Electronics/Electronics Formulas/Series Circuits/Series RC

The total impedance of the circuit

${\displaystyle Z=Z_{R}+Z_{L}}$

${\displaystyle Z=R+j\omega L}$

${\displaystyle Z={\frac {1}{R}}(1+j\omega T)}$

${\displaystyle T={\frac {L}{R}}}$

ist order Differential equation of the circuit

${\displaystyle L{\frac {di}{dt}}+iR=0}$

${\displaystyle {\frac {di}{dt}}+i{\frac {R}{L}}=0}$

${\displaystyle \int {\frac {di}{i}}=-{\frac {R}{L}}\int dt}$

${\displaystyle Lni=-{\frac {t}{T}}+c}$

The root of the equation is an Exponential Decaqy function characterised the Natural Response of the circuit

${\displaystyle i=Ae^{(}-{\frac {t}{T}})}$

${\displaystyle Z=Z_{R}+Z_{L}}$

${\displaystyle Z=R\angle 0+\omega L\angle 90}$

${\displaystyle Z=|Z|\angle \theta }$

${\displaystyle Z={\sqrt {R^{2}+(\omega L)^{2}}}\angle \omega {\frac {L}{R}}}$

Phase Change, Frequency change relate to the change in value of RC

${\displaystyle Tan\theta =\omega {\frac {L}{R}}=2\pi f{\frac {L}{R}}=2\pi {\frac {1}{t}}{\frac {L}{R}}}$

Series RC is characterised by

1st ordered Differential equation of the circuit at equilibrium.

${\displaystyle {\frac {di}{dt}}+{\frac {1}{T}}=0}$

Natural Reponse of the circuit is the Exponential Decay

${\displaystyle v=Ae^{(}-{\frac {t}{T}})}$

${\displaystyle T=RC}$