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Total Spectra

Generally, in each segment, three time-dependent processes run simultaneously oxygen transport in the GDL, oxygen transport in the CCL, and the double layer charging. The fourth time-dependent process is oxygen transport in the channel, which links the segments. To understand the contribution of each process to the local spectra, the respective time derivatives will be switched on one by one. [Pg.436]

Note Catalyst layer volumetric capacitance is estimated with the data (Adapted from Makharia, R., Mathias, M. F., and Baker, D. R. 2005. J. Electmchem. Soc., 152, A970-A977). [Pg.437]

FIGURE 5.25 Schematic of the interference of the local and transported perturbations. [Pg.438]

These local spectra consist of two overlapped semicircles, corresponding to the CCL (HF domain) and GDL (LF domain). However, a sophisticated fitting algorithm is necessary to separate the contribution of the transport in the GDL. [Pg.438]

One may expect this effect to be periodical along the frequency axis the perturbation from the zeroth segment arrives at the last segment in the same phase as the local perturbation, if an even number of half-waves fits into the channel length  [Pg.439]


Despite myriad tools to reannotate spectra and identify PTMs, their general efficacy is still limited, and only a small part of the total spectra are identified with high confidence. Moreover, there is no consensus PTM analysis pipeline yet, and therefore efforts need to be placed in the development of new software and the combination of the existing solutions in order to increase both detection coverage and confidence of PTMs. [Pg.409]

Fig. 3. An example of the automatic phase correction method as described by Witjes and co-workers In (a) are five representative spectra for a small expanded region in a H NMR spectra data set containing 15 total spectra. Note the small differences in phase shift between the spectra, most notable in the central spectrum. In (b) the same NMR spectra are shown following three iterations of the phase and frequency correction. The (c) first five initial loadings (P for the NMR data set reveal that the first loading (Pi) is a good descriptor of the desired spectral line shape, while higher loadings (P2 and P3) contain the majority of the information concerning phase shifts and frequency shifts between spectra in the data set. Fig. 3. An example of the automatic phase correction method as described by Witjes and co-workers In (a) are five representative spectra for a small expanded region in a H NMR spectra data set containing 15 total spectra. Note the small differences in phase shift between the spectra, most notable in the central spectrum. In (b) the same NMR spectra are shown following three iterations of the phase and frequency correction. The (c) first five initial loadings (P for the NMR data set reveal that the first loading (Pi) is a good descriptor of the desired spectral line shape, while higher loadings (P2 and P3) contain the majority of the information concerning phase shifts and frequency shifts between spectra in the data set.
Figure 6.22 Absorption total spectra for normal stromal prostate as reconstructed by the FPT at Np = 54 (top panel (i)) and Np = 800 (bottom panel (ii)), based on in vitro MRS data from Ref. [54]. Figure 6.22 Absorption total spectra for normal stromal prostate as reconstructed by the FPT at Np = 54 (top panel (i)) and Np = 800 (bottom panel (ii)), based on in vitro MRS data from Ref. [54].
In Figure 6.7, computed extinction spectra for the particle assemblies before and after the nanostructural changes are presented. The results from image analysis are used to compute extinction spectra of 368 particles with varying size parameters the total spectra of the sample are added up before (solid curve)... [Pg.192]

The concentration of proteins in blood plasma is 60 mg mL . In order to minimize any contribution to the signal by dissolved species [743], the ATR measurements are conducted in very dilute protein solutions ( 1 mg mL ). However, this is not the case with coated ATR, where the thickness of the thin-film substrate controls the penetration depth (see Section 4.1.3 for more detail). For example, at a solution concentration of 60 mg mL and under the optical conditions of 45° Ge MIRE coated with a 0.4-p,m-thick polymer coating, the contribution of the bulk solution was estimated to be 0.47% of the total spectra [769]. When it is necessary to follow adsorption at higher protein concentrations, special cells and measurement protocols based on internal standards are used for correcting for the bulk protein signal, which are discussed in detail by Jakobsen and Strand [743],... [Pg.614]

Figure 3.8 Vibronic two-photon absorption spectra of Sila-1f and 2 2a-2f of 4-dimethylamino-4 -Me-trans-stilbene calculated with B3LYP at the HF geomet7. Franck-Condon contribution, Herzberg-Teller contribution, and total spectra are shown for lifetime broadening of 0.10 eV (left panels) and 0.01 eV (right panels), respectively. The dashed line corresponds to the vertical transition [18]. (Reproduced with permission.)... Figure 3.8 Vibronic two-photon absorption spectra of Sila-1f and 2 2a-2f of 4-dimethylamino-4 -Me-trans-stilbene calculated with B3LYP at the HF geomet7. Franck-Condon contribution, Herzberg-Teller contribution, and total spectra are shown for lifetime broadening of 0.10 eV (left panels) and 0.01 eV (right panels), respectively. The dashed line corresponds to the vertical transition [18]. (Reproduced with permission.)...
Figure 7. Consecutive S Ip core-level spectra recorded on the surface of a D-PS sample. Total spectra acquisition time ( ) 15 minutes, (o) 30 minutes, ( ) 60 minutes, (0) 105 minutes, (A) 180 minutes and (A) 240 minutes... Figure 7. Consecutive S Ip core-level spectra recorded on the surface of a D-PS sample. Total spectra acquisition time ( ) 15 minutes, (o) 30 minutes, ( ) 60 minutes, (0) 105 minutes, (A) 180 minutes and (A) 240 minutes...
Depending on whether a single molecular polariz-cibility or site polarizabilities are attributed to the molecules under study rather different spectral contributions and total spectra were obtained. Thus despite... [Pg.291]


See other pages where Total Spectra is mentioned: [Pg.163]    [Pg.163]    [Pg.600]    [Pg.171]    [Pg.391]    [Pg.416]    [Pg.309]    [Pg.474]    [Pg.61]    [Pg.344]    [Pg.734]    [Pg.216]    [Pg.461]    [Pg.119]    [Pg.436]    [Pg.453]    [Pg.242]    [Pg.89]   


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Absorption total shape spectra

Attenuated Total Infrared Internal Reflectance (ATR) Spectroscopy (Spectra-Tech)

Attenuated Total Reflectance spectra

Attenuated Total Reflectance spectra of Nafion

Attenuated total reflectance infrared spectra

Attenuated total reflection spectrum

Autocorrelation function and total absorption spectrum

Converged absorption total shape spectra

Total coincidence spectrum

Total correlation spectroscopy spectra

Total emission spectrum

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