Lorentz force of electromagnetism is a force of the future. The light at the end of the tunnel.
Lorentz force of electromagnetism is a force of the future. The light at the end of the tunnel.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
Do you mean that all electromagnetism will eventually becom Lorenz force?
If so, what is Lorenz force made of?
Lorentz force is the same force as electromagnetic force. It is the sum of electric force and magnetic force.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
I've been doing many mathematical workings which have taken me to an important discoverment towards EM being unified with Gravity throughout the electromagnetic equations and spetial relativity.Originally Posted by AntonioLao
Aren't you forgetting the nonlinear field equations of general relativity?
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
No. But GR's math leads to complications with QM. Whiles if I do a re-unification of Maxwell and young Einstein, I could avoid older Einstein's problem with Bohr, Heisenberg and all the other quantum guys, and therefore be nearrer to a TOE.Originally Posted by AntonioLao
I've decided to adopt this method because it's easier to re-formulate one of the halfs than putting them to gether form how they are, specially if I don't want to go into illusionary theories: strings, aether...
Are you then using the more general Poincare group instead of the usual Lorentz group? http://en.wikipedia.org/wiki/Poincare_group
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
Still haven't gone on to that. But up to what I see, neither of them satisfy my math, so I wil have to develop a "Garridonian Group" which is good enough.Originally Posted by AntonioLao
Can you show me your tentative algebra? Associativity, commutativity, distributativity, identity, inversibility, etc?Originally Posted by GUILLE
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
I will write a paper. But I have no time neough to think much about it, for now.Originally Posted by AntonioLao
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