This is the circuit I got from an example in a book "Practical Electronics for Inventors", on page 48:
How can one understand that \$0=R\frac{dI}{dt}+\frac{1}{C}I\$ implies \$I=I_0e^{\frac{-t}{RC}}\$?
This is the circuit I got from an example in a book "Practical Electronics for Inventors", on page 48:
How can one understand that \$0=R\frac{dI}{dt}+\frac{1}{C}I\$ implies \$I=I_0e^{\frac{-t}{RC}}\$?
This should help (it helped me!!): -
The final formula is written as V/R instead of Io but it means the current at time = 0.
Copied from http://www.intmath.com/differential-equations/6-rc-circuits.php in case you need the full article. This took me back a few years!
First by algebraic manipulation, then by integration.
For the first step, divide all terms by R.
For the second step, subtract one of the RHS terms from both sides.
Then the equation should be in a form with a standard integral, so just integrate it. You should now have the result.