prawo _ Coulomba |
£ |
* •—i ii u |
V = — [potencjał] |
4x? r' ■ f = 3,35*10'* — = k = 2.99 * 10' [N* m / C) 4>nr |
$ 1F = LT/1C ę = Ctf[lF = lC/P] |
fe-wrfensafory |
równolegle :
nat _ pola
r F 1 $ |
C.-ŻC |
$ 4/3!" r1 | |
szeregowo : | |
M = py-P = pE sin 0 |
1 ^ 1 |
P = <?£ |
—=z— C _ C |
«*» * ♦» i ii | |
-• * |
natężenie _ prądu |
Gauss |
da 1= —[M = lC/s] dt |
* = d> £*rf,? = ^ | |
■ ■ |
U |
R=-[\Ci = \VSA] | |
I | |
(X |
J |
£ = — [przewodni] [1F / m] |
P= I*U[\V*A = \- |
f • |
5 |
a | |
£ = —[p/as2cąj>2«a] |
2f
■