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Absorption intensity ratio, time

Figure 10.2 Time dependence of absorption intensity ratio of 330 nm to 630 nm (/330//630) in UV-Vis spectra of EB/NMP solution (mole ratio of EB/Fe = 1/10, measured in 3.5 wt% NaCl solution at 25 °C) [45]. Figure 10.2 Time dependence of absorption intensity ratio of 330 nm to 630 nm (/330//630) in UV-Vis spectra of EB/NMP solution (mole ratio of EB/Fe = 1/10, measured in 3.5 wt% NaCl solution at 25 °C) [45].
The initial single beam dispersive spectrometers that did not, at the time, produce digitised spectra (this would have allowed for baseline correction) were soon replaced by double beam spectrometers. This more complex arrangement can directly yield the spectrum corrected for background absorption. The use of two distinct but similar optical paths, one as a reference and the other for measurement, allows the alternate measurement of the transmitted intensity ratios at each wavelength. [Pg.169]

After exposure to methane the IR spectra of manganese oxide showed absorption bands, which are characteristic of the C-H stretching vibrations (CHs 2962, 2872 cm CH2 2926, 2853 cm and CH 2890 cm ) [9]. The intensity of the C-H bands increased, if the exposure time to methane increased (Figs. 2,3). The intensity of the band at 1050 cm, which is assigned to V3(Si-0) of silica was used as an internal reference (Fig. 2). the intensity ratio for the CH2 and CH3 groups estimated for samples after 30 min reaction with methane, was found to be about five [10]. Thus XPS and FTIR surface analysis showed that carbonaceous material formed on the MnOx catalyst surface consists of CHx hydrocarbon deposits and manganese carbide species. [Pg.658]

Kinetics of Thermal Decomposition. In order to examine the kinetics of thermal decomposition reactions, relative changes in IR absorption Intensity at 2120, 1250 and 1160 cm (Fig. 1), corresponding to SiH, SlCHg and NH groups, respectively, were studied as a function of pyrolysis time. Absorption data were evaluated as the ratio of areas under the peaks, A/A A being the initial... [Pg.240]

This technique utilizes a pulse pump-probe experiment and monitors the absorption of a weak probe beam in the presence of a strong pump beam. Fig. 8 depicts the experimental set-up for a two-beam pump-probe experiment, which includes homodyne and heterodyne Kerr gate measurements and polarization-controlled transient absorption measurement. Generally, the input beam is produced from an amplified pulse laser system with 1 KHz repetition rate, which can produce picosecond or femtosecond pulses. This pumping light beam is divided into two beams by a beam-splitter with an intensity ratio of 30 1 therefore, the one with the stronger intensity will act as the pump and the weaker one will be the probe. The position of the sample is where these two beams focus and overlap spatially. The time delay between the pulses from these two beams is controlled by a retroreflec-... [Pg.170]

Pyrene derivatives are the widest used probes for qualitative solubilization [365] by virtue of the solvatochromic shifts of the absorption bands [255], the excimer formation [145,186], the polarity dependent quantum yields [197] and fluorescence life-times [185-187, 196, 197, 202, 215, 292], and the pyrene fluorescence fine structure [65, 74,78,103,112,167, 224, 363, 371] the intensity ratio of the fluorescence bands I at 372 nm and III at 383 nm is a convenient measure for the polarity of the environment of the pyrene label ( py -scale I/III values increase with polarity, cf. Fig. 27). As, however, the fluorescence of pyrene is very sensitive to the experimental set-up [372], absolute I/III values reported by different groups are difficult to compare. [Pg.34]

The modes of all three hydrides SiH, S1H2, and SiHs are observed simultaneously in the 2100-cm range however, the absorption intensities differ for hydrophobic and hydrophilic wafers. For a hydrophobic surface, the ratio AR/R is approximately 100 times higher than for a bonded hydrophilic sample [79]. In addition to Si—H, O2—Si—H (2200 cm ) and O3—Si—H (2250 cm ) vibration modes and O—H stretch modes (3725 cm ) are also observed (Fig. 6.18 [84]). [Pg.495]

A = absorbance c = concentration d = path length / = frequency 1,5 = absorption dissymmetry ratio glujjj = luminescence dissymmetry ratio I = light intensity J = total angular quantum number t = time = extinction coefficient A = wavelength a = standard deviation. [Pg.327]

It is often experimentally convenient to use an analytical method that provides an instrumental signal that is proportional to concentration, rather than providing an absolute concentration, and such methods readily yield the ratio clc°. Solution absorbance, fluorescence intensity, and conductance are examples of this type of instrument response. The requirements are that the reactants and products both give a signal that is directly proportional to their concentrations and that there be an experimentally usable change in the observed property as the reactants are transformed into the products. We take absorption spectroscopy as an example, so that Beer s law is the functional relationship between absorbance and concentration. Let A be the reactant and Z the product. We then require that Ea ez, where e signifies a molar absorptivity. As initial conditions (t = 0) we set Ca = ca and cz = 0. The mass balance relationship Eq. (2-47) relates Ca and cz, where c is the product concentration at infinity time, that is, when the reaction is essentially complete. [Pg.34]


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Absorption intensity ratio, time dependence

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