Chapter 3: Problem 56
Explain why the properties of polycrystalline materials are most often isotropic.
Chapter 3: Problem 56
Explain why the properties of polycrystalline materials are most often isotropic.
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Get started for freeCalculate the radius of a tantalum atom, given that Ta has a BCC crystal structure, a density of \(16.6 \mathrm{g} / \mathrm{cm}^{3},\) and an atomic weight of \(180.9 \mathrm{g} / \mathrm{mol}.\)
(a) Draw an orthorhombic unit cell, and within that cell a \((02 \overline{1})\) plane. (b) Draw a monoclinic unit cell, and within that cell a (200) plane.
Niobium has an atomic radius of 0.1430 nm and a density of \(8.57 \mathrm{g} / \mathrm{cm}^{3} .\) Determine whether it has an FCC or BCC crystal structure.
(a) Derive planar density expressions for \(\mathrm{BCC}(100)\) and (110) planes in terms of the atomic radius \(R.\) (b) Compute and compare planar density values for these same two planes for molybdenum.
Figure 3.21 shows an x-ray diffraction pattern for lead taken using a diffractometer and monochromatic x-radiation having a wavelength of \(0.1542 \mathrm{nm}\); each diffraction peak on the pattern has been indexed. Compute the interplanar spacing for each set of planes indexed; also determine the lattice parameter of Pb for each of the peaks.
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