For All Force Fields
|
Units |
||
Force |
F=eq |
N |
|
Electric Field Strength |
e=F/q |
N/C |
|
Work (electric potential energy) |
W=EE=qDV |
J |
|
Electric Potential |
V |
||
Uniform Electric Fields see note |
Point Charge Electric Fields |
||
Force |
see above for all force fields |
F=kq1q2/r**2 |
N |
Electric Field Strength |
e=V/d |
e=kq/r**2 |
N/C |
Work (electric potential energy) |
W=DEE
=eqd
|
EE=kq1q2/r |
J |
Electric Potential |
V=ed |
V=kq/r |
V |
| note: Although these equations are stated to be true for uniform fields they can be true for any field if the limit of the variables is infinitely small. For example E=V/d could be expressed in any field as e=DV/Dd where D - "delta" means change in. In this example we would say that the electric field strength is the gradient of the potential. |
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