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NASA Scientific and Technical Aerospace Reports

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for normal physiological function of animals <strong>and</strong> humans. The Food <strong>and</strong> Nutrition Board of the National Academy of Science<br />

(NAS) sets an adequate intake for manganese at 2.3 mg/day for men <strong>and</strong> 1.8 mg/day for women, <strong>and</strong> an upper limit for daily<br />

intake at 11 mg for adults (IOM, 2002). Manganese has a low aesthetic threshold in water. Based on staining <strong>and</strong> taste, EPA<br />

has set a secondary level for manganese at 0. 05 mg/L which is below the level that may present a health concern. Available<br />

data suggest that regulation of manganese in public water does not present a meaningful basis for health risk reduction. EPA<br />

will present a determination <strong>and</strong> further analysis in the Federal Register Notice covering the Contaminant C<strong>and</strong>idate List<br />

proposals.<br />

NTIS<br />

Contaminants; Dosage; Exposure; Health; Manganese; Risk<br />

20040050381 Lawrence Livermore National Lab., Livermore, CA<br />

Inductively Coupled Plasma Mass Spectrometery Uranium Error Propagation<br />

Hickman, D. P.; Maclean, S. C.; Shepley, D.; Shah, R. K.; Jul. 2001; 12 pp.; In English<br />

Report No.(s): DE2004-15006257; UCRL-ID-145113; No Copyright; Avail: Department of Energy Information Bridge<br />

The Hazards Control Department at Lawrence Livermore National Laboratory (LLNL) uses Inductively Coupled Plasma<br />

Mass Spectrometer (ICP/MS) technology to analyze uranium in urine. The ICP/MS used by the Hazards Control Department<br />

is a Perkin-Elmer Elan 6000 ICP/MS. The Department of Energy Laboratory Accreditation Program requires that the total<br />

error be assessed for bioassay measurements. A previous evaluation of the errors associated with the ICP/MS measurement<br />

of uranium demonstrated a (+-) 9.6% error in the range of 0.01 to 0.02(micron)g/l. However, the propagation of total error<br />

for concentrations above <strong>and</strong> below this level have heretofore been undetermined. This document is an evaluation of the errors<br />

associated with the current LLNL ICP/MS method for a more exp<strong>and</strong>ed range of uranium concentrations.<br />

NTIS<br />

Plasmas (Physics); Mass Spectrometers; Inductively Coupled Plasma Mass Spectrometry<br />

20040050575 Kyoto Univ., Japan<br />

Memoirs of the Faculty of Science, Kyoto University: Series of Physics, Astrophysics Geophysics <strong>and</strong> Chemistry,<br />

Volume 45<br />

March 2004; ISSN 0368-9689; 103 pp.; In English; Copyright; Avail: Other Sources<br />

Time evolution of the 113s(sub 1/2) state of Rb-85 in a pulsed electric field was investigated at the region of the first<br />

avoided-crossing with its adjacent manifold. The state was initially prepared by laser excitations at a well isolated Stark<br />

position from the manifold, <strong>and</strong> driven into an electric field (FT) over the first avoided crossing point with various slew-rates.<br />

The s(sub 1/2) state was then field-ionized with a following high slew-rate pulsed electric field; Specifically in this field<br />

ionization process with high slew-rate regime, a constant transverse electric field was applied to enhance the tunneling field<br />

ionization process resulting from the angular momentum rotation due to the effect of a rotating electric field. Three paths<br />

through the Stark map were identified with sharp peaks in the ionization field-strength observed. One path corresponds to the<br />

autoionization-like process, while the other two paths are due to the tunneling processes with an adiabatic <strong>and</strong> a non-adiabatic<br />

transitions, respectively. Transition rates to these ionization paths, measured as a function of the slew rate, were found to be<br />

strongly dependent on how deep the state is driven into the manifold-merged region at F(sub r) before the fast ionization-pulse<br />

was subsequently applied. Quantum theoretical predictions, taking into account explicitly the occurrence of the multilevel<br />

avoided crossings, reproduce well the experimental transition rates to the paths leading to the tunneling field-ionization. The<br />

transitions leading to the autoionization-like process, however, show different behavior from those to the tunneling process,<br />

indicating an interference effect in the process.<br />

Author<br />

Astrophysics; Universities; Geophysics; Chemistry; Science<br />

20040050662 Florida Univ., Gainesville, FL<br />

Conjugated Polyelectrolytes: Synthesis <strong>and</strong> Applications<br />

Pinto, Mauricio R.; Schanze, Kirk S.; Apr. 28, 2002; 18 pp.; In English<br />

Contract(s)/Grant(s): DAAD19-00-1-0002<br />

Report No.(s): AD-A420917; UF-NIF-10; ARO-40422.55-MS; No Copyright; Avail: CASI; A03, Hardcopy<br />

Conjugated polyelectrolytes are conjugated polymers that feature ionic side groups which render the materials soluble in<br />

water <strong>and</strong> other polar solvents. In this review we summarize recent work which has been carried out to synthesize a variety<br />

of new conjugated polyelectrolyte structures, including those with poly(paraphenylene), poly(phenylene vinylene) <strong>and</strong><br />

28

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