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Upper absorption limit

As mentioned in Section 19.4, niobium may accumulate in plants, but is not an essential nutrient for either humans or animals. Studies on the metabolism of niobium compounds are few in number, but most utilize the radionuclide Nb, which is a by-product of fissionable material. The absorption of Nb from the gastrointestinal tract varies, but an upper absorption limit of 5% of the amount ingested has been reported in several species (Thomas et al. 1967, Cuddihy... [Pg.1042]

Molecular size can be further limiting factor in oral absorption [61]. The Lipinski rule-of-5 proposes an upper MW limit of 500 as being acceptable for orally absorbed compounds [9]. Size and shape parameters are generally not measured, but rather calculated. One measured property is the so-called cross-sectional area, which is obtained from surface activity measurements [62],... [Pg.9]

Figure 6.18 Plot of dose qo vs. the dimensionless solubility-dose ratio 1/6. The curves indicate 90% absorption for three radius sizes 10, 25, and 50 /xm assuming Peff = 1.2 X 10-2 cmmin-1. Since the value assigned to Peff corresponds to the upper boundary limit (expressed in apparent permeability values, [170]) of the borderline permeability region of QBCS [224], compounds of category II of QBCS exhibiting complete absorption are located above the curves. Figure 6.18 Plot of dose qo vs. the dimensionless solubility-dose ratio 1/6. The curves indicate 90% absorption for three radius sizes 10, 25, and 50 /xm assuming Peff = 1.2 X 10-2 cmmin-1. Since the value assigned to Peff corresponds to the upper boundary limit (expressed in apparent permeability values, [170]) of the borderline permeability region of QBCS [224], compounds of category II of QBCS exhibiting complete absorption are located above the curves.
Carabine and Norrish found results somewhat different from those of the other studies. Furthermore, they also found that a small amount of O3 accelerated the non-explosive reaction, but did not raise the upper ignition limit. They studied the flash photolysis of B2H6-O2 mixtures with radiation below 2000 A. Intermediates BH, OH, BO, and BO2 were monitored by absorption spectroscopy. Water was not a final product of the reaction unless the B2H6 was completely consumed. Almost surely it was produced, but was removed in a rapid reaction with B2H6. [Pg.108]

Hazard Toxic by ingestion, inhalation, and skin absorption. Combustible. Upper explosive limit 22%. A skin irritant. [Pg.280]

Fig. 7. Lower and Upper Detection Limits. When a measurement process has both minimum and maximum signal bounds, as in radioactive decay and optical absorption spectrometry, LLD and ULD must both be considered. Dashed line signal lower and upper detection limits map onto the age and concentration lower and upper limits (arrows) via the exponential function. Fig. 7. Lower and Upper Detection Limits. When a measurement process has both minimum and maximum signal bounds, as in radioactive decay and optical absorption spectrometry, LLD and ULD must both be considered. Dashed line signal lower and upper detection limits map onto the age and concentration lower and upper limits (arrows) via the exponential function.
PHa + Oj- Products. The rate constants k were measured at 300 K by flash photolysis (FP) of PH3/O2/N2 mixtures (0.35 3.5 to 17 250 to 270 Torr) and PH3/O2 mixtures (0.35 1.5 Torr), above the upper and below the lower explosion limit, followed by absorption of radiation near 455 nm (from a pulsed dye laser) by PH2. k = (1.2 0.3)x10" at a total pressure of -270 Torr (i.e., above the upper explosion limit) was derived from the dependence of the effective rate constant k ff=d ln([PH2]o/[PH2])/dt on the O2 partial pressure, k = (0.8 0.2) x10" at 1.85 Torr (i.e., below the lower explosion limit) was obtained from a computer calculation of keff with known rate constants for PH3 + H PH2 + H2 (see p. 233) and 2PH2+M P2H4+M (see below). The agreement of both k values points to a pressure-independent reaction PH2 + 02 products. The step PH2 + 02 P02 + H2 is probably responsible for the observed rapid decay of PH2 [3, 4]. A later measurement of the removal of rotationally thermalized PH2 (X Bi, v = 0) in the presence of O2 by laser-induced fluorescence (LIF) under pseudo-first-order conditions gave k = 2.7x10 . The removal of vibrationally excited PH2 by O2 was also investigated [5]. [Pg.89]

Table 8.4 Upper wavelength absorption limits of some solvents... Table 8.4 Upper wavelength absorption limits of some solvents...
Several well-characterized crystals for frequency doubling or frequency sum up to 0.25 pm which corresponds to the fourth harmonic of the YAG laser frequency (1.053 pm), are proposed by crystal manufacturers with outstanding conversion efficiencies. This upper frequency limitation around 0.25 pm results from the onset of absorption above this frequency and concomitant heating in practically all efficient doubling crystals there are similar limitations towards the mid- and far-IR spectrum because of strong absorption bands there due to IR active lattice modes (phonons, vibrations) and one resorts here to other nonlinear processes and coupling schemes. [Pg.533]

The marked differences between light water and heavy water with iv-spect to moderating ability and thermal neutron absorption cross. -ci ti.c. make solutions in both solvents of interest for reactor use. (iennrai i- speaking, the upper temperature limit of solution stability occurs abn 10°C lower in heavy-water solutions than in light-water solutions. [Pg.86]

Fig. 26. Dependence of the degradation rate on the upper temperature limit used in temperature-induced cycling of La 3EUo, Ni4, iMno4. The vertical axis represents IC divided by the number of cycles needed to achieve a loss of 50% of the absorption capacity (after Cohen et al., J980a). Fig. 26. Dependence of the degradation rate on the upper temperature limit used in temperature-induced cycling of La 3EUo, Ni4, iMno4. The vertical axis represents IC divided by the number of cycles needed to achieve a loss of 50% of the absorption capacity (after Cohen et al., J980a).
In photoselection experiments eosin-SCN, when completly immobilized in rigid media, behaves as an ideal linear absorber. Under proper experimental conditions we obtained values of the absorption anisotropy of r(0)=0.37 which were very close to the upper theoretical limit (0.4) (see Ref.5). [Pg.580]

The absorption of SO for oleum production is carried out over a relatively narrow temperature range. The upper temperature is set to provide a reasonable partial pressure driving force for the oleum concentration used. The lower practical temperature limit is the freezing point of oleums, which is high enough to be a problem in shipping and handling as well. For some oleum uses it is practical to add small amounts of HNO as an antifreeze (100). [Pg.187]


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Upper Limit

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