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Photoconversion Experiments

There are a number of recommended model pollutants for photoconversion experiments in water, as shown using Photo-CREC-Water I and II reactors (refer to sections 2.10.1 and 2.10.2). Phenol dissolves well in water and is not stripped significantly by the airflow, as proven experimentally by Salaices et al (2002). Methylene blue has strong [Pg.58]

It is recommended to monitor a number of parameters such as temperature, reaction time, pH, and radiation transmission conditions during the progress of the photocatalytic reaction. [Pg.59]

The overall reaction rate can also be followed using a Total Organic Carbon Analyzer (e.g. Shimadzu 5050) with an autosampler ASI 5000. The TOC analysis is based on the oxidation of the sample in a combustion chamber heated at 680° using platinum as a catalyst. In this instrument, the total sample carbon (TC) and the total inorganic carbon (IC) content are measured using different analytical methods. Vials with [Pg.59]

For photocatalytic conversion of model pollutants in air (refer to section 2.10.5), model pollutants such as iso-propanol, acetone, and acetaldehyde are recommended to be used. Acetone and iso-propanol injections of 40, 50, and 60/xl of the liquid pollutant can be employed in the 14.7 L Photo-CREC-Air reactor. For acetaldehyde 30,40, and 50 /xl liquid injections can be used to get the desired initial pollutant concentrations. A gas chromatograph (HP 5890) equipped with a HP-3393A integrator, a TCD and aPoropak Q packed column are adequate to identify and quantify chemical species, including product intermediates and carbon dioxide. Examples of this type of photocatalytic experiments for the photoconversion of model pollutants in air are provided in Chapter VIII. [Pg.60]

Ait-Ichou, I., Formenti, M., Pommier, B., and Teichner, S., 1985, Photocatalytic dehydrogenation of isopropanol on Pt/Ti02 Catalysts, J. Catal., 91 293-307. [Pg.61]


The proposed model appears to be adequate to monitor the changes in acetone concentration in the gas phase during the photoconversion experiments. [Pg.153]

Later experiments (4 ) were designed to determine a cell e.m.f. for the plutonium disproportionation system with a particular light source. Concentration quotients for the light and dark conditions, Qg and Qj, were determined, and an energy difference of 1.65 kcal (32 mV) was calculated by the relation -RTln C /Qd This reversible photochemical shift may be the only single-element system known at this time and certainly is the simplest such system. Even though the radioactive properties could prevent development and utilization of a plutonium photoconversion system, these studies certainly suggest that similar nonradioactive and more acceptable systems could be discovered and developed. [Pg.270]

The first series of ejqieriments was conducted with no fhotocatalyst in the reactor. During these experiments, a temperature dependance of the reaction was observed photoconversion of methane decreased sharply with decreased tenperature and was not observed below 70°C. This observation irr jlies that a non-photochemical process is part of the reaction sequence. Sevaal experiments were perform where the ten rerature of the reactor was allowed to cycle between 60°C and 95 C. In all ergreriments, as Ae tengrerature... [Pg.410]

Valentin, G., Verheggen, C., Piolot, T., Neel, H., Coppey-Moisan, M. and Bertrand, E. (2005). Photoconversion of YFP into a CFP-like species during acceptor photobleaching FRET experiments. Nat. Methods 2, 801. [Pg.230]

We demonstrate by using ultrafast time resolved spectroscopy that the photoconversion from dihydroazulene (DHA) to vinylheptafulvene (VHF) is governed by two mechanisms The ring opening proceeds on the excited energy surface on the picosecond time scale. It is followed by an internal conversion to the VHF ground state that is accelerated by the presence of a conical intersection in the case of cyclopenta-DHA. This conical intersection hinders the photoinduced back reaction from the final VHF products. However, we successfully photo-converted the cyanophenyl-VHF-cis back to the DHA in an experiment with two delayed pulses. This opens the route to the development of bistable dihydroazulene switches. [Pg.279]

To this aim we study the DHA/VHF photoconversion in an approach that combines broadband transient absorption with 100 fs pulses and two color experiments with sub-30 fs pulses. The former provides a clear identification of the transient states involved in the process, while the later allows us to determine precisely the kinetics of the process. Through the analysis of the coherent signal observed in addition we are able to identify the structural evolution of DHA directly after the application of the ultrashort pump pulse. [Pg.279]

This idea was probed by irradiating two samples of CN-DHA with the same concentration and volume in a one pump pulse and a two pump pulses experiment [7] In the one pulse experiment the photoconversion to CN-VHF-trans was triggered at 340 nm under similar conditions as in the two color time resolved measurements. The irradiation time t was chosen such that a significant amount of CN-VHF-trans was converted. In the two pulses experiment an additional pulse at 530 nm which was delayed by 25 ps from the first pulse excited the transient CN-VHF-cis for the same time t. After the irradiation much less CN-VHF-trans is found in the two pulse experiment than in the one pulse experiment (Fig. 4). We conclude that a significant amount of CN-DHA was regenerated from the transient species by the second pulse. Photodegradation and thermal activation by the 530 nm pulses were eliminated as possible reasons for the observed effect. [Pg.282]

Low temperature experiments have shown the formation of hypso intermediates from several species [99,103,105-107]. The study of early photoconversion processes in squid [108], which also involved the evaluation of the relative quantum yields among the four pigments (squid rhodopsin, squid batho-, hypso- and isorhodopsin) showed that hypsorhodopsin is a common intermediate of rhodopsin and isorhodopsin there is no direct conversion between rhodopsin and isorhodopsin bathorhodopsin is not converted directly to hypsorhodopsin and both rhodopsin and isorhodopsin convert more efficiently to bathorhodopsin than to hypsorhodopsin. While a temperature dependence of the relaxation processes from the excited state of rhodopsin, and an assumption that batho could be formed from one of the high vibrational levels of the ground state hypso have been invoked to explain these findings [108], the final clarification of this matter awaits results from subpicosecond laser photolysis experiments at liquid helium temperature. [Pg.299]

The rate of photoconversion in a heterogeneous process is normally expressed in terms of a limited number of variables that should include the concentrations of the species present, the reactor volume, and the amount of catalyst irradiated in this particular volume. In the case of the immersion well-stirred photochemical reactor, currently used in photocatalytic experiments, the rate (r) expression for photoconversion is given by [199]... [Pg.488]

In order to clarify the dependence of the initial photoconversion rate with f-i Pa), Salaices et al. (2001) developed experiments with phenol with a changing incident absorbed radiation. As suggested by a number of authors (Okamoto et al., 1985 Ollis, 1991 Pelizzetti et al., 1993 Trillas et al., 1996, 1992 Wei et al., 1994), it is proven that at low levels of absorbed incident radiation there is a lineai relationship between the initial photoconversion rate of phenol and the incident absorbed radiation, r, =... [Pg.7]

Experiments performed using MeB have intrinsic advantages as MeB blue s colour disappears as photoconversion progresses and provides a quick assessment of the reactor performance. This colour change is easy to follow via spectrophotometery (k = 664 nm). [Pg.135]

The results in Table III show the effect of various amines of different ionisation potential on the photopolymerisation of 2-hydroxyethylmethacrylate in nitrogen saturated water initiated by the benzophenone with the structure 2. As found earlier for the water soluble thioxanthones ( ), the percentage photoconversion decreases with increasing ionisation potential of the amine. In all of these experiments, oxygen had a strong quenching effect on the photopolymerisation. It would appear, therefore, that in aqueous media the photoinduced polymerisation of the acrylate monomer occurs solely via the lowest excited triplet state of the benzophenone molecule to form an exciplex with the amine co-synergist (Schemel ). [Pg.76]

The infiuence of supported Au particles on the photoconversion of NO2 has been investigated by simultaneous detection of gas phase and surface species using DRIFTS by Ramakrishnan et al. [24]. The nanosized Au-supported catalyst was prepared by deposition of pre-prepared Au nanoparticle precursor solution onto titania. The catalysts were illuminated in the in situ reaction chamber by a 365 nm 50 mW LED UV source coupled with fiber optics while simultaneously collecting the diffuse reflectance spectra. Adsorption of NO2 is negligible in dark however, new absorption bands arose between 1200 and 1800 cm after starting illumination of the catalyst (Figure 4.1). The band intensities observed with Au-supported catalysts increase markedly with N O2 photocatalytic conversion in the quadrupled gas phase. Marked increase of activity has also been confirmed for the photooxidation of phenol in parallel batch experiments. [Pg.68]

Preliminary studies of the trans-cis photisomerization kinetics recommended an irradiation time of at least 15 minutes to reach the photostationary state and to have the maximum photoconversion for all dyes. This time was therefore used in all photoisomerization experiments. Molar absorption coefficients, e,rans and Ecu, of the photochromic molecules dispersed in the polymer matrix were calculated from absorbance measurements, using the Lambert-Beer law ... [Pg.68]


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Photoconversion

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