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Journal articles on the topic 'N dynamics'

Author: Grafiati

Published: 4 June 2021

Last updated: 5 February 2022

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1

Mikishanina, E. A. "Dynamics of a Controlled Articulated $n$-trailer Wheeled Vehicle." Nelineinaya Dinamika 17, no. 1 (2021): 39–48. http://dx.doi.org/10.20537/nd210104.

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This article is devoted to the study of the dynamics of movement of an articulated $n$-trailer wheeled vehicle with a controlled leading car. Each link of the vehicle can rotate relative to its point of fixation. It is shown that, in the case of a controlled leading car, only nonholonomic constraint equations are sufficient to describe the dynamics of the system, which in turn form a closed system of differential equations. For a detailed analysis of the dynamics of the system, the cases of movement of a wheeled vehicle consisting of three symmetric links are considered, and the leading link (leading car) moves both uniformly along a circle and with a modulo variable velocity along a certain curved trajectory. The angular velocity remains constant in both cases. In the first case, the system is integrable and analytical solutions are obtained. In the second case, when the linear velocity is a periodic function, the solutions of the problem are also periodic. In numerical experiments with a large number of trailers, similar dynamics are observed.

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2

Li, Tanping, Yaowen Cui, John Mathaga, Revati Kumar, and Daniel G. Kuroda. "Hydration and vibrational dynamics of betaine (N,N,N-trimethylglycine)." Journal of Chemical Physics 142, no. 21 (June 7, 2015): 212438. http://dx.doi.org/10.1063/1.4919795.

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3

Chapman, Curtis F., Richard S. Fee, and Mark Maroncelli. "Solvation dynamics in N-methylamides." Journal of Physical Chemistry 94, no. 12 (June 1990): 4929–35. http://dx.doi.org/10.1021/j100375a032.

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4

Gukov, S., I. R. Klebanov, and A. M. Polyakov. "Dynamics of (n,1) strings." Physics Letters B 423, no. 1-2 (March 1998): 64–70. http://dx.doi.org/10.1016/s0370-2693(98)00090-2.

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5

Winkler, B., I. Kaiser, M. Chall, G. Coddens, B. Hennion, and R. Kahn. "Dynamics of N(CH3)4GeCl3." Physica B: Condensed Matter 234-236 (June 1997): 70–71. http://dx.doi.org/10.1016/s0921-4526(96)00883-6.

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6

Klotz, Alexander R. "Bubble dynamics in N dimensions." Physics of Fluids 25, no. 8 (August 2013): 082109. http://dx.doi.org/10.1063/1.4817803.

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7

Spiegel, Heide, Michael Pfeffer, and Johannes Hösch. "N Dynamics under Reduced Tillage." Archives of Agronomy and Soil Science 48, no. 5 (January 2002): 503–12. http://dx.doi.org/10.1080/03650340215644.

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8

Miller, Tomasz, Michał Eckstein, Paweł Horodecki, and Ryszard Horodecki. "Generally covariant N-particle dynamics." Journal of Geometry and Physics 160 (February 2021): 103990. http://dx.doi.org/10.1016/j.geomphys.2020.103990.

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9

Barrera, Carlos, Nathan W. C. Leigh, Bastián Reinoso, Amelia M. Stutz, and Dominik Schleicher. "Small-N collisional dynamics – V. From N ≲ 10 to N ≳ 103." Monthly Notices of the Royal Astronomical Society 502, no. 3 (January 27, 2021): 3374–84. http://dx.doi.org/10.1093/mnras/stab207.

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ABSTRACT Direct collisions between finite-sized particles occur commonly in many areas of astrophysics. Such collisions are typically mediated by chaotic, bound gravitational interactions involving small numbers of particles. An important application is stellar collisions, which occur commonly in dense star clusters, and their relevance for the formation of various types of stellar exotica. In this paper, we return to our study of the collision rates and probabilities during small-number chaotic gravitational interactions ($N\, \lesssim$ 10), moving beyond the small-number particle limit and into the realm of larger particle numbers ($N\, \gtrsim$ 103) to test the extent of validity of our analytic model as a function of the particle properties and the number of interacting particles. This is done using direct N-body simulations of stellar collisions in dense star clusters, by varying the relative numbers of particles with different particle masses and radii. We compute the predicted rate of collisions using the mean free path approximation, adopting the point-particle limit and using the sticky-star approximation as our collision criterion. We evaluate its efficacy in the regime where gravitational focusing is important by comparing the theoretical rates to numerical simulations. Using the tools developed in previous papers in this series, in particular Collision Rate Diagrams, we illustrate that our predicted and simulated rates are in excellent agreement, typically consistent with each other to within 1 standard deviation.

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10

Elpidoforou, Nikolaos, Ioannis Skarmoutsos, Emmanouil Kainourgiakis, Vasilios Raptis, and Jannis Samios. "Local structure and translational dynamics of NMF (N-methylformamide)–DMF (N,N-dimethylformamide) mixtures, via molecular dynamics simulation." Journal of Molecular Liquids 226 (January 2017): 16–27. http://dx.doi.org/10.1016/j.molliq.2016.09.039.

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11

Sanford, Todd, Sang-Yun Han, Matthew A. Thompson, Robert Parson, and W. Carl Lineberger. "Photodissociation dynamics of IBr−(CO2)n, n<15." Journal of Chemical Physics 122, no. 5 (February 2005): 054307. http://dx.doi.org/10.1063/1.1839178.

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12

Yashonath, S., and C. N. R. Rao. "Structure and dynamics of polar liquids: A molecular dynamics investigation of N,N-dimethyl formamide." Chemical Physics 155, no. 3 (September 1991): 351–56. http://dx.doi.org/10.1016/0301-0104(91)80111-t.

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13

Ouled Mohamed Sghaier, Mohsen, Krystyna Holderna-Natkaniec, Aneta Wozniak-Braszak, Piotr Czarnecki, and Slaheddine Chaabouni. "Structure and internal dynamics of N,N-diethylethylendiammonium pentachloroantimoniate(III)–N,N-diethylethylendiammonium dichloride." Polyhedron 70 (March 2014): 85–91. http://dx.doi.org/10.1016/j.poly.2013.12.011.

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14

Ovchinnikov, Igor V., and Kang L. Wang. "Stochastic dynamics and combinatorial optimization." Modern Physics Letters B 31, no. 31 (November 6, 2017): 1750285. http://dx.doi.org/10.1142/s0217984917502852.

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Natural dynamics is often dominated by sudden nonlinear processes such as neuroavalanches, gamma-ray bursts, solar flares, etc., that exhibit scale-free statistics much in the spirit of the logarithmic Ritcher scale for earthquake magnitudes. On phase diagrams, stochastic dynamical systems (DSs) exhibiting this type of dynamics belong to the finite-width phase (N-phase for brevity) that precedes ordinary chaotic behavior and that is known under such names as noise-induced chaos, self-organized criticality, dynamical complexity, etc. Within the recently proposed supersymmetric theory of stochastic dynamics, the N-phase can be roughly interpreted as the noise-induced “overlap” between integrable and chaotic deterministic dynamics. As a result, the N-phase dynamics inherits the properties of the both. Here, we analyze this unique set of properties and conclude that the N-phase DSs must naturally be the most efficient optimizers: on one hand, N-phase DSs have integrable flows with well-defined attractors that can be associated with candidate solutions and, on the other hand, the noise-induced attractor-to-attractor dynamics in the N-phase is effectively chaotic or aperiodic so that a DS must avoid revisiting solutions/attractors thus accelerating the search for the best solution. Based on this understanding, we propose a method for stochastic dynamical optimization using the N-phase DSs. This method can be viewed as a hybrid of the simulated and chaotic annealing methods. Our proposition can result in a new generation of hardware devices for efficient solution of various search and/or combinatorial optimization problems.

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15

Stajic, J. "The dynamics of dipolar interactions." Science 349, no. 6250 (August 20, 2015): 838–40. http://dx.doi.org/10.1126/science.349.6250.838-n.

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16

Kachru, Shamit. "Aspects of N=1 string dynamics." Nuclear Physics B - Proceedings Supplements 61, no. 1-2 (February 1998): 42–57. http://dx.doi.org/10.1016/s0920-5632(97)00518-5.

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17

FLETCHER, ALASTAIR N., and DANIEL A. NICKS. "Quasiregular dynamics on the n-sphere." Ergodic Theory and Dynamical Systems 31, no. 1 (January 18, 2010): 23–31. http://dx.doi.org/10.1017/s0143385709001072.

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AbstractIn this paper, we investigate the boundary of the escaping set I(f) for quasiregular mappings on ℝn, both in the uniformly quasiregular case and in the polynomial type case. The aim is to show that ∂I(f) is the Julia set J(f) when the latter is defined, and shares properties with the Julia set when J(f) is not defined.

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18

Haidar, Ali T., and Hans R. Thierstein. "Coccolithophore dynamics off Bermuda (N. Atlantic)." Deep Sea Research Part II: Topical Studies in Oceanography 48, no. 8-9 (January 2001): 1925–56. http://dx.doi.org/10.1016/s0967-0645(00)00169-7.

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19

Wang, H. Y., and R. Lesar. "O(N) algorithm for dislocation dynamics." Philosophical Magazine A 71, no. 1 (January 1995): 149–64. http://dx.doi.org/10.1080/01418619508242962.

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20

Rauscher, Phillip M., Kenneth S. Schweizer, Stuart J. Rowan, and Juan J. de Pablo. "Dynamics of poly[n]catenane melts." Journal of Chemical Physics 152, no. 21 (June 7, 2020): 214901. http://dx.doi.org/10.1063/5.0007573.

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21

Carloni, S., P. K. S. Dunsby, S. Capozziello, and A. Troisi. "Cosmological dynamics of R n gravity." Classical and Quantum Gravity 22, no. 22 (October 31, 2005): 4839–68. http://dx.doi.org/10.1088/0264-9381/22/22/011.

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22

Sazdjian, H. "Relativistic dynamics for N-body systems." Physics Letters B 208, no. 3-4 (July 1988): 470–74. http://dx.doi.org/10.1016/0370-2693(88)90649-1.

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23

Matsumoto, Akio, and Ferenc Szidarovszky. "Delay Stability of n-Firm Cournot Oligopolies." Mathematics 8, no. 9 (September 18, 2020): 1615. http://dx.doi.org/10.3390/math8091615.

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The dynamic behavior of n-firm oligopolies is examined without product differentiation and with linear price and cost functions. Continuous time scales are assumed with best response dynamics, in which case the equilibrium is asymptotically stable without delays. The firms are assumed to face both implementation and information delays. If the delays are equal, then the model is a single delay case, and the equilibrium is oscillatory stable if the delay is small, at the threshold stability is lost by Hopf bifurcation with cyclic behavior, and for larger delays, the trajectories show expanding cycles. In the case of the non-equal delays, the stability switching curves are constructed and the directions of stability switches are determined. In the case of growth rate dynamics, the local behavior of the trajectories is similar to that of the best response dynamics. Simulation studies verify and illustrate the theoretical findings.

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24

Rommel-Möhle, Kerstin, and Hans-Jörg Hofmann. "Conformation dynamics in peptides: quantum chemical calculations and molecular dynamics simulations on N-acetylalanyl-N'-methylamide." Journal of Molecular Structure: THEOCHEM 285, no. 2 (October 1993): 211–19. http://dx.doi.org/10.1016/0166-1280(93)87036-d.

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25

Chen, Xiao, Jia-dan Xue, and Xu-ming Zheng. "Decay Dynamics of N, N-Dimethylthioacetamide in S3(ππ*) State." Chinese Journal of Chemical Physics 28, no. 1 (February 27, 2015): 27–34. http://dx.doi.org/10.1063/1674-0068/28/cjcp1409152.

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26

Hassan, Sk Sarif, Moole Parameswar Reddy, and Ranjeet Kumar Rout. "Dynamics of the Modified n-Degree Lorenz System." Applied Mathematics and Nonlinear Sciences 4, no. 2 (August 22, 2019): 315–30. http://dx.doi.org/10.2478/amns.2019.2.00028.

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AbstractThe Lorenz model is one of the most studied dynamical systems. Chaotic dynamics of several modified models of the classical Lorenz system are studied. In this article, a new chaotic model is introduced and studied computationally. By finding the fixed points, the eigenvalues of the Jacobian, and the Lyapunov exponents. Transition from convergence behavior to the periodic behavior (limit cycle) are observed by varying the degree of the system. Also transiting from periodic behavior to the chaotic behavior are seen by changing the degree of the system.

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27

CYRIL, X., J. ANGELES, and A. MISRA. "EFFICIENT INVERSE DYNAMICS OF GENERAL N-AXIS ROBOTIC MANIPULATORS." Transactions of the Canadian Society for Mechanical Engineering 13, no. 4 (December 1989): 91–95. http://dx.doi.org/10.1139/tcsme-1989-0015.

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Presented in this paper is an efficient scheme to solve the inverse dynamics problem associated with robotic manipulators of arbitrary architecture, using the recursive Newton-Euler formulation. The scheme’s efficiency derives from the use of suitable coordinate frame to represent the vector quantities and the suitable manipulation of the vector operations. The computational complexities of this and other general dynamical formulations published so far are compared. In conclusion, it is observed that not only the dynamical formulation methodology, but also the judicious representation and manipulation of the vector quantities contribute to the computational efficiency of the algorithm. An example is presented to show the validity of the computational scheme.

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28

Wrobel, L. C. "Computational fluid dynamics." Engineering Analysis with Boundary Elements 9, no. 2 (January 1992): 192. http://dx.doi.org/10.1016/0955-7997(92)90070-n.

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29

Kioupis, Loukas I., and Edward J. Maginn. "Rheology, dynamics, and structure of hydrocarbon blends: a molecular dynamics study of n-hexane/n-hexadecane mixtures." Chemical Engineering Journal 74, no. 1-2 (July 1999): 129–46. http://dx.doi.org/10.1016/s1385-8947(99)00053-4.

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30

Barthel, Josef, Richard Buchner, and Bernhard Wurm. "The dynamics of liquid formamide, N-methylformamide, N,N-dimethylformamide, and N,N-dimethylacetamide. A dielectric relaxation study." Journal of Molecular Liquids 98-99 (May 2002): 51–69. http://dx.doi.org/10.1016/s0167-7322(01)00309-9.

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31

Tayyem, Muna T., Mohammad B. Zughul, and Mansour H. Almatarneh. "Molecular dynamics simulation of N-octyl-N-quaternized chitosan derivatives as a drug carrier." Journal of Theoretical and Computational Chemistry 17, no. 04 (June 2018): 1850025. http://dx.doi.org/10.1142/s0219633618500256.

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The dynamic amphiphilic behavior of N-octyl-N-quaternized chitosan derivatives in aqueous solution is investigated using molecular dynamics (MD) simulations. It is found that quaternization decreases the intra-chain hydrogen bond formation which leads to reduced rigidity of the chitosan backbone. The effect of octyl substitution is much less pronounced. Analysis of hydrogen bonding reveals the presence of a hydrogen bond within the quaternized glucosamine unit, which causes the distortion of the usual chair conformation. Also, H-bond formation with the solvent water molecules was found to stabilize the intra-chain HO3-O5 hydrogen bond. Additionally, an aqueous solution containing the 10%-N-octyl-50%-N-quaternized chitosan derivative (1O5QCS) and the anti-cancer drug 10-hydroxycamptothecin (10-HCPT) was also investigated using MD simulations. It was found that van der Waals and electrostatic forces have virtually equal contributions to the nonbonded interactions responsible for complexation. Furthermore, H-bond formation between drug and drug carrier contributes to lactone ring stability and subsequent bioavailability.

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32

Smith, B., D. Wårlind, A. Arneth, T. Hickler, P. Leadley, J. Siltberg, and S. Zaehle. "Implications of incorporating N cycling and N limitations on primary production in an individual-based dynamic vegetation model." Biogeosciences Discussions 10, no. 11 (November 28, 2013): 18613–85. http://dx.doi.org/10.5194/bgd-10-18613-2013.

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Abstract. The LPJ-GUESS dynamic vegetation model uniquely combines an individual- and patch-based representation of vegetation dynamics with ecosystem biogeochemical cycling from regional to global scales. We present an updated version that includes plant and soil N dynamics, analysing the implications of accounting for C-N interactions on predictions and performance of the model. Stand structural dynamics and allometric scaling of tree growth suggested by global databases of forest stand structure and development were well-reproduced by the model in comparison to an earlier multi-model study. Accounting for N cycle dynamics improved the goodness-of-fit for broadleaved forests. N limitation associated with low N mineralisation rates reduces productivity of cold-climate and dry-climate ecosystems relative to mesic temperate and tropical ecosystems. In a model experiment emulating free-air CO2 enrichment (FACE) treatment for forests globally, N-limitation associated with low N mineralisation rates of colder soils reduces CO2-enhancement of NPP for boreal forests, while some temperate and tropical forests exhibit increased NPP enhancement. Under a business-as-usual future climate and emissions scenario, ecosystem C storage globally was projected to increase by c. 10%; additional N requirements to match this increasing ecosystem C were within the high N supply limit estimated on stoichiometric grounds in an earlier study. Our results highlight the importance of accounting for C-N interactions not only in studies of global terrestrial C cycling, but to understand underlying mechanisms on local scales and in different regional contexts.

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33

Nakayama, Takeshi, Fujio Minami, and Kuon Inoue. "Exciton dynamics in short-period (GaAs)n/(AlAs)n superlattices with n=8−15." Journal of Luminescence 53, no. 1-6 (July 1992): 380–82. http://dx.doi.org/10.1016/0022-2313(92)90178-c.

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34

Cho, Yong-Hoon, J. J. Song, H. Lim, Byung-Doo Choe, J. I. Lee, and D. Kim. "Recombination dynamics in n-AlxGa1−xAs/n-In0.5Ga0.5P type-II heterostructures." Applied Physics Letters 73, no. 9 (August 31, 1998): 1245–47. http://dx.doi.org/10.1063/1.122369.

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35

Deb, Sanghamitra, Xinxin Cheng, and Peter M. Weber. "Structural Dynamics and Charge Transfer in Electronically Excited N,N′-Dimethylpiperazine." Journal of Physical Chemistry Letters 4, no. 16 (August 6, 2013): 2780–84. http://dx.doi.org/10.1021/jz401499q.

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36

Lipciuc, M. Laura, Sara H. Gardiner, Tolga N. V. Karsili, Jason W. L. Lee, David Heathcote, Michael N. R. Ashfold, and Claire Vallance. "Photofragmentation dynamics of N,N-dimethylformamide following excitation at 193 nm." Journal of Chemical Physics 147, no. 1 (July 7, 2017): 013941. http://dx.doi.org/10.1063/1.4983704.

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37

Aleshkin, V. Ya, and D. I. Burdeinyi. "Temporal dynamics of impurity photoconductivity in n-GaAs and n-InP." Physics of the Solid State 56, no. 5 (May 2014): 917–21. http://dx.doi.org/10.1134/s1063783414050023.

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38

Yang, Liulin, and Yanming Dong. "Crystal morphology study of N,N′-diacetylchitobiose by molecular dynamics simulation." Carbohydrate Research 346, no. 15 (November 2011): 2457–62. http://dx.doi.org/10.1016/j.carres.2011.08.020.

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39

Smith, B., D. Wårlind, A. Arneth, T. Hickler, P. Leadley, J. Siltberg, and S. Zaehle. "Implications of incorporating N cycling and N limitations on primary production in an individual-based dynamic vegetation model." Biogeosciences 11, no. 7 (April 10, 2014): 2027–54. http://dx.doi.org/10.5194/bg-11-2027-2014.

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Abstract. The LPJ-GUESS dynamic vegetation model uniquely combines an individual- and patch-based representation of vegetation dynamics with ecosystem biogeochemical cycling from regional to global scales. We present an updated version that includes plant and soil N dynamics, analysing the implications of accounting for C–N interactions on predictions and performance of the model. Stand structural dynamics and allometric scaling of tree growth suggested by global databases of forest stand structure and development were well reproduced by the model in comparison to an earlier multi-model study. Accounting for N cycle dynamics improved the goodness of fit for broadleaved forests. N limitation associated with low N-mineralisation rates reduces productivity of cold-climate and dry-climate ecosystems relative to mesic temperate and tropical ecosystems. In a model experiment emulating free-air CO2 enrichment (FACE) treatment for forests globally, N limitation associated with low N-mineralisation rates of colder soils reduces CO2 enhancement of net primary production (NPP) for boreal forests, while some temperate and tropical forests exhibit increased NPP enhancement. Under a business-as-usual future climate and emissions scenario, ecosystem C storage globally was projected to increase by ca. 10%; additional N requirements to match this increasing ecosystem C were within the high N supply limit estimated on stoichiometric grounds in an earlier study. Our results highlight the importance of accounting for C–N interactions in studies of global terrestrial N cycling, and as a basis for understanding mechanisms on local scales and in different regional contexts.

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40

Petrilla, Brad A., Mario F. Trujillo, and Michael Micci. "n-HEPTANE DROPLET VAPORIZATION USING MOLECULAR DYNAMICS." Atomization and Sprays 20, no. 7 (2010): 581–93. http://dx.doi.org/10.1615/atomizspr.v20.i7.20.

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41

Mysore, Shreesh P. "N-cadherin, spine dynamics, and synaptic function." frontiers in Neuroscience 2, no. 2 (December 15, 2008): 168–75. http://dx.doi.org/10.3389/neuro.01.035.2008.

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42

Cao, N., Y. B. Long, Z. G. Zhang, J. Yuan, L. J. Gao, B. R. Zhao, S. P. Zhao, Q. S. Yang, J. Zhao, and Panming Fu. "Quasiparticle relaxation dynamics in n-type superconductor." Physica C: Superconductivity 468, no. 11-12 (June 2008): 894–97. http://dx.doi.org/10.1016/j.physc.2008.02.004.

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43

V. Zenkov, Dmitry, and Anthony M. Bloch. "Dynamics of the n-dimensional Suslov problem." Journal of Geometry and Physics 34, no. 2 (June 2000): 121–36. http://dx.doi.org/10.1016/s0393-0440(99)00058-3.

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44

Lebedev, V. T., G. T�r�k, L. Cser, G. K�li, and A. I. Sibilev. "Molecular dynamics of poly(N-vinylcaprolactam) hydrate." Applied Physics A: Materials Science & Processing 74 (December 1, 2002): s478—s480. http://dx.doi.org/10.1007/s003390101111.

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45

Sui, Xiukai, Rui Cong, Kun Li, and Long Wang. "Evolutionary dynamics of N-person snowdrift game." Physics Letters A 379, no. 45-46 (December 2015): 2922–34. http://dx.doi.org/10.1016/j.physleta.2015.08.029.

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46

Wei, Zhengrong, Ying Tang, Qiusha Zheng, and Bing Zhang. "Photodissociation dynamics of n-C5H11Br at 234nm." Optics Communications 265, no. 2 (September 2006): 532–36. http://dx.doi.org/10.1016/j.optcom.2006.03.065.

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47

Bernays, Elizabeth. "Functional Dynamics of Phytophagous Insects.T. N. Ananthakrishnan." Quarterly Review of Biology 70, no. 3 (September 1995): 347. http://dx.doi.org/10.1086/419114.

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48

Hidalgo, Rubén A., Gerardo Honorato, and Francisco Valenzuela-Henriquez. "On the dynamics of n-circle inversion." Nonlinearity 32, no. 4 (March 12, 2019): 1242–74. http://dx.doi.org/10.1088/1361-6544/aaf8d9.

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49

Huong, Pham V., Stéphanie Bouchet, and Jean-Claude Launay. "Cristal-growth dynamics of n-doped gaAs." Proceedings, annual meeting, Electron Microscopy Society of America 50, no. 2 (August 1992): 1544–45. http://dx.doi.org/10.1017/s0424820100132352.

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Microstructure of epitaxial layers of doped GaAs and its crystal growth dynamics on single crystal GaAs substrate were studied by Raman microspectroscopy with a Dilor OMARS instrument equipped with a 1024 photodiode multichannel detector and a ion-argon laser Spectra-Physics emitting at 514.5 nm.The spatial resolution of this technique, less than 1 μm2, allows the recording of Raman spectra at several spots in function of thickness, from the substrate to the outer deposit, including areas around the interface (Fig.l).The high anisotropy of the LO and TO Raman bands is indicative of the orientation of the epitaxial layer as well as of the structural modification in the deposit and in the substrate at the interface.With Sn doped, the epitaxial layer also presents plasmon in Raman scattering. This fact is already very well known, but we additionally observed that its frequency increases with the thickness of the deposit. For a sample with electron density 1020 cm-3, the plasmon L+ appears at 930 and 790 cm-1 near the outer surface.

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50

Mehdipour, Nargess, and Saideh Bagheri. "Molecular dynamics simulation of nanoconfined n-decane." Journal of Molecular Liquids 180 (April 2013): 101–6. http://dx.doi.org/10.1016/j.molliq.2013.01.004.

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