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Spectrum of the gas

Structural data are in the diagram these data were obtained from the microwave spectrum of the gas at low temperatures. The long (weak) N-N bond is notable (cf. 145 pm in hydrazine, p. 428). In this N2O3 resembles N2O4 (p. 455). [Pg.454]

The femtosecond spectrum of the gas-phase Nal molecule as it dissociates into the separate atoms. A peak in the lower spectrum is observed whenever the bond distance in Nal reaches a certain value. [Pg.652]

The pyramidal structure of symmetry Cg for FCIO2 was also confirmed by vibrational spectroscopy. E. A. Smith et al. (271) and Arvia and Aymonino (6) reported the infrared spectrum of the gas. D. F. Smith et al. (270) studied the infrared spectrum of the gas, measured the 3501-3701 i6Q i8o isotopic shifts, recorded the Raman spectrum of the liquid, and carried out a normal coordinate analysis. The observed frequencies and their assignment are summarized in Table XIII. [Pg.350]

C. Runge and Paschen found, however, that the spectrum of the gas from cleveite gave a yellow line which was double. Not until the Ds line of solar helium had also been conclusively proved to be double, did Runge and Paschen admit the existence of helium in cleveite (69, 72). [Pg.789]

Gates from the flash and laser irradiation of Pittsburgh seam (hvab) coal were investigated to determine the action of high temperatures on coal. Temperatures in excess of 1000°C. were reached with both types of irradiation. Craters about 300 microns in diameter were produced in the coal with millisecond pulses from the laser unit rated at 1.7 joules output. Gaseous products from the laser and flash irradiations showed 21% and 8% acetylene, respectively. Diacetylene, vinylacetylene, and other products to molecular weight 130 were indicated in the mass spectrum of the gas from the laser study. The results indicated that the distributions of products obtained from the flash and laser irradiations of coal were different from that produced in high temperature carbonization. [Pg.636]

Turn on the FABMS Gun with no target in the source. The pressure in the source chamber will increase when a gas gun is used but show no effect with a cesium gun. The spectrum of the gas, be it xenon or argon, will be observed - or cesium from a cesium gun. [Pg.137]

It should also be remembered that the selection rules derived here are relevant to the free molecule and may break down in the liquid or solid state. This is the case, for example, with the electric dipole forbidden 4g transition in ethylene, where v4 is the au torsional vibration shown in Figure 6.23. It is not observed in the infrared spectrum of the gas but is observed weakly in the liquid and solid phases. [Pg.172]

Specimen Conditioning. The sample was first placed in the preparation chamber and heated to 350 C. During this first heating in vacuum, there was normally some evolution of gas. The mass spectrum of the gas closely matched that of the tetrafluorethylene monomer. [Pg.225]

There have been detailed studies on the electronic absorption spectrum of the gas, and the magnetic circular dichroism spectrum has also been recorded and assigned 577,578,580 such spectra were also obtained for the aqueous solution.581 The electronic spectrum of the solid in an argon matrix at 20 K was measured and assigned.580 An energy level diagram was constructed on the basis of the... [Pg.589]

In this molecule, the hydrogen fluoride molecule, there is a single covalent bond (shared-electron-pair bond), which holds the hydrogen atom and the fluorine atom firmly together. The distance between the nuclei of these two atoms is 0.92A, according to experimental determination made by the study of the spectrum of the gas. [Pg.235]

The infrared spectrum of the gas is simple and requires no more than six fundamentab for complete assignment. A hypofluorite, FONF, molecule, could not have higher than C, symmetry (since F-O-N would be bent) and this would require nine dbtinct infrared-active fundamentab. Evidently the molecular symmetry of the new oxyfluoride is close to T, since the band contours of the degenerate fundamentals, of species e (J. bands), of which there are three in C, symmetry, are not readily dbtingubhed from the three a modes ( bands). Tentative assignments based on symmetry, are as follows (in cm. ) ... [Pg.249]

Interestingly, a normal mode coordination analysis of the Ni(C04)(PC3)2 fragment has shown that also in the case of the Ni-complex only species 7 and 9 are formed which can form only by insertion of the CO2 molecule in one 0-0 bond. This result and the finding that the FTIR spectrum of the gas evolved during the reaction have shown the presence of the CO2 free molecule, bring to... [Pg.679]

With the help of Sir William Crookes, the inventor of the discharge tube, Ramsay and Lord Rayleigh found that the emission spectrum of the gas did not match any of the known elements. The gas was a new element They determined its atomic mass to be 39.95 amu and called it argon, which means "the lazy one" in Greek. [Pg.320]

Cyclohexene was dried and vacuum-distilled before use. It was degassed by three freeze-punp-thaw cycles and stored over activated molecular sieves in a glass bulb. It was introduced into the reactor via vapor phase transfer through a high vacuum manifold (base pressure <10 Torr). After 30 mins, the epoxide yield was quantified on an HP 6890 GC/MS equipped with a J W Scientific DBl capilary column. At the end of each experiment, Ti analysis was performed (15) and epoxide/Ti ratios were calculated. For kinetics experiments, silica powder containing the /ert-butylperoxotitanium complex was prepared in an in situ reactor and the reaction initiated by addition of olefin. The IR spectrum of the gas phase above the silica was recorded at timed intervals. Pseudo-first-order rate constants... [Pg.539]

The rate of expoxidation was measure in situ via the uptake of cyclohexene vapor by the catalyst. At low pressures (ca. 10 Torr), cyclohexene does not adsorb on the unmodified silica surface nor on either of the silica-supported 2-alkoxide conplexes 1 and 3. However, the addition of cyclohexene vapor to 2 resulted in a rapid, exponential loss of v(C=C) intensity in the IR spectrum of the gas phase above the silica-supported complex. Figure 2. We infer that epoxidation results in adsorption of cyclohexene oxide on the catalyst surface. [Pg.542]


See other pages where Spectrum of the gas is mentioned: [Pg.882]    [Pg.334]    [Pg.326]    [Pg.795]    [Pg.798]    [Pg.288]    [Pg.149]    [Pg.451]    [Pg.452]    [Pg.536]    [Pg.996]    [Pg.302]    [Pg.225]    [Pg.233]    [Pg.584]    [Pg.612]    [Pg.398]    [Pg.126]    [Pg.130]    [Pg.177]    [Pg.180]    [Pg.288]    [Pg.157]    [Pg.158]    [Pg.159]    [Pg.160]    [Pg.365]    [Pg.1087]    [Pg.128]    [Pg.882]    [Pg.398]    [Pg.178]    [Pg.176]    [Pg.584]   
See also in sourсe #XX -- [ Pg.49 ]




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