ELECTRICAL CONDUCTIVITY OF METALS

Electrical Conductivity in Metals

  • Drift velocity (Vd): Defined as the average velocity that a particle (electrons, in the case of metals) attains due to an electric field.

  • Thermal velocity (uav): The average velocity due to thermal energy, which is a more rapid movement of free electrons before any electric field is applied.

  • Mean free path (l): Refers to the average distance a particle travels between collisions.


Quantitative Relationships

  • Current density (J):

    • Represents the current per unit area flowing through a conductor.

    • Defined as: J=racdQdAimesdtJ = rac{dQ}{dA imes dt}

    • Average drift velocity: Vd=rac1Nimes(V<em>x1+V</em>x2++VxN)Vd = rac{1}{N} imes (V<em>{x1} + V</em>{x2} + … + V_{xN})

    • Time dependent current is indicated with the average drift represented in terms of time and electric field.


Drift Velocity Calculations

  • Formula for drift velocity under a varying electric field:

    • Vdx=rac1Nimes[U<em>x1+U</em>x2++UxN]Vdx = rac{1}{N} imes [U<em>{x1} + U</em>{x2} + … + U_{xN}]

    • Drift mobility expression:

    • U<em>dx=racauˉE</em>xmeU<em>{dx} = rac{\bar{ au} E</em>x}{m_e}

    • Drift current density: J<em>x=enUˉE</em>xJ<em>x = en\bar{U} E</em>x

    • Electric field (E): A factor affecting drift velocity.


Electron Drift Mobility in Metals

  • Example Calculation:

    • Given parameters:

    • Conductivity of copper (extsˉ=5.9imes105extScm1\bar{ ext{s}} = 5.9 imes 10^5 ext{ S cm}^{-1})

    • Density (ρCu=8.96extgcm3ρ_{Cu} = 8.96 ext{ g cm}^{-3})

    • Atomic mass (Mat=63.5extgmol1M_{at} = 63.5 ext{ g mol}^{-1})

    • Performing Calculations:

    • Number density of conduction electrons:

      • n=racρ<em>CuimesN</em>AMatn = rac{ρ<em>{Cu} imes N</em>A}{M_{at}}

      • Result: n=8.5imes1022extelectronscm3n = 8.5 imes 10^{22} ext{ electrons cm}^{-3}

  • Drift Mobility Calculation:

    • ildeμˉd=raceimesnsˉ\bar{ ilde{μ}}_d = rac{e imes n}{\bar{s}}

    • ildeμˉd=rac5.9imes105extScm1eimesn\bar{ ilde{μ}}_d = rac{5.9 imes 10^5 ext{ S cm}^{-1}}{e imes n}

    • Computed mobility: ildeμˉd=43.4extcm2extV1exts1\bar{ ilde{μ}}_d = 43.4 ext{ cm}^2 ext{ V}^{-1} ext{ s}^{-1}


Relaxation Time and Mean Free Path

  • Mean free path (λ):

    • Formulated as: λ=uˉimestˉλ = \bar{u} imes \bar{t}

    • Where uˉ\bar{u} is average velocity and tˉ\bar{t} is average time between collisions.

  • Relaxation time (τ):

    • Represents the average time interval between collisions:

    • τ=racMdenτ = rac{M_d}{en}

    • This is crucial in understanding conductivity and mobility.


Drift Velocity and Mean Speed

  • Calculating applied electric field for a given drift velocity:

    • Required conditions: Drift velocity of electrons to equal 0.1% of their mean speed (uextapproximately106extms1u ext{ approximately } 10^6 ext{ m s}^{-1})

    • So, Vdx=103extms1Vdx = 10^3 ext{ m s}^{-1}

    • Applied electric field: Ex=rac2.3imes105extVm143.4imes104extm2extV1exts1E_x = rac{2.3 imes 10^5 ext{ V m}^{-1}}{43.4 imes 10^{-4} ext{ m}^2 ext{ V}^{-1} ext{ s}^{-1}}

  • Current Density Calculation:

    • J<em>x=σE</em>x=(5.9imes107extSm1)(2.3imes105extVm1)J<em>x = σ E</em>x = (5.9 imes 10^7 ext{ S m}^{-1})(2.3 imes 10^5 ext{ V m}^{-1})

    • Resulting current density: 1.4imes1013extAm21.4 imes 10^{13} ext{ A m}^{-2}

    • Converted: 1.4imes107extAmm21.4 imes 10^{7} ext{ A mm}^{-2}


Temperature Dependence of Resistivity

  • Causes:

    • Scattering due to thermal vibrations of atoms.

    • Increased temperature increases average electron velocity and atomic vibrations (1)

  • Mean free path under varying temperatures:

    • S=racЬΥimesAS = rac{Ь}{Υ} imes A

    • Where N represents concentration; for a scattering center: SimesUimesTN=1S imes U imes T_{N} = 1


Thermal Vibrations and Scattering

  • Average kinetic energy of oscillating atoms:

    • Boltzmann approximation: rac12Ma2ω2extapproximatelyequalsrac32kTrac{1}{2} M a^2 ω^2 ext{ approximately equals } rac{3}{2} kT

    • This links energy associated with thermal vibration to resistivity.

  • Lattice scattering-limited conductivity: Occurs due to electron scattering via thermal vibrations of lattice atoms.


Resistance Change with Temperature

  • Resistance formula:

    • Rρ=ATR ∝ ρ = A T

  • Example scenario: Resistance change calculation from summer 20°C20° C to winter 30°C-30° C:

    • racR<em>summerR</em>winterR<em>summer=racT</em>summerT<em>winterT</em>summerrac{R<em>{summer} - R</em>{winter}}{R<em>{summer}} = rac{T</em>{summer} - T<em>{winter}}{T</em>{summer}}

    • Result: 0.171 ext{ or } 17 ext{%}


Drift Mobility Estimates Under Conditions

  • Estimating drift mobility using fundamental physical constants and density of copper:

    • Drift mobility equation in use:

    • σ=enμˉdσ = e n \bar{μ}_d

  • Calculating mean speed and other parameters:

    • S=rac2πkTextAtmosphericpressureS = rac{2πkT}{ ext{Atmospheric pressure}}


Matthiessen's Rule for Resistivity and Temperature Coefficient

  • Conception of Matthiessen's Rule:

    • This principle states that the total resistivity (ρρ) is the sum of intrinsic resistivity due to perfect lattice + additional resistivity due to impurities.

  • Temperature coefficient of resistivity (α):

    • Defined as the fractional change in resistivity per unit temperature increase: racΔρρ0ΔTrac{Δρ}{ρ_0ΔT}

    • Where $ρ0$ is the resistivity at a reference temperature $T0$.

  • Apply this concept in determining how resistivity varies with temperature, indicating both temperature independent constants A & B.