Clear window time

For an air/glass interface, tan 0b = n, the refractive index of glass. In a gas laser, the light must be reflected back and forth between mirrors and through the gas container hundreds of times. Each time the beam passes through the cavity, it must pass through transparent windows at the ends of the gas container (Figure 18.10b), and it is clearly important that this transmission be as efficient as possible. 

A janitor surrounded by sensitive instruments may be like a bull in a china shop. In one laboratory, the janitors were not allowed to clean anything above floor level, including windows, without supervision by laboratory personnel. Janitors should not be allowed to handle containers of flammable or hazardous waste. Laboratory personnel should clear the floors completely when the janitor announces that it is time for floor waxing. 

Within the potential range where Ru(bpy)3 remains in the aqueous phase, photocurrent responses are clearly observed with a slow rising time of the order of 10 s as shown in Fig. 14(a). According to the convention employed by these authors, positive currents correspond to the transfer of a negative charge from water to DCE. No photoresponses were observed in the absence of either the dye in the aqueous phase or TCNQ in DCE. Further analysis of the interfacial behavior of the product TCNQ revealed that the ion transfer occurred outside of the polarizable window [cf. Fig. 14(d)], confirming that these photoresponses are not affected by coupled ion-transfer processes. An earlier report also showed photoeffects for the photoreduction of the viologen under similar conditions [131]. 

Polycarbonate can be readily injection molded. Polycarbonates typically require only a short injection molding cycle time, because the polymer flows into the mold easily and solidifies rapidly. We injection mold polycarbonate to produce a wide variety of commercial goods, including compact disks, jewel cases, aircraft windows, kitchen utensils, and clear refrigerators drawers. Polycarbonates are also found in a wide range of disposable medical devices, such as the flow locks on intravenous tubes and the hard, disposable components of dialysis machines. Impact resistant polycarbonate is used to manufacture sports and other safety helmets. Glass fiber reinforced polycarbonate is used in the housings for power tools. 

The most important statistic represents the final plateau of the CDF and the area AUCoo of the corresponding PDF between t = 0 and t = oo. It clearly quantifies the extent of the relevant process, which is in proportion to the applied dose D, or a constant fraction or multiple f D of this, in case of overdose, chemical degradation, etc. Proportionality with dose is violated only if the process contains nonlinear or time-dependent steps such as early loss by defecation, absorption windows, chemical degradation, or non-linear presystemic (first-pass) elimination. 

At this point, it is worthwhile to return on the theoretical basis of the kinetic method, and make some considerations on the assumptions made, in order to better investigate the validity of the information provided by the method. In particular some words have to been spent on the effective temperamre The use of effective parameters is common in chemistry. This usually implies that one wishes to use the form of an established equation under conditions when it is not strictly valid. The effective parameter is always an empirical value, closely related to and defined by the equation one wishes to approximate. Clearly, is not a thermodynamic quantity reflecting a Maxwell-Boltzmann distribution of energies. Rather, represents only a small fraction of the complexes generated that happen to dissociate during the instrumental time window (which can vary from apparatus to apparatus). 

The steady-state luminescence spectra of three different plastics are characterized by blue luminescence with Amax = 445-465 nm, while much broader liuninescence band with yellow color characterizes the dolomite rocks. These spectra are different, but not enough to differentiate between them from big distance. The decay properties have been also checked in order to improve the selective feature. It was found that luminescence intensity of rocks in the blue part of the spectrum is drastically diminished after specific delay time, while the decrease of intensity in the yellow part of the spectrum is mush more moderate. Liuninescence intensity of all plastics also diminishes after such delay, nevertheless remaining mush stronger then intensity of rocks luminescence in the blue part of the spectrum. The comparison of plastic and rock time-resolved spectra in specific time window clearly demonstrate that they are absolutely different, which made confident discrimination possible (Fig. 7.3). 

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