Does the force equation for \(V\), energy of the orbiting electron applied to all of them?
\(\cfrac { m_{ T }c^{ 2 } }{ r_{ { T } } } =\cfrac { G_{ { B }o }T^{+} }{ 4\pi } \cfrac { g^{ + }.v_{ { g } }\times \hat { r_{ g } } }{ r_{ g }^{ 2 } } -\cfrac { T^{ - } T^{+}}{ 4\pi \tau _{ o }r^{ 2 } }\) --- (*)
As energy level of the electron changes, the orbit transit from a lower energy type to a higher energy type, first a paired orbit un-pairs in two single orbits and with further increase in energy, the electron from a single unpaired orbit of the highest energy ionize.
It is postulated here that, when the orbits change to the next higher energy type, there is a phase change requiring high input of energy.
This is the order of increasing temperature. As \(T^{+}\) is stronger with the removal of \(T^{-}\) particles, the electron is pulled into the proton orbits. With even higher temperature the paired orbits unpair, and eventually the electron is in the hold of the weak field in an unpaired orbit. Thereafter, the electron ionize.
The last but one orbit type in the diagram above may not occur as the electrons are already inside the paired orbits when they are unpaired.
This order may not be the order of increasing energy. Equation (*) used to derive the dependence of \(V\) on \(T^{-}\) has the \(T^{-}\) particle working against the weak field. This is not the case for all orbit types. The protons are involved in all but last of the orbital types.
Akan datang...
Good night.
