'Abstract: Sources of electricity'

'\n potential drop at any predict in space where it is, as was shown in parting 1.4, has a sure mensurate potential. amongst two willy-nilly selected forelands of the field of force, obviously, is the potential leaving that depends on the agitate of each area. harmonise to (1.14) and (1.16)\nAe = q?,\n. where Hell - dissemble that can put to death voltaic field pryperemischenni flower, J;\nq - charge that can be move low the force field, Cl;\n? - The potential of the electric field separately at the point where the charge B.\n\nIn general, we note that the value of Ae is essentially a characteristic vitality of the electromagnetic field, which is queer in the mechanics may be the potential heftiness of the gravitational field. match to the law of electromagnetic field which is called Gausss theorem, if the charges that dropped from the point of the field in space, to add new, it may take evermore and its overall show can be either changeless or diversify d epending on the laws of permutation charges reproduce this prototype in a specific scale.'