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Статті в журналах з теми "State mode"

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Автор: Grafiati

Опубліковано: 30 травня 2022

Оновлено: 31 травня 2022

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1

Jun-Xiang, Zhang, Jing Jie-Tai, Xie Chang-De, and Peng Kun-Chi. "Quantum State Sharing by Using Two-Mode and Single-Mode Squeezed State Lights." Chinese Physics Letters 22, no. 11 (October 27, 2005): 2751–54. http://dx.doi.org/10.1088/0256-307x/22/11/007.

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2

Hao, Haitian, Carlo Scalo, and Fabio Semperlotti. "Flexural-mode solid-state thermoacoustics." Mechanical Systems and Signal Processing 148 (February 2021): 107143. http://dx.doi.org/10.1016/j.ymssp.2020.107143.

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3

Zhang Qian, Li Fu-Li, and Li Hong-Rong. "Teleportation of a two-mode Gaussian state through double two-mode-squeezed-state quantum channels." Acta Physica Sinica 55, no. 5 (2006): 2275. http://dx.doi.org/10.7498/aps.55.2275.

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4

Kovalenko, G. P., and S. V. Kolomiets. "Periodic Oscillating Modes in Single-Mode Solid-State Lasers." Telecommunications and Radio Engineering 61, no. 3 (2004): 256–71. http://dx.doi.org/10.1615/telecomradeng.v61.i3.60.

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5

Hao, Shu-Hong, Xian-Shan Huang, and Dong Wang. "General Single-Mode Gaussian Operation with Two-Mode Entangled State." Chinese Physics Letters 34, no. 7 (July 2017): 070301. http://dx.doi.org/10.1088/0256-307x/34/7/070301.

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6

HU, LI-YUN, and HONG-YI FAN. "SQUEEZING ENHANCED THREE-MODE ENTANGLED STATE." Modern Physics Letters B 22, no. 22 (August 30, 2008): 2055–61. http://dx.doi.org/10.1142/s0217984908016662.

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Анотація:

By virtue of the technique of integration within an ordered product of operators (Fan et al., Ann. Phys.321 (2006) 480) we construct a kind of three-mode entangled squeezed state in the Fock space, which exhibits stronger squeezing in one quadrature than that of the usual two-mode squeezed vacuum state.

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7

Li, Min, Kaiming Yang, Yu Zhu, Haihua Mu, and Chuxiong Hu. "State/Model-Free Variable-Gain Discrete Sliding Mode Control for an Ultraprecision Wafer Stage." IEEE Transactions on Industrial Electronics 64, no. 8 (August 2017): 6695–705. http://dx.doi.org/10.1109/tie.2016.2645893.

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8

Sidlauskaite, Justina, Edmund Sonuga-Barke, Herbert Roeyers, and Roeljan Wiersema. "State-to-state switching in ADHD: Default mode network abnormalities." International Journal of Psychophysiology 108 (October 2016): 29. http://dx.doi.org/10.1016/j.ijpsycho.2016.07.090.

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9

Zhao, Bin, Zhigang Sun, and Hua Guo. "State-to-State Mode Specificity: Energy Sequestration and Flow Gated by Transition State." Journal of the American Chemical Society 137, no. 50 (December 11, 2015): 15964–70. http://dx.doi.org/10.1021/jacs.5b11404.

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10

Zhang, Zexin, Jinrong Tian, Youshuo Cui, Yunfeng Wu, and Yanrong Song. "Dynamics of multi-state in a simplified mode-locked Yb-doped fiber laser." Chinese Optics Letters 20, no. 8 (2022): 081402. http://dx.doi.org/10.3788/col202220.081402.

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11

Tang, T. F., X. Q. Xu, G. Q. Li, J. L. Chen, V. S. Chan, T. Y. Xia, X. Gao, D. Z. Wang, and J. G. Li. "Edge-localized-mode simulation in CFETR steady-state scenario." Nuclear Fusion 62, no. 1 (December 2, 2021): 016008. http://dx.doi.org/10.1088/1741-4326/ac3294.

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Анотація:

Abstract The EPED1 model and self-consistent core-pedestal coupling in integrated modeling are used to design the pedestal structure of the China Fusion Engineering Testing Reactor (CFETR) steady-state scenario. The key parameters, such as β p and q 95, are based on the grassy edge-localized-mode (ELM) experimental database. In this work, we use the BOUT++ six-field two-fluid code to simulate the onset of the ELM in the CFETR steady-state scenario. The ELM size is around 0.2% in nonlinear simulations, which is in the experimental range of the grassy ELM discharges, 0.1%–1% observed in multiple tokamak devices. Linear and nonlinear simulations show that the dominant high-n ballooning modes peak around n = 40. Compared to type-I ELM crashing dynamics, grassy ELM crashing has a smaller initial crash and is then followed by three phases of turbulence spreading, which are dominated by multi-modes, a high-n mode of n = 45 and low-n mode of n = 5, respectively. In contras to type-I ELM, the perturbation of the high-n mode has a narrow width around ψ = 0.95, and magnetic island formation and reconnection occur only beyond ψ = 0.95, leading to a small initial crash. Mode–mode interaction in the multi-mode coexistence stage stops the growth of individual modes and reduces the transport of particles and heat, and these are the two reasons why the ELM size is small. In–out asymmetry of transient heat flux with a ratio of E out/E in = 3.5 is found during grassy ELM crash. The rise and delay times of the heat flux match the calculation from the free-streaming model. To evaluate the erosion of the divertor target, the energy fluence at the outer divertor target is calculated, which is 0.029 MJ m−2, 5.5 times smaller than the tungsten melting limit 0.16 MJ m−2. The calculated energy fluency still follows the experimental scaling law from type-I ELM experiments. The fluctuation eddies in the toroidal direction show a filament structure at the outer mid-plane. Parallel heat flux patterns with a toroidal mode number n = 10 are found at the outer divertor with an amplitude of 680 MW m−2.

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12

PADMANABHAN, SANDEEP, and YANN-HANG LEE. "EFFICIENT STATE-SAVING ARCHITECTURES FOR POWER-MODE SWITCHING." International Journal of Software Engineering and Knowledge Engineering 15, no. 02 (April 2005): 379–88. http://dx.doi.org/10.1142/s0218194005001914.

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Time and energy is expended in switching between power modes (e.g., active, hibernate, sleep, etc.). Powering off cache is one major reason for this. When there is a switch in the power-mode involving cache power-off, the system spends time and energy in filling the cache with new data (inherent cache misses). In our technique, before powering off the cache, we save its state in Embedded DRAM and bring it back when the previous power mode is restored. Our experiments have showed that in a majority of cases the cache contents are too valuable to be erased. By saving the contents we can reduce switching speed and energy. We present a heuristic to save the most relevant cache contents so that power and delay overheads are minimized. To measure the area overhead a synthesizable VHDL model was designed.

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13

Li-Yun, Hu, and Fan Hong-Yi. "Two-Variable Hermite Polynomial Excitation of Two-Mode Squeezed Vacuum State as Squeezed Two-Mode Number State." Communications in Theoretical Physics 50, no. 4 (October 2008): 965–70. http://dx.doi.org/10.1088/0253-6102/50/4/35.

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14

Chai, Chin-lin. "Two-mode nonclassical state via superpositions of two-mode coherent states." Physical Review A 46, no. 11 (December 1, 1992): 7187–91. http://dx.doi.org/10.1103/physreva.46.7187.

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15

Fujimoto, Yukinobu, and Kazumasa Miyake. "Mode–mode coupling theory of itinerant electron antiferromagnetism in superconducting state." Journal of Physics: Condensed Matter 24, no. 40 (September 4, 2012): 405701. http://dx.doi.org/10.1088/0953-8984/24/40/405701.

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16

Mensik, Miroslav, and Stanislav Nespurek. "Role of Mode-mode Coupling in Short-time Excited State Decay." Czechoslovak Journal of Physics 55, no. 5 (May 2005): 579–92. http://dx.doi.org/10.1007/s10582-005-0062-6.

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17

Aston, P. "Numerical methods for steady-state mode interactions." IMA Journal of Numerical Analysis 16, no. 3 (July 1, 1996): 435–56. http://dx.doi.org/10.1093/imanum/16.3.435.

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18

Seeley, G., and T. Keyes. "Normal‐mode analysis of liquid‐state dynamics." Journal of Chemical Physics 91, no. 9 (November 1989): 5581–86. http://dx.doi.org/10.1063/1.457664.

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19

Choi, Jin-Hee, Eduardo A. Misawa, and Gary E. Young. "A Study on Sliding Mode State Estimation." Journal of Dynamic Systems, Measurement, and Control 121, no. 2 (June 1, 1999): 255–60. http://dx.doi.org/10.1115/1.2802463.

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The design of sliding observers is discussed in the paper. The sliding observer is shown to have a simple structure and to be robust with respect to bounded nonlinearities and uncertainties. The Lyapunov-like stability method is used to investigate the stability of sliding observers without assuming the matching condition and a computer-aided design methodology is suggested. A numerical example based on an inverted pendulum with moving support is used to illustrate the proposed design methodology.

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20

Berman, Joel M., and Lionel Goodman. "The a2g mode in ground state benzene." Journal of Chemical Physics 87, no. 3 (August 1987): 1479–87. http://dx.doi.org/10.1063/1.453257.

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21

Paul, H., P. Törmä, T. Kiss, and I. Jex. "Two-mode state reconstruction using photon chopping." Journal of Modern Optics 44, no. 11-12 (November 1997): 2395–404. http://dx.doi.org/10.1080/09500349708231890.

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22

Kalashnikov, V. L., V. P. Kalosha, V. P. Mikhaĭlov, I. G. Poloĭko, and M. I. Demchuk. "Passive mode locking in widebandcwsolid-state lasers." Quantum Electronics 23, no. 2 (February 28, 1993): 125–28. http://dx.doi.org/10.1070/qe1993v023n02abeh002954.

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23

Qian, Xiao-Qing, and Tong-Qiang Song. "Squeezing Transformation of Three-Mode Entangled State." Communications in Theoretical Physics 44, no. 5 (November 2005): 911–16. http://dx.doi.org/10.1088/6102/44/5/911.

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24

Hong-Yi, Fan, and Fan Yue. "Teleportation of a Two-Mode Squeezed State." Chinese Physics Letters 19, no. 2 (February 2002): 159–62. http://dx.doi.org/10.1088/0256-307x/19/2/305.

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25

He, Rui, Hong-Yi Fan, Jun Song, and Jun Zhou. "Laguerre-Polynomial-Weighted Two-Mode Squeezed State." International Journal of Theoretical Physics 55, no. 7 (February 29, 2016): 3329–37. http://dx.doi.org/10.1007/s10773-016-2962-6.

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26

Fan, Rui-qin, Hong-guang Yang, and Zhi-ming Bai. "Two-mode squeezed state of nanomechanical resonators." Applied Mathematics and Mechanics 30, no. 9 (September 2009): 1161–67. http://dx.doi.org/10.1007/s10483-009-0910-y.

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27

Wenlong Tian, Wenlong Tian, Jiangfeng Zhu Jiangfeng Zhu, Zhaohua Wang Zhaohua Wang, and Zhiyi Wei Zhiyi Wei. "Efficient femtosecond optical parametric oscillator pumped by all solid-state mode-locking Yb:YCOB laser." Chinese Optics Letters 13, no. 1 (2015): 011901–11903. http://dx.doi.org/10.3788/col201513.011901.

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28

Parker, Ryan C., Jaewoo Joo, and Timothy P. Spiller. "Photonic hybrid state entanglement swapping using cat state superpositions." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 476, no. 2243 (November 2020): 20200237. http://dx.doi.org/10.1098/rspa.2020.0237.

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We propose the use of hybrid entanglement in an entanglement swapping protocol, as means of distributing a Bell state with high fidelity to two parties. The hybrid entanglement used in this work is described as a discrete variable (Fock state) and a continuous variable (cat state super- position) entangled state. We model equal and unequal levels of photonic loss between the two propagating continuous variable modes, before detecting these states via a projective vacuum-one-photon measurement, and the other mode via balanced homodyne detection. We investigate homodyne measurement imperfections, and the associated success probability of the measurement schemes chosen in this protocol. We show that our entanglement swapping scheme is resilient to low levels of photonic losses, as well as low levels of averaged unequal losses between the two propagating modes, and show an improvement in this loss resilience over other hybrid entanglement schemes using coherent state superpositions as the propagating modes. Finally, we conclude that our protocol is suitable for potential quantum networking applications which require two nodes to share entanglement separated over a distance of 5 -- 10 km , when used with a suitable entanglement purification scheme.

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29

Kadochnikov, I. N., B. I. Loukhovitski, and A. M. Starik. "A modified model of mode approximation for nitrogen plasma based on the state-to-state approach." Plasma Sources Science and Technology 24, no. 5 (August 20, 2015): 055008. http://dx.doi.org/10.1088/0963-0252/24/5/055008.

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30

Kroutikova, N., C. A. Hernandez-Aramburo, and T. C. Green. "State-space model of grid-connected inverters under current control mode." IET Electric Power Applications 1, no. 3 (2007): 329. http://dx.doi.org/10.1049/iet-epa:20060276.

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31

Galatenko, G. V. "Dugdale-type model for a mixed-mode crack: plane stress state." International Applied Mechanics 47, no. 1 (June 2011): 78–85. http://dx.doi.org/10.1007/s10778-011-0445-2.

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32

Lo Iudice, N., A. A. Raduta, and D. S. Delion. "Scissors mode and nuclear deformation in the generalized coherent state model." Physics Letters B 300, no. 3 (February 1993): 195–98. http://dx.doi.org/10.1016/0370-2693(93)90352-i.

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33

Xue-Fen, Xu, and Zhu Shi-Qun. "Single-mode photon number measurement for the squeezed two-mode number state." Chinese Physics B 18, no. 4 (March 17, 2009): 1512–16. http://dx.doi.org/10.1088/1674-1056/18/4/037.

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34

Kim, Young Jong, Hyun-Gyu Kim, and Seyoung Im. "Mode decomposition of three-dimensional mixed-mode cracks via two-state integrals." International Journal of Solids and Structures 38, no. 36-37 (September 2001): 6405–26. http://dx.doi.org/10.1016/s0020-7683(00)00408-x.

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35

Li, X. C., H. Y. Fan, and Z. H. Li. "Collapse of a two-mode squeezed state after registeringn-single mode photons." Journal of Modern Optics 59, no. 11 (June 20, 2012): 988–91. http://dx.doi.org/10.1080/09500340.2012.691562.

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36

Xu, Xiao-Yin, Sheng-Shuai Liu, and Jie-Tai Jing. "Amplification of entangled beam based on four-wave mixing process." Acta Physica Sinica 71, no. 5 (2022): 050301. http://dx.doi.org/10.7498/aps.71.20211324.

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Two-mode entangled state is an important quantum resource for quantum information. In this paper, the amplification of a single mode of two-mode entangled state (single-mode amplification scheme) and two modes of two-mode entangled state (two-mode amplification scheme) are theoretically proposed. Here, the optical beam splitter model is used to simulate the vacuum noise introduced by the loss in the optical transmission process. By utilizing the positivity under partial transpose criterion, we analyze the effect of the gain of the four-wave mixing process on the entanglement degree of the initial two-mode entangled state in two different amplification schemes. In these two schemes, we set the gain of the initial two-mode entangled state generation process to be 1.5, 2.5 and 50.0 respectively, and then change the gain of the amplification process in a certain range. We also set the transmission efficiency of the amplified beams for each of the two schemes to be a definite value. The results show that the entanglement of the initial two-mode entangled state decreases with the gain increasing under the condition of specific transmission loss in two schemes. When the gain does not exceed a certain value, the entanglement of the initial two-mode entangled state can be maintained. Then, with the increase of the gain, the entanglement of the initial two-mode entangled state will disappear. Moreover, the entanglement of the initial two-mode entangled state of the two-mode amplification scheme disappears faster than that of the single-mode amplification scheme. Our theoretical results pave the way for the experimental realization of the amplification of two-mode entangled state based on four-wave mixing process.

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37

Majid, Abdul, Raden Sumiharto, and Setyawan Bekti Wibisono. "Identifikasi Model dari Pesawat Udara Tanpa Awak Sayap Tetap Jenis Bixler." IJEIS (Indonesian Journal of Electronics and Instrumentation Systems) 5, no. 1 (May 1, 2015): 43. http://dx.doi.org/10.22146/ijeis.7152.

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AbstrakModel terbang merupakan bagian penting dalam pembangunan sistem kontrol suatu pesawat udara tanpa awak sayap tetap, terutama dalam pembangunan sistem kendali mandiri atau autopilot pesawat. Dengan model terbang, gerak terbang pesawat dapat direpresentasikan dan disimulasikan. Pada penelitian ini, model terbang dihasilkan melalui identifikasi sistem atau pemodelan pesawat udara tanpa awak sayap tetap jenis Bixler. Identifikasi sistem dilakukan berdasarkan eksperimen (pengambilan data terbang) dan digunakan struktur model state-space. Terdapat tiga tahapan dalam penelitian ini, pemodelan gerak terbang pesawat, pengambilan data terbang, dan identifikasi model terbang. Melalui tiga tahapan tersebut, diperoleh model terbang pesawat sayap tetap jenis Bixler yang dapat merepresentasikan gerak terbang pesawat yang terbagi dalam 2 mode, mode longitudinal dan mode lateral.Diperoleh model terbang mode longitudinal pesawat udara tanpa awak sayap tetap jenis Bixler menggunakan 13 parameter menggunakan struktur model state-space orde 4. Model terbang mode lateral pesawat udara tanpa awak sayap tetap jenis Bixler menggunakan 11 parameter menggunakan struktur model state-space orde 4. Kata kunci—UAV, Identifikasi Sistem, Pemodelan AbstractFlight model is one of importing thing in fixed-wing unmanned aerial vehicle (UAV) control system development, mainly in the aircraft autopilot. Through this flight model, the aircraft motion can be represented and simulated.In this research, the flight model is obtained through system identification and system modelling of Bixler fixed-wing unmanned aerial vehicle. System identification is based on experiment data and use state-space model structure. There are three stages in this research, aircraft motion system modelling, flight data collecting, and flight model identification. Through those three stages, Bixler fixed-wing unmanned aerial vehicle flight model is obtained as represented in two modes, longitudinal mode and lateral modeThe Bixler fixed-wing unmanned aerial vehicle longitudinal mode flight model is obtained using 13 parameters. The lateral mode is obtained using 11 parameters. All modes are in 4th order state space model structure. Keywords— UAV, System Identification, Modelling

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38

Armenise, Iole, and Elena Kustova. "Effect of Asymmetric Mode on CO2 State-to-State Vibrational-Chemical Kinetics." Journal of Physical Chemistry A 122, no. 44 (October 15, 2018): 8709–21. http://dx.doi.org/10.1021/acs.jpca.8b07523.

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39

Ren, Gang, Jiangang Qi, and Tong-qiang Song. "AnN-mode squeezed vacuum state in Fock space as an entangled state." Journal of Physics A: Mathematical and Theoretical 40, no. 33 (August 1, 2007): 10311–18. http://dx.doi.org/10.1088/1751-8113/40/33/022.

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40

Oudejans, L., and R. E. Miller. "Mode dependence of the state-to-state vibrational dynamics of HCN–HF." Chemical Physics 239, no. 1-3 (December 1998): 345–56. http://dx.doi.org/10.1016/s0301-0104(98)00358-9.

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41

Kurtz, Lukas, Angelika Hofmann, and Regina de Vivie-Riedle. "Ground state normal mode analysis: Linking excited state dynamics and experimental observables." Journal of Chemical Physics 114, no. 14 (April 8, 2001): 6151–59. http://dx.doi.org/10.1063/1.1355658.

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42

Shan-Jun, Ma, and Wang Shu-Jing. "A Kind of Atomic Coherent State as a Two-Mode Squeezed State." Communications in Theoretical Physics 52, no. 3 (September 2009): 511–16. http://dx.doi.org/10.1088/0253-6102/52/3/25.

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43

Wu, E., Yong Hong Ma, Li Xia Zeng, and Xiao An Zhang. "Continuous Variable Remote State Preparation with a Two-Mode Squeezed Vacuum State." International Journal of Theoretical Physics 47, no. 6 (November 6, 2007): 1600–1605. http://dx.doi.org/10.1007/s10773-007-9600-2.

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44

Jing, Wei, Yang Xia, Min Li, Yan Cui, Mingming Chen, Miaomiao Xue, Daqing Guo, Bharat B. Biswal, and Dezhong Yao. "State-independent and state-dependent patterns in the rat default mode network." NeuroImage 237 (August 2021): 118148. http://dx.doi.org/10.1016/j.neuroimage.2021.118148.

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45

Dao-ming, Lu. "Quantum Properties of Single-Mode Squeezing and Two-Mode Squeezing Repeated Role Two-Mode Vacuum State." International Journal of Theoretical Physics 54, no. 7 (January 14, 2015): 2289–98. http://dx.doi.org/10.1007/s10773-014-2451-8.

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46

Smithson, Sean C., and Sheldon S. Williamson. "A Unified State-Space Model of Constant-Frequency Current-Mode-Controlled Power Converters in Continuous Conduction Mode." IEEE Transactions on Industrial Electronics 62, no. 7 (July 2015): 4514–24. http://dx.doi.org/10.1109/tie.2015.2412514.

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47

Drexel, Michael V., Jerry H. Ginsberg, and Bassem R. Zaki. "State Space Implementation of the Algorithm of Mode Isolation." Journal of Vibration and Acoustics 125, no. 2 (April 1, 2003): 205–13. http://dx.doi.org/10.1115/1.1547463.

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The Algorithm of Mode Isolation (AMI) extracts modal properties from complex frequency response data. Previous work used classic undamped modes as the analytical framework for the algorithm. The present work extends the algorithm to implement damped modal analysis, in which the eigenvalues and eigenvectors are complex. In order to assess how well this reformulation performs when natural frequencies are close and drive point mobilities are low, a prototypical system consisting of a cantilever beam with attached subsystems is introduced. One of these subsystems is selected to be a tuned vibration absorber for the isolated beam, so the system features a combination of modes whose natural frequencies are close and modes whose drive point mobility is low. The time domain response of this system is evaluated, contaminated with substantial white noise, and then FFT processed in order to obtain synthetic complex frequency response data. The performance of AMI is evaluated by comparing extracted values for natural frequency, modal damping ratio, and complex normal mode vectors to the analytical values. The results reveal that the pair of modes having proximite natural frequencies are accurately identified. Natural frequencies and damping ratios for those modes whose drive mobility is low are identified by processing the ensemble of frequency response functions, but identification of normal mode coefficients for such modes remains problematic.

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48

Kamenev, Yurii Borisovich, Georgii Alekseevich Shtompel', and Yurii Vasil'evich Skachkov. "Accelerated charge method of the lead-acid batteries. 2. Constant current charge." Electrochemical Energetics 13, no. 2 (2013): 70–76. http://dx.doi.org/10.18500/1608-4039-2013-13-2-70-76.

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Strategy of the accelerated mode of the charge of the lead-acid batteries, including constant current charge to 80% state-of-charge and a pulse charge to 100% is considered. Various modes one — and two-stage constant current charges are studied in this work, and the estimation of influence of these modes on effectiveness ratio of a charge and a heat-up of batteries is yielded. The data, which allows reasonably choose the mode of the first stage of the accelerated charge to 80% state-of-charge, are presented.

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49

Bauer, S. E., D. Wright, D. Koch, E. R. Lewis, R. McGraw, L. S. Chang, S. E. Schwartz, and R. Ruedy. "MATRIX (Multiconfiguration Aerosol TRacker of mIXing state): an aerosol microphysical module for global atmospheric models." Atmospheric Chemistry and Physics Discussions 8, no. 3 (May 29, 2008): 9931–10003. http://dx.doi.org/10.5194/acpd-8-9931-2008.

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Abstract. A new aerosol microphysical module MATRIX, the Multiconfiguation Aerosol TRacker of mIXing state, and its application in the Goddard Institute for Space Studies (GISS) climate model (ModelE) is described. This module, which is based on the quadrature method of moments (QMOM), represents nucleation, condensation, coagulation, internal and external mixing, and cloud-drop activation and provides aerosol particle mass and number concentration and particle size information for up to 16 mixed-mode aerosol populations. Internal and external mixing among aerosol components sulfate, nitrate, ammonium, carbonaceous aerosols, dust and sea-salt particles are represented. The solubility of each aerosol mode, which is explicitly calculated based on its soluble and insoluble components, enables calculation of the dependence of cloud drop activation on the microphysical characterization of multiple soluble modes. A detailed model description and results of box-model simulations of various mode configurations are presented. The number concentration of aerosol particles activated to cloud drops depends on the mode configuration. Simulations on the global scale with the GISS climate model are evaluated against aircraft and station measurements of aerosol mass and number concentration and particle size. The model accurately captures the observed size distributions in the aitken and accumulation modes up to particle diameter 1 μm, in which sulfate, nitrate, black and organic carbon are predominantly located; however the model underestimates coarse-mode number concentration and size, especially in the marine environment.

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50

Peng, Zhangli, Sara Salehyar, and Qiang Zhu. "Stability of the tank treading modes of erythrocytes and its dependence on cytoskeleton reference states." Journal of Fluid Mechanics 771 (April 20, 2015): 449–67. http://dx.doi.org/10.1017/jfm.2015.187.

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We studied the tank treading motion of an erythrocyte (red blood cell, or RBC) in linear shear flows by using a boundary-element fluid-dynamics model coupled with a multiscale structural model of the cell. The purpose was to investigate the correlation between the reference (stress-free) state of the cytoskeleton and the cell dynamics in shear flows with relatively high capillary numbers. We discovered that there exist two distinctive modes of tank treading, mode 1 and mode 2. In mode 1 the membrane elements originating from the dimple areas keep close to the central plane, whereas in mode 2 these elements remain near the farthermost locations from the central plane. Mode 1 is also characterized by significantly higher breathing and swinging oscillations. During tank treading one mode may become unstable and switch to the other. Their stability depends on the viscosity ratio and the capillary number. At a fixed viscosity ratio, when the capillary number is increased the cell experiences sequentially a region dominated by mode 2, a mode 1/mode 2 bistable region and a region dominated by mode 1. More profoundly, these regions are highly sensitive to the reference state of the cytoskeleton. For example, compared with a cell with a biconcave reference state, a cell with a spheroidal reference state features a much smaller region dominated by mode 2. This finding may guide experiments to identify the actual reference state of these cells.

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