forked from eggy/eifueo
ece106: add voltage intro
This commit is contained in:
parent
12bf988532
commit
6b9197ae25
@ -310,3 +310,22 @@ Generally:
|
|||||||
|
|
||||||
1. Determine $\vec E$ outside the slab.
|
1. Determine $\vec E$ outside the slab.
|
||||||
2. Set one outside surface and one inside surface as a pillbox and apply rules.
|
2. Set one outside surface and one inside surface as a pillbox and apply rules.
|
||||||
|
|
||||||
|
## Electrostatic potential
|
||||||
|
|
||||||
|
At a point $P$, the electrostatic potential $V_p$ or voltage is the work done per unit positive test charge from infinity to bring it to point $P$ by an external agent.
|
||||||
|
|
||||||
|
$$
|
||||||
|
V_p=\lim_{q\to 0^+}\frac{W_i}{q} \\
|
||||||
|
W_I=\int^p_\infty\vec F_I\bullet \vec{dl}
|
||||||
|
$$
|
||||||
|
|
||||||
|
Because the desired force acts opposite to the force from the electric field, as long as $\vec E$ is known at each point:
|
||||||
|
|
||||||
|
$$V_p=-\int^p_\infty\vec E\bullet\vec{dl}$$
|
||||||
|
|
||||||
|
The work done only depends on initial and final positions — it is conservative, thus implying Kirchoff's voltage law.
|
||||||
|
|
||||||
|
Where $\vec dl$ is the path of the test charge and $\vec dr$ is the direct path from infinity through the point to the charge, because $dr=|dl|\cos\theta$:
|
||||||
|
|
||||||
|
$$\vec E\bullet\vec{dl}=Edr$$
|
||||||
|
Loading…
Reference in New Issue
Block a user