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12
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6544226089
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Macroscopic energies without the surface energy term were proposed in the classic work of R. Hill, J. Mech. Phys. Solids 11, 357 (1963); the general structure, starting from a variational formulation, has been examined in J. R. Willis, IMA J. Appl. Math. 43, 231 (1989); J. F. Toland and J. R. Willis, SIAM (Soc. Ind. Appl. Math.) J. Math. Anal. 20, 1283 (1989). Bounding the properties of nonlinear composites was initiated by J. R. Willis, J. Appl. Mech. 50, 1202 (1983); J. R. Willis, in Homogenization and Effective Properties of Materials and Media, edited by J. L. Ericksen, D. Kinderlehrer, R. Kohn, and J. L. Lions (Springer, New York, 1986), pp. 245-263; D. R. S. Talbot and J. R. Willis, IMA J. Appl. Math. 35, 39 (1985).
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(1963)
J. Mech. Phys. Solids
, vol.11
, pp. 357
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Hill, R.1
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13
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0024886271
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Macroscopic energies without the surface energy term were proposed in the classic work of R. Hill, J. Mech. Phys. Solids 11, 357 (1963); the general structure, starting from a variational formulation, has been examined in J. R. Willis, IMA J. Appl. Math. 43, 231 (1989); J. F. Toland and J. R. Willis, SIAM (Soc. Ind. Appl. Math.) J. Math. Anal. 20, 1283 (1989). Bounding the properties of nonlinear composites was initiated by J. R. Willis, J. Appl. Mech. 50, 1202 (1983); J. R. Willis, in Homogenization and Effective Properties of Materials and Media, edited by J. L. Ericksen, D. Kinderlehrer, R. Kohn, and J. L. Lions (Springer, New York, 1986), pp. 245-263; D. R. S. Talbot and J. R. Willis, IMA J. Appl. Math. 35, 39 (1985).
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(1989)
IMA J. Appl. Math.
, vol.43
, pp. 231
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Willis, J.R.1
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14
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6544226089
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Macroscopic energies without the surface energy term were proposed in the classic work of R. Hill, J. Mech. Phys. Solids 11, 357 (1963); the general structure, starting from a variational formulation, has been examined in J. R. Willis, IMA J. Appl. Math. 43, 231 (1989); J. F. Toland and J. R. Willis, SIAM (Soc. Ind. Appl. Math.) J. Math. Anal. 20, 1283 (1989). Bounding the properties of nonlinear composites was initiated by J. R. Willis, J. Appl. Mech. 50, 1202 (1983); J. R. Willis, in Homogenization and Effective Properties of Materials and Media, edited by J. L. Ericksen, D. Kinderlehrer, R. Kohn, and J. L. Lions (Springer, New York, 1986), pp. 245-263; D. R. S. Talbot and J. R. Willis, IMA J. Appl. Math. 35, 39 (1985).
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(1989)
SIAM (Soc. Ind. Appl. Math.) J. Math. Anal.
, vol.20
, pp. 1283
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Toland, J.F.1
Willis, J.R.2
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15
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0020917543
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Macroscopic energies without the surface energy term were proposed in the classic work of R. Hill, J. Mech. Phys. Solids 11, 357 (1963); the general structure, starting from a variational formulation, has been examined in J. R. Willis, IMA J. Appl. Math. 43, 231 (1989); J. F. Toland and J. R. Willis, SIAM (Soc. Ind. Appl. Math.) J. Math. Anal. 20, 1283 (1989). Bounding the properties of nonlinear composites was initiated by J. R. Willis, J. Appl. Mech. 50, 1202 (1983); J. R. Willis, in Homogenization and Effective Properties of Materials and Media, edited by J. L. Ericksen, D. Kinderlehrer, R. Kohn, and J. L. Lions (Springer, New York, 1986), pp. 245-263; D. R. S. Talbot and J. R. Willis, IMA J. Appl. Math. 35, 39 (1985).
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(1983)
J. Appl. Mech.
, vol.50
, pp. 1202
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Willis, J.R.1
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16
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6544226089
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edited by J. L. Ericksen, D. Kinderlehrer, R. Kohn, and J. L. Lions Springer, New York
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Macroscopic energies without the surface energy term were proposed in the classic work of R. Hill, J. Mech. Phys. Solids 11, 357 (1963); the general structure, starting from a variational formulation, has been examined in J. R. Willis, IMA J. Appl. Math. 43, 231 (1989); J. F. Toland and J. R. Willis, SIAM (Soc. Ind. Appl. Math.) J. Math. Anal. 20, 1283 (1989). Bounding the properties of nonlinear composites was initiated by J. R. Willis, J. Appl. Mech. 50, 1202 (1983); J. R. Willis, in Homogenization and Effective Properties of Materials and Media, edited by J. L. Ericksen, D. Kinderlehrer, R. Kohn, and J. L. Lions (Springer, New York, 1986), pp. 245-263; D. R. S. Talbot and J. R. Willis, IMA J. Appl. Math. 35, 39 (1985).
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(1986)
Homogenization and Effective Properties of Materials and Media
, pp. 245-263
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Willis, J.R.1
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17
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0002023333
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Macroscopic energies without the surface energy term were proposed in the classic work of R. Hill, J. Mech. Phys. Solids 11, 357 (1963); the general structure, starting from a variational formulation, has been examined in J. R. Willis, IMA J. Appl. Math. 43, 231 (1989); J. F. Toland and J. R. Willis, SIAM (Soc. Ind. Appl. Math.) J. Math. Anal. 20, 1283 (1989). Bounding the properties of nonlinear composites was initiated by J. R. Willis, J. Appl. Mech. 50, 1202 (1983); J. R. Willis, in Homogenization and Effective Properties of Materials and Media, edited by J. L. Ericksen, D. Kinderlehrer, R. Kohn, and J. L. Lions (Springer, New York, 1986), pp. 245-263; D. R. S. Talbot and J. R. Willis, IMA J. Appl. Math. 35, 39 (1985).
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(1985)
IMA J. Appl. Math.
, vol.35
, pp. 39
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Talbot, D.R.S.1
Willis, J.R.2
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18
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0024281332
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In the absence of a surface energy term, P. Ponte Castañeda and J. R. Willis, Proc. R. Soc. London, Ser. A 416, 217 (1998) proved that the overall energy of a nonlinear viscous composite is convex. Application of similar arguments shows that the overall macroscopic energies W̃(Ē) and C̃(Ē) are convex.
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(1998)
Proc. R. Soc. London, Ser. A
, vol.416
, pp. 217
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Ponte Castañeda, P.1
Willis, J.R.2
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20
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0031124862
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R. Lipton, Institute for Mathematics and Its Applications Preprint Series, 1995 (unpublished), Preprint Number 1339; SIAM (Soc. Ind. Appl. Math.) J. Math. Anal. 57, 347 (1997).
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(1997)
SIAM (Soc. Ind. Appl. Math.) J. Math. Anal.
, vol.57
, pp. 347
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23
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85034556916
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submitted
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We mention, in the context of linear two-phase composites, the recent and relevent work of Y. Benveniste and T. Miloh, J. Appl. Phys. (submitted) Motivated by the results given in Lipton and Vernescu Ref. 16 and in Lipton Ref. 14, they have developed a method for choosing a nonconstant interfacial conductivity so that the field external to the inclusion remains undisturbed when linear boundary conditions for the electric potential are given. Their results apply to a large class of inclusion shapes.
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J. Appl. Phys.
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Benveniste, Y.1
Miloh, T.2
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