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Experimental methods, transient

The most popular, and also a very accurate, experimental method for measuring nonselective spin-lattice relaxation-rates is the inversion recovery (180°-r-90°-AT-PD)NT pulse sequence. Here, t is the variable parameter, the little t between pulses, AT is the acquisition time, PD is the pulse delay, set such that AT-I- PD s 5 x T, and NT is the total number of transients required for an acceptable signal-to-noise ratio. Sequential application of a series of two-pulse sequences, each using a different pulsespacing, t, gives a series of partially relaxed spectra. Values of Rj can... [Pg.138]

Whereas other experimental methods have been used to obtain values of kti no other method provides values of k-t or equilibrium data. There are, however, several important limitations of our method. First, the method is restricted to relatively fast hole transport processes that can compete with charge recombination of the Sa -G+ radical ion pair (Fig. 6). This precludes the use of strong acceptors which can oxidize A as well as G (Fig. 2a). We find that hole transport cannot compete with charge recombination in such systems, even when a charge gradient is constructed which should favor hole transport [35]. Second, the method is unable to resolve the dynamics of systems in which return hole transport, k t, is very slow (<104 s-1) or systems in which multiple hole transport processes occur. Third, since the guanine cation radical cannot be detected by transient spectroscopy, the method is dependent upon the analysis of the behavior of Sa-. In section 3.4 we de-... [Pg.62]

Infrared Measurements. Elementary-step models can be fit to transient gas-phase data (5) which are obtained by the methods described above. The models will then predict the surface intermediate concentration during transients and at steady state. It is clear that it is also important to observe these surface species experimentally, during transients as well as at steady state. Infrared spectroscopy can be used during catalysis in the presence of the gas phase, so it plays an important role in transient studies. [Pg.5]

Figure 4.1. Time scales for rotational motions of long DNAs that contribute to the relaxation of the optical anisotropy r(t). Experimental methods used to study these motions in different time ranges are also indicated along with the authors and dates of some early work in each case. FPA, Fluorescence polarization anisotropy (Refs. 15, 18-20, and 87) TPD, transient photodichroism (Refs. 28 and 62) TEB, transient electric birefringence (Refs. 26 and 27) DDLS, depolarized dynamic light scattering (Ref. 116) TED, transient electric dichroism (Refs. 25, 115, and 130) Microscopy, time-resolved fluorescent microscopy (Ref. 176). Figure 4.1. Time scales for rotational motions of long DNAs that contribute to the relaxation of the optical anisotropy r(t). Experimental methods used to study these motions in different time ranges are also indicated along with the authors and dates of some early work in each case. FPA, Fluorescence polarization anisotropy (Refs. 15, 18-20, and 87) TPD, transient photodichroism (Refs. 28 and 62) TEB, transient electric birefringence (Refs. 26 and 27) DDLS, depolarized dynamic light scattering (Ref. 116) TED, transient electric dichroism (Refs. 25, 115, and 130) Microscopy, time-resolved fluorescent microscopy (Ref. 176).
QM modeling is a useful tool with which to obtain insight into reaction mechanisms. In particular, it is possible to study the structure and properties of transient intermediates and transition states not easily accessed by experimental methods. [Pg.455]

Radical 44 is generated by electron transfer from the parent pyrimidine to the optically generated (308 nm laser pulse) triplet states of anthroquinone-2,6-disulfonic acid. The experimental method detects transient species in the time range of 40 ns to 10 ps after the laser pulse. At pH = 1.0, the primary cation radical is the only radical found 40 ns after the pulse. The spectrum of this radical disappears at a time shorter than 1.0 ps after the pulse. A second spectrum observed 5 ps after the pulse, is attributed to radical 46, which was thought to form by net OH- addition to C6 of the cation radical. At pH = 7.0, the N3... [Pg.258]

Fig. 4. Energy below the conduction band of levels reported in the literature for GaP. States are arranged from top to bottom chronologically, then by author. At the left is an indication of the method of sample growth or preparation liquid phase epitaxy (LPE), liquid encapsulated Czochralski (LEC), irradiated with 1-MeV electrons (1-MeV e), and vapor phase epitaxy (VPE). Next to this the experimental method is listed photoluminescence (PL), photoluminescence decay time (PLD), junction photocurrent (PCUR), photocapacitance (PCAP), transient capacitance (TCAP), thermally stimulated current (TSC), transient junction dark current (TC), deep level transient spectroscopy (DLTS), photoconductivity (PC), and optical absorption (OA). Fig. 4. Energy below the conduction band of levels reported in the literature for GaP. States are arranged from top to bottom chronologically, then by author. At the left is an indication of the method of sample growth or preparation liquid phase epitaxy (LPE), liquid encapsulated Czochralski (LEC), irradiated with 1-MeV electrons (1-MeV e), and vapor phase epitaxy (VPE). Next to this the experimental method is listed photoluminescence (PL), photoluminescence decay time (PLD), junction photocurrent (PCUR), photocapacitance (PCAP), transient capacitance (TCAP), thermally stimulated current (TSC), transient junction dark current (TC), deep level transient spectroscopy (DLTS), photoconductivity (PC), and optical absorption (OA).
In most cases reactivity in addition reactions to the triple bond increases with increasing angle deformation. For transient cycloalkynes comparative studies of the reactivity, e.g. competition experiments, are one of the few experimental methods to assess ring strain in these reactive intermediates. [Pg.202]

Relative rate constants for reactions of OH have been measured by competitive methods in 7-irradiated solutions where product formation or reactant destruction have been monitored. These methods have generally been of low accuracy and can sometimes be misleading because of the possible complications in the processes between the initial reaction and the final products. Several competitors that allow the competition at the initial step to be followed became available for use with the pulse radiolysis technique in 1965 (Adams et al., 1965). Most of the rate constants for OH reported in the literature have been determined by this method. Numerous rates have also been determined by pulse radiolysis in an absolute way, i.e. by directly observing the kinetics of the formation of transient absorption or of the decay of the parent compound absorption. Direct observation of OH (or of H) by pulse radiolysis cannot help in obtaining reaction rates, because the absorption is in the far ultraviolet and one can observe only the tail of this absorption which at 200-250nm has a very low extinction coefficient ( 500 M -1 cm-1) (Pagsberg et al., 1969). A review of the experimental methods and summary of the rate constants of OH reactions has recently been published (Dorfman and Adams, 1973) and another compilation of rate constants is currently being prepared (Farhataziz and Ross, 1975). [Pg.236]

The most widely used unsteady state method for determining diffusivities in porous solids involves measuring the rate of adsorption or desorption when the sample is subjected to a well defined change in the concentration or pressure of sorbate. The experimental methods differ mainly in the choice of the initial and boundary conditions and the means by which progress towards the new position of equilibrium is followed. The diffusivities are found by matching the experimental transient sorption curve to the solution of Fick s second law. Detailed presentations of the relevant formulae may be found in the literature [1, 2, 12, 15-17]. For spherical particles of radius R, for example, the fractional uptake after a pressure step obeys the relation... [Pg.371]

While transient photocurrent and photoinduced discharge techniques are the conventional methods for measuring photogeneration efficiencies, these cannot be readily employed in the presence of trapping. A further limitation is that it is difficult to separate the field dependence of the photogeneration process from field dependencies associated with an injection or interfacial process (Seki, 1970, 1972a). As such, it is difficult to apply the method to dispersions or two-phase materials. Experimental methods that may avoid these limitations are... [Pg.143]

The experimental method used in TEOM for diffusion measurements in zeolites is similar to the uptake and chromatographic methods (i.e., a step change or a pulse injection in the feed is made and the response curve is recorded). It is recommended to operate with dilute systems and low zeolite loadings. For an isothermal system when the uptake rate is influenced by intracrystalline diffusion, with only a small concentration gradient in the adsorbed phase (constant diffusivity), solutions of the transient diffusion equation for various geometries have been given (ii). Adsorption and diffusion of o-xylene, / -xylene, and toluene in HZSM-5 were found to be described well by a one-dimensional model for diffusion in a slab geometry, represented by Eq. (7) (72) ... [Pg.358]

The stability of the initially generated A-chloroamide remains so far controversial. On the one hand, A-chloroamides are assumed to be "transient products" [258], while on the other hand, they were described to represent "long-lived species" [230]. This obvious discrepaney may result from two different reasons. First, this might result from the different experimental methods that were used Schiller et al. [258] uses NMR spectroseopy, while Rees et al. [230] applies the 5-thio-2-nitrobenzoic aeid (TNB) assay [261] to monitor the stability of the A-chloroamides. It is not yet clear, whether that... [Pg.840]

These transient experiments strongly suggested a correlation between the alloy crystal structure and H2S tolerance. However, due to limitations of the experimental method (finite H2S availability, competition for the available H2S by other metal surfaces, relatively short test durations and the limited data set), more representative, steady-state performance experiments were deemed essential for an accurate assessment of the impact of H2S on membrane performance. [Pg.43]

Recommendations on experimental methods for the determination and the compilation of molar absorption coefficients for transient species in solution have been proposed by Bonneau, Carmichael, and Hug . Note should be taken of the proposals put forward. [Pg.8]


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Transient method

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