AP EAMCET /Physics

DC Circuits & Kirchhoff's Laws

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DC Circuits & Kirchhoff’s Laws

(AP EAMCET – Physics – Beginner Notes)


1. What is a DC Circuit?

  • DC = Direct Current – a steady flow of electrons.
  • Think of a water pipe that always flows in one direction.
  • A circuit is a closed loop that lets the current travel from the battery, through wires, and back.

2. Basic Electrical Terms

Term Everyday Analogy Short Definition
Voltage (V) Water pressure “Push” that moves electrons.
Current (I) Water flow Number of electrons passing a point each second.
Resistance (R) Narrow pipe How hard it is for electrons to move.
Power (P) Work done by water Energy used per second (V × I).

3. Ohm’s Law – The Simple Rule

V = I × R
(Voltage = Current × Resistance)

  • If you know two of V, I, R, you can find the third.
  • Example
    • Battery: 9 V
    • Resistor: 3 Ω
    • Find current:
      I = V / R = 9 V / 3 Ω = 3 A

4. Series Circuits

  • Components connected end‑to‑end.
  • The same current flows through each part.
  • Voltage adds up.
  • Resistance adds up.

Example

Battery (12 V) → Resistor R1 (2 Ω) → Resistor R2 (4 Ω) → Battery
  • Total R = 2 Ω + 4 Ω = 6 Ω
  • Current I = 12 V / 6 Ω = 2 A
  • Voltage across R1 = I × R1 = 2 A × 2 Ω = 4 V
  • Voltage across R2 = 8 V

5. Parallel Circuits

  • Components connected side‑by‑side.
  • The same voltage appears across each branch.
  • Current splits – each branch gets part of the total current.
  • Total resistance is less than the smallest resistor.

Example

Battery (12 V) → Junction → R1 (4 Ω) || R2 (6 Ω) → Return to Battery
  • Voltage across each resistor = 12 V
  • Current through R1 = 12 V / 4 Ω = 3 A
  • Current through R2 = 12 V / 6 Ω = 2 A
  • Total current = 3 A + 2 A = 5 A

6. Kirchhoff’s Laws – Rules for Complex Circuits

6.1 Kirchhoff’s Current Law (KCL) – “What Goes In, Comes Out”

  • At any junction, the sum of currents entering equals the sum of currents leaving.
  • Water‑pipe analogy: If 5 L/min of water enters a junction and 3 L/min leaves one branch, 2 L/min must leave the other branch.

Example

      I1
   ────────►
   |        |
   |        |
   |        |
   └───────► I3
      I2
  • Let I1 = 4 A, I2 = 3 A.
  • KCL: I1 + I2 = I3 → 4 A + 3 A = 7 A (so I3 = 7 A).

6.2 Kirchhoff’s Voltage Law (KVL) – “No Energy is Lost”

  • Around any closed loop, the sum of voltage rises and drops is zero.
  • Think of a roller coaster: the energy you gain climbing up is exactly the energy you lose going down.

Example

Battery (12 V) → Resistor R1 (2 Ω) → Resistor R2 (4 Ω) → Back to Battery
  • Current I = 12 V / (2 Ω + 4 Ω) = 2 A
  • Voltage across R1 = I × R1 = 4 V
  • Voltage across R2 = I × R2 = 8 V
  • KVL check: 12 V (rise) – 4 V – 8 V = 0 V (works!)

7. Quick Problem – Putting It All Together

Problem
A 10 V battery is connected to three resistors:

  • R1 = 2 Ω (series)
  • R2 = 3 Ω (parallel with R3)
  • R3 = 6 Ω

Find the current through each resistor.

Solution

  1. Find equivalent resistance of R2‖R3
    [ R_{23} = \frac{1}{\frac{1}{3}+ \frac{1}{6}} = \frac{1}{\frac{1}{2}} = 2,\Omega ]

  2. Total resistance (R1 + R23)
    [ R_{\text{total}} = 2,\Omega + 2,\Omega = 4,\Omega ]

  3. Total current from battery
    [ I_{\text{total}} = \frac{V_{\text{battery}}}{R_{\text{total}}} = \frac{10,V}{4,\Omega} = 2.5,A ]

  4. Current through R1 – same as total current
    [ I_{R1} = 2.5,A ]

  5. Voltage across R1
    [ V_{R1} = I_{R1} \times R1 = 2.5,A \times 2,\Omega = 5,V ]

  6. Voltage across R2 & R3 (same because they’re parallel)
    [

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