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Latvian Journal of Physics and Technical Sciences

The Journal of Institute of Physical Energetics

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Juan A. Aledo, Luis G. Diaz, Silvia Martinez and Jose C. Valverde

, LNCS 10388 1 13 2017 [2] J.A. Aledo, L.G. Diaz, S. Martinez, J.C. Valverde, On the periods of parallel dynamical systems, Complexity 2017 (2017), Article ID 7209762, 6 pages. 10.1155/2017/7209762 . Aledo J.A. Diaz L.G. Martinez S. Valverde J.C. On the periods of parallel dynamical systems Complexity 2017 2017 Article ID 7209762 6 10.1155/2017/7209762 [3] J.A. Aledo, L.G. Diaz, S. Martinez, J.C. Valverde, On periods and equilibria of sequential dynamical systems, Inf. Sci. 409–410 (2017) 27–34. 10.1016/j.ins.2017.05.002 . Aledo J.A. Diaz L.G. Martinez S

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S.O. Pyskunov, Yu.V. Maksimyk and V.V. Valer

strains: ( Δ σ i j ) m = C i j k l ( { Δ ε k l } m − { ( Δ ε k l ) T } m ) . $$\begin{array}{} \displaystyle [{\left( {\Delta {\sigma _{ij}}} \right)_m} = {C_{ijkl}}\left( {{{\left\{ {\Delta {\mkern 1mu} {\varepsilon _{kl}}} \right\}}_m} - {{\left\{ {{{\left( {\Delta {\mkern 1mu} {\varepsilon _{kl}}} \right)}^T}} \right\}}_m}} \right). \end{array}$$ (10) Creep problem solution considering damage accumulation is being executed by means of step-by-step algorithm on the parameter of time. When starting each iteration n of a step m , stress values σ ij are

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Arturo Álvarez-Arenas, Juan Belmonte-Beitia and Gabriel F. Calvo

biological literature, there is a vast range of values for the diffusion and proliferation coefficients. To carry out the estimations, we resort to the following value for the proliferation ρ = 0.2 day −1 , which is in the range [0.01–0.5] day −1 , taken from [ 28 , 54 ] and D = 0.05 mm 2 /day (which is in the range [0.0004–0.1] mm 2 /day) [ 39 ]. Finally, we take α = 1/10 day −1 , L = 85 mm, x 0 = 10 mm, c = c min = 2 ( 1 − β ) , $\begin{array}{} c=c_{\text{min}}=2\sqrt{(1-\beta)}, \end{array} $ M = 0.3, b = 0.005, a = ( cc 2 − 4 ( 1 − β − V

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M. Černeckytė, M. Kurmis, A. Andziulis and G. Gaigals

References 1. Meisel, F., & Bierwirth, C. (2011). A unified approach for the evaluation of quay crane scheduling models and algorithms. Computers & Operations Research, 683-693. doi:10.1016/j.cor.2010.08.001 2. Bierwirth, C., & Meisel, F. (2010). A survey of berth allocation and quay crane scheduling problems in container terminals. European Journal of Operational Research , 615-627. doi:10.1016/j.ejor.2009.05.031 3. W. Yan, Y. Huang, D. Chang, & J. He. (2011). An investigation into knowledge

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M. Kurmis, D. Dzemydiene, R. Didziokas and J. Trokss

., Loke, S. W., & Rahayu, W. (2013). Mobile cloud computing: A survey. Future Generation Computer Systems, 29 (1), 84-106. doi:10.1016/j.future.2012.05.023 4. Liu, K., & Dong, L. (2012). Research on Cloud Data Storage Technology and its Architecture Implementation. Procedia Engineering, 29 , 133-137. doi:10.1016/j.proeng.2011.12.682 5. Mao, H., Xiao, N., Shi, W., & Lu, Y. (2012). Wukong: A cloud-oriented file service for mobile Internet devices. Journal of Parallel and Distributed Computing, 72 (2), 171-184. doi:10.1016/j.jpdc.2011.10

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V. Korsaks, B. Berzina and L. Trinklere

.(b), 224 , (11), 4147-4151. DOI: 10.1002/pssb.200776109. Hua Chen, Ying Chen, Yun Liu, Chao-Nan Xu, & Jim S. Williams. (2007). Light emission and excitonic effect of boron nitride nanotubes observed by photoluminescent spectra. Optical Materials, 29 , 1295-1298. DOI:10.1016/j.optmat.2006.05.006 Berzina, B., Trinkler, L., Krutohvostov, R.,. Williams, R.T, Carroll, D. L., Czerw, R., & Shishonok, E. (2005). Photoluminescence excitation spectroscopy in boron nitride nanotubes compared to microcrystalline h-BN and c

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S. Upnere

single flexible tube predicted by the quasi-steady model in tube bundles. Journal of Fluids and Structures , 56 , 107–123. DOI: 10.1016/j.jfluidstructs.2015.05.004 6. Mahon, J., & Meskell. C. (2013). Estimation of the time delay associated with damping controlled fluidelastic instability in a normal triangular tube array. Journal of Pressure Vessel Technology , 135 , 030903-1-7. DOI: 10.1115/1.4024144 7. Price, S.J. (1995). A review of theoretical models for fluidelastic instability of cylinder arrays in cross-flow. Journal of Fluids and Structures

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M. Krasovska, V. Gerbreders, V. Paskevics, A. Ogurcovs and I. Mihailova

., Maccato, C., Sada, C., Sberveglieric, G., and Tondellod, E. (2010). Urchin-like ZnO nanorod arrays for gas sensing applications. CrystEngComm 12(11), 3419-3421, DOI: 10.1039/ C0CE00139B. 7. Guo, X., Zhao, Q., Li, R., Pan, H., Guo, X., Yin, A., and Dai, W. (2010). Synthesis of ZnO nanofowers and their wettabilities and photocatalytic properties. Opt Express 18(17): 18401-6. DOI: 10.1364/OE.18.018401. 8. Xi, Y., Song, J., Xu, S., Yang, R., Gao, Z., Hu, C. and Wang, Z. (2009). Growth of ZnO nanotube arrays and nanotube based piezoelectric

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I. Pukite, A. Grekis, I. Geipele and N. Zeltins

., & Hoakao, K. (2011). Establishment of the methodology to guide energy – Efficiency renovation of existing residential buildings in China. In International Conference on Computer Distributed Control and Intelligent Environmental Monitoring, 19 – 20 February 2011 (pp. 2203–2210). DOI: http://dx.doi.org/10.1016/j.enbuild.2011.05.005 11. Palm, J., & Reindl, K. (2016). Understanding energy efficiency in Swedish residential building renovation: A practice theory approach. Energy Research & Social Science, 11 , 247–255. ISSN: 2214-6296. DOI: http://doi.org/10.1016/j