And we are back to a singular charge when we add three \(\psi\)s separated by equal distance. The problem is \(\psi\) also disappeared.
The total mass density of the system, \(m_{\rho\,s}\) is,
\(m_{ \rho \, s }=3m_{ \rho }\)
How does such composite \(\psi\)s oscillates? What is surprising is that the expressions for \(F_{\rho}\) and \(\psi\) lend themselves to such additions.
\(_n\psi=\psi_1+\psi_2+...\psi_n\)
\(_n\psi \equiv \psi\)
Algebra of charges comes naturally as the algebraic manipulation of the functions for \(F_{\rho}\) and \(\psi\). If the group of three oscillates together at \(a_\psi\),
they behave just like three times a singular negative charge.
