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handbook of carbon, graphite, diamond and fullerenes

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16 Carbon, Graphite, Diamond, <strong>and</strong> Fullerenes<br />

case <strong>of</strong> the <strong>carbon</strong> atom, the valence electrons are the two 2p orbitals.<br />

Carbon in this state would then be divalent, since only these two electrons<br />

are available for bonding.<br />

Divalent <strong>carbon</strong> does indeed exist <strong>and</strong> is found in some highly reactive<br />

transient-organic intermediates such as the carbenes (for instance methylene).<br />

However, the <strong>carbon</strong> allotropes <strong>and</strong> the stable <strong>carbon</strong> compounds are<br />

not divalent but tetravalent, which means that four valence electrons are<br />

present. 16 ' Howthis increase in valence electrons occurs is reviewed in Sec.<br />

3.0.<br />

The <strong>carbon</strong> valence electrons are relatively easily removed from the<br />

<strong>carbon</strong> atom. This occurs when an electric potential is applied which<br />

accelerates the valence electron to a level <strong>of</strong> kinetic energy (<strong>and</strong> corresponding<br />

momentum) which is enough to <strong>of</strong>fset the binding energy <strong>of</strong> this<br />

electron to the atom. When this happens, the <strong>carbon</strong> atom becomes ionized<br />

forming a positive ion (cation). The measure <strong>of</strong> this binding energy is the<br />

ionization potential, the first ionization potential being the energy necessary<br />

to remove the first outer electron, the second ionization potential, the<br />

second outer second electron, etc. The ionization energy is the product <strong>of</strong><br />

the elementary charge (expressed in volts) <strong>and</strong> the ionization potential,<br />

expressed in electron volts, eV (one eV being the unit <strong>of</strong> energy accumulated<br />

by a particle with one unit <strong>of</strong> electrical charge while passing though a<br />

potential difference <strong>of</strong> one volt).<br />

The first ionization potentials <strong>of</strong> <strong>carbon</strong> <strong>and</strong> other atoms close to<br />

<strong>carbon</strong> in the Periodic Table are listed in Table 2.2. It should be noted that<br />

the ionization energy gradually (but not evenly) increases going from the<br />

first element <strong>of</strong> a given shell to the last. For instance, the value for lithium<br />

is 5.39 V <strong>and</strong> for neon, 21.56 V. It is difficult to ionize an atom with a<br />

complete shell such as neon, but easy to ionize one with a single-electron<br />

shell such as lithium.<br />

As shown in Table 2.2 above, <strong>carbon</strong> is located half-way between the<br />

two noble gases, helium <strong>and</strong> neon. When forming a compound, <strong>carbon</strong> can<br />

either lose electrons <strong>and</strong> move toward the helium configuration (which it<br />

does when reacting with oxygen to form CO2), or it can gain electrons <strong>and</strong><br />

move toward the neon configuration (which it does when combining with<br />

other <strong>carbon</strong> atoms to form <strong>diamond</strong>).<br />

The six ionization potentials <strong>of</strong> the <strong>carbon</strong> atom are shown in Table 2.3.

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