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4
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0027551703
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C. F. Schmidt, K. Svoboda, N. Lei, I. B. Petsche, L. E. Berman, C. R. Safinya, and G. S. Grest, Science 259, 952 (1993).
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(1993)
Science
, vol.259
, pp. 952
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Schmidt, C.F.1
Svoboda, K.2
Lei, N.3
Petsche, I.B.4
Berman, L.E.5
Safinya, C.R.6
Grest, G.S.7
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6
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85035236456
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Due to entanglement problems during the process of cytoskeleton extraction and fixing to a substrate, the precise degree of regularity of the spectrin network is uncertain. From the membrane shear modulus (approximately [formula presented], 5, the stress-free filament length (approximately [formula presented]), and [formula presented] the effective dimensionless temperature τ for a Hookean spring model of the network is estimated as [formula presented] Such a model is therefore in a relatively low-temperature state.
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Due to entanglement problems during the process of cytoskeleton extraction and fixing to a substrate, the precise degree of regularity of the spectrin network is uncertain. From the membrane shear modulus (approximately 10-5 N/m) 5, the stress-free filament length (approximately 10-7 m), and kBT≈4×10-21 N m, the effective dimensionless temperature τ for a Hookean spring model of the network is estimated as τ≈0.04. Such a model is therefore in a relatively low-temperature state.
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12
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0031236192
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As we have discussed, a critical point seems to be impossible. It should be noted that the simulations in question are done with an ensemble of fixed volume and fixed shape. The latter restriction may frustrate collapse of the network so as to force the formation of a superlattice (see Fig. 44 of the present reference). Also, the reported results appear to be restricted to mesh areas above the phase coexistence region, except at very low temperature. JPGCE8
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W. Wintz, R. Everaers, and U. Seifert, J. Phys. I 7, 1097 (1997). As we have discussed, a critical point seems to be impossible. It should be noted that the simulations in question are done with an ensemble of fixed volume and fixed shape. The latter restriction may frustrate collapse of the network so as to force the formation of a superlattice (see Fig. 44 of the present reference). Also, the reported results appear to be restricted to mesh areas above the phase coexistence region, except at very low temperature.JPGCE8
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(1997)
J. Phys. I
, vol.7
, pp. 1097
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Wintz, W.1
Everaers, R.2
Seifert, U.3
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13
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85035198960
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The conventional Lagrangian strain [formula presented] with respect to the state [formula presented] is related by [formula presented]
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The conventional Lagrangian strain E with respect to the state M̃ is related by E=(1/2)[(MM-1)T(MN-1)-1].
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15
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0030269818
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JPGCE8
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M. J. Bowick, J. Phys. I 6, 1321 (1996). JPGCE8
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(1996)
J. Phys. I
, vol.6
, pp. 1321
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Bowick, M.J.1
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