A Pauling bond-energy excess subtracts a chosen like-atom baseline from the unlike-atom bond-dissociation energy. For an unequal-input arithmetic example, stipulate , and , all with one dissociation convention. The arithmetic mean baseline and excess are
The arithmetic-baseline Pauling scale model therefore gives . The bond-dissociation energy is not itself the excess: subtracting the baseline is essential. All three numbers are stipulated, not experimental values for named chemical elements.
Changing the baseline changes the model. For the same stipulated inputs, a geometric mean baseline would be , yielding an excess of and a difference of approximately . It is a different construction, even though both start from the same bond-dissociation energies. State which baseline is used before comparing electronegativity differences.
The arithmetic-baseline Pauling scale also has a useful inverse: a difference of corresponds to an excess of , and a difference of corresponds to . Doubling the electronegativity difference quadruples the modeled excess. Interchanging the endpoint labels changes neither quantity; the square root alone cannot choose the direction of bond polarization.
In The Nature of the Chemical Bond. IV. The Energy of Single Bonds and the Relative Electronegativity of Atoms (printed pp. 3576–3578, Table II and equation (1)), Linus Pauling organized excess energies for chemical bonds into an approximately additive map of their square roots. He also identified a limitation: his H–F map separation of predicted an excess of , exceeding his table's value by . Those are historical values and a historical model discrepancy, not modern recommended inputs.[ref]

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