pressurization. This process is responsible for droplets break up and the formation of emulsions which are difficult to treat. An experimental study of water in oil dispersion droplets break up in localized pressure drop is presented. To accomplish that, an apparatus simulating a gate valve was constructed. Droplet Size Distribution (DSD) was measured by laser light scattering. Oil physical properties were controlled and three different break up models were compared with the

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33

BOTTA, Oana Daciana, István MAGOS, and Corneliu BALAN. "Experimental study on the formation and break-up of fluid bubbles." INCAS BULLETIN 12, no. 1 (2020): 27–34. http://dx.doi.org/10.13111/2066-8201.2020.12.1.3.

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The study of fluid surfaces plays an important role in understanding the interfaces encountered in biological systems, as it allows for the investigation of the basic characteristics such as the formation, stability and permeability. Moreover, the adhesion and the fusion of biological membranes can be better understood by the experimental investigations of drops and bubbles formation in controlled dynamical processes. These studies have the potential to generate novel and value information for medical applications in the diagnosis and therapy using microfluidic-based biosensors and controlled

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34

Jeffries, Martin O., and Kim Morris. "Some aspects of ice phenology on ponds in central Alaska, USA." Annals of Glaciology 46 (2007): 397–403. http://dx.doi.org/10.3189/172756407782871576.

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AbstractIce phenology (freeze-up, break-up and duration) was monitored for five seasons between autumn 2001 and spring 2006 at 11 small, shallow ponds in the boreal forest of central Alaska, USA. The sequence in which freeze-up (FU; day of 100% ice cover) and break-up (BU; day of zero ice cover) occurred at the 11 ponds showed moderately high to very high coherence each season. This was probably due to FU and BU being poorly correlated with pond morphometry (area, depth). BU is strongly correlated with April mean air temperature; a ±1˚C change in mean April air temperature is equivalent to a ±

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35

Stratmann, F., H. Siebert, G. Spindler, et al. "New-particle formation events in a continental boundary layer: First results from the SATURN experiment." Atmospheric Chemistry and Physics Discussions 3, no. 2 (2003): 1693–731. http://dx.doi.org/10.5194/acpd-3-1693-2003.

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Abstract. During the SATURN experiment, which took place from 27 May to 4 June 2002, new particle formation in the continental boundary layer was investigated. Simultaneous ground-based and tethered-balloon-borne measurements were performed, including meteorological parameters, particle number concentrations and size distributions, gaseous precursor concentrations and SODAR and LIDAR observations. Newly formed particles were observed inside the residual layer, before the break-up process of the nocturnal inversion, and inside the mixing layer throughout the break-up of the nocturnal inversion

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36

Stratmann, F., H. Siebert, G. Spindler, et al. "New-particle formation events in a continental boundary layer: first results from the SATURN experiment." Atmospheric Chemistry and Physics 3, no. 5 (2003): 1445–59. http://dx.doi.org/10.5194/acp-3-1445-2003.

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Abstract. During the SATURN experiment, which took place from 27 May to 14 June 2002, new particle formation in the continental boundary layer was investigated. Simultaneous ground-based and tethered-balloon-borne measurements were performed, including meteorological parameters, particle number concentrations and size distributions, gaseous precursor concentrations and SODAR and LIDAR observations. Newly formed particles were observed inside the residual layer, before the break-up process of the nocturnal inversion, and inside the mixing layer throughout the break-up of the nocturnal inversion

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37

Škarica, Mihovil. "Process of local government fragmentation in Croatia: From a big-bang to a status quo." Miscellanea Geographica 25, no. 1 (2021): 46–53. http://dx.doi.org/10.2478/mgrsd-2020-0043.

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Abstract The paper explores and explains the fragmentation process in Croatian local government during the transition period from 1990 onwards. Special focus is given to the emergence of new municipalities (municipal splits/secessions) that occurred after the new two-tier local government system was established in 1993. Excessive fragmentation of territorial structure at the beginning of the 1990s was a systematic and centrally driven reform that was meant to break with the inherited local government model and break up its territorial structure as radically as possible. While the initial overh

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38

Wu, Xi Wang, Jian Zhong Xiao, Feng Xia, Yong Gang Hu, and Zhou Peng. "A Simple Method to Disperse Carbon Nanotubes by Shearing Process." Advanced Materials Research 335-336 (September 2011): 255–59. http://dx.doi.org/10.4028/www.scientific.net/amr.335-336.255.

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The key problem to prepare carbon nanotubes (CNTs) reinforced ceramic matrix composites is how to break up massive agglomerates of CNTs and disperse uniformly CNTs. We obtain the CNTs-Al2O3composite powder by shear treatment on melted CNTs-Al2O3-agents mixture. Microstructure observations of CNTs-Al2O3composite powder show that CNTs can be dispersed uniformly by shearing process. The rheological results also affirm the conclusion. According to the rheological theory, we build the ideal dispersion model of CNTs-Al2O3suspension system and discuss the dispersion mechanism.

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39

LASHERAS, J. C., E. VILLERMAUX, and E. J. HOPFINGER. "Break-up and atomization of a round water jet by a high-speed annular air jet." Journal of Fluid Mechanics 357 (February 25, 1998): 351–79. http://dx.doi.org/10.1017/s0022112097008070.

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The near- and far-field break-up and atomization of a water jet by a high-speed annular air jet are examined by means of high-speed flow visualizations and phase Doppler particle sizing techniques. Visualization of the jet's near field and measurements of the frequencies associated with the gas–liquid interfacial instabilities are used to study the underlying physical mechanisms involved in the primary break-up of the water jet. This process is shown to consist of the stripping of water sheets, or ligaments, which subsequently break into smaller lumps or drops. An entrainment model of the near

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40

Double, Oliver. "Tragedy Plus Time: Transforming Life Experience into Stand-Up Comedy." New Theatre Quarterly 33, no. 2 (2017): 143–55. http://dx.doi.org/10.1017/s0266464x17000057.

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In this article, Oliver Double examines the process of turning traumatic personal experience into viable stand-up comedy material by offering a detailed account of the creative process behind his 2015 show Break a Leg. Drawing on Bergson, Brecht, and Noël Carroll, he explores the origins of comic ideas in personal observation, and argues for a two-stage process of joke creation. This is fleshed out in a detailed examination of a particular routine, in which he uses Koestler's concept of bisociation to show how an initial observation was shaped into a series of punchlines. He also discusses aut

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41

Ramazani-Moghaddam-Arani, A., M. Mahjour-Shafiei, H. R. Amir-Ahmadi, et al. "Spin observables in the three-body break-up process near the quasi-free limit in deuteron–deuteron scattering." Physics Letters B 725, no. 4-5 (2013): 282–86. http://dx.doi.org/10.1016/j.physletb.2013.07.041.

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42

Kozlov, V. S., and F. B. Shuman. "Using the energy of a controlled explosion to break up large hard-to-process metal objects into scrap." Metallurgist 41, no. 5-6 (1997): 182–86. http://dx.doi.org/10.1007/bf02767862.

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43

MacAyeal, Douglas R., Marianne H. Okal, Jonathan E. Thom, Kelly M. Brunt, Young-Jin Kim, and Andrew K. Bliss. "Tabular iceberg collisions within the coastal regime." Journal of Glaciology 54, no. 185 (2008): 371–86. http://dx.doi.org/10.3189/002214308784886180.

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AbstractDuring 2000–07, five giant icebergs (B15A, B15J, B15K, C16 and C25) adrift in the southwestern Ross Sea, Antarctica, were instrumented with global positioning system (GPS) receivers and other instruments to monitor their behavior in the near-coastal environment. The measurements show that collision processes can strongly influence iceberg behavior and delay their progress in drifting to the open ocean. Collisions appear to have been a dominant control on the movement of B15A, the largest of the icebergs, during the 4-year period it gyrated within the limited confines of Ross Island, th

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44

Perovich, Donald K., Jacqueline A. Richter-Menge, and Walter B. Tucker. "Seasonal changes in Arctic sea-ice morphology." Annals of Glaciology 33 (2001): 171–76. http://dx.doi.org/10.3189/172756401781818716.

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AbstractThe morphology of the Arctic sea-ice cover undergoes large changes over an annual cycle. These changes have a significant impact on the heat budget of the ice cover, primarily by affecting the distribution of the solar radiation absorbed in the ice-ocean system. In spring, the ice is snow-covered and ridges are the prominent features. The pack consists of large angular floes, with a small amount of open water contained primarily in linear leads. By the end of summer the ice cover has undergone a major transformation. The snow cover is gone, many of the ridges have been reduced to hummo

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45

Mostaghimi, Javad, and Sanjeev Chandra. "Splat formation in plasma-spray coating process." Pure and Applied Chemistry 74, no. 3 (2002): 441–45. http://dx.doi.org/10.1351/pac200274030441.

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The paper describes recent developments in modeling formation of plasma-spray coatings. This is a stochastic process in which particle-impact conditions, thermophysical properties, substrate topology, and temperature all play important roles in determining the structure of coating. Specific attention is paid to the simulation of droplet impact and solidification under plasma-spraying conditions. Results of 3-dimensional models show that on a flat surface solidification may cause splashing and break-up of the impacting particle. Undercooling effects result in faster solidification and, thus, sm

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46

Holladay, Holly Willson, and Amanda Nell Edgar. "‘I’m never gonna stop watching it’: The paradox of parasocial break-ups in a post-object era." Journal of Fandom Studies 7, no. 3 (2019): 213–27. http://dx.doi.org/10.1386/jfs_00001_1.

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In this article, we propose an understanding of parasocial relationships, in which fans build an affective relationship with characters and television programmes, as fandom’s emotional interior. Rather than being structured by fan productivity and community, parasocial relationships exist in a private, intimate space as fans develop deep emotional bonds with characters. When a series concludes, fans must therefore reconcile the dissolution of these relationships in a personal way, a process called the parasocial break-up. However, the current media landscape fosters the sense that the fan obje

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47

Alpaslan Kocamemi, B., and D. Dityapak. "Real-time process dynamics monitoring in Anammox reactors." Water Science and Technology 70, no. 2 (2014): 183–91. http://dx.doi.org/10.2166/wst.2014.130.

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Process dynamics in Anammox systems were evaluated through continuous monitoring of pH, oxidation reduction potential (ORP) and conductivity in two separate newly started-up sequencing batch reactors, one seeded with an enriched Anammox sludge and the other seeded with mixed activated sludge. The pH and ORP profiles exhibited characteristic patterns depending on the process dynamics during early start-up, start-up and enrichment phases of the operational period of 410 days. The simultaneously continuing processes of the start-up period showed apparent indicative trend lines in pH and ORP profi

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Al-Asheh, Sameer, and Fawzi Banat. "Packed-Bed Removal of Copper and Zinc Ions Using Chemically-Treated Chicken Feathers." Energy & Environment 14, no. 4 (2003): 461–72. http://dx.doi.org/10.1260/095830503322364467.

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In this work, the sorption of copper by chemically treated chicken feathers was tested via packed-bed column. Chicken feathers were selected as adsorbent based on its high availability as environmental waste. The alkaline-treated chicken feathers column showed good sorption capacity toward copper and zinc ions. It was proved that an increase in metal concentration or flow rate of the influent solution shortens the break-through time. The break-through time increased with the bed depth. The break-through time occurred earlier when zinc was passed through the column rather than copper, but the b

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Valtonen, M. "Three-Body Problem and Multiple Stellar Systems." International Astronomical Union Colloquium 191 (August 2004): 146–51. http://dx.doi.org/10.1017/s0252921100008678.

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AbstractThree-body processes go on in star clusters where binary stars meet single stars and frequently form temporary triple systems. The triples are typically unstable and break up into a new binary and a single star. Also a simple scattering of a single star from a binary may take place. Both processes can be handled by the statistical theories of three-body break-up and scattering. Here we apply the theory to binary stars, assuming that binaries have been involved in the three-body process. The distributions of binary periods, eccentricities and mass ratios are discussed from this point of

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TSUDA, Shinichi, Naoki TANI, and Nobuhiro YAMANISHI. "A Construction of a Multi-Process Cavitation Model for Cold Water (Implementation of Inception/Collapse and Coalescence/Break-up)." TRANSACTIONS OF THE JAPAN SOCIETY OF MECHANICAL ENGINEERS Series B 78, no. 790 (2012): 1165–80. http://dx.doi.org/10.1299/kikaib.78.1165.

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