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1
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0001247349
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A. Lobkovsky, S. Gentges, Hao Li, D. Morse, and T. A. Witten, Science 270, 1482 (1995).SCIEAS
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(1995)
Science
, vol.270
, pp. 1482
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Lobkovsky, A.1
Gentges, S.2
Morse, D.3
Witten, T.A.4
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10
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85037198772
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The Gaussian curvature is defined as the product of the two principle curvatures, and the mean curvature is defined as the half sum of the two principle curvatures
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The Gaussian curvature is defined as the product of the two principle curvatures, and the mean curvature is defined as the half sum of the two principle curvatures.
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13
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85037239176
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(private communication)
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L. Mahadevan (private communication).
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Mahadevan, L.1
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14
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85037227725
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Th. von Kármán and H.-S. Tsien, J. Aeronaut. Sci, 8, 303 (1941)
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Th. von Kármán and H.-S. Tsien, J. Aeronaut. Sci, 8, 303 (1941).
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18
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85037196119
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Th. von Kármán, in Encyklopädie der Mathematischen Wissenschafen (Forchungsarbeiten, Berlin, 1910), Vol. IV.4, p. 349
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Th. von Kármán, in Encyklopädie der Mathematischen Wissenschafen (Forchungsarbeiten, Berlin, 1910), Vol. IV.4, p. 349.
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22
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85037200241
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The range of the strain relief temperature is between (Formula presented)C and (Formula presented)C for ETP copper and between (Formula presented)C and (Formula presented)C for DHP copper
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The range of the strain relief temperature is between (Formula presented)C and (Formula presented)C for ETP copper and between (Formula presented)C and (Formula presented)C for DHP copper.
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24
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85037186012
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The deflection due to vertical displacement of the border is given by the expression (Formula presented), where (Formula presented) is the Poisson coefficient, (Formula presented) is the thickness of the plate, (Formula presented) is the bending moment, and (Formula presented); the length of these waves is (Formula presented), which is negligible with respect to the crease length and the panel length
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The deflection due to vertical displacement of the border is given by the expression (Formula presented), where (Formula presented) is the Poisson coefficient, (Formula presented) is the thickness of the plate, (Formula presented) is the bending moment, and (Formula presented); the length of these waves is (Formula presented), which is negligible with respect to the crease length and the panel length.
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25
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85037195183
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When the crease appears, the region around the crease then acquires a zero curvature and the strip buckles like a planar plate
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When the crease appears, the region around the crease then acquires a zero curvature and the strip buckles like a planar plate.
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26
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85037233892
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L. Landau and E. Lifchitz, Théorie de l’Élasticité (Mir, Moscow, 1967)
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L. Landau and E. Lifchitz, Théorie de l’Élasticité (Mir, Moscow, 1967).
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29
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0039905589
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Z. Zhang, H. T. Davis, R. S. Maier, and D. M. Kroll, Phys. Rev. B 52, 5404 (1995).PRBMDO
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(1995)
Phys. Rev. B
, vol.52
, pp. 5404
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Zhang, Z.1
Davis, H.T.2
Maier, R.S.3
Kroll, D.M.4
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30
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85037177575
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We performed the scaling by including logarithmic contributions in the bending energy; the scaling is qualitatively the same
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We performed the scaling by including logarithmic contributions in the bending energy; the scaling is qualitatively the same.
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