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Figure 16-17. Left transmission electron micrograph of small single crystals of Ooct-OPV5 scale bar 5 pnt. The arrows indicate the 6-axis direction. Right electron diffraction pattern of the same single crystals. The arrow indicates the 613 relteclion spot (crysial dimensions 5x40 pm2 Philips STiiM CM 12 operated at 120 kV. lnslilul Charles Sudron, Strasbourg). Figure 16-17. Left transmission electron micrograph of small single crystals of Ooct-OPV5 scale bar 5 pnt. The arrows indicate the 6-axis direction. Right electron diffraction pattern of the same single crystals. The arrow indicates the 613 relteclion spot (crysial dimensions 5x40 pm2 Philips STiiM CM 12 operated at 120 kV. lnslilul Charles Sudron, Strasbourg).
The drawn cell corresponds to a unit cell of diamond (a-Sn Si-I) that has been strongly compressed in one direction. Right coordination about a tin (or Si) atom with bond lengths cf. the atom in the dashed octant... [Pg.121]

Figure 8.37 Mixing quality in a Ross LPD mixer with right-left elements [60]. The term RL-90 means that the plates alternate directions right and then left, and the C" is the number of n elements in the mixer (courtesy of Han Meijer of Technische Universiteit Eindhoven)... Figure 8.37 Mixing quality in a Ross LPD mixer with right-left elements [60]. The term RL-90 means that the plates alternate directions right and then left, and the C" is the number of n elements in the mixer (courtesy of Han Meijer of Technische Universiteit Eindhoven)...
Fig. 7.1 Left-hand panel The s band structure for a simple cubic lanice in the 100> and 111> directions. Right-hand panel The s band density of states for a simple cubic lattice. Fig. 7.1 Left-hand panel The s band structure for a simple cubic lanice in the 100> and 111> directions. Right-hand panel The s band density of states for a simple cubic lattice.
Fig. 10 (a) 3D-sketch of the cell cross section according to Fig. 12. (b) Sketch of the laser focus, (c) The laser beam is scanned along the y-direction. Right phase contrast image of arbitrary pattern written into critical sample. The bright regions show an enrichment of PDMS, the dark ones a depletion (enrichment of PEMS)... [Pg.163]

Fig. 13 Comparative study of symmetric and asymmetric electroactive nanoarrays for the study of cell adhesion and polarization (a) DPN was used to pattern a SAM nanospot of hydroquinone-terminated alkanethiolates for subsequent RGD immobilization and cell adhesion, (b) Lateral force microscopy image of a symmetric nanoarmy (left) and fluorescent cell having a diffusive nucleus-centrosome-Golgi vector that indicates no preferential migratory direction (right), (c) Cell polarity vectors orient toward the direction of higher RDG density on asymmetric nanoarrays, (d) Higher magnification of the cell polarization vector (above) and its schematic (below). Reproduced from [37, 38] with permission. Copyright The American Chemical Society, 2008... Fig. 13 Comparative study of symmetric and asymmetric electroactive nanoarrays for the study of cell adhesion and polarization (a) DPN was used to pattern a SAM nanospot of hydroquinone-terminated alkanethiolates for subsequent RGD immobilization and cell adhesion, (b) Lateral force microscopy image of a symmetric nanoarmy (left) and fluorescent cell having a diffusive nucleus-centrosome-Golgi vector that indicates no preferential migratory direction (right), (c) Cell polarity vectors orient toward the direction of higher RDG density on asymmetric nanoarrays, (d) Higher magnification of the cell polarization vector (above) and its schematic (below). Reproduced from [37, 38] with permission. Copyright The American Chemical Society, 2008...
Moritz Traube 4 rejected this explanation on the ground that carbon monoxide does not decompose steam at the temperature of the electric spark, for reaction (i) is reversible and under these conditions proceeds m the direction right to left. [Pg.85]

Air-cooled heat exchangers include a tube bundle, which generally has spiral-wound fins upon the tubes, and a fan, which moves air across the tubes and is provided with a driver. Electric motors are the most commonly used drivers typical drive arrangements require a V belt or a direct right-angle gear. A plenum and structural supports are basic components. Louvers are often used ... [Pg.900]

Figure 2 Interplay between HR and NHR. (a) When a DSB occurs (top), it can be resected and used to copy a donor chromosome (red) during HR (left) or rejoined directly (right), sometimes inaccurately (jagged line). HR and NHR lead to recombination by crossover resolution and engagement of a different DSB (green), respectively (bottom), (b) A timeline shows a period during which NHEj may be iteratively attempted before DSB resection after which, HR is attempted. Alternative pathways (below) might lead to rejoining, but these are often less efficient and uncommon when the above pathways are functioning normally. Figure 2 Interplay between HR and NHR. (a) When a DSB occurs (top), it can be resected and used to copy a donor chromosome (red) during HR (left) or rejoined directly (right), sometimes inaccurately (jagged line). HR and NHR lead to recombination by crossover resolution and engagement of a different DSB (green), respectively (bottom), (b) A timeline shows a period during which NHEj may be iteratively attempted before DSB resection after which, HR is attempted. Alternative pathways (below) might lead to rejoining, but these are often less efficient and uncommon when the above pathways are functioning normally.
Before starting to screen for a suitable CSP some general considerations have to be taken into account to optimize the separation in the best direction right from the beginning. The required purity and amount and time frame should be known as well as some limitations with regard to solvents or other process conditions, e.g. temperature range. In addition it should be known if only one or both enantiomers have to be delivered in purified form. [Pg.162]

Fig. 3.38 Contact mode AFM height image of egg PC vesicles adsorbed on glass captured with an imaging force of 30 pN left) and 50 pN right). The halo in the fast scan direction right to left) indicates that the tip can no longer track the surface features accurately, when imaging force and noise of the deflection signal become comparable ( 30 pN in this case). When the imaging forces are increased to 50 pN, the surface is tracked better. The asymmetry of the features can be explained by tip convolution effects (asymmetry of the probe tip) [87]... Fig. 3.38 Contact mode AFM height image of egg PC vesicles adsorbed on glass captured with an imaging force of 30 pN left) and 50 pN right). The halo in the fast scan direction right to left) indicates that the tip can no longer track the surface features accurately, when imaging force and noise of the deflection signal become comparable ( 30 pN in this case). When the imaging forces are increased to 50 pN, the surface is tracked better. The asymmetry of the features can be explained by tip convolution effects (asymmetry of the probe tip) [87]...
Fig. 24. Snapshot of the atomic configuration after a fluence of 1000 CFj at 100 eV and normal incidence. A side view is shown, with the positive z-direction up and the positive r-direction right. The periodic transverse boundaries of the cell are rendered as translucent planes the boundary facing the viewer is cut away. Si. dark gray C, gray F. white. (From Abrams and Graves. 1999.)... Fig. 24. Snapshot of the atomic configuration after a fluence of 1000 CFj at 100 eV and normal incidence. A side view is shown, with the positive z-direction up and the positive r-direction right. The periodic transverse boundaries of the cell are rendered as translucent planes the boundary facing the viewer is cut away. Si. dark gray C, gray F. white. (From Abrams and Graves. 1999.)...
Figure 5.5 Experimental TEM micrographs of CS400 (left) and simulated images for three beam directions (right). The 5nm scale applies for the four images, (a) Highlighted are examples of dot-like segments, (h) short segments, and (c) stacks of short segments. (Adapted from Ref. [27].)... Figure 5.5 Experimental TEM micrographs of CS400 (left) and simulated images for three beam directions (right). The 5nm scale applies for the four images, (a) Highlighted are examples of dot-like segments, (h) short segments, and (c) stacks of short segments. (Adapted from Ref. [27].)...
Figure 2.4 Band broadening by longitudinal diffusion. Left Sample zone immediately after injection. It will spread out in all three axes of space (arrow directions). Right Samplezoneat a later moment. It is larger now due to diffusion and it has also been transported by the flowing mobile phase. Figure 2.4 Band broadening by longitudinal diffusion. Left Sample zone immediately after injection. It will spread out in all three axes of space (arrow directions). Right Samplezoneat a later moment. It is larger now due to diffusion and it has also been transported by the flowing mobile phase.
Figure 1.3.13 Polycatenation of ID motifs 2D entangled layers from parallel catenation of undulating ladders (laterally catenated by two other ladders by each side) (left), and of nanotube motifs (center) 3D superstructure from catenation of ladders running in different directions (right). Figure 1.3.13 Polycatenation of ID motifs 2D entangled layers from parallel catenation of undulating ladders (laterally catenated by two other ladders by each side) (left), and of nanotube motifs (center) 3D superstructure from catenation of ladders running in different directions (right).
Figure 5.17 Left valence-band photoemission spectra from a seven-monolayer-thick HCP (0001) Co film on W taken with linearly polarized radiation for opposite magnetization directions. Right corresponding asymmetry values for binding energies between —2 eV and Ep-Experiment (Bansmann et al. 2000). Figure 5.17 Left valence-band photoemission spectra from a seven-monolayer-thick HCP (0001) Co film on W taken with linearly polarized radiation for opposite magnetization directions. Right corresponding asymmetry values for binding energies between —2 eV and Ep-Experiment (Bansmann et al. 2000).
Fig. 2.14. Left An arbitrary conformation of a Ph3PX molecule is specified by three torsion angles 0, 02>03> f°r the phenyl groups labeled A,B,C in a clockwise sequence when viewed down the X-P direction. Right Definition of torsion angle 0... Fig. 2.14. Left An arbitrary conformation of a Ph3PX molecule is specified by three torsion angles 0, 02>03> f°r the phenyl groups labeled A,B,C in a clockwise sequence when viewed down the X-P direction. Right Definition of torsion angle 0...
Fig. I Two-dimensional pyramidal wavelet decomposition Each of the four channels in one band of the 2-D WT can be named using the following notation LLI, LHI, HLI, HHI, where I is the 2-D image, L stands for a low-pass filter, H stands for a high-pass filter, and the filters are applied first along the y direction (right position), and then along the x direction (left position). Three bands of the wavelet decomposition are displayed. Fig. I Two-dimensional pyramidal wavelet decomposition Each of the four channels in one band of the 2-D WT can be named using the following notation LLI, LHI, HLI, HHI, where I is the 2-D image, L stands for a low-pass filter, H stands for a high-pass filter, and the filters are applied first along the y direction (right position), and then along the x direction (left position). Three bands of the wavelet decomposition are displayed.
The polarization ellipse along with a designation of the rotation direction (right- or left-handed) fully describes the temporal evolution of the real electric vector at a fixed point in space. This evolution can also be visualized by plotting the curve in (9,tp,t) coordinates described by the tip of the electric vector as a function of time. For example, in the case of an elliptically polarized plane wave with right-handed polarization, the curve is a right-handed helix with an elliptical projection onto the Ocp - plane centered around... [Pg.25]

Figure 6. Lattice structure and orientation ofYSZ thin films. TEM image ofYSZ/MgO cross section (left) and the electron diffraction pattern along (001) direction (right) [19],... Figure 6. Lattice structure and orientation ofYSZ thin films. TEM image ofYSZ/MgO cross section (left) and the electron diffraction pattern along (001) direction (right) [19],...
Fig. 1.25. Left Schematic of a double hehx. Middle A DNA double helix with base pairs and sequence direction. Right Structure of a DNA helix showing the parallel base pairs inside the helix. Fig. 1.25. Left Schematic of a double hehx. Middle A DNA double helix with base pairs and sequence direction. Right Structure of a DNA helix showing the parallel base pairs inside the helix.
In 1922, T. De Donde (1870-1957) proposed to use the derivative of free enthalpy over the reaction depth as parameter of chemical affinity. Its value shows the change in maximum useful work with each 1 mole step of a reaction and is measured in joules per 1 mole, i.e., it shows the propellant force of the reaction per 1 mole of the substance (Figure 1.9). Positive values of chemical affinity A. indicate the excess of reactants and the reactions direction from left to right, negative ones, the excess of products and reactions direction right to left in the reactions equation. In the process of relaxation A tends to 0. [Pg.62]

Fig. 4.7 Simulated pointing position with an absolute pointing error (left) and the absolute pointing error distribution in the x direction (right) including a gaussian fit to the data with Op =2 arcsec... Fig. 4.7 Simulated pointing position with an absolute pointing error (left) and the absolute pointing error distribution in the x direction (right) including a gaussian fit to the data with Op =2 arcsec...
Fig. 6.13. Auger electron yield carbon K-edge NEXAFS spectra of rubbed poly-imide (top), ion beam irradiated polyimide (middle), and ion beam irradiated amorphous carbon (bottom) for the indicated geometries. The intensity ratios of the plotted TT resonances characterize the in-plane asymmetry (left column) and the molecular tilt direction (right column). Fig. 6.13. Auger electron yield carbon K-edge NEXAFS spectra of rubbed poly-imide (top), ion beam irradiated polyimide (middle), and ion beam irradiated amorphous carbon (bottom) for the indicated geometries. The intensity ratios of the plotted TT resonances characterize the in-plane asymmetry (left column) and the molecular tilt direction (right column).
Fig. 5. Equatorial scattering intensity of undeformed iPP at room temperature and during strain hardening at elevated temperatures. The curves always show a projection of the angular range of 2 ° around the equatorial direction. Right WAXS-pattems, azimuthal angle vs. scattering angle 20 at three characteristic points imdeformed as well as immediately before failure at room temperature and 150 °C. Fig. 5. Equatorial scattering intensity of undeformed iPP at room temperature and during strain hardening at elevated temperatures. The curves always show a projection of the angular range of 2 ° around the equatorial direction. Right WAXS-pattems, azimuthal angle vs. scattering angle 20 at three characteristic points imdeformed as well as immediately before failure at room temperature and 150 °C.

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