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Three-dimension structures

In general, dendrimers of size G-0 through G-3 have open, asymmetric, and flexible structures with effectively no protected internal areas, due to a large freedom of motion in their branches, and they can readily accommodate additional covalent attachments to their surfaces. See Figures 73-7.5 for illustrations of the two-dimension and three-dimension structure of a... [Pg.352]

Figure 15. Three dimensioned structures generated by the formation of dendritic pores on an n(110) substrate.1,14... Figure 15. Three dimensioned structures generated by the formation of dendritic pores on an n(110) substrate.1,14...
Holmes, D. F., Gilpin, C. J., Baldock, C., Ziese, U., Koster, A. J., and Kadler, K. E. (2001). Corneal collagen fibril structure in three dimensions Structural insights... [Pg.369]

Figure 5.5 Retrieval of protein structure from Protein Data Bank The atomic coordinates of protein three-dimension structures can be retrieved from PDB (http //www.rcsb.org/pdb) by entering PDB id (e.g. IRNO) or keyword (e.g. pancreatic ribonuclease). The query search returns a list of hits from which the desired PDB file can be selected (click Explore), then viewed (select View structure as shown), analyzed (select Structure neighbor. Geometry or Sequence detail) and retrieved (select Download/Display file). Figure 5.5 Retrieval of protein structure from Protein Data Bank The atomic coordinates of protein three-dimension structures can be retrieved from PDB (http //www.rcsb.org/pdb) by entering PDB id (e.g. IRNO) or keyword (e.g. pancreatic ribonuclease). The query search returns a list of hits from which the desired PDB file can be selected (click Explore), then viewed (select View structure as shown), analyzed (select Structure neighbor. Geometry or Sequence detail) and retrieved (select Download/Display file).
No particular three dimensioned structure can be allotted to a linear random coll. This Is because the molecule exhibits a great deal of rotation about the various segments In the... [Pg.125]

One more application area is composite materials where one wants to investigate the 3D structure and/or reaction to external influences. Fig.3a shows a shadow image of a block of composite material. It consists of an epoxy matrix with glass fibers. The reconstructed cross-sections, shown in Fig.3b, clearly show the fiber displacement inside the matrix. The sample can be loaded in situ to investigate the reaction of matrix and fibers to external strain. Also absorption and transmission by liquids can be visualized directly in three-dimensions. This method has been applied to the study of oil absorption in plastic granules and water collection inside artificial plant grounds. [Pg.581]

ISlS/Draw has no genuine molecular visualization tool. The rotate tool changes only the 2D rotate tool into a 3D rotate tool which rotates 2D structures in three dimensions. In order to visualize chemical structures in different styles and perspectives, it is necessary to paste the drawing, e.g., to the ACD/3D Viewer. [Pg.146]

Anuther concept that is extremely powerful when considering lattice structures is the fi i i/imca/ lattice. X-ray crystallographers use a reciprocal lattice defined by three vectors a, b and c in which a is perpendicular to b and c and is scaled so that the scalar juoduct of a and a equals 1. b and c are similarly defined. In three dimensions this leads to the following definitions ... [Pg.159]

For a fluid, with no underlying regular structure, the mecin squared displacement gradually increases with time (Figure 6.9). For a solid, however, the mean squared displacement typically oscillates about a mean value. Flowever, if there is diffusion within a solid then tliis can be detected from the mean squared displacement and may be restricted to fewer than three dimensions. For example. Figure 6.10 shows the mean squared displacement calculated for Li+ ions in Li3N at 400 K [Wolf et al. 1984]. This material contains layers of LiiN mobility of the Li" " ions is much greater within these planes than perpendicular to them. [Pg.337]

The band-structure code, called BAND, also uses STO basis sets with STO fit functions or numerical atomic orbitals. Periodicity can be included in one, two, or three dimensions. No geometry optimization is available for band-structure calculations. The wave function can be decomposed into Mulliken, DOS, PDOS, and COOP plots. Form factors and charge analysis may also be generated. [Pg.333]

Crystal (we tested Crystal 98 1.0) is a program for ah initio molecular and band-structure calculations. Band-structure calculations can be done for systems that are periodic in one, two, or three dimensions. A separate script, called LoptCG, is available to perform optimizations of geometry or basis sets. [Pg.334]

The macmolplt graphics package is designed for displaying the output of GAMESS calculations. It can display molecular structures, including an animation of reaction-path trajectories. It also may be used to visualize properties, such as the electron density, orbitals, and electrostatic potential in two or three dimensions. [Pg.335]

Chemistry in three dimensions is known as stereochemistry At its most fundamental level stereochemistry deals with molecular structure at another level it is concerned with chemical reactivity Table 7 2 summarizes some basic definitions relating to molec ular structure and stereochemistry... [Pg.315]

The less simple polymers (like the epoxies, the polyesters and the formaldehyde-based resins) are networks each chain is cross-linked in many places to other chains, so that, if stretched out, the array would look like a piece of Belgian lace, somehow woven in three dimensions. These are the thermosets if heated, the structure softens but it does not melt the cross-links prevent viscous flow. Thermosets are usually a bit stiffer than amorphous thermoplastics because of the cross-links, but they cannot easily be crystallised or oriented, so there is less scope for changing their properties by processing. [Pg.228]

Figure 1.1 The amino acid sequence of a protein s polypeptide chain is called Its primary structure. Different regions of the sequence form local regular secondary structures, such as alpha (a) helices or beta (P) strands. The tertiary structure is formed by packing such structural elements into one or several compact globular units called domains. The final protein may contain several polypeptide chains arranged in a quaternary structure. By formation of such tertiary and quaternary structure amino acids far apart In the sequence are brought close together in three dimensions to form a functional region, an active site. Figure 1.1 The amino acid sequence of a protein s polypeptide chain is called Its primary structure. Different regions of the sequence form local regular secondary structures, such as alpha (a) helices or beta (P) strands. The tertiary structure is formed by packing such structural elements into one or several compact globular units called domains. The final protein may contain several polypeptide chains arranged in a quaternary structure. By formation of such tertiary and quaternary structure amino acids far apart In the sequence are brought close together in three dimensions to form a functional region, an active site.
Fletterick, R.J., Schroer, T, Matela, R.J. Molecular Structure Maaomolecules in Three Dimensions. Oxford, UK Blackwell Scientific, 1985. [Pg.12]

For a given structure, the values of S at which in-phase scattering occurs can be plotted these values make up the reciprocal lattice. The separation of the diffraction maxima is inversely proportional to the separation of the scatterers. In one dimension, the reciprocal lattice is a series of planes, perpendicular to the line of scatterers, spaced 2Jl/ apart. In two dimensions, the lattice is a 2D array of infinite rods perpendicular to the 2D plane. The rod spacings are equal to 2Jl/(atomic row spacings). In three dimensions, the lattice is a 3D lattice of points whose separation is inversely related to the separation of crystal planes. [Pg.267]

Band gap engineetring confined hetetrostruciutres. When the thickness of a crystalline film is comparable with the de Broglie wavelength, the conduction and valence bands will break into subbands and as the thickness increases, the Fermi energy of the electrons oscillates. This leads to the so-called quantum size effects, which had been precociously predicted in Russia by Lifshitz and Kosevich (1953). A piece of semiconductor which is very small in one, two or three dimensions - a confined structure - is called a quantum well, quantum wire or quantum dot, respectively, and much fundamental physics research has been devoted to these in the last two decades. However, the world of MSE only became involved when several quantum wells were combined into what is now termed a heterostructure. [Pg.265]


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See also in sourсe #XX -- [ Pg.4 ]

See also in sourсe #XX -- [ Pg.127 ]




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