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Patterns helical

The inductively coupled plasma source (Fig. 20.11) comprises three concentric silica quartz tubes, each of which is open at the top. The argon stream that carries the sample, in the form of an aerosol, passes through the central tube. The excitation is provided by two or three turns of a metal induction tube through which flows a radio-frequency current (frequency 27 MHz). The second gas flow of argon of rate between 10 and 15 L min-1 maintains the plasma. It is this gas stream that is excited by the radio-frequency power. The plasma gas flows in a helical pattern which provides stability and helps to isolate thermally the outside quartz tube. [Pg.774]

Fig. 6. Spectral monitoring of the thermal denaturation of the highly helical, Ala-rich peptide Ac-(AAAAK)3AAAA-YNH2 in D20 from 5 to 60°C, as followed by changes in the amide V IR (left) and VCD (right). IR show a clear shift to higher wavenumber from the dominant a-helical peak (here at an unusually low value, 1637 cm-1, due to full solvation of the helix) to a typical random coil value ( 1645 cm-1). VCD loses the (—,+,—) low-temperature helical pattern to yield a broad negative couplet, characteristic of a disordered coil, at high temperature. Spectra were normalized to A = 1.0 by 45°C. Fig. 6. Spectral monitoring of the thermal denaturation of the highly helical, Ala-rich peptide Ac-(AAAAK)3AAAA-YNH2 in D20 from 5 to 60°C, as followed by changes in the amide V IR (left) and VCD (right). IR show a clear shift to higher wavenumber from the dominant a-helical peak (here at an unusually low value, 1637 cm-1, due to full solvation of the helix) to a typical random coil value ( 1645 cm-1). VCD loses the (—,+,—) low-temperature helical pattern to yield a broad negative couplet, characteristic of a disordered coil, at high temperature. Spectra were normalized to A = 1.0 by 45°C.
The (I ,S)-nomenclature still reminds the user of the right and left handed helical pattern arising from Fresnel s 29> interpretation of optical activity. These patterns are characterized by the combination of a translational and a rotational direction. The Ta skeletal symmetry of tetracoordinate systems submits itself to the pictorial models not applicable to other configurational types. The CIP rules may as well be used to define a configurational nomenclature on the basis of the Fischer projection. If one specified that in such a projection of an (R)-... [Pg.29]

A low-energy in vitro form of nucleosome packing was observed in nucleosome core particle crystals (Finch et al., 1977). Two variants of these crystals occurred, (a) Wavy columns of nucleosomes stacked one on top of each other with an axial repeat of 340 A were obtained upon crystallization of nucleosomes containing proteolytically cleaved histones (Finch et al., 1977). (b) Straight columns of closely packed nucleosomes, 110 A in diameter, were obtained upon crystallization of nucleosomes with intact histones (Finch and Klug, 1978). In both these structures histone-histone contacts between nucleosomes are implied. Similar face-to-face packing of nucleosomes in arcs and helical patterns was observed in the EM by Dubochet and Noll (1978). [Pg.38]

An amorphous material sometimes referred to as amorphous poly(ethylene oxide), aPEO, consists of medium but randomly-variable length segments of poly(ethylene oxide) joined by methyleneoxide units. Fig. 5.13 (Wilson, Nicholas, Mobbs, Booth and Giles, 1990). These methyleneoxide units break up the regular helical pattern of poly(ethylene oxide) and in doing so suppress crystallisation. The aPEO host polymer and its salt complexes can crystallise below room temperature, but this is not detrimental to the properties of the polymer-salt complexes at or above room temperature. Similarly, dimethyl siloxy units have been introduced between medium length poly(ethylene oxide) units to produce an amorphous polymer. Fig. 5.14 (Nagoka, Naruse, Shinohara and Watanabe, 1984). [Pg.107]

Fig. 16. Ciystal structure of human HO-1 (163). The heme and His25 ligand are shown. The proximal and distal helices are highlighted. Note the break iu the normal helical pattern in the distal helix directly over the heme. Fig. 16. Ciystal structure of human HO-1 (163). The heme and His25 ligand are shown. The proximal and distal helices are highlighted. Note the break iu the normal helical pattern in the distal helix directly over the heme.
FIGURE 10.2 Commonly occurring repetitive helical patterns for polypeptides. (From Coates J. and Carraher, C. Polymer News, 9(3), 77, 1983. With permission.)... [Pg.306]

Each coat subunit in the Ff viruses is coiled into an a-helical rod of 7 nm length. These are arranged in the virus in a right-handed helical pattern with a pitch of 1.5 nm and with 4.4 subunits per turn (Fig. 7-7). The protein rods are inclined to the helix axis and extend inward. This arrangement permits a "knobs-in-holes" hydrophobic bonding between subunits. The helix of pitch 1.5 nm is the primary or one-start helix. However, in every regular helical structure we can also trace a two-start helix, a three-start helix, etc. In this instance the five-start helix is easiest to see. [Pg.334]

In order to model this type of flow field geometrically, Beltrami found that it was necessary to consider a three-dimensional circular axisymmetric flow in which the velocity and vorticity field lines described a helical pattern. This helicoidal flow field was unique in that the pitch of the circular helices decreased as the radius from the central axis increased. This produces a specialized shear effect between the field lines of successively larger cylindrical tubes constituting the respective helices. In the limit of such a field, the central axis of the flow also serves as a field line (see Fig. 3). [Pg.531]

Fig. 7 Schematic view of the different approaches used to model the chiral interactions between DNA double helices, (a) DNA duplexes are viewed as clean cylinders with charged helical patterns of negative phosphates and positive adsorbed counterions. Reproduced with permission from [18], (b) Duplexes interact via steric interlocking of backbone and grooves and through electrostatic repulsion of the phosphate groups. Reproduced with permission from [14]... Fig. 7 Schematic view of the different approaches used to model the chiral interactions between DNA double helices, (a) DNA duplexes are viewed as clean cylinders with charged helical patterns of negative phosphates and positive adsorbed counterions. Reproduced with permission from [18], (b) Duplexes interact via steric interlocking of backbone and grooves and through electrostatic repulsion of the phosphate groups. Reproduced with permission from [14]...
Today, the atomic mechanism that causes the piezoelectric effect is well understood. Quartz, for example, consists of long chains of silicate (Si042-) groups arranged in a helical pattern, as shown in the diagram below. In any one silicate group, the atoms are arranged... [Pg.112]

In order to exploit the lipophilic core of the cylindrical aggregate, V,A, V",A "-tetrakis[2-hydroxy-1,1 -bis(hydroxymethyl)ethyl]hexadec-8-yne-l,l,16,16-tetracarboxamide was prepared this unsaturated ar-borol, possesses a centrally located alkyne moiety, and upon dissolution in water forms a gel comprised of a similar stacking motif to the saturated counterpart. The electron micrograph of this gel showed a unique aggregation pattern, in which bundles of intertwined aggregate columns were formed. The resultant, inherently helical pattern is in stark contrast to the needle-like structures formed by the related [9]-10-[9]-arborol. [Pg.162]

Figure 25. Circular dichroism spectra of the classical polypeptide conformations extended into the vacuum ultraviolet region. Solid curve, a-helical pattern averaged from poly-L-alanine and poly(y-methyl-L-glutamate) data. Dashed curve, antiparallel /5-pleated sheet CD pattern due to films of Boc-(l -Ala)7-OMe [78]. Dotted curve, parallel /S-pleated sheet patterns were calibrated by solution spectra. Dash-dot curve, disordered collagen to provide a measure of a random structure. Reproduced, with permission, from [79]. Figure 25. Circular dichroism spectra of the classical polypeptide conformations extended into the vacuum ultraviolet region. Solid curve, a-helical pattern averaged from poly-L-alanine and poly(y-methyl-L-glutamate) data. Dashed curve, antiparallel /5-pleated sheet CD pattern due to films of Boc-(l -Ala)7-OMe [78]. Dotted curve, parallel /S-pleated sheet patterns were calibrated by solution spectra. Dash-dot curve, disordered collagen to provide a measure of a random structure. Reproduced, with permission, from [79].
Glycerol, used in spray mounting techniques may decorate the surface of the specimen on the mica surface. The protein surface structure of the TMV particle, which shows clearly a helical pattern in low-dose negative-stained and freeze-dried shadowcast images (106, 131), is not visible if the particles are applied to mica via glycerol spray. [Pg.104]

Fig. 11.18. The helical pattern found in the crystal structures of several c/s-amides. The helices I, II and II have different helix repeats. Views are given both parallel and perpendicular to the... Fig. 11.18. The helical pattern found in the crystal structures of several c/s-amides. The helices I, II and II have different helix repeats. Views are given both parallel and perpendicular to the...

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See also in sourсe #XX -- [ Pg.202 ]

See also in sourсe #XX -- [ Pg.56 ]




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