Microscopic properties of electrical resistance

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SUMMARY

The discussion centers on the microscopic properties that dictate electrical resistance, specifically focusing on the equation for resistivity: ρ = 2m/qNτ. Here, τ represents the time between electron collisions, while q is the electron charge, N is the number of free electrons, and m is the electron mass. Key factors influencing τ include material density, impurity concentration, and temperature, which affect scattering rates. The discussion references a paper by Valla et al. that details these influences on scattering in fermi liquid metals.

PREREQUISITES
  • Understanding of electrical resistivity and its equation
  • Knowledge of electron properties, including charge and mass
  • Familiarity with scattering mechanisms in materials
  • Basic concepts of quantum mechanics related to charge transport
NEXT STEPS
  • Read the paper by Valla et al. on scattering rates in fermi liquid metals
  • Explore the relationship between material density and electron collision time
  • Investigate the effects of temperature on electrical resistance
  • Study the impact of impurities and defects on charge transport
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Researchers, physicists, and materials scientists interested in the fundamental properties of electrical resistance and its microscopic determinants.

Jimmy87
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I have recently been learning about the microscope properties which dictates electrical resistance. The main equation (resistivity) in my textbook is:

\rho = 2m/qN\tau where \tau is the time between collisions of electrons with the atoms, q is the charge of the electron, N is the number of free electrons and m is the mass of the electron.

These properties are fixed for a given material. I am quite comfortable with why certain materials have more free electrons than others. But I was wondering if anyone knows what determines the time between collisions for a resistor (\tau). Say if a certain material has less time between collisions then what is it about the material that determines this? Is it to do with the density of the material, so a more dense material has more atoms per unit volume so there would be less time between collisions?

Thanks for any help
 
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The theory is much more involved because due to the quantum mechanical behaviour, scattering in an ideal lattice does not lead to resistivity. It is mostly scattering from impurities and defects, and, in very pure samples, also from phonons, i.e. fluctuations from the ideal positions of the ions. So the scattering time depends on concentration of impurities and on temperature.
 
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Jimmy87 said:
I have recently been learning about the microscope properties which dictates electrical resistance. The main equation (resistivity) in my textbook is:

\rho = 2m/qN\tau where \tau is the time between collisions of electrons with the atoms, q is the charge of the electron, N is the number of free electrons and m is the mass of the electron.

These properties are fixed for a given material. I am quite comfortable with why certain materials have more free electrons than others. But I was wondering if anyone knows what determines the time between collisions for a resistor (\tau). Say if a certain material has less time between collisions then what is it about the material that determines this? Is it to do with the density of the material, so a more dense material has more atoms per unit volume so there would be less time between collisions?

Thanks for any help

I recommend you read this paper by Valla et al.

http://arxiv.org/abs/cond-mat/9904449

On the top of page 2, they wrote down all the factors that influences the scattering rate, which is the inverse of the collision time. You will see the type of scattering in a typical fermi liquid metal that can influence charge transport.

Zz.
 
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