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Bond, flipping rotation

The case of polyatomics, which is considered in more detail below, follows analogously. The point to keep in mind is that the symmetry restricts the number of distinguishable states. The symmetry number is the number of equivalent (indistinguishable) positions into which a molecule can be carried by rigid body rotation. For example s = 12 for CH4 since the molecule can be held by a CH bond and rotated into three equivalent positions, and there are four CH bonds. Similarly for benzene s = 12 since there are six indistinguishable positions for rotation about an axis perpendicular to the plane of the molecule (and through its center), and six more when the molecule is flipped over. [Pg.110]

The photoisomerization of all-s-trans-all-trans 1,3,5,7-octatetraene at 4.3 K illustrates the need for a new mechanism to explain the observed behavior [150]. Upon irradiation, all-s-trans-all-trans 1,3,5,7-octatetraene at 4.3 K undergoes conformational change from all-s-trans to 2-s-cis. Based on NEER principle (NonEquilibrium of Excited state Rotamers), that holds good in solution, the above transformation is not expected. NEER postulate and one bond flip mechanism allow only trans to cis conversion rotations of single bonds are prevented as the bond order between the original C C bonds increases in the excited state. However, the above simple photochemical reaction is explainable based on a hula-twist process. The free volume available for the all-s-trans-all-trans 1,3,5,7-octatetraene in the //-octane matrix at 4.3 K is very small and under such conditions, the only volume conserving process that this molecule can undergo is hula-twist at carbon-2. [Pg.593]

Fig. 5.4 The r (N1-C1-C2-C3) and q> (Cl-C2-C3-C4) dihedral angles of the green fluorescent protein chromophore. In the protein R, is Gly67 and R2 is Ser65, and in HBDI, an often used model compound, = R2 = CH3. In r one-bond flips (r-OBF) the dihedral rotation occurs around the r torsional angle, in a (p-OBF it is around the (p dihedral angle, in a hula twist (HT) the (p and r dihedral angles concertedly rotate. Fig. 5.4 The r (N1-C1-C2-C3) and q> (Cl-C2-C3-C4) dihedral angles of the green fluorescent protein chromophore. In the protein R, is Gly67 and R2 is Ser65, and in HBDI, an often used model compound, = R2 = CH3. In r one-bond flips (r-OBF) the dihedral rotation occurs around the r torsional angle, in a (p-OBF it is around the (p dihedral angle, in a hula twist (HT) the (p and r dihedral angles concertedly rotate.
For ds-trans isomerization in highly condensed media at very low temperature <77 K, liu and Hammond postulated mechanisms called one-bond flip and hula-twist mecdianism [35-38]. According to the H-T mechanism, isomerization takes place not by the one-bond rotation around the double bond but by the concomitant twist of the double bond and the adjacent single bond to accomplish the double-bond isomerization (Figure 4.10). These mechanisms were assumed to reduce free volume... [Pg.108]

We have seen that alkanes are not locked into a single conformation Rotation around the central carbon-carbon bond m butane occurs rapidly mterconvertmg anti and gauche conformations Cyclohexane too is conformationally mobile Through a process known as ring inversion, chair-chair mterconversion, or more simply ring flipping, one chair conformation is converted to another chair... [Pg.119]

The double-headed arrow is intended to imply the existence of a resonance hybrid a stmcture with an electronic distribution intermediate between the two shown. Every instmctor knows the hazards of this portrayal. Firstly, the doubleheaded arrow is misinterpreted by some students to mean either (i) that there is an equilibrium condition involving the two different species, or (ii) that flipping occurs between the two species. A second problem is demonstrated by those students who ask Are these not the same If we rotate one of the molecules by 60°, we see that they are identical . We can hypothesise that the latter problem may be exacerbated by the tendency of textbooks (and probably teachers) to talk about these two different resonance stmctures as though we are referring to two different molecules - when, in fact, we are talking about different electron distributions in just one molecule. It seems so important for instractors to refer to just one set of six carbon atoms joined by ct bonds, and then to discuss alternative distributions of the six TT electrons within that system. [Pg.18]

Figure 4.14 (a) The boat conformation of cyclohexane is formed by "flipping" one end of the chair form up (or down). This flip requires only rotations about carbon-carbon single bonds, (b) Ball-and-stick model of the boat conformation, (c) A space-filling model. [Pg.156]

The temperature dependent T data are shown in Fig. 9. 7j values decrease from 28 ms at 21°C with increasing temperature, and show a minimum of 6.4 ms at 80° C. These results indicate the presence of the motion with a Larmor frequency of 30 MHz at this temperature. This minimum was found to be attributed to the flipping motion of a phenyl ring from the result of our other experiments discussed in later section.13 The jump rates of the flipping motion were estimated with a two-site jump model that a C-2H bond jumps between two equivalent sites separated by 180°, and that the angle made by the C-2H bond and the rotational axis is 60°. The quadrupole coupling constant of 180 kHz and the asymmetry parameter approximated to zero were used in the calculation. The calculated values for fitting with the... [Pg.308]

The major reasons for using intrinsic fluorescence and phosphorescence to study conformation are that these spectroscopies are extremely sensitive, they provide many specific parameters to correlate with physical structure, and they cover a wide time range, from picoseconds to seconds, which allows the study of a variety of different processes. The time scale of tyrosine fluorescence extends from picoseconds to a few nanoseconds, which is a good time window to obtain information about rotational diffusion, intermolecular association reactions, and conformational relaxation in the presence and absence of cofactors and substrates. Moreover, the time dependence of the fluorescence intensity and anisotropy decay can be used to test predictions from molecular dynamics.(167) In using tyrosine to study the dynamics of protein structure, it is particularly important that we begin to understand the basis for the anisotropy decay of tyrosine in terms of the potential motions of the phenol ring.(221) For example, the frequency of flips about the C -C bond of tyrosine appears to cover a time range from milliseconds to nanoseconds.(222)... [Pg.52]

Figure 13.1 Correction of a structure by side-chain flipping. The original structure after CNS refinement is shown in (a) and after the recommended correction of WHATCHECK in (b). Carbon atoms are grey, oxygens white, and nitrogens black. Asn 144 and Glu 145 are the labelled adjacent residues in a helix, shown as a ribbon. After a 180 degree rotation about the chi-2 dihedral of Asn 144, the side chain amide nitrogen is now in position to hydrogen bond, shown as the labelled dashed line, to the carboxylate of Glu 145. Image rendered by ribbons. Figure 13.1 Correction of a structure by side-chain flipping. The original structure after CNS refinement is shown in (a) and after the recommended correction of WHATCHECK in (b). Carbon atoms are grey, oxygens white, and nitrogens black. Asn 144 and Glu 145 are the labelled adjacent residues in a helix, shown as a ribbon. After a 180 degree rotation about the chi-2 dihedral of Asn 144, the side chain amide nitrogen is now in position to hydrogen bond, shown as the labelled dashed line, to the carboxylate of Glu 145. Image rendered by ribbons.
Fig. 5. Types of motion in proteins detected by nmr. Rotation about methyl groups is easily detected from threefold symmetry and is rapid. Rotation or flipping about the C(J—Cy bonds of tyrosine or phenylalanine has been observed readily (see text) because of the twofold symmetry of the aromatic ring. Rotation of more complex side chains is more difficult to define because of the lack of symmetry. Fig. 5. Types of motion in proteins detected by nmr. Rotation about methyl groups is easily detected from threefold symmetry and is rapid. Rotation or flipping about the C(J—Cy bonds of tyrosine or phenylalanine has been observed readily (see text) because of the twofold symmetry of the aromatic ring. Rotation of more complex side chains is more difficult to define because of the lack of symmetry.

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See also in sourсe #XX -- [ Pg.91 ]




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