Shortcut Methods

Shortcut Methods and Tricks

1. Temperature Dependence of Resistivity

  • Remember the approximate value of the temperature coefficient of resistivity for copper: 0.0039/°C.
  • For small temperature changes, the change in resistivity can be approximated as:

Δρ=ρ0αΔT where:

  • Δρ is the change in resistivity
  • ρ0 is the resistivity at the reference temperature
  • α is the temperature coefficient of resistivity
  • ΔT is the change in temperature.

2. Mobility and Resistivity

  • The mobility of charge carriers is inversely proportional to their mass.
  • The resistivity of a material is inversely related to the mobility of its charge carriers. This means that a material with high mobility will have a low resistivity, and vice versa.

Sample Problems

1. Temperature Dependence of Resistivity

A copper wire has a resistance of 1 Ω at 25°C. What will its resistance be at 50°C?

Solution:

Using the formula for the change in resistivity:

ΔR=R0α(T2T1)

where R0=1 Ω, α=0.0039/°C, T1=25 °C, and T2=50 °C

Substituting these values into the equation, we get:

ΔR=1Ω0.0039/°C(50°C25°C)=0.0975Ω

Therefore, the resistance of the copper wire at 50°C will be:

R=R0+ΔR=1Ω+0.0975Ω=1.0975Ω

2. Mobility and Resistivity

A semiconductor material has a mobility of 0.1 m^2/V-s and a resistivity of 10^-3 ohm-m. What is the concentration of charge carriers in the material?

Solution:

The conductivity of the material can be calculated using the formula:

σ=neμ

where:

  • σ is the conductivity in S/m
  • n is the concentration of charge carriers in m^-3
  • e is the elementary charge in coulombs
  • μ is the mobility in m^2/V-s

Substituting the given values into the equation, we get:

103S/m=n×1.602×1019C×0.1m2/Vs n=103S/m1.602×1019C×0.1m2/Vs=6.24×1015m3

Therefore, the concentration of charge carriers in the semiconductor material is 6.24 x 10^15 m^-3.



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