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Study Guide: Physics Electromagnetism - How to Solve: RC Circuit (Charging/Discharging, Time Constant) – IIT JEE Guide
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Physics Electromagnetism - How to Solve: RC Circuit (Charging/Discharging, Time Constant) – IIT JEE Guide

By Fatskills Exam Guides Team — the exam nerds behind 28,500+ quizzes and 2.1M practice questions across 500+ global exams.

⏱️ ~6 min read

How to Solve: RC Circuit (Charging/Discharging, Time Constant) – IIT JEE Guide

(For Students & Teachers – Ready-to-Record Script Included)

Introduction

"Master RC circuits, and you unlock 5–10 marks in IIT JEE—questions on charging/discharging, time constants, and graph analysis appear every year. Miss this, and you’re leaving easy marks on the table."

(On camera: Hold up a past JEE paper with an RC circuit question highlighted.) "This is a 4-mark question from JEE Main 2022. Today, you’ll learn how to solve it in under 2 minutes."

WHAT YOU NEED TO KNOW FIRST

Before diving in, ensure you understand: 1. Ohm’s Law & Kirchhoff’s Voltage Law (KVL) – How voltage divides in a loop. 2. Exponential Functions – The shape of ( e^{-t/RC} ) and ( 1 - e^{-t/RC} ). 3. Basic Calculus (Differentiation/Integration) – Only for derivation (not required for solving problems in JEE).

(On camera: Flash a quick recap slide of Ohm’s Law and exponential graphs.)

KEY TERMS & FORMULAS

Key Terms

Term Definition
RC Circuit A circuit with a resistor (R) and capacitor (C) in series.
Time Constant (τ) Time for the capacitor to charge to 63.2% or discharge to 36.8% of its final value.
Charging Capacitor gains charge (voltage increases).
Discharging Capacitor loses charge (voltage decreases).
Steady State When the capacitor is fully charged/discharged (current = 0).

Formulas

(All formulas are MEMORISE THIS unless marked otherwise.)

  1. Time Constant (τ)
    [
    \tau = R \times C
    ]
  2. ( R ) = Resistance (Ω)
  3. ( C ) = Capacitance (F)
  4. Unit: Seconds (s)

  5. Charging a Capacitor (Voltage vs. Time)
    [
    V_C(t) = V_0 (1 - e^{-t/\tau})
    ]

  6. ( V_C(t) ) = Voltage across capacitor at time ( t )
  7. ( V_0 ) = Supply voltage (battery voltage)
  8. ( t ) = Time (s)
  9. ( \tau = RC )

  10. Discharging a Capacitor (Voltage vs. Time)
    [
    V_C(t) = V_0 e^{-t/\tau}
    ]

  11. ( V_0 ) = Initial voltage across capacitor

  12. Current During Charging/Discharging
    [
    I(t) = \frac{V_0}{R} e^{-t/\tau}
    ]

  13. Current decreases exponentially in both cases.

  14. Charge on Capacitor (Q = CV)

  15. Charging: ( Q(t) = Q_0 (1 - e^{-t/\tau}) )
  16. Discharging: ( Q(t) = Q_0 e^{-t/\tau} )
  17. ( Q_0 = C V_0 )

  18. Energy Stored in Capacitor
    [
    U = \frac{1}{2} C V^2
    ]
    (Given on exam sheet, but useful for energy-based questions.)

(On camera: Point to each formula and say:) "Memorise these 4 equations—they’re your weapons for every RC circuit problem."

STEP-BY-STEP METHOD

Step 1: Identify the Circuit Type

  • Charging: Battery is connected, switch is closed.
  • Discharging: Battery is disconnected, capacitor discharges through resistor.

Step 2: Find the Time Constant (τ)

[ \tau = R \times C ] - If multiple resistors/capacitors, find equivalent R/C first.

Step 3: Write the Correct Voltage/Current Equation

  • Charging: ( V_C(t) = V_0 (1 - e^{-t/\tau}) )
  • Discharging: ( V_C(t) = V_0 e^{-t/\tau} )

Step 4: Plug in Given Values

  • Substitute ( t, R, C, V_0 ) into the equation.
  • If asked for current, use ( I(t) = \frac{V_0}{R} e^{-t/\tau} ).

Step 5: Solve for the Unknown

  • Isolate the variable (e.g., ( t, R, V )).
  • Use logarithms if needed (e.g., ( e^{-t/\tau} = 0.5 ) → ( t = \tau \ln 2 )).

Step 6: Check Units & Reasonableness

  • ( \tau ) should be in seconds.
  • Voltage should never exceed ( V_0 ) during charging.
  • Current should decrease over time.

(On camera: Demonstrate each step on a whiteboard with a simple circuit.)

WORKED EXAMPLES

Example 1 – Basic (Charging)

Problem: A 1000 Ω resistor and 100 μF capacitor are connected to a 10 V battery. Find the voltage across the capacitor after 0.1 s.

Solution: 1. Identify: Charging circuit. 2. Time Constant:
[
\tau = R \times C = 1000 \times 100 \times 10^{-6} = 0.1 \text{ s}
] 3. Voltage Equation:
[
V_C(t) = V_0 (1 - e^{-t/\tau}) = 10 (1 - e^{-0.1/0.1}) = 10 (1 - e^{-1})
] 4. Calculate:
[
e^{-1} \approx 0.3679 \implies V_C = 10 (1 - 0.3679) = 6.32 \text{ V}
]

What we did and why: - Used the charging formula because the battery is connected. - Calculated ( \tau ) first, then substituted into the exponential equation.

Example 2 – Medium (Discharging + Equivalent Resistance)

Problem: A 500 Ω resistor and 200 μF capacitor are initially charged to 12 V. They are then connected to a 1000 Ω resistor. Find the voltage after 0.2 s.

Solution: 1. Identify: Discharging through two resistors in series (500 Ω + 1000 Ω = 1500 Ω). 2. Time Constant:
[
\tau = R_{eq} \times C = 1500 \times 200 \times 10^{-6} = 0.3 \text{ s}
] 3. Voltage Equation:
[
V_C(t) = V_0 e^{-t/\tau} = 12 e^{-0.2/0.3} = 12 e^{-2/3}
] 4. Calculate:
[
e^{-2/3} \approx 0.5134 \implies V_C = 12 \times 0.5134 = 6.16 \text{ V}
]

What we did and why: - Recognized that discharging involves all resistors in the path. - Combined resistors first, then used the discharging formula.

Example 3 – Exam-Style (Disguised Question)

Problem (JEE Main 2020): A capacitor of capacitance ( C ) is charged to a potential ( V ). It is then connected to a resistor ( R ). The time taken for the charge to reduce to ( \frac{1}{e} ) of its initial value is: (A) ( RC ) (B) ( \frac{RC}{2} ) (C) ( 2RC ) (D) ( RC \ln 2 )

Solution: 1. Identify: Discharging problem. 2. Charge Equation:
[
Q(t) = Q_0 e^{-t/\tau}
] 3. Given: ( Q(t) = \frac{Q_0}{e} )
[
\frac{Q_0}{e} = Q_0 e^{-t/\tau} \implies e^{-1} = e^{-t/\tau}
] 4. Solve for ( t ):
[
-1 = -\frac{t}{\tau} \implies t = \tau = RC
] 5. Answer: (A) ( RC )

What we did and why: - Recognized that ( \frac{1}{e} ) implies ( t = \tau ). - Avoided overcomplicating—exponential decay simplifies neatly.

COMMON MISTAKES

MISTAKE WHY IT HAPPENS CORRECT APPROACH
Using charging formula for discharging (or vice versa) Confusing the two scenarios. Charging: ( 1 - e^{-t/\tau} ) Discharging: ( e^{-t/\tau} )
Forgetting to find equivalent R/C Assuming only one resistor/capacitor exists. Always simplify the circuit first.
Mixing up ( V_0 ) (supply vs. initial voltage) Using battery voltage for discharging. Charging: ( V_0 ) = battery voltage. Discharging: ( V_0 ) = initial capacitor voltage.
Ignoring units (μF vs. F, kΩ vs. Ω) Not converting to base units. Always convert to Farads (F) and Ohms (Ω).
Assuming current is constant Forgetting that current decays exponentially. Current always follows ( I(t) = \frac{V_0}{R} e^{-t/\tau} ).

(On camera: Hold up a red card for each mistake and say:) "This is a 2-mark error. Don’t let it happen to you."

EXAM TRAPS

TRAP HOW TO SPOT IT HOW TO AVOID IT
Hidden resistors in series/parallel Circuit diagram shows multiple resistors. Simplify the circuit before calculating ( \tau ).
Asking for "time to reach 50% charge" Tricks you into using ( t = \tau ). 50% charge ≠ 63.2% (use ( t = \tau \ln 2 )).
Energy-based questions (e.g., heat dissipated) Asks for energy, not voltage/current. Use ( U = \frac{1}{2} CV^2 ) and energy conservation.

(On camera: Show a past JEE question with a trap highlighted.) "Examiners love this trick—spot it, and you save 3 minutes."

1-MINUTE RECAP

(Speak naturally, as if to a friend the night before the exam.)

"Alright, listen up. RC circuits are all about two things: the time constant ( \tau = RC ), and exponential decay. Here’s the cheat sheet:

  1. Charging? Use ( V = V_0 (1 - e^{-t/\tau}) ).
  2. Discharging? Use ( V = V_0 e^{-t/\tau} ).
  3. Current? Always ( I = \frac{V_0}{R} e^{-t/\tau} ).
  4. Time to reach X% charge? Set ( V = X\% \times V_0 ) and solve for ( t ).
  5. Multiple resistors? Combine them first—no shortcuts.

Memorise these 4 equations, and you’re golden. Now go crush that exam."

(On camera: Point to the formulas one last time and smile.) "You’ve got this."



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