Lab 6: R-C Circuits Only 6 more labs to go!! A capacitor is a device used to store energy. In this lab we will measure how a capacitor “stores” up or discharges energy. If we use Kirkchoff’s loop rule to the circuit below we get the following equation: R Vapplied VR VC 0 C Q Vapplied IR 0 C Remember the definition of current is: So the equation becomes: Q I t Q Q Vapplied R 0 t C Switch Vapplied This equation is called a differential equation. t RC The solution to this differential equation is: Q CVapplied 1 e This tells us that the charge on the capacitor is exponential in time. t RC Q CVapplied 1 e t Q CVapplied 1 e CVapplied Charge, Q Q = CVapplied t = RC = time (s) Since we now know how the capacitor charges up we can write an equation that describes the voltage as a function of time: t Voltage, V Vcap Q RC Vapplied 1 e C t = RC = time (s) C is called the RC-time constant. It represents the time which the voltage drop across the capacitor reaches 63% of it’s max value. Let’s look at this example: R = 105 C = 5 F 1. Find the time constant, C. C RC 105 5F 0.5 sec Switch Vapplied = 12 V 2. Find the charge on the capacitor at t = 0.2 sec t 0.2 sec RC 0 . 5 sec 1.9 105 C Q CVapplied 1 e 5F 12V 1 e 3. Find the voltage on the capacitor at t = 0.3 sec Vcap t 0.3sec RC 0 . 5 sec 5.42V Vapplied 1 e 12V 1 e 4. How long will it take the capacitor to charge to 9V? Vcap t t RC 0 . 5 sec t 0.69 sec Vapplied 1 e 9V 12V 1 e Now we will look at how the capacitor discharges its energy. Let’s look at this circuit: R C Use Kirchoff’s loop: VR VC 0 Switch The solution to this differential equation is: Q Q0 e t RC V0Ce t RC If we take the derivative of this equation with respect to time we can get the current: Charge, Q Q IR 0 C Q Q R 0 t C time (s) Q0 I e RC t RC 1. R=105 Find the voltage across the capacitor at time, t = 0.3 s. Vcap V0 e t RC 9Ve 0.3 sec 0.5 sec C=5F 4.94V Switch 2. How long will it take the capacitor to reach 3 v? Vcap V0e t RC Vcap V0 e t RC Vapplied = 9V Vcap t ln RC V0 Vcap 3V 0.5 sec ln 0.55s t RC ln 9V V0