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Space hydrogen

Alkaline 25-lQQ Mature technology No precious metals Must use pure hydrogen Space... [Pg.527]

Figure 15. Position of state T2f relative to Fermi energy A2 = Ep = T2f as a function of tetrahedral hydrogen-hydrogen spacing in dihydride structures... Figure 15. Position of state T2f relative to Fermi energy A2 = Ep = T2f as a function of tetrahedral hydrogen-hydrogen spacing in dihydride structures...
The process can be operated at moderate pressures, 50 - 70 bar at reactor outlet. Temperatures have to be low (below 320 °C) to achieve deep hydrogenation. Space velocities are low (below 0,5 hr ) if low product aromatic contents of e.g. 5 vol% are required. The first step of the process is not different from a typical diesel hydrotreating unit. Five different catalyst types in staged loading can be used to obtain the required desulfurization and hydrogenation level. Catalysts are only available under license. At the spring NPRA meeting of 1995 it was announced that 13 companies have taken a license. This impressive success is for an important... [Pg.110]

IQNS is another local probe, but in the reciprocal space.117 In general, the incoherent cross-section of hydrogens dominates all the others, and the incoherent scattering function Sinc(2, ) carries information on the hydrogen space and time trajectory... [Pg.148]

The bottom of the reactor was equipped with a stainless steel sleeve. A small amount of fibrefrax was placed on top of the stainless steel sieve. The reactor was filled with 5 grams of catalyst, sealed of and checked for pressure leaks. Fischer-Tropsch synthesis was performed at a space velocity (H2+CO) of 185 cm min g (STP). Before the Fischer-Tropsch synthesis the catalyst was reduced in situ under a constant flow of hydrogen (space velocity = 185 cm min g STP) at 563 K. During the Fischer-Tropsch synthesis 10% argon (103 cm min STP) was passed through the reactor as internal standard. [Pg.50]

THERMAL INSULATION FOR LIQUID HYDROGEN SPACE TANKAGE. [Pg.172]

In Figure 7.15, a plot of the optimal reactor stmctures forming the BTX AR boundary in benzene, toluene, hydrogen space is given. Had Sam, Alex, and Donald constmcted the AR for the BTX system initially, they would have been able to determine the limits of hydrogen production as well as understood the optimal reactor stmctures needed to achieve these limits. [Pg.204]

There are also two symmetrical bending vibrations which are Ai vibrations for these two molecules. These are the symmetrical bendings of the CHa and CFa groups. This motion is one where the bonds are bent symmetrically rather than stretch as in the previous case. We can visualize this bending for CHa by drawing the hydrogens spaced equidistant from each other and from the carbon. The three can now bend toward and away from the axis formed by the carbon and the center of the plane of the three hydrogens. [Pg.3]

The helium gas originally in the vacuum space is removed once liquid nitrogen temperature has been achieved, while the helium gas in the liquid hydrogen space is replaced by liquid hydrogen. This permits the inner container and its contents to be cooled in process step 3-4 to 20.4 K, the temperature of liquid hydrogen. [Pg.128]

Pressurising by external use of a non-condensing gas. For example, helium is used for pressurising LOX and liquid hydrogen space rocket tanks. [Pg.114]

The carbon atom has a share in eight electrons (Ne structure) whilst each hydrogen atom has a share in two electrons (He structure). This is a gross simplification of covalent bonding, since the actual electrons are present in molecular orbitals which occupy the whole space around the five atoms of the molecule. [Pg.415]

Despite its success in reproducing the hydrogen atom spectmm, the Bolir model of the atom rapidly encountered difficulties. Advances in the resolution obtained in spectroscopic experiments had shown that the spectral features of the hydrogen atom are actually composed of several closely spaced lines these are not accounted for by quantum jumps between Bolir s allowed orbits. However, by modifying the Bolir model to... [Pg.3]

The major role of TOF-SARS and SARIS is as surface structure analysis teclmiques which are capable of probing the positions of all elements with an accuracy of <0.1 A. They are sensitive to short-range order, i.e. individual interatomic spacings that are <10 A. They provide a direct measure of the interatomic distances in the first and subsurface layers and a measure of surface periodicity in real space. One of its most important applications is the direct determination of hydrogen adsorption sites by recoiling spectrometry [12, 4T ]. Most other surface structure teclmiques do not detect hydrogen, with the possible exception of He atom scattering and vibrational spectroscopy. [Pg.1823]

Figure C3.2.5. Strongest tunnelling patliways between surface histidines and tire iron atom in cytochrome c. Steps in patliways are denoted by solid lines (covalent bonds), dashed lines (hydrogen bonds), and tlirough-space contacts (dotted lines). Electron transfer distance to His 72 is 5 A shorter tlian in His 66, yet tire two rates are approximately... Figure C3.2.5. Strongest tunnelling patliways between surface histidines and tire iron atom in cytochrome c. Steps in patliways are denoted by solid lines (covalent bonds), dashed lines (hydrogen bonds), and tlirough-space contacts (dotted lines). Electron transfer distance to His 72 is 5 A shorter tlian in His 66, yet tire two rates are approximately...
Methane, CH4, for example, has a central carbon atom bonded to four hydrogen atoms and the shape is a regular tetrahedron with a H—C—H bond angle of 109°28, exactly that calculated. Electrons in a lone pair , a pair of electrons not used in bonding, occupy a larger fraction of space adjacent to their parent atom since they are under the influence of one nucleus, unlike bonding pairs of electrons which are under the influence of two nuclei. Thus, whenever a lone pair is present some distortion of the essential shape occurs. [Pg.38]

Two ligands may be able to position a hydrogen-bond acceptor in different locations in space yet still vith the same hydrogen-bond donor. [Pg.674]

This discussion will be limited to functions of one variable that can be plotted in 2-space over the interval considered and that constitute the upper boundar y of a well-defined area. The functions selected for illustration are simple and well-behaved, they are smooth, single valued, and have no discontinuities. When discontinuities or singularities do occur (for example the cusp point of the Is hydrogen orbital at the nucleus), we shall integrate up to the singularity but not include it. [Pg.9]


See other pages where Space hydrogen is mentioned: [Pg.282]    [Pg.79]    [Pg.282]    [Pg.79]    [Pg.23]    [Pg.33]    [Pg.137]    [Pg.2222]    [Pg.465]    [Pg.568]    [Pg.54]    [Pg.60]    [Pg.163]    [Pg.170]    [Pg.41]    [Pg.268]    [Pg.23]    [Pg.101]    [Pg.219]    [Pg.390]    [Pg.521]    [Pg.665]    [Pg.674]    [Pg.702]    [Pg.53]    [Pg.149]    [Pg.174]    [Pg.175]    [Pg.66]    [Pg.34]   
See also in sourсe #XX -- [ Pg.392 , Pg.393 ]




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