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Dependence of light intensity

When molecules absorb visible or ultraviolet light, they are transformed from their ground state to the electronically excited states with high-energy contents. At room temperature. [Pg.43]

Such solutions, which are used to measure light intensities, are known as aclinometers. At pH ca. 3.5, the Fe(II) formed reacts with 1,10-phenanthioline to form the well-known red complex [Fe(phen)3l + (ferroin), whose molar absorption coefficient at 510 nm is well established ( = 11100 cm M ). [Pg.44]

Experiment 3.5. Experimental determination of the effect of light exposure on the photodecomposition of potassium ferrioxalate [9] [Pg.44]

Material. Stopwatch, colorimeter, 1 cm glass or plastic cuvettes, 1 dm volumetric flask, 250 cm Erlenmeyer flask, 1 cm graduated pipette. [Pg.44]

Experimental procedure. Prepare potassium ferrioxalate by adding, with stirring, a solution of potassium oxalate (1.5 M) to iron(lll) chloride (1.5 M) in the volume ratio 3 1. Recrystallise the precipitate obtained from water, and dry the potassium ferrioxalate crystals obtained and store in the dark. Prepare a 0.006 M solution of this actinometer in a 1 dm flask by dissolving 2.847 g of the crystals obtained in 800 cm water and adding sufficient [Pg.44]


Light emitted by chemiluminescent substrate was expressed in relative light units (RLU). The time dependence of light intensity was measured and the peak intensity was converted into percent of inhibition relative to control. We expressed the results as total antioxidant potential, expressed as percent inhibition TAPcl = ((max RLUconiroi) - (max RLUsampie)) 100 / (max RLUcontroi). Figure 1 shows the correlation between sum of phenolic compounds... [Pg.362]

Fjg. 19. Dependence of the intensity of the ESR signal on the wavelength of incident light of a complex of a polyfschiff base) (prepared from 4,4 -diacetyldiphenyl sulfide) with bromine mole ratio 1 4.8... [Pg.33]

In recent years, high-resolution x-ray diffraction has become a powerful method for studying layered strnctnres, films, interfaces, and surfaces. X-ray reflectivity involves the measurement of the angnlar dependence of the intensity of the x-ray beam reflected by planar interfaces. If there are multiple interfaces, interference between the reflected x-rays at the interfaces prodnces a series of minima and maxima, which allow determination of the thickness of the film. More detailed information about the film can be obtained by fitting the reflectivity curve to a model of the electron density profile. Usually, x-ray reflectivity scans are performed with a synchrotron light source. As with ellipsometry, x-ray reflectivity provides good vertical resolution [14,20] but poor lateral resolution, which is limited by the size of the probing beam, usually several tens of micrometers. [Pg.247]

Oxygen evolution rate of photosynthetic microalga Haematococcus pluvialis depending on light intensity and quality... [Pg.157]

A thorough insight into the comparative photoelectrochemical-photocorrosion behavior of CdX crystals has been motivated by the study of an unusual phenomenon consisting of oscillation of photocurrent with a period of about 1 Hz, which was observed at an n-type CdTe semiconductor electrode in a cesium sulfide solution [83], The oscillating behavior lasted for about 2 h and could be explained by the existence of a Te layer of variable width. The dependence of the oscillation features on potential, temperature, and light intensity was reported. Most striking was the non-linear behavior of the system as a function of light intensity. A comparison of CdTe to other related systems (CdS, CdSe) and solution compositions was performed. [Pg.229]

The rate of photolytic transformations in aquatic systems also depends on the intensity and spectral distribution of light in the medium (24). Light intensity decreases exponentially with depth. This fact, known as the Beer-Lambert law, can be stated mathematically as d(Eo)/dZ = -K(Eo), where Eo = photon scalar irradiance (photons/cm2/sec), Z = depth (m), and K = diffuse attenuation coefficient for irradiance (/m). The product of light intensity, chemical absorptivity, and reaction quantum yield, when integrated across the solar spectrum, yields a pseudo-first-order photochemical transformation rate constant. [Pg.29]

Fig. 10. The dependence of SH intensity in the mixed monolayer of C180AZ0N02 C1180C00H=1 1 on incident angle, a) and b) are p-polarized SH intensity when p- and s-polarized light was incident, respectively. Fig. 10. The dependence of SH intensity in the mixed monolayer of C180AZ0N02 C1180C00H=1 1 on incident angle, a) and b) are p-polarized SH intensity when p- and s-polarized light was incident, respectively.
The quantum efficiency of photo electrochemical reactions may vary from 2 to 4 the effective dissolution valence may vary from 2 to 4 and the efficiency of hydrogen evolution may vary from zero to near 1 depending on light intensity and potential. [Pg.184]

Network formation by photopolymerization has been studied for tetraethyleneglycol diacrylate (TEGDA) using isothermal calorimetry (DSC), isothermal shrinkage measurement and dynamic mechanical thermal analysis (DMTA). Due to vitrification the polymerization does not go to completion at room temperature. The ultimate conversion as measured by DSC seems to depend on light intensity. This can be explained by the observed delay of shrinkage with respect to conversion. [Pg.409]

With a somewhat stiffer monomer, 1,6-hexanediol diacrylate, (HDDA) we have previously observed that the ultimate conversion as measured with differential scanning calorimetry (DSC) also depends on light intensity. This has been attributed to the experimentally observed delay of shrinkage with respect to chemical conversion (7). In principle, such a dependence of conversion on intensity should show up in the mechanical properties as well. However, these are difficult to measure with thin samples of HDDA. [Pg.410]

For most practical photopolymerizations there is appreciable attenuation of light intensity with penetration and the dependence of polymerization rate on monomer, photoinitiator, and light intensity is more complex (see Eqs. 3-54 and 3-55 for exact definitions). Equation 3-54 is especially useful for analyzing the practical aspects of a photopolymerization. When polymerizing any specific thickness of reaction system it is important to know Rp at various depths (e.g., front, middle, and rear surfaces) than to know only the total Rp for that system thickness. If the thickness is too large, the polymerization rate in the rear (deeper) layers will be too low, and those layers will be only partially polymerized—the result would be detrimental because the product s properties (especially the physical properties) would be... [Pg.223]

A Raman spectrum is a plot of light intensity versus photon energy. In the vibrational spectroscopy it is usual to express the photon energy by the wavenumbers, defined as v = 1/A. In the Raman spectroscopy the use of absolute wavenumbers would be impractical, because the wavelength and, with that, the absolute wavenumber of each obtained Raman bands must always depend on the wavenumber of the incident light vq. However, only the... [Pg.260]

The OH concentration is then calculated from the rate of loss of NO, the CO concentration, and the known rate constants. In contrast to the observations of Carter et al. (1982), the chamber OH radical source was found to depend on light intensity and temperature, but not on N02. [Pg.881]


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