1946
DOI: 10.1103/revmodphys.18.409
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The Elastic Constants of Anisotropic Materials

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Cited by 518 publications
(220 citation statements)
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“…This property was studied much earlier when the elastic moduli of single crystals were measured, 61,79 in which anisotropy was noted to be virtually always present, even in cubic materials, cubic structures requiring three independent elastic constants. Directionally negative values, however, largely went unnoticed because n usually averages out positive for the randomized microstructure of polycrystalline materials.…”
Section: Renaissance Through Interdisciplinarity: Ca 1970 To the Prementioning
confidence: 99%
“…This property was studied much earlier when the elastic moduli of single crystals were measured, 61,79 in which anisotropy was noted to be virtually always present, even in cubic materials, cubic structures requiring three independent elastic constants. Directionally negative values, however, largely went unnoticed because n usually averages out positive for the randomized microstructure of polycrystalline materials.…”
Section: Renaissance Through Interdisciplinarity: Ca 1970 To the Prementioning
confidence: 99%
“…The elastic constants, primarily the compliances, of bulk silver have been measured by several sources [30][31][32][33][34][35] -the most recent by Wolfenden et al 35 Using the expressions for calculating the Young's modulus, E, outlined in Nye 36 , Wolfenden's measurements can be presented in terms of directional Young's moduli as shown in Table II. This table illustrates that in bulk silver, the directionally-dependent Young's modulus, E, is greater in the <111> than in the <200> and <220> directions (E<111> > E<110> > E<100>). If the silver nanoparticles behaved like the bulk material, this would mean that the nanoparticles would more likely compress in the {200} direction than the {111} direction.…”
Section: A Elastic Constantsmentioning
confidence: 99%
“…To directly compare these literature values to the reduced modulus recorded here, we calculate the temperature dependent reduced modulus of Al by (5) where E is the Young's modulus, ν is the Poisson's ratio, and subscripts d and s refer to the properties of diamond and the sample material (in this case Al), respectively. For accuracy, we use both a temperature dependent ν s (values for which are also taken from literature [68][69][70][71][72][73] ) and E d, which is equal to 74 (6) where the superscript RT denotes the room temperature modulus of diamond (~150 GPa 53 ) and c is an empirical constant (-1.027 x 10 -4 K -1 ). Because ν d is usually well-approximated as temperature independent, we use 0.07 53 .…”
Section: Aluminummentioning
confidence: 99%
“…The hardness decreases with temperature as expected for a crystalline metal ( Figure 10A) 52 Although hot hardness values for aluminum are reported in literature, corresponding modulus data are apparently not available. However, temperature-dependent elastic properties for >99.9% pure single-crystal Al have been measured by acoustic methods [68][69][70][71][72][73] . To directly compare these literature values to the reduced modulus recorded here, we calculate the temperature dependent reduced modulus of Al by (5) where E is the Young's modulus, ν is the Poisson's ratio, and subscripts d and s refer to the properties of diamond and the sample material (in this case Al), respectively.…”
Section: Aluminummentioning
confidence: 99%