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Helium reaction

Let us do a little bookkeeping with the exact masses of these nuclei. Actually we will simplify a bit and use the exact masses of the atoms. This will make no difference. The masses of the atoms differ from the nuclear masses by the masses of the number of electrons in each atom. We have shown that electrons are conserved in nuclear changes. Exact masses of atoms (that is, exact masses of each isotopic species and not the chemical atomic weights shown on the inside back cover) are readily available. For our hydrogen-helium reaction we have... [Pg.121]

The rate coefficient for quenching N2+(B22, u = 0) in collisions with helium [reaction (11.23)] is relatively small. [Pg.190]

Figure 5. The C-ls XPS spectra for LDPE film treated with 5% and 15% mixtures of fluorine in helium. Reactions carried out in the dark region of the plasma. Figure 5. The C-ls XPS spectra for LDPE film treated with 5% and 15% mixtures of fluorine in helium. Reactions carried out in the dark region of the plasma.
Several instniments have been developed for measuring kinetics at temperatures below that of liquid nitrogen [81]. Liquid helium cooled drift tubes and ion traps have been employed, but this apparatus is of limited use since most gases freeze at temperatures below about 80 K. Molecules can be maintained in the gas phase at low temperatures in a free jet expansion. The CRESU apparatus (acronym for the French translation of reaction kinetics at supersonic conditions) uses a Laval nozzle expansion to obtain temperatures of 8-160 K. The merged ion beam and molecular beam apparatus are described above. These teclmiques have provided important infonnation on reactions pertinent to interstellar-cloud chemistry as well as the temperature dependence of reactions in a regime not otherwise accessible. In particular, infonnation on ion-molecule collision rates as a ftmction of temperature has proven valuable m refining theoretical calculations. [Pg.813]

Fusion of a nucleus of with one of helium gives 0 Eventually the helium too becomes de pleted and gravitational attraction causes the core to contract and its temperature to increase to the point at which various fusion reactions give yet heav ler nuclei... [Pg.6]

To achieve the very low initial fluorine concentration in the LaMar fluorination process initially a helium or nitrogen atmosphere is used in the reactor and fluorine is bled slowly into the system. If pure fluorine is used as the incoming gas, a concentration of fluorine may be approached asymptotically over any time period (Fig. 3). It is possible to approach asymptotically any fluorine partial pressure in this manner. The very low initial concentrations of fluorine in the system greatiy decreases the probabiUty of simultaneous fluorine coUisions on the same molecules or on adjacent reaction sites. [Pg.276]

The reactions of deuterium, tritium, and helium-3 [14762-55-17, He, having nuclear charge of 1, 1, and 2, respectively, are the easiest to initiate. These have the highest fusion reaction probabiUties and the lowest reactant energies. [Pg.150]

Helium, plentiful in the cosmos, is a product of the nuclear fusion reactions that are the prime source of stellar energy. The other members of the hehum-group gases are thought to have been created like other heavier elements by further nuclear condensation reactions occurring at the extreme temperatures and densities found deep within stars and in supernovas. [Pg.4]

Metallui ical. To prevent reaction with atmospheric oxygen and nitrogen, some metals must be shielded using an inert gas when heated or melted (94). AppHcations in metals processing account for most argon consumption and an important part of helium usage (see AfETALLURGY). [Pg.14]

Use of excess sodium drives the reaction, usually done under an argon or helium blanket, to completion. After cooling, the excess sodium is leached with alcohol and the sodium and potassium fluorides are extracted with water, leaving a mass of metal powder. The metal powder is leached with hydrochloric acid to remove iron contamination from the cmcible. [Pg.23]

Oil Contamination of Helium Gas. For more than 20 years, helium gas has been used in a variety of nuclear experiments to collect, carry, and concentrate fission-recoil fragments and other nuclear reaction products. Reaction products, often isotropically distributed, come to rest in helium at atmospheric concentration by coUisional energy exchange. The helium is then allowed to flow through a capillary and then through a pinhole into a much higher vacuum. The helium thus collects, carries, and concentrates products that are much heavier than itself, electrically charged or neutral, onto a detector... [Pg.367]

Hot atom reactions have also been used to label organic compounds with T. Irradiation of helium-3 with neutrons according to the nuclear reaction produces very energetic tritium atoms that can displace ordinary hydrogen in organic compounds. This procedure is not very selective, and the labeling pattern must be determined to enable the tritiated product to be used effectively as a tracer (34). [Pg.14]


See other pages where Helium reaction is mentioned: [Pg.12]    [Pg.231]    [Pg.183]    [Pg.369]    [Pg.12]    [Pg.12]    [Pg.231]    [Pg.183]    [Pg.369]    [Pg.12]    [Pg.1349]    [Pg.1832]    [Pg.2949]    [Pg.28]    [Pg.236]    [Pg.3]    [Pg.168]    [Pg.209]    [Pg.208]    [Pg.255]    [Pg.185]    [Pg.275]    [Pg.277]    [Pg.150]    [Pg.150]    [Pg.155]    [Pg.15]    [Pg.383]    [Pg.448]    [Pg.224]    [Pg.276]    [Pg.543]    [Pg.168]    [Pg.186]    [Pg.476]    [Pg.116]    [Pg.320]    [Pg.12]    [Pg.13]    [Pg.14]    [Pg.143]    [Pg.345]   
See also in sourсe #XX -- [ Pg.3 , Pg.349 ]




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