Electrostatic force between two charges¶
Also known as Coulomb’s law, it is an experimental law that calculates the amount of force between two electrically charged particles at rest.
Also see the scalar law.
Notes:
If a given charge is in the vicinity of a system of point charges, then the net law can be found via the principle of superposition.
Notation:
\(\varepsilon_0\) (
epsilon_0) isvacuum_permittivity.
Conditions:
The charges are small.
The charges are at rest.
Links:
- force¶
Vector of the electrostatic
forceexperienced by thefirst_chargein the vicinity of thesecond_chargein vacuum.
- Symbol:
F_12- Latex:
\({\vec F}_{12}\)
- Dimension:
force
- Symbol:
q_1- Latex:
\(q_{1}\)
- Dimension:
charge
- Symbol:
q_2- Latex:
\(q_{2}\)
- Dimension:
charge
- position_vector¶
Position vector drawn from the
second_chargeto thefirst_charge.
- Symbol:
d_21- Latex:
\({\vec d}_{21}\)
- Dimension:
length
- force_law¶
F_12 = q_1 * q_2 / (4 * pi * epsilon_0) * d_21 / norm(d_21)^3- Latex:
- \[{\vec F}_{12} = \frac{q_{1} q_{2}}{4 \pi \varepsilon_0} \frac{{\vec d}_{21}}{\left \Vert {\vec d}_{21} \right \Vert^{3}}\]
- position_vector_law¶
d_21 = sign(q_1 * q_2) * sqrt(Abs(q_1 * q_2) / (4 * pi * epsilon_0)) * F_12 / norm(F_12)^(3/2)- Latex:
- \[{\vec d}_{21} = \operatorname{sign}{\left(q_{1} q_{2} \right)} \sqrt{\frac{\left|{q_{1} q_{2}}\right|}{4 \pi \varepsilon_0}} \frac{{\vec F}_{12}}{\left \Vert {\vec F}_{12} \right \Vert^{\frac{3}{2}}}\]