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T Geometry

The interaction diagram of Fig. 45 provides the basis for our discussion. Here, the AO s of the central atom interact with the three group MO s which span the three hydrogen atoms in the T geometry. The following trends can be noted ... [Pg.143]

Both single and double cyclizations of the Schiff bases 65A and 66A occur in the multicomponent tautomeric mixtures derived from as- and /ra t-cyclohexane aminodiols 69 and 70, to give monocyclized ring forms of C-2-epimeric perhydro-l,3-benzoxazines (B and G) and oxazolidines (D and E), besides 7,ll-dioxa-9-azatricyclo[7.2.1.0 °]-dodecane diastereomers 67 and 68 (Scheme 10). The tautomeric ratios are found to satisfy by Equation (1) (Table 1) and are influenced by the cis- or rra t-geometry of the cyclohexane substituents in the Schiff base (A). For the equilibria... [Pg.383]

To illustrate this approximation, let us consider a pressure flow in which the driving-force pressure drop varies with time. We set dp/dt and d /dt in the equations of continuity and motion, respectively, equal to zero and proceed to solve the problem as if it were a steady-state one, that is, we assume AP to be constant and not a function of time. The solution is of the form v = v(x, A P t), geometry, etc.). Because AP was taken to be a constant, v is also a constant with time. The pseudo-steady-state approximation pretends that the foregoing solution holds for any level of AP and that the functional dependence of v on time is v(x,-, t) = v(x,-, AP(t), geometry, etc.). The pseudo-steady state approximation is not valid if the values of A(pv)/At (At being the characteristic time of fluctuation of AP) obtained using this approximation contribute to an appreciable fraction of the mean value of the applied AP. [Pg.63]

The I111 compounds (13-IV) and (13-V) are also well characterized, with the expected T geometry at the iodine atom. [Pg.575]

A better geometry does improve the agreement. The RMSE of the chemical shifts, computed at MP2/tzp with the HF, MP2, and CCSD(T) geometries, are 9.55, 5.62, and 5.06ppm, respectively. Unfortunately, the computed chemical shifts at CCSD(T)/qz2p//CCSD(T)/cc-pVTZ are still in error the RMS is 4.78 ppm for the carbon shifts and 0.26ppm for the proton shifts. Including a correction for... [Pg.81]

COg, with all atoms in the d s state, has a very stable closed shell configuration with a T geometry (compare Ref.19). [Pg.135]

The results of large-order SRS calculations for the linear and T-shaped geometries of the HeH2 complex are presented in Table 4. An inspection of this table shows that also for this system the SRS expansion appears to be convergent. Compared to the He dimer case the convergence is slower. Also the error of the second order treatment is somewhat larger than for He2 3% and 0.8% for the linear and T geometries of the complex, respectively. [Pg.183]

Figure 2. Optimized structures (MP2/ 6-31+G ) for (A) the slipped parallel (C2h symmetry) and (B) T-geometries (C2v symmetry) of the CO2 dimer (C) the T-structure (C2v symmetry) and (D) the proton side (Cs symmetry) configuration of the HCHO-CO2 complexes 39). Figure 2. Optimized structures (MP2/ 6-31+G ) for (A) the slipped parallel (C2h symmetry) and (B) T-geometries (C2v symmetry) of the CO2 dimer (C) the T-structure (C2v symmetry) and (D) the proton side (Cs symmetry) configuration of the HCHO-CO2 complexes 39).
Another commonly used setup for measurements of anisotropy is the T geometry" (Fig. 5.18). [Pg.81]

The sample (usually a cuvette) is measured from both sides under different polarisation angles. Two detectors and a router are used to detect Ip and L simultaneously [58, 59]. The T geometry with routed detection has twice the efficiency of a sequential measurement. Moreover, possible counting loss due to the dead time of the TCSPC module affects both channels in the same way and therefore does not affect the measured intensity ratio. The dual-detector routing technique is even able to record dynamic changes of the lifetime and depolarisation time. The drawback is that the instrument response functions of the two detectors are different,... [Pg.81]

Some extremely unfortunate situations can also occur in systems with several parallel detection paths. Often light reflected back from one detection path can enter the other one. A typical example is the T geometry" often used for anisotropy experiments, see Fig. 7.26. [Pg.286]

Table B.3 (con t) Geometry Parameters for unsaturated oxygenated species ... Table B.3 (con t) Geometry Parameters for unsaturated oxygenated species ...

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See also in sourсe #XX -- [ Pg.81 ]




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