Current Electricity Class 12 Physics – Complete NCERT RBSE Notes

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Current Electricity - Class 12 Physics | Chapter 3 NCERT

Current Electricity

विद्युत धारा | Class 12 Physics - Chapter 3 | NCERT + RBSE 2026

This chapter strictly follows NCERT Class 12 Physics textbook and examination pattern for CBSE, RBSE and other state boards

Subject:Physics
Class:12 (RBSE + NCERT)
Chapter:3
Topic:Current Electricity
Year:2025-26
Status:Complete & Verified
Key Physical Constants & Units:
• Elementary charge: e = 1.602 × 10⁻¹⁹ C
• Current unit: 1 A = 1 C/s (Ampere)
• Resistance unit: 1 Ω = 1 V/A (Ohm)
• Power unit: 1 W = 1 J/s (Watt)
• Electron mass: me = 9.1 × 10⁻³¹ kg

Learning Objectives

After completing this chapter, students will be able to:

  • Define electric current and understand its microscopic origin in conductors
  • State and apply Ohm's law to solve circuit problems
  • Explain drift velocity and its relationship with current
  • Understand the origin of resistivity in materials
  • Analyze temperature dependence of resistance in conductors and semiconductors
  • Calculate electrical energy and power consumed in circuits
  • Define EMF and internal resistance of cells
  • Analyze combinations of cells in series and parallel
  • Apply Kirchhoff's laws to solve complex circuit problems
  • Understand and apply the Wheatstone bridge principle

1. Introduction

From Static to Dynamic Electricity

Chapter 1 & 2: Electrostatics
• Charges at rest
• Electric field, potential
• No current flow

Chapter 3: Current Electricity
• Charges in motion
• Sustained flow of charge
• Practical applications: circuits, devices

Applications: All electronic devices, power systems

In Chapters 1 and 2, we studied charges at rest (electrostatics). Now we move to current electricity, which deals with charges in motion. Electric current is the foundation of all electrical and electronic devices we use daily.

Understanding current flow, resistance, and energy transfer is essential for analyzing circuits, designing electronic systems, and solving practical electrical problems.

2. Electric Current

Current as Charge Flow

Charge ΔQ flows through cross-section
in time interval Δt

Current I = ΔQ/Δt

Direction: From + to − (conventional)
Actually: Electrons flow − to +

2.1 Definition

Electric current is defined as the rate of flow of electric charge through a conductor.

Electric Current
I = ΔQ/Δt = dQ/dt

SI Unit: Ampere (A) = Coulomb/second (C/s)

Nature: Scalar quantity (has magnitude, but direction is conventional)

2.2 Direction of Current

Conventional vs Electron Flow
  • Conventional current: Direction of flow of positive charges (+ to −)
  • Electron flow: Direction of electron motion (− to +)
  • In metallic conductors: Only electrons move (ions fixed in lattice)
  • Convention: We use conventional current direction (+ to −)

2.3 Types of Current

  • Direct Current (DC): Current flows in one direction only (e.g., from batteries)
  • Alternating Current (AC): Current periodically reverses direction (e.g., household supply)

3. Electric Currents in Conductors

Microscopic View of Current in Conductor

No Electric Field: Electrons move randomly
• Random thermal motion
• No net displacement
• Current = 0

Electric Field Applied: Electrons drift
• Superimposed drift motion
• Net displacement toward +ve terminal
• Current flows

In a metallic conductor:

  • Free electrons undergo random thermal motion (speeds ~ 10⁶ m/s)
  • No net current in absence of electric field (random directions cancel)
  • When electric field applied: electrons acquire small drift velocity (~10⁻⁴ m/s) superimposed on thermal motion
  • This organized drift creates electric current

3.1 Drift Velocity

Drift Velocity
vd = eEτ/me

where:

  • vd = drift velocity
  • e = electronic charge
  • E = electric field
  • τ = relaxation time (average time between collisions)
  • me = mass of electron
Key Points About Drift
  • Drift velocity is very small (10⁻⁴ m/s) compared to thermal velocity (10⁶ m/s)
  • Proportional to electric field: vd ∝ E
  • Current still flows quickly because all electrons start drifting simultaneously
  • Signal propagates at speed of light, not at drift velocity

4. Ohm's Law

Ohm's Law: V-I Relationship

For ohmic conductor at constant temperature:

V ∝ I

V = IR

V-I graph: Straight line through origin
Slope = Resistance (R)

Ohm's law states that the current through a conductor is directly proportional to the potential difference across it, provided the physical conditions (temperature, etc.) remain constant.

Ohm's Law
V = IR

Or equivalently:

I = V/R or R = V/I

where:

  • V = potential difference (Volt)
  • I = current (Ampere)
  • R = resistance (Ohm, Ω)

4.1 Resistance

Resistance is the property of a conductor that opposes the flow of current.

Resistance Formula
R = ρL/A

where:

  • R = resistance (Ω)
  • ρ = resistivity of material (Ω·m)
  • L = length of conductor (m)
  • A = cross-sectional area (m²)
Dependencies of Resistance
  • R ∝ L: Longer wire → more resistance
  • R ∝ 1/A: Thicker wire → less resistance
  • R ∝ ρ: Depends on material property (resistivity)
  • R depends on temperature (discussed later)

4.2 Conductance

Conductance is the reciprocal of resistance, measuring ease of current flow.

Conductance
G = 1/R

SI Unit: Siemens (S) or mho (℧) = 1/Ω

5. Drift of Electrons and Origin of Resistivity

Electron Motion in Conductor

Electron accelerates in field → gains velocity

Collides with ion → loses directed velocity

Accelerates again → gains velocity

Collides again...

Average steady drift velocity = vd
Resistance arises from collisions

5.1 Current and Drift Velocity Relationship

Deriving I in Terms of Drift Velocity

Consider a conductor of length L and cross-sectional area A with n free electrons per unit volume.

In time Δt, electrons drift a distance vdΔt

Volume of segment = AvdΔt

Number of electrons in segment = nAvdΔt

Total charge = neAvdΔt

Current I = Charge/Time = neAvdΔt/Δt

I = neAvd

5.2 Origin of Resistivity

Resistivity arises from collisions of electrons with:

  • Lattice ions (vibrating due to thermal energy)
  • Impurities and defects in the crystal structure
  • Other electrons

These collisions randomize electron motion, preventing unlimited acceleration and creating resistance to current flow.

6. Mobility

Mobility
μ = vd/E = eτ/me

Unit: m²/(V·s)

Definition: Drift velocity acquired per unit electric field

Understanding Mobility
  • Mobility measures how easily electrons move through conductor
  • Higher mobility → lower resistivity → better conductor
  • Depends on relaxation time τ (time between collisions)
  • Different for different materials and charge carriers

7. Limitations of Ohm's Law

Ohmic vs Non-Ohmic Materials

OHMIC: V-I graph is straight line
Examples: Metals at constant T

NON-OHMIC: V-I graph is curved
Examples: Diodes, transistors, thermistors

Ohm's law is not a universal law. It has limitations:

When Ohm's Law Fails
  1. Semiconductors: Resistance depends on voltage/current
  2. Vacuum tubes: Non-linear V-I characteristics
  3. Diodes: Current flows in one direction only
  4. Electrolytes: Resistance changes with current
  5. At very high electric fields: Heating effects dominate
  6. At very low temperatures: Superconductivity (R = 0)

Ohmic conductors: Materials that obey Ohm's law (constant R at constant T)

Non-ohmic conductors: Materials that don't obey Ohm's law (R varies with V or I)

8. Resistivity of Various Materials

Classification by Resistivity

CONDUCTORS: ρ ~ 10⁻⁸ to 10⁻⁶ Ω·m
Metals: Cu, Ag, Al

SEMICONDUCTORS: ρ ~ 10⁻³ to 10⁵ Ω·m
Si, Ge, GaAs

INSULATORS: ρ ~ 10¹⁰ to 10¹⁷ Ω·m
Glass, Rubber, Mica
Material Resistivity (Ω·m) at 20°C Type
Silver 1.6 × 10⁻⁸ Conductor (best)
Copper 1.7 × 10⁻⁸ Conductor
Aluminum 2.7 × 10⁻⁸ Conductor
Tungsten 5.6 × 10⁻⁸ Conductor
Iron 10 × 10⁻⁸ Conductor
Nichrome 100 × 10⁻⁸ Alloy (heating element)
Silicon 0.1 to 60 Semiconductor
Glass 10¹⁰ to 10¹⁴ Insulator
Key Observations
  • Silver is the best conductor, but copper is more commonly used (cheaper)
  • Semiconductors have intermediate resistivity
  • Insulators have very high resistivity (10²⁰ times that of conductors)
  • Alloys like nichrome have higher resistivity than pure metals (used in heaters)

9. Temperature Dependence of Resistivity

Resistivity vs Temperature

METALS: ρ increases with T
More thermal vibration → more collisions

SEMICONDUCTORS: ρ decreases with T
More charge carriers available at higher T

SUPERCONDUCTORS: ρ = 0 below Tc

9.1 Metallic Conductors

Temperature Coefficient of Resistivity
ρT = ρ₀[1 + α(T − T₀)]

where:

  • ρT = resistivity at temperature T
  • ρ₀ = resistivity at reference temperature T₀
  • α = temperature coefficient of resistivity (°C⁻¹)

For metals: α > 0 (positive)

Physical explanation: As temperature increases, lattice ions vibrate more vigorously, causing more frequent collisions with electrons, increasing resistivity.

9.2 Semiconductors

For semiconductors:

  • Resistivity decreases with increasing temperature (α < 0)
  • At higher T, more electrons gain energy to jump to conduction band
  • Number of charge carriers increases significantly
  • This effect dominates over increased collision rate

9.3 Superconductivity

Some materials show zero resistance below a critical temperature Tc:

  • Mercury: Tc = 4.2 K
  • Lead: Tc = 7.2 K
  • High-temperature superconductors: Tc up to 138 K

10. Electrical Energy and Power

Energy Transfer in Circuit

Battery does work on charges

Charges flow through resistor

Energy converted to heat (I²Rt)

Power dissipated = VI = I²R = V²/R

10.1 Electrical Energy

Electrical Energy
W = VIt = I²Rt = (V²/R)t

SI Unit: Joule (J)

Practical Unit: kilowatt-hour (kWh)

1 kWh = 3.6 × 10⁶ J

10.2 Electrical Power

Electrical Power (Three Forms)
P = VI
P = I²R
P = V²/R

SI Unit: Watt (W) = Joule/second (J/s)

Which Formula to Use?
  • P = VI: When both V and I are known
  • P = I²R: When I and R are known (useful for series circuits)
  • P = V²/R: When V and R are known (useful for parallel circuits)
  • All three are equivalent (derivable from Ohm's law)

11. Cells, EMF, and Internal Resistance

Cell Structure and Circuit Model

Real Cell = Ideal EMF source + Internal resistance

ε (EMF) ——[r]—— Terminals

Terminal voltage: V = ε − Ir
(Less than EMF when current flows)

11.1 Electromotive Force (EMF)

EMF (ε)

Definition: Work done per unit charge by the cell in moving charge from negative to positive terminal through the cell.

ε = W/Q

SI Unit: Volt (V)

EMF vs Terminal Voltage
  • EMF (ε): Maximum potential difference (when no current flows)
  • Terminal voltage (V): Actual voltage across terminals when current flows
  • Relationship: V = ε − Ir (where r is internal resistance)
  • V < ε when current flows (due to voltage drop across r)

11.2 Internal Resistance

Internal resistance (r) is the resistance offered by the electrolyte and electrodes inside the cell.

Terminal Voltage
V = ε − Ir

where:

  • V = terminal voltage
  • ε = EMF of cell
  • I = current through cell
  • r = internal resistance

11.3 Types of Cells

Type Description Examples Reversible?
Primary Cells Chemical reaction irreversible Dry cell, Alkaline No
Secondary Cells Can be recharged Lead-acid, Li-ion Yes

12. Cells in Series and Parallel

Cell Combinations

SERIES: [ε₁,r₁]—[ε₂,r₂]—[ε₃,r₃]
• EMFs add (if same polarity)
• Internal resistances add
• Higher voltage, same current capacity

PARALLEL: [ε,r₁] ∥ [ε,r₂] ∥ [ε,r₃]
• EMF remains same
• Internal resistance decreases
• Same voltage, higher current capacity

12.1 Cells in Series

n Identical Cells in Series
εeq = nε
req = nr

Current in external resistance R:

I = nε/(R + nr)
When to Use Series
  • When higher voltage is needed
  • When external resistance R >> internal resistance nr
  • Example: Flashlight (multiple batteries in series)

12.2 Cells in Parallel

n Identical Cells in Parallel
εeq = ε
req = r/n

Current in external resistance R:

I = ε/(R + r/n)
When to Use Parallel
  • When higher current is needed
  • When external resistance R << internal resistance r
  • To increase current capacity and battery life

13. Kirchhoff's Rules

Kirchhoff's Two Laws

KCL (Current Law):
At any junction: ΣIin = ΣIout
(Charge conservation)

KVL (Voltage Law):
In any closed loop: ΣV = 0
(Energy conservation)

Kirchhoff's laws are powerful tools for analyzing complex circuits that cannot be simplified using series-parallel combinations.

13.1 Kirchhoff's Current Law (KCL)

Junction Rule (KCL)

Statement: At any junction in a circuit, the sum of currents entering equals the sum of currents leaving.

ΣIin = ΣIout

Or equivalently (taking directions into account):

ΣI = 0

Basis: Conservation of electric charge (no accumulation at junction)

13.2 Kirchhoff's Voltage Law (KVL)

Loop Rule (KVL)

Statement: The algebraic sum of all potential differences in any closed loop is zero.

ΣV = 0

Or equivalently:

Σε = ΣIR

Basis: Conservation of energy (work done around closed path is zero)

13.3 Sign Conventions

Applying Kirchhoff's Laws

For KCL:

  • Current entering junction: positive
  • Current leaving junction: negative

For KVL (traversing loop):

  • Across resistor (direction of current): −IR (potential drops)
  • Across resistor (opposite to current): +IR (potential rises)
  • Across EMF (− to + terminal): +ε (potential rises)
  • Across EMF (+ to − terminal): −ε (potential drops)

14. Wheatstone Bridge

Wheatstone Bridge Circuit

A
/ \
/ \
R₁/ \R₂
/ \
B——R₅——C
\ /
R₃\ /R₄
\ /
\ /
D

R₅ = Galvanometer (detects current)
Balanced: No current through R₅

The Wheatstone bridge is a circuit used to measure unknown resistance with high accuracy.

14.1 Principle

Four resistances R₁, R₂, R₃, R₄ are arranged in a bridge configuration with a galvanometer G between points B and C.

Balanced Wheatstone Bridge

Condition for Balance: No current through galvanometer

R₁/R₂ = R₃/R₄

Or equivalently:

R₁R₄ = R₂R₃

14.2 Applications

  • Measuring unknown resistance: If three resistances known, fourth can be calculated
  • Strain gauges: Measuring small changes in resistance
  • Temperature sensors: Using thermistors in bridge circuit
  • Meter bridge: Practical implementation using uniform wire
Using Wheatstone Bridge

To find unknown resistance R₄:

  1. Connect known resistances R₁, R₂, R₃
  2. Adjust until galvanometer shows zero (balanced)
  3. Calculate: R₄ = R₂R₃/R₁
  4. Accuracy depends on sensitivity of galvanometer

Practice Questions

Multiple Choice Questions (20 MCQs)

Q1. SI unit of electric current is:

(a) Volt
(b) Ampere
(c) Ohm
(d) Watt

Answer: (b) Ampere
1 Ampere = 1 Coulomb/second (C/s)

Q2. Ohm's law is given by:

(a) V = I/R
(b) V = IR
(c) I = VR
(d) R = VI

Answer: (b) V = IR
Potential difference = Current × Resistance

Q3. Resistance of a conductor is proportional to:

(a) Length only
(b) Area only
(c) L/A
(d) A/L

Answer: (c) L/A
R = ρL/A, so R ∝ L/A

Q4. Drift velocity of electrons in conductor is typically:

(a) 10⁶ m/s
(b) 10³ m/s
(c) 10⁻⁴ m/s
(d) 3 × 10⁸ m/s

Answer: (c) 10⁻⁴ m/s
Very small compared to thermal velocity (10⁶ m/s)

Q5. Current I = neAvd. Here n represents:

(a) Number of electrons
(b) Free electron density
(c) Charge carrier mobility
(d) Relaxation time

Answer: (b) Free electron density
n = number of free electrons per unit volume

Q6. For metallic conductors, temperature coefficient α is:

(a) Positive
(b) Negative
(c) Zero
(d) Infinite

Answer: (a) Positive
Resistance increases with temperature in metals

Q7. Power dissipated in resistor P =:

(a) VI
(b) I²R
(c) V²/R
(d) All of these

Answer: (d) All of these
All three forms are equivalent: P = VI = I²R = V²/R

Q8. 1 kWh equals:

(a) 3.6 × 10³ J
(b) 3.6 × 10⁶ J
(c) 3.6 × 10⁹ J
(d) 1000 J

Answer: (b) 3.6 × 10⁶ J
1 kWh = 1000 W × 3600 s = 3.6 × 10⁶ J

Q9. EMF of cell is:

(a) Always equal to terminal voltage
(b) Greater than terminal voltage when current flows
(c) Less than terminal voltage
(d) Independent of current

Answer: (b) Greater than terminal voltage when current flows
V = ε − Ir, so ε > V when I ≠ 0

Q10. Internal resistance of ideal cell is:

(a) Zero
(b) Infinite
(c) 1 Ω
(d) Depends on EMF

Answer: (a) Zero
Ideal cell has zero internal resistance (r = 0)

Q11. n identical cells in series have equivalent EMF:

(a) ε
(b) nε
(c) ε/n
(d) n²ε

Answer: (b) nε
EMFs add in series combination

Q12. n identical cells in parallel have equivalent internal resistance:

(a) nr
(b) r
(c) r/n
(d) n²r

Answer: (c) r/n
Internal resistances in parallel: req = r/n

Q13. Kirchhoff's current law is based on conservation of:

(a) Energy
(b) Charge
(c) Momentum
(d) Power

Answer: (b) Charge
KCL: ΣIin = ΣIout (charge conservation)

Q14. Kirchhoff's voltage law is based on conservation of:

(a) Energy
(b) Charge
(c) Current
(d) Resistance

Answer: (a) Energy
KVL: ΣV = 0 around closed loop (energy conservation)

Q15. In balanced Wheatstone bridge:

(a) R₁ = R₂ = R₃ = R₄
(b) R₁/R₂ = R₃/R₄
(c) R₁R₂ = R₃R₄
(d) R₁ + R₂ = R₃ + R₄

Answer: (b) R₁/R₂ = R₃/R₄
Balanced condition for Wheatstone bridge

Q16. Best conductor among these is:

(a) Copper
(b) Silver
(c) Aluminum
(d) Iron

Answer: (b) Silver
Lowest resistivity (1.6 × 10⁻⁸ Ω·m)

Q17. Resistivity of semiconductors with temperature:

(a) Increases
(b) Decreases
(c) Remains constant
(d) First increases then decreases

Answer: (b) Decreases
More charge carriers at higher temperature

Q18. Mobility of charge carrier is:

(a) vd × E
(b) vd/E
(c) E/vd
(d) vd + E

Answer: (b) vd/E
μ = drift velocity per unit electric field

Q19. Which device does NOT obey Ohm's law?

(a) Copper wire
(b) Carbon resistor
(c) Semiconductor diode
(d) Nichrome wire

Answer: (c) Semiconductor diode
Non-linear V-I characteristic (non-ohmic)

Q20. Unit of resistivity is:

(a) Ω
(b) Ω·m
(c) Ω/m
(d) m/Ω

Answer: (b) Ω·m
From R = ρL/A, ρ has unit Ω·m

Formula Sheet

Concept Formula Unit
Current I = Q/t = dQ/dt A (Ampere)
Ohm's Law V = IR V, A, Ω
Resistance R = ρL/A Ω (Ohm)
Current (drift) I = neAvd A
Drift velocity vd = eEτ/me m/s
Mobility μ = vd/E = eτ/me m²/(V·s)
Resistivity (T) ρT = ρ₀[1 + α(T − T₀)] Ω·m
Power P = VI = I²R = V²/R W (Watt)
Energy W = Pt = VIt J (Joule)
Terminal voltage V = ε − Ir V
Cells in series εeq = nε, req = nr V, Ω
Cells in parallel εeq = ε, req = r/n V, Ω
KCL ΣIin = ΣIout A
KVL ΣV = 0 (closed loop) V
Wheatstone bridge R₁/R₂ = R₃/R₄ Dimensionless
Chapter Connections

Previous Chapter: Chapter 2 - Electrostatic Potential and Capacitance (Potential, energy, capacitors)

Current Chapter: Chapter 3 - Current Electricity (Current, resistance, circuits, Kirchhoff's laws)

Next Chapter: Chapter 4 - Moving Charges and Magnetism (Magnetic effects of current)

Current electricity bridges static charges (Ch 1-2) with magnetic effects (Ch 4) and forms the foundation for understanding all electrical circuits and devices.

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