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Since these directions are parallel to the crystal principal axis, the shear stress components (i ≠ j) are zero.
The anisotropic material properties for the copper are defined along three planes of symmetry that are parallel to the crystal axes.
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In the following introduction, we take the x, y, and z directions to be parallel to the crystal's [110], [ 1 1 ̄ 0 ], and [001] directions, respectively.
The {2 2 0} and {0 4 0} faces are parallel to the elongation direction of the crystal, while the other faces are at the needle tips direction.
The molecules in the single molecule single crystals and bands are parallel to the substrate, an individual double-striation appearing to consist of a 'double edge', folded chain, lamella more or less normal to the substrate.
In the lamellar crystals, the molecular backbone chains are parallel to the lamellar plane with the alkyl side chains interdigitation in the thickness of lamella.
In each case the polarized FTIR spectra reveal that the absorbance of the NH2 symmetric stretch increases when the polarization is parallel to the long direction of the crystal, indicating that the CPh=N bonds aligned along the channels.
The long axis of the crystals is parallel to the a axis, which corresponds to the channel axis.
By small area X-ray diffraction measurement, it was confirmed that a-axis of unit cell of PTT crystal was parallel to the radial direction of the spherulite.
We found that the b-axis of PLLA crystal was parallel to the lamellae growth direction confirmed using X-ray diffraction.
The crystals were cut so that their face normals were parallel to the orthogonal, and directions, and electric field was applied across the crystal faces normal to the direction.
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