Current Electricity
विद्युत धारा | Class 12 Physics - Chapter 3 | NCERT + RBSE 2026
| Subject: | Physics |
| Class: | 12 (RBSE + NCERT) |
| Chapter: | 3 |
| Topic: | Current Electricity |
| Year: | 2025-26 |
| Status: | Complete & Verified |
• 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
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
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.
SI Unit: Ampere (A) = Coulomb/second (C/s)
Nature: Scalar quantity (has magnitude, but direction is conventional)
2.2 Direction of Current
- 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
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
where:
- vd = drift velocity
- e = electronic charge
- E = electric field
- τ = relaxation time (average time between collisions)
- me = mass of electron
- 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
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.
Or equivalently:
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.
where:
- R = resistance (Ω)
- ρ = resistivity of material (Ω·m)
- L = length of conductor (m)
- A = cross-sectional area (m²)
- 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.
SI Unit: Siemens (S) or mho (℧) = 1/Ω
5. Drift of Electrons and Origin of Resistivity
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
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
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
Unit: m²/(V·s)
Definition: Drift velocity acquired per unit electric field
- 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: 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:
- Semiconductors: Resistance depends on voltage/current
- Vacuum tubes: Non-linear V-I characteristics
- Diodes: Current flows in one direction only
- Electrolytes: Resistance changes with current
- At very high electric fields: Heating effects dominate
- 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
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 |
- 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
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
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
Battery does work on charges
↓
Charges flow through resistor
↓
Energy converted to heat (I²Rt)
↓
Power dissipated = VI = I²R = V²/R
10.1 Electrical Energy
SI Unit: Joule (J)
Practical Unit: kilowatt-hour (kWh)
1 kWh = 3.6 × 10⁶ J
10.2 Electrical Power
SI Unit: Watt (W) = Joule/second (J/s)
- 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
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)
Definition: Work done per unit charge by the cell in moving charge from negative to positive terminal through the cell.
SI Unit: Volt (V)
- 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.
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
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
Current in external resistance R:
- When higher voltage is needed
- When external resistance R >> internal resistance nr
- Example: Flashlight (multiple batteries in series)
12.2 Cells in Parallel
Current in external resistance R:
- When higher current is needed
- When external resistance R << internal resistance r
- To increase current capacity and battery life
13. Kirchhoff's Rules
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)
Statement: At any junction in a circuit, the sum of currents entering equals the sum of currents leaving.
Or equivalently (taking directions into account):
Basis: Conservation of electric charge (no accumulation at junction)
13.2 Kirchhoff's Voltage Law (KVL)
Statement: The algebraic sum of all potential differences in any closed loop is zero.
Or equivalently:
Basis: Conservation of energy (work done around closed path is zero)
13.3 Sign Conventions
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
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.
Condition for Balance: No current through galvanometer
Or equivalently:
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
To find unknown resistance R₄:
- Connect known resistances R₁, R₂, R₃
- Adjust until galvanometer shows zero (balanced)
- Calculate: R₄ = R₂R₃/R₁
- 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
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
Potential difference = Current × Resistance
Q3. Resistance of a conductor is proportional to:
(a) Length only
(b) Area only
(c) L/A
(d) A/L
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
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
n = number of free electrons per unit volume
Q6. For metallic conductors, temperature coefficient α is:
(a) Positive
(b) Negative
(c) Zero
(d) Infinite
Resistance increases with temperature in metals
Q7. Power dissipated in resistor P =:
(a) VI
(b) I²R
(c) V²/R
(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
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
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
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
EMFs add in series combination
Q12. n identical cells in parallel have equivalent internal resistance:
(a) nr
(b) r
(c) r/n
(d) n²r
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
KCL: ΣIin = ΣIout (charge conservation)
Q14. Kirchhoff's voltage law is based on conservation of:
(a) Energy
(b) Charge
(c) Current
(d) Resistance
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
Balanced condition for Wheatstone bridge
Q16. Best conductor among these is:
(a) Copper
(b) Silver
(c) Aluminum
(d) Iron
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
More charge carriers at higher temperature
Q18. Mobility of charge carrier is:
(a) vd × E
(b) vd/E
(c) E/vd
(d) 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
Non-linear V-I characteristic (non-ohmic)
Q20. Unit of resistivity is:
(a) Ω
(b) Ω·m
(c) Ω/m
(d) m/Ω
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 |
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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