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A Classical Model of Dipole Polarizability

At equilibrium these two forces must be equal and so the displacement d satisfies [Pg.285]

The induced dipole moment is Qd and the polarizability (here a scalar) is Qd/E so that [Pg.285]

Apart from the factor of 4rreo, the polarizability of an atom is determined in this model by the volume. If we had been working in cgs (old-fashioned electromagnetic quantities) rather than SI (modem ones), we would have found a = a and for this reason people speak of the polarizability volume. [Pg.286]

The SI units of polarizability are Fm. Alternatively, since Fm = N we can quote polarizabilities as C N m or C m J , which is the normal form. In the atomic system, it is usual to quote polarizabilities in multiples of e a E.  [Pg.286]

The polarizability of the inert gas atoms does indeed increase with their size, as can be seen from Table 17.1. [Pg.286]


See other pages where A Classical Model of Dipole Polarizability is mentioned: [Pg.285]    [Pg.285]    [Pg.327]   


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