vault backup: 2026-11-07 12:19:53
This commit is contained in:
1 parent
b5b1948553
commit
cd4ca2217e
2 files changed
+5
-2
No files matched your search
@@ -5,8 +5,10 @@ A capacitor stores electrical charge. As the charge accumulates on one side of t
|
||||
- The impedance of a capacitor is $Z = \frac{1}{j \omega C}$
|
||||
- A capacitor resists change in voltage
|
||||
- Voltage cannot change instantly across a capacitor, but current can.
|
||||
- Voltage across a discharging capacitor is $v(t) = v_0 e^{-\frac{t}{R C}}$
|
||||
- Voltage across a charging capacitor: $V_0(1 - e^(-\frac{t}{R C}))$
|
||||
- Voltage across a discharging capacitor is $v(t) = V_0 e^{-\frac{t}{R C}}$
|
||||
- $v_0$ is initial voltage when discharging begins
|
||||
- $R$ is the total resistance faced by the capacitor
|
||||
- $C$ is the capacitance of the circuit
|
||||
- Capacitors in parallel add, and capacitors in series inverse-add $
|
||||
- Capacitors in parallel add, and capacitors in series inverse-add $1/c = 1/c_1 + 1/c_2$
|
||||
- $\tau = R C$
|
||||
Reference in new issue
Block a user