Voltage is line integral of electric field¶
In electrostatics, voltage change between two points can be found as the line integral of the electric field along any path connecting the two points.
Conditions:
- Applies to electrostatic fields, although electrostatic approximation might be used for electromagnetic fields at lower frequencies. 
Links:
- Symbol:
- V
- Latex:
- \(V\) 
- Dimension:
- voltage
- distance¶
- euclidean_distancetraveled.
- Symbol:
- s
- Latex:
- \(s\) 
- Dimension:
- length
- electric_field_component¶
- Component of the electric field vector tangent to the integration path. See - electric_field_strength.
- Symbol:
- E_s(s)
- Latex:
- \(E_{s}{\left(s \right)}\) 
- Dimension:
- voltage/length
- Symbol:
- s_0
- Latex:
- \(s_{0}\) 
- Dimension:
- length
- Symbol:
- s_1
- Latex:
- \(s_{1}\) 
- Dimension:
- length
- law¶
- V = -Integral(E_s(s), (s, s_0, s_1))- Latex:
- \[V = - \int\limits_{s_{0}}^{s_{1}} E_{s}{\left(s \right)}\, ds\]