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Transient process data

The extruder would operate for several hours to days at steady state, and then for no apparent reason It would flow surge for several hours. After a period of time, the extruder would return to a steady-state operation and would remain there until the cycle repeated. Problem diagnosis was impossible without transient process data. Moreover, molten resin would frequently flow out the vent, especially during times of unsteady-state operation. [Pg.570]

The backbone of the DeNOx process over mononuclear TMI encaged in zeolites can be epitomized in the form of three interconnected cycles associated with the formation of the N2 and 02 reaction products (Figure 2.6), inferred from the steady state and transient rate data combined with spectroscopic evidence for surface species and... [Pg.34]

Nanosecond flash kinetic spectroscopy was also carried out on 2-hydroxy benzophenone and the copolymer (11). No transients could be detected in the nanosecond time scale, suggesting that the ground state enol [S (lb) in scheme 1] has a lifetime less than 1 x 10 9 sec. These results strongly imply that processes (3) and (4) are responsible for the deactivation of singlet energy in these systems. A small, non zero triplet yield is postulated in the copolymer both to account for the photodegradation data and the transient spectral data. Triplet... [Pg.33]

As has already been mentioned, picosecond pulsed radiolysis offers great possibilities for studying the short-lived transient processes. In Ref. 326 the solutions of 2,5-diphenyloxazol (DPO) in different solvents were irradiated by picosecond electron pulses obtained from an accelerator. The authors have found two types of excitations of DPO, which they have named the fast and the slow excitations. With fast excitation the luminescence appears during the electron pulse and stops growing at the end of the pulse, after 10 ps. With slow excitation the luminescence is formed within 1 ns. At small DPO concentrations the observed intensity of fast luminescence cannot be explained by direct excitation by electrons (cf. data of Ref. 325). Analyzing the results of experiments with different solvents and different types of additives, Katsumura et al.326 conclude that the main part of the fast luminescence of DPO is due to VCR absorption. [Pg.354]

Analysis of the transient decay data using the kinetic model shown in Figure 20b provides a rate constant of khop = 1.0 0.5 x 10 s" for the hole-hopping processes in the hairpins 3,5,6G3 and 4,6,7G3. This rate is consistent with the failure of hole hopping to compete with charge recombination in 2,4,5G3 (k r = 1.0 x 10 ° s ). It... [Pg.1827]

Durrant and co-workers performed ultra-fast interfacial electron injection studies with cM-Ru(dcb)2(NCS)2-Ti02 in 1 1 ethylene carbonate-propylene carbonate solvent and were able to observe both the oxidized sensitizer and the electron in Ti02 by time-resolved absorption spectroscopy [202]. Unfortunately, at long observation wavelengths, X = 650-900 nm, these absorption features overlapped with each other, making assignments and analysis difficult. Detailed analysis of the transient absorption data indicate that the electron injection process is at least bi-phasic with 50 % injecting in less than 150 fs and 50 % in 1.2 ps. [Pg.2769]

The combined procedure described above, which uses only sorption and steady state permeation data, specifies all five of the sorption and tran rt model parameters without requiring reference to the independenfly measured time lags, Com-pariscm of tiieoretically predicted time lags with flie experimentally meaaired values provides a rigorous test of the internal consistency of the transport and sorption data as well as a check of the applicability of the partial immobSization model for description of the transient processes. [Pg.77]

Figure 6.4. The 400 MHz HMQC spectra of 6.2 recorded (a) with and (b) without carbon decoupling during data collection. In the absence of decoupling, each crosspeak appears with doublet structure along f2 arising from Jch. These doublets are merely the usual C satellites observed in the ID proton spectrum. IK t2 data points were collected for 256 ti increments of 2 transients each. Data were processed with n/2 shifted sine-bells in both dimensions and presented in phase-sensitive mode. Zero-filling once in t resulted in digital resolutions of 4 and 40 Hz/pt in f2 and fi respectively. Figure 6.4. The 400 MHz HMQC spectra of 6.2 recorded (a) with and (b) without carbon decoupling during data collection. In the absence of decoupling, each crosspeak appears with doublet structure along f2 arising from Jch. These doublets are merely the usual C satellites observed in the ID proton spectrum. IK t2 data points were collected for 256 ti increments of 2 transients each. Data were processed with n/2 shifted sine-bells in both dimensions and presented in phase-sensitive mode. Zero-filling once in t resulted in digital resolutions of 4 and 40 Hz/pt in f2 and fi respectively.
The end points of any linear segment, x(ti) and x(ti+i), are either interpolated from the data or taken as actual data points as in the Boxcar method. These piecewise linear approximation techniques perform well for steady-state process data with little noise, but are inadequate for process data with important low amplitude transients and are inefficient for data with relevant high frequency features. Also, the line segments used in the approximation satisfy a local, not a global error criterion. [Pg.130]

The design responses of the transient processes have been acquired by means of the unit model BYTE. Eight criterial conditions are assessed which are posed on the controlled quantities. It is by meeting these criteria that it can be demonstrated that control system quality corresponds to the requirements defined in the design specifications. The criteria structure makes possible an automated processing of the measured data. [Pg.99]


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See also in sourсe #XX -- [ Pg.549 , Pg.570 ]




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