| magneticity
Dirac postulated the existence of magnetic monopoles in 1931. In spite of continued experimental researches, no monopole has been found. It is now believed that these failures are consequences of a lack of understanding of the underlying magnetic as well as electric topology. However, both can be described using the topology of two distinct magnetic helicities. They are used to describe the stability of stellar systems from their births to their death of billions of years. This stability implies that charged particles such as electrons and protons should contain both helicities within their sub-quantum structures.
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Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
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