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R-C circuits

R-C circuits. So far we considered stationary situations only meaning:. Next step in generalization is to allow for time dependencies. For consistency we follow the textbook notation where time dependent quantities are labeled by lowercase symbols such as i =I(t), v=V(t), etc .

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R-C circuits

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  1. R-C circuits So far we considered stationary situations only meaning: Next step in generalization is to allow for time dependencies For consistency we follow the textbook notation where time dependent quantities are labeled by lowercase symbols such as i=I(t), v=V(t), etc Let’s charge a capacitor again -q +q Vab=Va-Vb Vb Va

  2. What happens during the charging process The capacitor starts to accumulate charge A voltage vab starts to build up which is given by The transportation of charge to the capacitor means a current i is flowing The current gives rise to a voltage drop across the resistor R which reads: Using Kirchhoff’s loop rule we conclude With the definition of current as Inhomogeneous first order linear differential equation Since in the very first moment when the switch is closed there is not charge in the capacitor we have the initial condition q(t=0)=0

  3. Lets consider common strategies to solve such a differential equation We use intuition to get an idea of the solution. We know that initially q=0 and after a long time when the charging process is finished i=0 and hence q t Let’s guess and check if it works and, if so, let’s determine the time constant  Substitution into

  4. Our guess works if we chose Guessing is a common strategy to solve differential equations In the case of a linear first order differential equation there is a systematic integration approach which always works with q(t=0)=0 with

  5. q t After time 63% of Qf reached How does the time dependence of the current look like i I0/e t

  6. Now let’s discharge a capacitor Using Kirchhoff’s loop rule in the absence of an emf we conclude homogeneous first order linear differential equation In the very first moment when the switch is closed the current is at maximum and determined by the charge Q(t=0)=Q0 initially in the capacitor Current is opposite to the direction on charging

  7. We close the chapter with an energy consideration for a charging capacitor When multiplying i by the time dependent current i Rate at which energy is stored in the capacitor Power delivered by the emf Rate at which energy is dissipate by resistor Total energy supplied by the battery (emf) Half of the energy delivered by the battery is stored in the capacitor no matter what the value of R or C is ! Total energy stored in capacitor is

  8. Let’s check this surprising result by calculating the energy dissipated in R which must be the remaining half of the energy delivered by the emf with with

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