Schematic view

Schematic view showing the principle of nuclear magnetic resonance.

Figure 1 Schematic view of the measurement setup used in the experiment...

Figure Bl.19.16. Schematic view of the force sensor for an AFM. The essential features are a tip, shown as a rounded cone, a spring, and some device to measure the deflection of the spring. (Taken from [74], figure 6.)...

Figure Bl.27.8. Schematic view of Picker s flow microcalorimeter. A, reference liquid B, liquid under study P, constant flow circulating pump and 2, Zener diodes acting as heaters T and T2, thennistors acting as temperature sensing devices F, feedback control N, null detector R, recorder Q, themiostat. In the above A is the reference liquid and C2is the reference cell. When B circulates in cell C this cell is the working cell. (Reproduced by pemiission from Picker P, Leduc P-A, Philip P R and Desnoyers J E 1971 J. Chem. Thermo. B41.)...

Figure C3.2.3. Schematic view of a scanning tunnelling microscope. From Chen C J 1993 Introduction to Scanning Tunnelling Microscopy (Oxford Oxford University Press).

Figure 6 shows a two-dimensional schematic view of an individual ion s path in the ion implantation process as it comes to rest in a material. The ion does not travel in a straight path to its final position due to elastic collisions with target atoms. The actual integrated distance traveled by the ion is called the range, R The ion s net penetration into the material, measured along the vector of the ion s incident trajectory, which is perpendicular to the... 

Fig. 9. Schematic view of the development of the concentration profile of ions implanted from low (L), medium (M), and high (H) doses. The projected...

Figure 1 A schematic view of (a) a low temperature simulation that is confined by high energy baiTiers to a small region of the energy landscape and (b) a high temperature simulation that can overcome those barriers and sample a larger portion of conformational space.

Figure 3.6 Four-helix bundles frequently occur as domains in a proteins. The arrangement of the a helices is such that adjacent helices in the amino acid sequence are also adjacent in the three-dimensional structure. Some side chains from all four helices are buried in the middle of the bundle, where they form a hydrophobic core, (a) Schematic representation of the path of the polypeptide chain in a four-helrx-bundle domain. Red cylinders are a helices, (b) Schematic view of a projection down the bundle axis. Large circles represent the main chain of the a helices small circles are side chains. Green circles are the buried hydrophobic side chains red circles are side chains that are exposed on the surface of the bundle, which are mainly hydrophilic.

Figure 4.16 A schematic view of the active site of tyrosyl-tRNA synthetase. Tyrosyl adenylate, the product of the first reaction catalyzed by the enzyme, is bound to two loop regions residues 38-47, which form the loop after p strand 2, and residues 190-193, which form the loop after P strand 5. The tyrosine and adenylate moieties are bound on opposite sides of the P sheet outside the catboxy ends of P strands 2 and 5.

Figure S.8 Schematic view down the fourfold axis of the tetrameric molecule of neuraminidase as It appeared on the cover of Nature, May 5, 1983.

Figure 11.6 A schematic view of the presumed binding mode of the tetrahedral transition state intermediate for the deacylation step. The four essential features of the serine proteinases are highlighted in yellow the catalytic triad, the oxyanion hole, the specificity pocket, and the unspecific main-chain substrate binding.

Figure 13.14 (a) Schematic diagram of the main chain and four almost invariant residues of the fourth WD repeat of Gp from transducin. The view is roughly perpendicular to the central tunnel and the plane of the sheet. The red stripes denote hydrogen bonds, (b) Schematic view of two WD repeats illustrating the structural relationships between two consecutive repeats. The first repeat is brown and the second repeat is orange. The positions of the four almost invariant residues in the first repeat are circled. (Adapted from J. Sondek et al., Nature 379 369-374, 1996.)... 

Figure 18.5 Schematic view of a diffraction experiment, (a) A narrow beam of x-rays (red) is taken out from the x-ray source through a collimating device. When the primary beam hits the crystal, most of it passes straight through, but some is diffracted by the crystal. These diffracted beams, which leave the crystal in many different directions, are recorded on a detector, either a piece of x-ray film or an area detector, (b) A diffraction pattern from a crystal of the enzyme RuBisCo using monochromatic radiation (compare with Figure 18.2b, the pattern using polychromatic radiation). The crystal was rotated one degree while this pattern was recorded.

Figure 1 Schematic view of a typical EXAFS experiment at a synchrotron radiation facility. Note that it is possible to record transmission and fluorescence EXAFS simultaneously with reference EXAFS.

Figure 2 Schematic view of the ion source region of the LIMS instrument in the PAI configuration.

Figure 2 presents a schematic view of the ion source region in the PAI configuration. A second high-irradiance, frequency quadrupled pulsed Nd—YAG laser is focused parallel to and above the sample surface, where it intercepts the plume of neutral species that are produced by the ablating laser. Appropriate focusing optics and pulse time-delay circuitry are used in this configuration. 

Fig. 5.3. Schematic view offerees encountered when the tip touches the sample surface. Bright circles symbolize tip atoms, dark circles symbolize sample atoms.

Fig. 5.5. Schematic view of the deflection sensing system as used in the NanoScope III AFM (Digital Instruments, Santa Barbara, CA, USA). The deflection ofthe cantilever is amplified by a laser beam focused on the rear ofthe cantilever and reflected towards a split photodiode detector.

Similar to the primers developed for cyanoacrylate resins, the solvent carrier plays an important role in facilitating interdiffusion of the primer and the substrate. Fig. 12 shows a schematic view of the top few microns of an injection molded TPO surface. 

Fig. 9. Schematic view of cylindrical shear modes for a nested tubule telescope mode (u,-) and rotary mode (wr).

Fig. 1 Schematic view of the surface-modified silica gels at present commercially available.

Rgure 6.32. Schematic view of vessel fragments flight after vessel bursts in three BLEVE tests (Schulz-Fbrberg et al. 1984). 

Figure 5.4-2 Schematic view of the continuous flow apparatus used for the enantioselective...

Figure 5 The schematical view of the latex particles obtained as the product of emulsion polymerization.

LEED, namely one with a, c(2x2) and one with a, p(2x2) superstructure. They are compatible with CusPt and CusPta layers. The first atomic layer was in both cases found by means of photoemission of adsorbed xenon to be pure copper. Details of the experimental work can be found in ref. 9 and 10. A schematic view of both structures can be seen in figure 1. Both consist of alternating layers of pure copper and of mixed composition. In the CuaPt case, the second and all other evenly numbered layers have equal numbers of copper and platinum atoms, whereas in the CusPta case the evenly numbered layers consist of thrice as many platinum as copper atoms. 

Figure 1 Schematic views of the CusPt (left panel) and CusPta (right panel) ordered structures. The squares indicate the unit cells.

Figure 2 Schematic views of the layer sequence of the ordered structures discussed in the text the CusPt single crystal (left panel), the ordered overlayer of CusPt on the Pt substrate (middle panel) and the ordered overlayer of CusPts on Pt (right panel).

Figure 4-232. Schematic view of the sensor arrangement in a steering tool.

Fig. 4.15 Schematic view of a small space-time region of a one-dimensional CA. The site-values in the. dotted region are completely determined by values in the surrounding lined area. See text for discussion.

Figure 1.2 A schematic view of an atom. The dense, positively charged nucleus contains most of the atom s mass and is surrounded by negatively charged electrons. The three-dimensional view on the right shows calculated electron-density surfaces. Electron density increases steadily toward the nucleus and is 40 times greater at the blue solid surface than at the gray mesh surface.

Figure 14-9. Schematic view of normally on (a) and normally off (b) MESFETs at zero gate voltage. In (a) a conducting channel already exists, while in (b) the depletion layer extends all over the channel.

Figure 14-10. Schematic view of the concluding channel of a TFT in Ihc accumulation mode al saturation.

Figure 14-6. Schematic view of three kinds or ficld-dl erl transistors (HKT) (a) mclal-insiilulor-scniicuiiduclor ITT (M1STUT), lb) metal-semiconductor l-TT (MUSTtiT), (c) Ihtn-lilni trausis-(c) lor (TIT).

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