Current Electricity - Mobility of Charge Carriers
Complete formula sheet, derivations, concept explanations, diagrams and exam-focused practice for CBSE Class 12, NEET, JEE Main, JEE Advanced, Olympiad, AP Physics, IB Physics and A-Level Physics.
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1. Formula Sheet First
Mobility connects microscopic motion of charge carriers with the macroscopic current measured in a circuit.
μ = vd/EMobility definitionvd = μEDrift velocity in fieldI = nAqvdCurrent through area AJ = nqvdCurrent densityJ = nqμEUsing mobilityσ = nqμConductivityρ = 1/σResistivityvd = eEτ/mDrude modelμ = eτ/mMobility from relaxation timeρ = m/(ne²τ)Metal resistivityσe = neeμeElectron contributionσ = e(neμe + nhμh)Semiconductor conductivitySymbols
2. What Is Mobility of Charge Carriers?
Simple Definition
Mobility tells how easily a charge carrier can move through a material when an electric field is applied.
Formal Definition
Mobility is the drift velocity acquired by a charge carrier per unit electric field: μ = vd/E.
Physical Meaning
High mobility means carriers gain larger drift velocity for the same electric field because collisions are less restrictive.
Importance
Mobility controls current density, conductivity, semiconductor speed, device performance and temperature behaviour.
3. Derivation of Mobility
Collisions with lattice ions, impurities and phonons disturb the accelerated motion. A larger relaxation time means fewer collisions and hence larger mobility.
4. Mobility of Electrons
Electron mobility is μe = vd,e/E. Electrons are negatively charged, so their drift is opposite to the applied electric field. Conventional current is in the direction of positive charge flow, therefore it is opposite to electron drift.
5. Mobility of Holes
A hole is the absence of an electron in a nearly filled valence band. It behaves like a positive charge carrier. Hole mobility is μh = vd,h/E. Holes drift in the direction of electric field and contribute to conventional current.
6. Electron Mobility vs Hole Mobility
| Point | Electron | Hole |
|---|---|---|
| Charge carrier | Actual electron | Vacancy acting as positive carrier |
| Direction of motion | Opposite to electric field | Along electric field |
| Charge | -e | +e |
| Mobility | Usually greater | Usually smaller |
| Role in current | Dominant in metals and n-type semiconductors | Important in p-type semiconductors |
| Metals | Primary carriers | Not used in simple metal conduction |
| Intrinsic semiconductor | Contributes with holes | Contributes with electrons |
| Extrinsic semiconductor | Majority in n-type | Majority in p-type |
| NEET/JEE importance | Direction, formula, conductivity | Semiconductor conductivity and comparison |
Electron mobility is usually greater because electrons often move in bands with smaller effective mass and less restrictive hopping compared with holes in the valence band.
7. Mobility in Metallic Conductors
Metals contain many free electrons moving among fixed lattice ions. In an electric field, electrons accelerate but repeatedly collide with ions, impurities and phonons. The average time between collisions is relaxation time τ.
When temperature increases in metals, lattice vibrations increase, relaxation time decreases, mobility decreases, resistance increases and conductivity decreases.
8. Mobility in Semiconductors
In intrinsic semiconductors, electrons and holes are thermally generated in equal numbers. In n-type semiconductors, electrons are majority carriers. In p-type semiconductors, holes are majority carriers.
9. Temperature Effect on Mobility
| Material | Temperature Increase Causes | Final Effect |
|---|---|---|
| Metals | Lattice vibrations increase, relaxation time decreases, mobility decreases. | Resistance increases and conductivity decreases. |
| Semiconductors | Mobility may decrease due to scattering, but carrier concentration increases strongly. | Conductivity increases and resistance decreases in usual intrinsic behaviour. |
10. Mobility, Conductivity and Resistivity
Example 1
If n = 8 × 10²⁸ m⁻³ and μ = 4 × 10⁻³ m²V⁻¹s⁻¹, then σ = neμ = 8×10²⁸ × 1.6×10⁻¹⁹ × 4×10⁻³ = 5.12×10⁷ S m⁻¹.
Example 2
If μ doubles while n remains constant, conductivity doubles and resistivity becomes half.
11. Mobility and Drift Velocity
The relation vd = μE means drift velocity is directly proportional to electric field for ohmic conditions. If voltage increases for fixed length, E = V/L increases and drift velocity increases. If length increases for fixed voltage, E decreases and drift velocity decreases. Area does not directly change vd for fixed E, but it changes current I = nAqvd. Temperature changes μ, so it indirectly changes vd.
12. Dimension and Unit of Mobility
18. Diagrams and Visuals
13-17. Exam Practice Bank With Accordion Solutions
Click any question to open the answer and explanation.
19. Common Student Mistakes
20. Exam Strategy
CBSE
Focus on definitions, derivations, units, dimensions and direct formula application.
NEET
Memorise formula links: μ, vd, J, σ, ρ and temperature effects.
JEE Main
Practise numerical chains combining E = V/L, vd = μE and I = nAqvd.
JEE Advanced
Handle multi-carrier conduction, graphs, varying field and semiconductor traps.
Olympiad
Build microscopic intuition: scattering, relaxation time, effective mass and model assumptions.
AP Physics
Connect microscopic current with circuit quantities and proportional reasoning.
IB Physics
Emphasise explanation quality, units, graph interpretation and uncertainty in models.
A-Level Physics
Practise drift velocity derivations, charge carrier density and resistivity links.
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