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CO2 molecule

The first step consists of the molecular adsorption of CO. The second step is the dissociation of O2 to yield two adsorbed oxygen atoms. The third step is the reaction of an adsorbed CO molecule with an adsorbed oxygen atom to fonn a CO2 molecule that, at room temperature and higher, desorbs upon fomiation. To simplify matters, this desorption step is not included. This sequence of steps depicts a Langmuir-Hinshelwood mechanism, whereby reaction occurs between two adsorbed species (as opposed to an Eley-Rideal mechanism, whereby reaction occurs between one adsorbed species and one gas phase species). The role of surface science studies in fomuilating the CO oxidation mechanism was prominent. [Pg.953]

Once prepared in S q witli well defined energy E, donor molecules will begin to collide witli batli molecules B at a rate detennined by tire batli-gas pressure. A typical process of tliis type is tire collision between a CgFg molecule witli approximately 5 eV (40 000 cm or 460 kJ mor ) of internal vibrational energy and a CO2 molecule in its ground vibrationless state 00 0 to produce CO2 in tire first asymmetric stretch vibrational level 00 1 [11,12 and 13]. This collision results in tire loss of approximately AE= 2349 cnA of internal energy from tire CgFg,... [Pg.2999]

In Figure 6.35 the region labelled B is a deep pocket, the bottom of which represents the CO2 molecule at equilibrium with rj = r2 = r. Regions Ai and A2 are valleys which are... [Pg.184]

The value of n in the polymeric adsorbed species (CO) is larger on the 3c sites than on die 4c and 5c sites. The CO2 molecule is much more suongly adsorbed, indicating ion formation on the oxide surface, and the evidence suggests... [Pg.125]

Under the conditions of temperature and ionic strength prevailing in mammalian body fluids, the equilibrium for this reaction lies far to the left, such that about 500 CO2 molecules are present in solution for every molecule of H2CO3. Because dissolved CO2 and H2CO3 are in equilibrium, the proper expression for H2CO3 availability is [C02(d)] + [H2CO3], the so-called total carbonic acid pool, consisting primarily of C02(d). The overall equilibrium for the bicarbonate buffer system then is... [Pg.53]

Calculations. The atoms of incorporated lsO is calculated from mass spectral data. When the ratio of the peak heights at mass-to-charge ratio (m/e) 44, 46 and 48 for CO2 is X-.Y-.Z, assuming that the height of each peak is strictly proportional to the number of CO2 molecules, the atom fraction of l80 in CO2, C, is given by ... [Pg.374]

Thermal desorption spectra of CO2 from a titania surface are shown in figure 2. It revealed two desorption peaks at temperature ca. 175 and 200 K. As reported, surface of titania have two structures which is similar to the results fomd by Tracy et al. [7]. Based on their study, it was confirmed that one peak at ca. 170 K was attributed to CO2 molecules bound to regular five-coordinate Ti site considered as the perfected titania structure. The second peak at ca. 200 K considered as the CO2 molecules bound to Ti referred to the... [Pg.718]

The most probable speeds of methane and carbon dioxide are slower than the most probable speed of hydrogen, but CH4 and CO2 molecules have larger masses than H2. When kinetic energy calculations are repeated for these gases, they show that the most probable kinetic energy is the same for all three gases. [Pg.296]

C05-0130. In 1990, carbon dioxide levels at the South Pole reached 351.5 parts per million by volume. (The 1958 reading was 314.6 ppm by volume.) Convert this reading to a partial pressure in atmospheres. At this level, how many CO2 molecules are there in 1.0 L of dry air at -45 °C ... [Pg.346]

To estimate the amount of energy absorbed or released in this reaction, we must compile an inventoiy of all the bonds that break and all the bonds that form. A ball-and-stick model shows that propane contains 8 C—H bonds and 2 C—C bonds. These bonds break in each propane molecule, and one ODO bond breaks in each oxygen molecule. Two CDO bonds form in each CO2 molecule, and two O—H bonds form in each H2 O molecule. In summary ... [Pg.384]

Thus, the RCOO radicals produced initially are unstable, and before (or while) undergoing dimerization, split up into simpler radicals and CO2 molecules. [Pg.290]

Formates and carbon monoxide are products of a shallow reduction of carbon dioxide (two electrons per one CO2 molecule). In the last few years, much attention has been paid the problem of obtaining products of deeper reduction (e.g., methanol or methane) which may be used as fuels in engines or in fuel cells. [Pg.293]

TABLE 13.1 Number of Electrons per Resulting CO2 Molecule Required for Oxidizing the Stable Adsorbed Decomposition Product from Adsorption of Ci Molecules to CO2, and Ci Adsorbate Coverage Relative to that of a Saturated CO Adlayer after Adsorption of Ci Reactants"... [Pg.419]

The mass spectrometric currents follow largely, but not completely the faradaic current signals. The contributions to the respective faradaic currents resulting from complete oxidation to CO2, which are calculated using the calibration constant K (see Section 13.2), are plotted as dashed lines in the top panels in Fig. 13.3. For the calculations of the partial reaction currents, we assumed six electrons per CO2 molecule formation and considered the shift in the potential scale caused by the time... [Pg.427]

The calibrated m/z = 44 and m/z = 60 ion currents were converted into the respective partial reaction faradaic currents as described above, and are plotted in Fig. 13.3c as dashed (m/z = 44) and dash-dotted (m/z = 60) lines, using electron numbers of 6 electrons per CO2 molecule and 4 electrons per formic acid molecule formation. The calculated partial current for complete methanol oxidation to CO2 contributes only about one-half of the measured faradaic current. The partial current of methanol oxidation to formic acid is in the range of a few percent of the total methanol oxidation current. The remaining difference, after subtracting the PtO formation/reduction currents and pseudocapacitive contributions as described above, is plotted in Fig. 13.3c (top panel) as a dotted line. As mentioned above (see the beginning of Section 13.3.2), we attribute this current difference to the partial current of methanol oxidation to formaldehyde. This way, we were able to extract the partial currents of all three major products during methanol oxidation reaction, which are otherwise not accessible. [Pg.433]

The current efficiencies for the different reaction products CO2, formaldehyde, and formic acid obtained upon potential-step methanol oxidation are plotted in Fig. 13.7d. The CO2 current efficiency (solid line) is characterized by an initial spike of up to about 70% directly after the potential step, followed by a rapid decay to about 54%, where it remains for the rest of the measurement. The initial spike appearing in the calculated current efficiency for CO2 formation can be at least partly explained by a similar artifact as discussed for formaldehyde oxidation before, caused by the fact that oxidation of the pre-formed COacurrent efficiency. The current efficiency for formic acid oxidation steps to a value of about 10% at the initial period of the measurement, and then decreases gradually to about 5% at the end of the measurement. Finally, the current efficiency for formaldehyde formation, which was not measured directly, but calculated from the difference between total faradaic current and partial reaction currents for CO2 and formic acid formation, shows an apparently slower increase during the initial phase and then remains about constant (final value about 40%). The imitial increase is at least partly caused by the same artifact as discussed above for CO2 formation, only in the opposite sense. [Pg.441]

The release of energy to the dye molecule or fluorescer is driven by the conformational instability of the C2O4 intermediate (the flat highly strained C2O4 prefers to be two linear CO2 molecules). The sensitized fluorescer, denoted fluorescer, returns to the ground state via the emission of light ... [Pg.141]

A detailed study of the C02- species on MgO has been carried out by Lunsford and Jayne 26). Electrons trapped at surface defects during UV irradiation of the sample are transferred to the CO2 molecule upon adsorption. By using 13C02 the hyperfine structure was obtained. The coupling constants are axx - 184, am = 184, and a = 230 G. An analysis of the data, similar to that carried out in Section II.B.2 for N02, indicates that the unpaired electron has 18% 2s character and 47% 2p character on the carbon atom. An OCO bond angle of 125° may be compared with an angle of 128° for CO2- in sodium formate. [Pg.315]

Any periodic distortion that causes polarization of a molecule can also cause interaction with the electric field component of radiation. An example is the asymmetric stretching vibration of the CO2 molecule, that creates a fluctuating dipole moment as shown below. [Pg.281]

Finally, we note a very clever isotope experiment done by Tatsuo Matsushima (2 4). The results are summarized in Figure 14 and show that when 1JC0 is preadsorbed on Pt and then a mixture of - - C0 and O2 is introduced into the gas phase, the product CO2 molecules initially formed all are labelled with - C. In fact the experiment is not quite so simple. An initial 002/ C02 ratio is measured (unity in... [Pg.53]

The linear metal-C02 coordination mode has been implicated in biological processes such as photos5mthesis and previously had been suggested for the crystal structure of the iron-containing enz5une a-ketoglutarate reductase (52). Therefore it appears likely that end-on 0-coordination is critical for binding, activation, and, most importantly, C-functionalization of the bound CO2 molecule. [Pg.24]


See other pages where CO2 molecule is mentioned: [Pg.1960]    [Pg.2997]    [Pg.3000]    [Pg.273]    [Pg.370]    [Pg.145]    [Pg.59]    [Pg.296]    [Pg.712]    [Pg.9]    [Pg.294]    [Pg.587]    [Pg.193]    [Pg.419]    [Pg.433]    [Pg.146]    [Pg.146]    [Pg.127]    [Pg.125]    [Pg.264]    [Pg.20]    [Pg.430]    [Pg.512]    [Pg.183]    [Pg.563]    [Pg.22]    [Pg.48]    [Pg.229]    [Pg.115]    [Pg.118]   
See also in sourсe #XX -- [ Pg.16 ]




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Enzymatic Conversion of CO2 (Carboxylation Reactions and Reduction to Energy-Rich Cl Molecules)

The CO2 Molecule

Transition of Highly Vibrationally Excited CO2 Molecules into the Vibrational Quasi Continuum

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