Electrical Mobility Calculator

Calculate charge carrier mobility, drift velocity, conductivity, diffusion coefficient, and relaxation time in semiconductors and conductors.

Drift Velocity
1,400 cm/s
Average velocity of carriers in the applied field
Electrical Conductivity
2.243e+2 S/m
σ = n·q·μ
Resistivity
4.459e-3 Ω·m
ρ = 1/σ
Diffusion Coefficient
3.621e-3 m²/s
From Einstein relation: D = μ·kT/q
Relaxation Time
8.597e-13 s
Mean time between carrier scattering events
Thermal Velocity
112,401 m/s
RMS thermal speed of carriers
Mean Free Path
9.663e-8 m
Average distance between scattering events

Mobility vs Temperature

100 K
7,275
150 K
3,960
200 K
2,572
250 K
1,840
300 K
1,400
350 K
1,111
400 K
909

Temperature Dependence Table

Temp (K)Mobility (cm²/V·s)Conductivity (S/m)
1007,2751.165e+3
1503,9606.344e+2
2002,5724.120e+2
2501,8402.948e+2
3001,4002.243e+2
3501,1111.780e+2
4009091.457e+2
4507621.221e+2
5006511.042e+2
Planning notes, formulas, and examples

About the Electrical Mobility Calculator

The electrical mobility calculator determines the transport properties of charge carriers in semiconductors and conductors. Carrier mobility (μ) is a fundamental material parameter that quantifies how quickly electrons or holes move through a material under an applied electric field, directly determining device performance in transistors, solar cells, and LEDs.

Mobility connects microscopic scattering physics to macroscopic electrical properties through the relationships: drift velocity v_d = μE, conductivity σ = nqμ, and the Einstein relation D = μkT/q. Higher mobility means carriers travel faster under the same field, enabling faster switching in transistors and higher current in power devices. Silicon has electron mobility of ~1400 cm²/V·s, while GaAs reaches ~8500 cm²/V·s, which is why GaAs excels in high-frequency applications.

This calculator computes drift velocity, conductivity, resistivity, diffusion coefficient, relaxation time, thermal velocity, and mean free path from the mobility and operating conditions. It also models the temperature dependence of mobility, which typically follows a T^(-3/2) power law for phonon-limited scattering in pure semiconductors.

When This Page Helps

Carrier mobility matters whenever you need to estimate how fast charge carriers will drift, how conductive a material will be, or how strongly temperature will affect transport. Students use it to connect the mobility equation to drift velocity and diffusion, while engineers use it to compare semiconductor materials and operating conditions.

This calculator is most useful when you want to turn a mobility value into the transport quantities that actually show up in devices and measurements.

How to Use the Inputs

  1. Enter the carrier mobility in cm²/V·s (standard semiconductor unit)
  2. Enter the applied electric field in V/cm
  3. Select the carrier type: electrons or holes
  4. Enter the operating temperature in Kelvin
  5. Enter the carrier concentration in cm⁻³
  6. Enter the effective mass ratio for the carrier type
  7. Review drift velocity, conductivity, diffusion, and scattering parameters
Formula used
Drift velocity: v_d = μ·E. Conductivity: σ = n·q·μ. Einstein relation: D = μ·kT/q. Relaxation time: τ = m*·μ/q. Thermal velocity: v_th = √(3kT/m*). Mean free path: λ = v_th · τ. Temperature dependence (lattice scattering): μ ∝ T^(−3/2).

Example Calculation

Result: Drift velocity: 1.4 × 10⁵ cm/s, σ = 0.224 S/m

Silicon electron mobility of 1400 cm²/V·s at 100 V/cm gives v_d = 1400 × 100 = 140,000 cm/s. With n = 10¹⁶ cm⁻³: σ = 10¹⁶ × 10⁶ × 1.6×10⁻¹⁹ × 1400 × 10⁻⁴ ≈ 0.224 S/m.

Tips & Best Practices

  • Use presets to explore mobility values for common semiconductors
  • At high fields (> 10⁴ V/cm in Si), velocity saturation limits the drift speed — this calculator uses the low-field linear model
  • Hole mobility is typically 2–3× lower than electron mobility in the same material
  • For heavily doped samples, use measured mobility values rather than intrinsic values
  • The T^(-3/2) temperature dependence is approximate — real materials show deviations due to multiple scattering mechanisms

Mobility and Transport

Mobility connects the microscopic scattering behavior of a semiconductor to the drift velocity you observe in an electric field. It also determines conductivity, diffusion, and relaxation time through a small set of related equations.

Temperature and Doping

Carrier mobility usually falls as temperature rises because phonon scattering increases. Heavy doping can also reduce mobility by adding impurity scattering. That is why measured values often matter more than textbook values when the material is heavily processed.

Practical Use

Use this calculator when you need a quick transport estimate for device design, material comparison, or a lab report that ties mobility to a measurable electrical response.

Sources & Methodology

Last updated:

Frequently Asked Questions

  • Mobility is limited by scattering mechanisms: lattice vibrations (phonons), ionized impurities, grain boundaries, and defects. In pure semiconductors at room temperature, phonon scattering dominates.