Exhaustive Guide to Capacitor Charging and Discharging Through a Resistor

Fundamentals of Capacitor Circuits

  • Circuit Components and Configuration:     * Power Supply: The circuit operates with a voltage source of +9V+9\,V.     * Resistor (RR): The resistor in the circuit has a value of 100kΩ100\,k\Omega.     * Capacitor (CC): The capacitor has a capacitance of 300μF300\,\mu F.     * Switch 1 (S1S_1): This switch is used to initiate the charging process when closed.     * Switch 2 (S2S_2): This switch is used to discharge the capacitor; pressing it briefly connects the capacitor to 0V0\,V, discharging it instantly.

The Time Constant (RCRC)

  • Definition and Calculation:     * The time constant, designated by the Greek letter tau (τ\tau), is the product of the resistance and the capacitance in a circuit.     * Formula: Time Constant=R×C\text{Time Constant} = R \times C     * Calculation for the provided circuit: 100kΩ×300μF=100,000Ω×0.0003F=30,000ms=30s100\,k\Omega \times 300\,\mu F = 100,000\,\Omega \times 0.0003\,F = 30,000\,ms = 30\,s.     * Therefore, 1RC=30s1\,RC = 30\,s.

  • Key Thresholds during Charging:     * 1RC1\,RC (30s30\,s): The capacitor charges to approximately 63%63\% of the supply voltage.     * 0.69RC0.69\,RC: This represents the time required for the capacitor to reach 50%50\% of the supply voltage.     * 5RC5\,RC: After five time constants, the capacitor is considered effectively fully charged (approximately 100%100\%).     * Intermediate Stages: Each subsequent time constant allows the capacitor to charge an additional 63%63\% of the remaining voltage difference between its current state and the supply voltage.

Capacitor Charging through a Resistor

  • Voltage Growth Calculation:     * The formula used to calculate the voltage across the capacitor (VCV_C) at any given time (tt) while charging is:     * VC=V×(1etRC)V_C = V \times (1 - e^{-\frac{t}{RC}})     * In this context, the power of ee corresponds to the number of time constants that have elapsed.

  • Example 1: Charging at t=60st = 60\,s:     * Given: t=60st = 60\,s, V=+9VV = +9\,V, RC=30sRC = 30\,s.     * VC=+9V×(1e60s100kΩ×300μF)V_C = +9\,V \times (1 - e^{-\frac{60\,s}{100\,k\Omega \times 300\,\mu F}})     * VC=+9V×(1e60s30s)V_C = +9\,V \times (1 - e^{-\frac{60\,s}{30\,s}})     * VC=+9V×(1e2)V_C = +9\,V \times (1 - e^{-2})     * VC=+9V×(10.135)V_C = +9\,V \times (1 - 0.135)     * VC=+9V×0.865=7.78VV_C = +9\,V \times 0.865 = 7.78\,V

  • Example 2: Charging at t=100st = 100\,s:     * Given: t=100st = 100\,s, V=+9VV = +9\,V, RC=30sRC = 30\,s.     * VC=+9V×(1e100s100kΩ×300μF)V_C = +9\,V \times (1 - e^{-\frac{100\,s}{100\,k\Omega \times 300\,\mu F}})     * VC=+9V×(1e3.33)V_C = +9\,V \times (1 - e^{-3.33})     * VC=+9V×(10.0357)V_C = +9\,V \times (1 - 0.0357)     * VC=+9V×0.9643=8.68VV_C = +9\,V \times 0.9643 = 8.68\,V

  • Determining Time from Voltage (Charging):     * To find the time required for a capacitor to reach a specific voltage, the formula is rearranged:     * t=R×C×ln(1VCV)t = -R \times C \times \ln(1 - \frac{V_C}{V})

  • Application: Reaching 7V7\,V while charging:     * t=100kΩ×300μF×ln(17V9V)t = -100\,k\Omega \times 300\,\mu F \times \ln(1 - \frac{7\,V}{9\,V})     * t=30s×ln(10.777)t = -30\,s \times \ln(1 - 0.777)     * t=30s×ln(0.222)t = -30\,s \times \ln(0.222)     * t=30s×(1.5)=45st = -30\,s \times (-1.5) = 45\,s

  • Application: Reaching 8V8\,V while charging:     * t=30s×ln(18V9V)t = -30\,s \times \ln(1 - \frac{8\,V}{9\,V})     * t=30s×ln(0.111)t = -30\,s \times \ln(0.111)     * t=30s×(2.2)=66st = -30\,s \times (-2.2) = 66\,s

Capacitor Discharging through a Resistor

  • Process Initiation: Set the circuit by pressing switch S1S_1 to charge the capacitor instantly, then release S1S_1 to allow the capacitor to discharge through the resistor RR.

  • Key Thresholds during Discharging:     * 1RC1\,RC (30s30\,s): The voltage across the capacitor drops by 63%63\% (meaning it falls to 37%37\% of its original value).     * 0.69RC0.69\,RC: The voltage drops by 50%50\%.     * 5RC5\,RC: The capacitor is considered effectively fully discharged (100%\approx 100\% drop).

  • Voltage Decay Calculation:     * The formula for the voltage across the capacitor while discharging is:     * VC=V×etRCV_C = V \times e^{-\frac{t}{RC}}

  • Example 1: Discharging at t=60st = 60\,s:     * Given: t=60st = 60\,s, V=+9VV = +9\,V, RC=30sRC = 30\,s.     * VC=+9V×e60s30sV_C = +9\,V \times e^{-\frac{60\,s}{30\,s}}     * VC=+9V×e2V_C = +9\,V \times e^{-2}     * VC=+9V×0.135=1.22VV_C = +9\,V \times 0.135 = 1.22\,V

  • Example 2: Discharging at t=100st = 100\,s:     * Given: t=100st = 100\,s, RC=30sRC = 30\,s.     * VC=+9V×e3.33V_C = +9\,V \times e^{-3.33}     * VC=+9V×0.0357=0.32VV_C = +9\,V \times 0.0357 = 0.32\,V

  • Determining Time from Voltage (Discharging):     * To find the time required for a capacitor to decay to a specific voltage:     * t=R×C×ln(VCV)t = -R \times C \times \ln(\frac{V_C}{V})

  • Application: Reaching 2V2\,V while discharging:     * t=100kΩ×300μF×ln(2V9V)t = -100\,k\Omega \times 300\,\mu F \times \ln(\frac{2\,V}{9\,V})     * t=30s×ln(0.222)t = -30\,s \times \ln(0.222)     * t=30s×(1.5)=45st = -30\,s \times (-1.5) = 45\,s

  • Application: Reaching 1V1\,V while discharging:     * t=30s×ln(1V9V)t = -30\,s \times \ln(\frac{1\,V}{9\,V})     * t=30s×ln(0.111)t = -30\,s \times \ln(0.111)     * t=30s×(2.2)=66st = -30\,s \times (-2.2) = 66\,s

Comparative Graphical Analysis

  • Symmetry in Charging and Discharging:     * Comparison at 66s66\,s: While charging, it takes 66s66\,s for the capacitor to reach 8V8\,V (within 1V1\,V of the supply voltage). Conversely, while discharging starting from 9V9\,V, it takes 66s66\,s for the capacitor to reach 1V1\,V (within 1V1\,V of zero).     * Comparison at 45s45\,s: While charging, the capacitor reaches 7V7\,V in 45s45\,s. While discharging, it takes 45s45\,s to reach 2V2\,V.     * Specific Voltage Levels at 2RC2\,RC (60s60\,s):         * Charging: VC=7.78VV_C = 7.78\,V         * Discharging: VC=1.22VV_C = 1.22\,V

Exercises

  • Upon reviewing these notes, complete the following from Chapter 2 of the 1A curriculum:     * Exercise 2.1     * Exercise 2.2     * Exercise 2.3
  • Submissions must be made via three separate, clear scans and uploaded to the Teams platform.