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Carbon dioxide linear shape

This determination of the molecular geometry of carbon dioxide and water also accounts for the fact that carbon dioxide does not possess a dipole and water has one, even though both are composed of polar covalent bonds. Carbon dioxide, because of its linear shape, has partial negative charges at both ends and a partial charge in the middle. To possess a dipole, one end of the molecule must have a positive charge and the other a negative end. Water, because of its bent shape, satisfies this requirement. Carbon dioxide does not. [Pg.154]

About 20% of the CO in the blood is carried in combination with hemoglobin as carbaminohemoglobrn, The balance of the combined carbon dioxide is carried as bicarbonate. A CO dissociation curve for blood can be prepared just as for oxygen, but the shape is not the same as for the latter. As the partial pressure of CO in the air increases, the amount in the blood increases the increase is practically linear in the higher ranges. Oxygen exerts a negative effect on the amount of CO which can be taken up by the blood. [Pg.291]

Consider a molecule of water and a molecule of carbon dioxide. Both water and carbon dioxide contain two atoms of the same element bonded to a third atom of another element. According to Figure 3.26, however, water and carbon dioxide molecules are different shapes. Why does carbon dioxide have a linear shape while water is bent ... [Pg.87]

In these two cases the dipole arrows cancel each other out because of the shape of the molecules. The linear shape of the molecule of carbon dioxide puts the dipole arrows in opposite directions to counterbalance each other. The same holds true for the tetrahedral molecular geometry found in carbon tetrachloride. Despite having polar bonds, these two molecules are nonpolar. There is no overall dipole moment in these molecules because the dipole arrows are of the same magnitude but lie in opposite directions in the molecule. This counterbalance causes the molecule to be nonpolar. [Pg.92]

According to the data of analysis of many adsorption systems, the first term in Equation 9 corresponding to the second order appears only v hen considering adsorption of relatively small molecules. They include molecules of linear shape, such as the diatomic gases, carbon dioxide, carbon monoxide, etc. Experimentally realizable orders, n, are integers from 3 to 6 in the general case. With larger polyatomic molecules, no adsorption space remains in the zeolite voids for final adsorption under the effect of dispersion forces. Then Equation 9 retains only the second term, and Uon is expressed by Equation 12. [Pg.75]

The shape of a molecule made of only two atoms, such as H2 or CO, is easy to determine. As shown in Figure 15, only a linear shape is possible when there are two atoms. Determining the shapes of molecules made of more than two atoms is more complicated. Compare carbon dioxide, CO2, and sulfur dioxide, SO2. Both molecules are made of three atoms. Although the molecules have similar formulas, their shapes are different. Notice that CO2 is linear, while SO2 is bent. [Pg.227]

B. H20]—Carbon dioxide and diatomic nitrogen have a linear shape. Methane has a tetrahedral shape. Water is the classic example of a bent shape. [Pg.148]

In pore characterization of carbonaceous materials, nitrogen and carbon dioxide have been commonly used. Nitrogen is used because it is readily available, while carbon dioxide is used as a probing molecxfle for smaller pores because of its small linear dimension and it can be used at temperatures close to the ambient temperature. Because of their shape, we should consider each molecule as a particle composing of many interaction sites. Each site on one molecule wiU interact with all sites of another molecule. We write below the interaction energy between a site a on a molecule i with a site i on a molecule j with a LJ 12-6 equation. [Pg.242]

When we are to determine how many electron groups that surround an atom, the Lewis structure can be of great help (see the previous section 2.23 Lewis structure). From the Lewis structure of a given molecule you can simply count how many bonds and lone pairs that surround an atom. That way you have the number of electron groups. The VSEPR theoiy tells us that these electron groups will be placed as far apart as possible. In the following example we will use the VSEPR theory to predict the molecular geometries of a water molecule and a carbon dioxide molecule. That way we will discover why a carbon dioxide molecule is linear and why a water molecule is V-shaped. [Pg.67]

The VSEPR theory has thus served as a tool that enabled us to explain why a carbon dioxide molecule is linear and why a water molecule is V-shaped. The VSEPR theory is a simple and usable tool to predict geometries of molecules when the Eewis structure is already available giving us the number of electron groups. [Pg.69]

If the notion that the migration of carbon dioxide from the reaction interface may be the rate-determining process appears unlikely, reference should be made to [15.4]. That suggests that the fundamental rate controlling step is the solid-state diffusion of CO2 through CaO in the region of the reaction interface . It contrasts the complex shape of the weight loss curve at atmospheric pressure with the linear relationship under vacuum. [Pg.143]

Carbon dioxide adsorption on li-X, Na-X and K-X was investigated via IR already in 1963 by Bertsch and Habgood [202]. N2O and CO2 are also isoelectronic compounds. Moreover, the molecules of both compounds are linear, have a similar shape and identical mass the dipole moment of N2O is small (0.167 debye), that of CO2 is zero the three fundamentals of their internal vibrations fall in the same range of wavenumbers [636-638] (cf. also [640]). However, due to the lower symmetry, nitrous oxide molecules possess more possibilities of orientation [596]. [Pg.119]

Azide is isoelectronic with carbon dioxide, and has the same linear shape. [Pg.354]

In Table 20.1 we compare the valence angles of some representative triatomic molecules or ions formed from elements in Groups 14 to 18. It is seen that the shapes of the molecules are determined by the numbCT of valence electrons carbon dioxide and aU other 16 valence electron species are linear, and species with 17 to 20 valence electrons are angular. When the number of valence electrons is increased to 22, the shape reverts to linearity. The author is not aware of any exception to this trend. [Pg.304]

This principle can be illustrated with the structure of a molecule of carbon dioxide (CO2). The central carbon atom of carbon dioxide is bonded to each oxygen atom by a double bond. Carbon dioxide is known to have a linear shape the bond angle is 180°. [Pg.46]

Water is known to have the geometric shape known as bent or V-shaped. Carbon dioxide exhibits a linear shape. BF3 forms a third molecular shape called trigonal planar since all the atoms lie in one plane in a triangular arrangement. One of the more common molecular shapes is the tetrahedron, illustrated by the molecule methane (CH4). [Pg.237]

Shapes of (a) carbon dioxide (CO2) and (b) acetylene (C2H2). In each case, the two regions of electron density are farthest apart if they form a straight line through the central atom and create an angle of 180°. Both carbon dioxide and acetylene are referred to as linear molecules. [Pg.16]

A water molecule (Figure 11.72) has modes of vibration similar to those shown for the carbon dioxide molecule. However, it is a V-shaped molecule rather than a linear molecule. All the vibration modes shown for the water molecule are infrared active. In a bent molecule the changes in bond dipole for symmetric stretching are not in opposite directions. They do not, therefore, cancel out vectorially and, since there is a change in the overall dipole moment of the molecule, infrared absorption occurs. [Pg.420]

A molecule can have only one center of symmetry, which may or may not coincide with an atom. For a molecule to have a center of symmetry, all atoms, with the exception of the one which may coincide with the center, must exist in paired sets. In carbon dioxide, the C atom is the center of symmetry. Of the typical molecular shapes mentioned in Tables 19.4 and 19.5, only the linear, square-planar, and the octahedral forms, as exemplified by BeCl2, XeF4, and SFe, respectively, have centers of symmetry. [Pg.399]


See other pages where Carbon dioxide linear shape is mentioned: [Pg.221]    [Pg.148]    [Pg.250]    [Pg.162]    [Pg.68]    [Pg.211]    [Pg.248]    [Pg.88]    [Pg.88]    [Pg.25]    [Pg.120]    [Pg.189]    [Pg.64]    [Pg.234]    [Pg.331]    [Pg.332]    [Pg.5]    [Pg.158]    [Pg.161]    [Pg.168]    [Pg.68]    [Pg.69]    [Pg.316]    [Pg.204]    [Pg.109]    [Pg.281]    [Pg.374]    [Pg.211]    [Pg.111]    [Pg.316]    [Pg.52]    [Pg.396]   
See also in sourсe #XX -- [ Pg.308 ]

See also in sourсe #XX -- [ Pg.308 ]

See also in sourсe #XX -- [ Pg.313 ]




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