J comput phys
Details for Molecular Dynamics (MD) Simulations
systems were simulated for 250 ns seconds, while the CBM-microfibril systems were simulated twice (independently) for 100 ns each. These simulations were carried out at 300 K using NAMD 2.10 (Phillips et al. 2005).The Langevin thermostat was used to control temperature (Schneider and Stoll 1978), and the SHAKE algorithm was used to fix the bond distances of all hydrogen atoms (Ryckaert et al ...
[DOC File]References – Chapter 1:
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Ault, J.P., and Mauchley, S.J. Ocean magnetic and electric observations. In Researches of the Department of Terrestrial Magnetism, vol 5, Carnegie Institution of Washington, D.C. (see chapter entitled Atmospheric-Electric Results Obtained Aboard Carnegie, 1915-1921.)
[DOC File]Introduction
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P. Singh1, D.D. Joseph2,3. S.K. Gurupatham1, B. Dalal1. and S. Nudurupati1 . 1Department of Mechanical Engineering, New Jersey Institute of Technology, Newark, NJ ...
[DOC File]A study on film boiling using a Coupled Level Set
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M.Sussman and Elbridge Gerry Pucket, A Coupled Level Set and Volume-of-Fluid Method for Computing 3D and Axisymmetric Incompresible Two-Phase Flows, J. Comput. Physc. 162, 301-337 (2000). Y.C.Chang, T.Y.Hou, B.Merriman and S.Osher, A Level Set Formulation of Eulerian Interface Capturing Methods for Incompressible Fluid Flows, J. Comput.
[DOC File]Stanley Osher - University of California, Los Angeles
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Shu, J. Comput. Phys., v185, #2 pp-309-341. Special Issue Methods and Applications of Analysis, dedicated to Osher on the 2003. occasion of his 60th birthday. Special Issue in honor of 60th birthday in honor of Stanley Osher, J. of Sci. 2003. Computing, v19, #1-3. ICIAM 2003 Pioneer Prize 2003
Model Paper for the Proceedings of the 7th International ...
where J is the Jacobian of the mapping, are weight constants and u represents external criteria for adapting the grid. ... J.S. “Adaptive Zoning for Singular Problems in Two Dimensions,” J. Comput. Phys. 46, 342-368, 1982. 1 . Title: Model Paper for the Proceedings of the 7th International Conference on Numerical Grid Generation in ...
[DOC File]Title: Instructions for Authors : Arial 14pt, bold, centred
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Phys. Rev. E 1993;47:1815-1819. [10] Shan X, Chen H. Simulation of nonideal gases and liquid-gas phase transitions by the lattice boltzmann equations. Phys. Rev. E 1994;49:2941-2948. [11] Shan X. Doolen G. Multicomponent lattice-boltzmann model with interparticle interaction. J. Stat. Phys 1995;81:379-393.
Supporting Online Material for
Our algorithm first randomly selects the required number of sites and calculates the mean probability of detection, p Ω ,n, Δ t , for the given sampling arrangement Ω j (under the given surveillance parameters, n, Δ t ), as described in the main text.We used this detection probability as the ‘objective function’ in the optimisation algorithm, which needs to be maximised.
PHS 398/2590 (Rev. 06/09), Biographical Sketch Format Page
J Comput Phys. 2013 Jul 1;244:4-21. Zhang Y, Liang X, Ma J, Jing Y, Gonzales MJ, Villongco C, Krishnamurthy A, Frank LR, Nigam V, Stark P, Narayan SM, McCulloch AD. An atlas-based geometry pipeline for cardiac Hermite model construction and diffusion tensor reorientation. Med Image Anal. 2012; 16(6):1130-41; PMID: 2284177
[DOCX File]Springer
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J Comput Phys. J Earth Simul. J Earth Syst Sci. J Environ Eng. J Exp Bot. J Fac Sci Hokkaido Univ. J Field Robot. J Fluid Mech. J Geophys Res. J Geophys Res Atmos. J Glaciol. J Great Lakes Res. J Hazard Mater A. J Heat Transf. J Hydraul Eng. J Hydrol. J Hydrometeorol. J Mar Res. J Mar Syst. J Math Pures Appl. J Meteorol. J Meteorol Soc Jpn.
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