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Intensity of irradiation

Intensity of Irradiation. As discussed below the ionic sample Sriginates from a small volume with a radius of approximately 1 mm., and one can visualize this volume as a sphere placed on top of the leak, oince the distance from the leak to the ion source (R = 3 cm.) is relatively large, we can use a point-source approximation to obtain j, the... [Pg.218]

I is the number of ions created per unit volume and time. The value used was / = 1.4 X 1010 ions cc.-1 sec.-1 which corresponds to irradiation with a 50-mc. source (see section on intensity of irradiation above) n is the number of ions per cc. Ion recombination coefficient... [Pg.222]

Ifi fluorescence intensity k proportionality factor lo intensity of irradiating hght e molar absorption coefficient a amount of substance applied d thickness of adsorbent layer... [Pg.28]

Fig. 2.2 Radius and pressure profiles in the case of Transient Cavitation (Typical profile at frequency of irradiation = 20 kHz, Intensity of irradiation = 0.12 W/m2 and initial radius of the nuclei = 0.001 mm)... Fig. 2.2 Radius and pressure profiles in the case of Transient Cavitation (Typical profile at frequency of irradiation = 20 kHz, Intensity of irradiation = 0.12 W/m2 and initial radius of the nuclei = 0.001 mm)...
Overall, it can be said that for single frequency operation an optimum intensity of irradiation should be selected, whereas for multiple frequency operation, existence of optimum intensity has not been observed but this cannot be generalized. [Pg.53]

In the sonochemical reactors, selection of suitable operating parameters such as the intensity and the frequency of ultrasound and the vapor pressure of the cavitating media is an essential factor as the bubble behavior and hence the yields of sonochemical transformation are significantly altered due to these parameters. It is necessary that both the frequency and intensity of irradiation should not be increased beyond an optimum value, which is also a function of the type of the application and the equipment under consideration. The liquid phase physicochemical properties should be adjusted in such a way that generation of cavitation events is eased and also large number of smaller size cavities are formed in the system. [Pg.63]

Moholkar et al. [11] studied the effect of operating parameters, viz. recovery pressure and time of recovery in the case of hydrodynamic cavitation reactors and the frequency and intensity of irradiation in the case of acoustic cavitation reactors, on the cavity behavior. From their study, it can be seen that the increase in the frequency of irradiation and reduction in the time of the pressure recovery result in an increment in the lifetime of the cavity, whereas amplitude of cavity oscillations increases with an increase in the intensity of ultrasonic irradiation and the recovery pressure and the rate of pressure recovery. Thus, it can be said that the intensity of ultrasound in the case of acoustic cavitation and the recovery pressure in the case of hydrodynamic cavitation are analogous to each other. Similarly, the frequency of the ultrasound and the time or rate of pressure recovery, are analogous to each other. Thus, it is clear that hydrodynamic cavitation can also be used for carrying out so called sonochemical transformations and the desired/sufficient cavitation intensities can be obtained using proper geometric and operating conditions. [Pg.73]

Literature data on cytotoxic effects of photoexcited fullerene C60 are controversial. In the studies on transformed B-lymphocytes of Raji fine, phototoxic action of water-soluble carboxy-C60 was not revealed even upon its concentration of 5 x 10 5 M (Irie et al., 1996). In the study (Kamat et al., 2000) damaging effect of fullerenes C60 in dependence on intensity of irradiation toward CHO cells has been demonstrated. Using microsomal fraction of rat liver that was treated with C -cyclodextrin complex, it was shown that already in 5-30 min after UV-irradiation the accumulation of LPO products occurs that is suppressed by antioxidants like ascorbic acid and a-tocopherol. Similar effect of fullerenes C60 has been revealed in microsomal fraction of the cells of ascitic sarcoma 180 (Kamat et al., 2000). [Pg.131]

Fluorescence excitation with a laser microbeam allows for a smaller region to be illuminated. Monitoring fluorescence with a sensitive photomultiplier tube also permits the use of lower intensities of irradiation for shorter periods of time. Therefore, unwanted photobleaching can be significantly reduced. If the spot size is adjusted to illuminate an entire cell, information analogous to spectrofluorometry or flow cytometry can be obtained on an individual cell basis with a high degree of temporal resolution. If the spot size is smaller than the cell, similar information can be obtained from a particular location within the cell. [Pg.161]

Acoustic intensity has a dramatic influence on the observed rates of sonochemical reactions. Below a threshold value, the amplitude of the sound field is too small to induce nucleation or bubble growth. Above the cavitation threshold, increased intensity of irradiation (from an immersion horn, for example) will increase the effective volume of the zone of liquid which will cavitate, and thus, increase the observed sonochemical rate. [Pg.1526]

Some measurements were taken to appraise the intensity of irradiation along the length of the chute. These are shown in the graph at the bottom of Figure 1. The intensity is more uniform than might be expected. However, the data are incomplete since the whole length was not examined. It was expected that a commercial installation will have quite different geometry, and therefore, its distribution will be more relevant. [Pg.142]

Flosdorf and Chambers (1933) reported that metal sulfides were oxidized in the presence of audible sound (1 to 15 kHz) while investigating the bactericidal action of audible sound however, Schmitt et al. (1929) were the first researchers to observe the rapid oxidation of dissolved H2S gas to colloidal sulfur during sonication at 750 kHz with a 250-W power source. They reported that an increase in the total pressure of the system (P02) led to higher oxidation rates up to a limiting critical pressure. This critical pressure depended on the amount of dissolved H2S gas and the intensity of irradiation. The primary oxidation product was found to be elemental sulfur. The overall reaction was thought to proceed via reactions of HS with OH radicals, HO radicals, or H202. [Pg.469]

The switching lifetime of the resonance frequency has been observed to exhibit an exponential dependence on the intensity of irradiation. 157 The intensities of the emission lines from each state are proportional to the probability of the TLS population in that site. This ratio is given by... [Pg.6]

Under the indicated conditions, the amount v of light quanta adsorbed by colloidal particle per second at the intensity of irradiating light Io 3 mW/cm2 = 0.8-10 8 Einsteins cm 2 may be easily found as ... [Pg.66]

The systematic study of foam bilayers from phospholipids [28,38-40] reveals that they do not rupture spontaneously at any concentration allowing their formation. That is why in the case of phospholipid foam bilayer the dependence of their mean lifetime on the bulk amphiphile concentration cannot be measured in contrast to foam bilayer from common surfactants [41,42], This infinite stability of phospholipid foam bilayers is the cause for the steep W(d) and W(C) dependences. In the case of AF foam bilayers this high stability was confirmed by a very sensitive method [19,43] consisting of a-particle irradiation of foam bilayers. As discussed in Sections 2.1.6 and 3.4.2.2, the a-particle irradiation substantially shortens the mean lifetime of foam bilayers. The experiments showed that at all temperatures and dilutions studied (even at d,), the foam bilayers from AF did not rupture even at the highest intensity of irradiation applied, 700 (iCi. [Pg.746]

The high intensity of irradiation in the zone close to the tip may produce radical species potentially interfering with the normal course of the experiment. [Pg.20]

A common practice for the determination of the intensity of irradiation is the use of physical devices that are based on either the internal or the external photo effect. The internal photo effect is exploited in semiconducting materials. Thus, photons absorbed by these materials cause a charge transfer from the valence band to the conducting band of the semiconductor. The resultant increase in conductivity is measured and is related to the number of photons impinging on the surface of the photodiode. Many types of photodiodes are known, the specific properties of which are tailored to their particular applications (for details, see Chapter 9). Thus, different sizes, response times, and signal-to-noise levels have been achieved. Moreover, such devices are inexpensive however, as will be discussed later, they... [Pg.140]

Figure 24. Relationship between the rate of polymerization (TMPTA) and the free energy change for photo-redox reaction for benzophenone -TAA initiating systems. Irradiation of the polymerization mixture was carried out using part of the UV emission (300-400 nm) of a xenon lamp (Philips CSX 150 W/1) with intensity of irradiation / = 120 mW cm . ... Figure 24. Relationship between the rate of polymerization (TMPTA) and the free energy change for photo-redox reaction for benzophenone -TAA initiating systems. Irradiation of the polymerization mixture was carried out using part of the UV emission (300-400 nm) of a xenon lamp (Philips CSX 150 W/1) with intensity of irradiation / = 120 mW cm . ...

See other pages where Intensity of irradiation is mentioned: [Pg.262]    [Pg.40]    [Pg.63]    [Pg.734]    [Pg.261]    [Pg.40]    [Pg.50]    [Pg.52]    [Pg.52]    [Pg.52]    [Pg.53]    [Pg.53]    [Pg.88]    [Pg.63]    [Pg.56]    [Pg.190]    [Pg.66]    [Pg.167]    [Pg.147]    [Pg.262]    [Pg.71]    [Pg.63]    [Pg.267]    [Pg.214]    [Pg.398]    [Pg.38]    [Pg.262]    [Pg.114]    [Pg.300]    [Pg.328]   
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