Plane, John

Figure 14 Angles y and iji defining the position of the normal to a given hkl crystal plane in the sample reference system. Ix, incident X-ray beam lhkl, diffracted intensity 6B, Bragg angle. Adapted from Lafrance et al. [82]. Reprinted with permission of John Wiley 8t Sons, Inc.

Secretary Morgenthau being needed urgently in Washington, he left by plane. I remained in London to negotiate the Hungarian offer. After I spoke to our Ambassador, John Winant, he decided to see Anthony Eden, the British Foreign Secretary. 

In 1822, the British astronomer Sir John Herschel observed that there was a correlation between hemihedralism and optical rotation. He found that all quartz crystals having the odd faces inclined in one direction rotated the plane of polarized light in one direction, while the enantiomorphous crystals rotate the polarized light in the opposite direction. 

Figure 1.24 Definition of Miller indices for an arbitrary plane (shaded area). From Z. Jastrzebski, The Nature and Properties of Engineering Materials, 2nd ed. Copyright 1976 by John Wiley Sons, Inc. This material is nsed by permission of John Wiley Sons, Inc.

Figure 5.10 Schematic illustration of (a) relative shear of two planes of atoms in a strained material and (b) shear stress as a function of relative displacement of the planes from their equilibrium positions. Reprinted, by permission, from C. Kittel, Introduction to Solid State Physics, 2nd ed., p. 517. Copyright 1957 by John Wiley Sons, Inc.

Figure 5.11 Schematic illustration edge dislocation motion in response to an applied shear stress, where (a) the extra half-plane is labeled as A (cf. Figure 1.28), (b) the dislocation moves one atomic distance to the right, and (c) a step forms on the crystal surface as the extra half-plane exits the crystal. Reprinted, by permission, from W. Callister, Materials Science and Engineering An Introduction, 5th ed., p. 155. Copyright 2000 by John Wiley Sons, Inc.

Fig. 7.134. The half-crystal (or kink) position. The figure shows the binding energy of an atom in a kink position and how the name half-crystal position has been derived. A represents the missing part of the bulk crystal above the surface plane, fithe missing half of the surface plane, and Cthe missing half of the atomic row along the step in front of the kink atom. Together they add the halfcrystal to a bulk crystal. (Reprinted from E. Budevski, G. Staikov, and W. J. Lorenz, Electrochemical Phase Formation and Growth, 18, copyright 1996, John Wiley Sons. Reproduced by permission of John Wiley Sons, Ltd.)...

Figure 13 Decomposition of a plane wave into spherical waves (a) real part. The plane wave result is shown in the upper right-hand comer, the individual partial wave contributions with a given ( value in the left-hand column, the sum of partial wave contributions up to the value ( = N in the right-hand column. From The picture book of quantum mechanics, S. Brandt and H. D. Dahmen, 1st edition 1985, John Wiley Sons, Inc, 1985 John Wiley and Sons Inc.

Fig. 2. Electrostatic potential maps for cytosine in the ring plane (kj/mol) a calculated with AMI b calculated with STO-3G. (Reproduced from [40] copyright-John Wiley Sons)...

The session chairmen, Patrick L. Brezonik, Richard A. Carrigan, Edward J. Green, John M. G Plane, and Barrie F. Taylor, gave considerable time during the symposium. 

We wish to thank John Plane, Kim Holmen, Dennis Savoie, and Rana Fine for helpful discussions on the subject of kinetic modelling and gas exchange. This work was supported by grant ATM 87-09802 from the National Science Foundation. 

Figure 4 Schematic illustrating the orientated growth of Api-40 fibrils along the hydrophilic step edges of highly orientated pyrolytic graphite (HOPG) in preference to assembly on the hydrophobic basal plane surface. Copyright (Losic, Martin et al., 2006). Reprinted with permission of John Wiley Sons, inc.

Fig. 11.22. Example structures for monolayer covalent bonding to edge plane pyrolytic graphite electrodes. (Reprinted from Techniques of Chemistry, Molecular Design of Electrode Surfaces, R. W. Murray, ed., Vol. 22, p. 143. Copyright 1992 John Wiley Sons. Reprinted by permission of John Wiley Sons, Inc.)...

Figure 1.4 Examples of lattice planes and their Miller indices. (After Lalena and Cleary, 2005. Copyright John Wiley Sons, Inc. Reproduced with permission.)...

Figure 1.7 View down the [001] direction of a tilt boundary between two crystals (A, B) with a misorientation angle of 36.9° about [001], The grain boundary is perpendicular to the plane of the page. Every fifth atom in the [010] direction in B is a coincidence point (shaded). The area enclosed by the CSL unit cell (bold lines) is five times that of the crystal unit cell, so 2 = 5. (After Lalena and Cleary, 2005. Copyright John Wiley Sons, Inc. Reproduced with permission.)...

Figure 26 A plot of the intensity of quartz in three binary mixtures compared to the intensity of the same plane in pure quartz as a function of the weight fraction of quartz in the mixtures. Conditions CuKa, d = 3.34 A, mass absorption coefficients, BeO 8.6 Si02 34.9 KCl 124cm /g. (Reprinted from Nuffield. John Wiley Sons, Inc)...

Figure 5,1,3 Atomic arrangements of the low-index surface planes of an FCC crystal. (Adapted from E. Masel, Principles of Adsorption and Reaction on Solid Surfaces, Wiley, New York, copyright 1996, p. 38, by permission of John Wiley Sons, Inc.)...

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