Current Electricity – Class 12 Physics Chapter 3 Notes & NCERT PDF
Notes and a simple summary of Chapter 3 of the NCERT Class 12 Physics book, with the official chapter PDF, flashcards, an MCQ quiz and an AI tutor for your doubts.
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Chapter 3: Current Electricity
Introduction
Chapter 3 moves from charges at rest to charges in motion. It explains what electric current is, how Ohm's law arises from the drift of electrons, how resistivity depends on material and temperature, how cells supply energy, and how to analyse circuits with Kirchhoff's rules and the Wheatstone bridge.
Key Concepts
3.2–3.3 Electric current
Current is the rate of flow of charge: I = ΔQ/Δt (for steady current I = q/t). SI unit ampere (A). By convention, current flows in the direction of positive-charge motion — opposite to electron flow in metals. Without a field, free electrons move randomly with no net flow; an applied field produces a net drift.
3.4 Ohm's law
V = IR, where R is the resistance (unit ohm, Ω). R = ρl/A: resistance grows with length and falls with cross-sectional area. ρ is the resistivity (Ω m), a material property. Current density j = I/A, and in vector form E = ρj (or j = σE, σ = 1/ρ = conductivity).
3.5 Drift of electrons — the origin of resistivity
In a field E, each electron accelerates (a = −eE/m) between collisions. Averaging over the relaxation time τ gives the drift velocity v_d = −eEτ/m. Then I = neAv_d, which leads to ρ = m/(ne²τ) — Ohm's law from microscopic physics.
3.6 Limitations of Ohm's law
Ohm's law is not universal: some devices have non-linear V–I graphs, current may depend on the sign of V (diodes), or V may not be a single-valued function of I (e.g. GaAs). These are non-ohmic devices.
3.7–3.8 Resistivity and temperature
Materials range from conductors (ρ ~ 10⁻⁸ Ω m) through semiconductors to insulators (ρ up to 10¹⁴–10¹⁶ Ω m). For metals, ρ_T = ρ₀[1 + α(T − T₀)] with a positive temperature coefficient α. Nichrome has high ρ and a small α (useful in heaters), manganin and constantan have very small α (standard resistors), and semiconductors have ρ decreasing with temperature (negative α).
3.9 Electrical energy and power
Power dissipated: P = VI = I²R = V²/R. Power transmission uses high voltage so that current, and hence line loss I²R_c, is small.
3.10–3.11 Cells, emf and internal resistance
The emf ε is the potential difference between the terminals of a cell on open circuit. With internal resistance r and external resistance R: I = ε/(R + r), and terminal voltage V = ε − Ir.
3.12 Kirchhoff's rules
3.13 Wheatstone bridge
Four resistances R₁, R₂, R₃, R₄ with a galvanometer across the middle. The bridge is balanced (no galvanometer current) when R₂/R₁ = R₄/R₃. This lets an unknown resistance be found accurately from three known ones.
Resistor combinations
Worked Examples
Formula / Key-Facts Sheet
Board Exam Focus
Key Terms
Electric current (विद्युत धारा), Current density (धारा घनत्व), Resistance (प्रतिरोध), Resistivity (प्रतिरोधकता), Conductivity (चालकता), Drift velocity (अपवाह वेग), Relaxation time (विश्रांति काल), Mobility (गतिशीलता), Temperature coefficient (ताप गुणांक), Electromotive force (विद्युत वाहक बल), Internal resistance (आंतरिक प्रतिरोध), Terminal voltage (टर्मिनल विभवांतर), Kirchhoff's rules (किरखोफ के नियम), Wheatstone bridge (व्हीटस्टोन सेतु), Power (शक्ति)
Common Mistakes
💡 Key Learning Points
- ✓Current, current density and Ohm's law (V = IR, R = ρl/A)
- ✓Drift velocity, relaxation time, mobility and the microscopic origin of resistivity
- ✓Temperature dependence of resistivity and limitations of Ohm's law
- ✓EMF, internal resistance, terminal voltage and combinations of cells
- ✓Kirchhoff's rules and the Wheatstone bridge
👨🏫 Teaching Tips
- →Show a real V–I graph for a resistor and a diode to contrast ohmic and non-ohmic behaviour
- →Use a crowd-in-a-corridor analogy for drift with collisions
- →Work Example 3.1 to show why drift speed is tiny
- →Measure a cell's terminal voltage with and without load to introduce internal resistance
- →Teach a fixed sign convention for Kirchhoff's loop rule and practise on two-loop circuits
- →Derive the Wheatstone balance condition directly from Kirchhoff's rules
- →Link P = I²R to why transmission lines use high voltage
📋 Assessment Questions
- Can students derive I = neAv_d and ρ = m/(ne²τ)?
- Can they compute terminal voltage and currents with internal resistance?
- Can they apply Kirchhoff's rules to a two-loop network?
- Can they derive and use the Wheatstone bridge condition?
- Can they explain how resistivity varies with temperature for metals and semiconductors?
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