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About LinkBacksAlthough magnetostatic potential exists, no useful energy could be derived from it. However, when variability is induced the result is an electromotive force (emf). This was discovered by Faraday in 1831 and also by Lenz in 1834. Now, these discoveries are widely known as Faraday’s laws of electromagnetic induction and Lenz’s law. Lenz’s principle says that the direction of the induced emf always opposes the magnetic force field that produces it. Although nature abhors the vacuum the emf reacts to its inductivity for useful energy expenditures. Equivalently, Lenz’s principle is also one of energy conservation.
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Thread: inductivity
- 07-22-2006, 04:06 PM #1Raider of the lost time
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inductivity
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
- 07-24-2006, 07:38 AM #2The Thinker
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Re: inductivity
Can the process be inversed, so that the electromotive force creates magnetic fields? And if it is possible, could that process be applied for any practical use of energy?
- 07-30-2006, 04:43 PM #3Raider of the lost time
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Re: inductivity
I think the inverse process is electromagnetism described by Maxwell's equations.
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
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