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3
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42749099324
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C. A. Murray S. W. Kamp J. M. Thomas J. R. Dutcher Phys. Rev. E: Stat., Nonlinear, Soft Matter Phys. 2004 69 061612
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Phys. Rev. E: Stat., Nonlinear, Soft Matter Phys.
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Murray, C.A.1
Kamp, S.W.2
Thomas, J.M.3
Dutcher, J.R.4
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6
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0000278288
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T. Nishikawa J. Nishida R. Ookura S. I. Nishimura S. Wada T. Karino M. Shimomura Mater. Sci. Eng., C 1999 8-9 495
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Mater. Sci. Eng., C
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Nishikawa, T.1
Nishida, J.2
Ookura, R.3
Nishimura, S.I.4
Wada, S.5
Karino, T.6
Shimomura, M.7
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25
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33746221078
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This is appropriate for modelling Dutcher films as while the thin films are on the order of 100 nm thick, the wavelengths of the undulations are on the order of micrometers. Large-scale microscopic models can capture the physics of polymer systems on the 100 nanometere scale, however, in order to capture the miscroscale undulations considered here a continuum model is required
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This is appropriate for modelling Dutcher films as while the thin films are on the order of 100 nm thick, the wavelengths of the undulations are on the order of micrometers. Large-scale microscopic models can capture the physics of polymer systems on the 100 nanometere scale, however, in order to capture the miscroscale undulations considered here a continuum model is required
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29
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33746221075
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The computer model consists of a discrete finite difference approximation of the continuum equations. Therefore, it is necessary to know the values of the internal forces at these discrete locations, such that the overall deformation is isotropic. To do this we used the lattice spring model (LSM) methodology. The LSM consists of a regular lattice of springs and can be shown to be equivalent to continuum elasticity theory
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y represent the interfaces between areas of positive and negative Δh
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30
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0035503826
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If a region of a LSM was to undergo a change in volume then this could be realised through the application of internal forces such that the equilibrium bond length changed length (bonds that straddle the circular domain have interpolated forces). By incorporating such internal forces, from a LSM and into our finite difference model of Dutcher films, we were able to obtain an isotropic volume change through the application of internal forces at discrete locations
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G. A. Buxton C. M. Care D. J. Cleaver Model. Simul. Mater. Sci. Eng. 2001 9 485
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(2001)
Model. Simul. Mater. Sci. Eng.
, vol.9
, pp. 485
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Buxton, G.A.1
Care, C.M.2
Cleaver, D.J.3
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