Nothing Special   »   [go: up one dir, main page]

Charging Discharging A Capacitor

Download as pdf or txt
Download as pdf or txt
You are on page 1of 2

Charging a Capacitor

𝐸 = 𝑉𝐶 + 𝑉𝑅
r 𝑞
= + 𝐼𝑅
𝐶
𝑞 𝑑𝑞
= + 𝑅
𝐶 𝑑𝑡
𝑑𝑞 𝑞
𝑜𝑟 𝑅 + =𝐸
𝑑𝑡 𝐶
𝑑𝑞 𝑑𝑡
𝑜𝑟 =
𝐸𝐶−𝑞 𝑅𝐶
Integrating both sides
𝑞 𝑑𝑞 1 𝑡
‫׬‬0 = ‫𝑡𝑑 ׬‬
𝐸𝐶−𝑞 𝑅𝐶 0
𝑡
𝑜𝑟 𝑞 = 𝐸𝐶 1 − 𝑒 −𝑅𝐶
𝑡

= 𝑞0 1 − 𝑒 𝑅𝐶

Where q0 = EC = maximum charge stored in the capacitor.


Differentiating
𝑡
𝑑𝑞
𝑖 = = 𝑖0𝑒 −𝑅𝐶
𝑑𝑡
The potential across the capacitor
𝑡
𝑞
𝑉𝐶 = = 𝐸 1 − 𝑒 −𝑅𝐶
𝐶
The potential across the resistor
𝑡
𝑉𝑅 = 𝑖𝑅 = 𝐸𝑒 −𝑅𝐶
𝐼 = 𝑒 −1 𝐼0 = 0.37𝑖0
and 𝑞 = 𝑞0 1 − 𝑒 −1 = 0.63𝑞0
RC has the dimension of time, is called time constant in
which the charge increases to 0.638 times the
1
equilibrium charge, and the current decreases to
𝑒
times the equilibrium current.
Discharging a Capacitor
r

0 = 𝑉𝑅 + 𝑉𝐶
𝑞
= 𝐼𝑅 +
𝐶
𝑑𝑞 𝑞
𝑜𝑟 𝑅 + =0
𝑑𝑡 𝐶
𝑞 𝑑𝑞 1 𝑡
𝑜𝑟 ‫𝑞 𝑞׬‬ =− ‫𝑡𝑑 ׬‬
0 𝑅𝐶 0
𝑡
𝑜𝑟 𝑞 = 𝑞0𝑒 𝑅𝑐

Instantaneous current
𝑑𝑞
𝐼=
𝑑𝑡
𝑡
−𝑅𝐶
= −𝐼0𝑒
When t = RC, q = q0/e = 0.37q0
t = RC is the time in which the charge
decreases to 0.37 times the
maximum charge q0.

You might also like