ELECTRICAL ENGINEERING
MATERIALS: CONDUCTING &
SUPERCONDUCTING MATERIALS
MR. ASIF L. JAMADAR
RELAXATION TIME, COLLISION TIME, FERMI ENERGY & MEAN
FREE PATH
 Relaxation Time
 Mean Free Path
 Collision are caused by thermal or
structure imperfection in lattice
Vx is not equal to zero
 At any instant the velocity is given by,
2
 The rate of change of velocity due to collision becomes
 The fractional force due to collision may be expressed as,
 The modified equation of electrons become
 In the absence of the external forces (-eE), the free motion satisfies,
 If is the initial drift velocity in non-equilibrium distribution then the
approach to equilibrium can be described by the solution of above equation,
 Consider relation of collision time of an electron with its probability of collision.
 Let dt/τc be the probability of an electron collide with lattice during short time dt
 We can write,
 From probability theory,
 In terms of dt/τc we have,
 From above equations,
 By comparing first & last equation,
 By integrating the above eaquation for R(t)=1 at t=0 then,
 The probability that collision occurs before time (t + dt)
 The probability that collision occurs before time t
 Therefore the probability that collision occurs during time dt, between time t &
(t + dt) is,
 Keeping the above equation in view, the average time that elapses between
collision may be written as
 We know,
 By substituting the above equation and solving the integral, we get,
 For isotropy material, the mean time of collision is same as the relaxation time
that is,
τc = τr
 The mean path of an electron ( λ ) is defined as
 WF is the Fermi level of electrons (Fermi Energy)
 At any temperature T, the probability of a state corresponding to an energy W
being occupied by an electron is given by
 The velocity of an electron with Fermi energy ( VF) is given by,
 So Mean Free Path is
 The magnitude of WF is of the order of several electron volts.
THANK
YOU
8

Electrical Engineering Material Part-XV

  • 1.
    ELECTRICAL ENGINEERING MATERIALS: CONDUCTING& SUPERCONDUCTING MATERIALS MR. ASIF L. JAMADAR
  • 2.
    RELAXATION TIME, COLLISIONTIME, FERMI ENERGY & MEAN FREE PATH  Relaxation Time  Mean Free Path  Collision are caused by thermal or structure imperfection in lattice Vx is not equal to zero  At any instant the velocity is given by, 2
  • 3.
     The rateof change of velocity due to collision becomes  The fractional force due to collision may be expressed as,  The modified equation of electrons become  In the absence of the external forces (-eE), the free motion satisfies,  If is the initial drift velocity in non-equilibrium distribution then the approach to equilibrium can be described by the solution of above equation,
  • 4.
     Consider relationof collision time of an electron with its probability of collision.  Let dt/τc be the probability of an electron collide with lattice during short time dt  We can write,  From probability theory,  In terms of dt/τc we have,  From above equations,  By comparing first & last equation,
  • 5.
     By integratingthe above eaquation for R(t)=1 at t=0 then,  The probability that collision occurs before time (t + dt)  The probability that collision occurs before time t  Therefore the probability that collision occurs during time dt, between time t & (t + dt) is,  Keeping the above equation in view, the average time that elapses between collision may be written as
  • 6.
     We know, By substituting the above equation and solving the integral, we get,  For isotropy material, the mean time of collision is same as the relaxation time that is, τc = τr  The mean path of an electron ( λ ) is defined as  WF is the Fermi level of electrons (Fermi Energy)
  • 7.
     At anytemperature T, the probability of a state corresponding to an energy W being occupied by an electron is given by  The velocity of an electron with Fermi energy ( VF) is given by,  So Mean Free Path is  The magnitude of WF is of the order of several electron volts.
  • 8.