Where Rh is the Hall’s constant (Hall’s coefficient)
Z is an assumed number of electrons released by one
atom to the conductivity zone.
Z kernel is the number of external electrons of the
atomic kernel on the last shell.
The lattice type is the type of the metal crystal
structure at room temperature and, in some cases, at phase transition
temperatures (1).
Conclusions
In spite of the rough reasoning the table shows that
the greater number of electrons gives the atom of the element to the
conductivity zone, the more positive is the Hall’s constant. On the contrary
the Hall’s constant is negative for the elements which have released one or two
electrons to the conductivity zone, which doesn’t contradict to the conclusions
of Payerls. A relationship is also seen between the conductivity electrons (Z)
and valency electrons (Z kernel) stipulating the crystal structure.
The phase transition of the element from one lattice
to another can be explained by the transfer of one of the external electrons of
the atomic kernel to the metal conductivity zone or its return from the
conductivity zone to the external shell of the kernel under the influence of external
factors (pressure, temperature).
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