MAXWELL’S INDUCTANCE
      BRIDGE
INTRODUCTION
 Different types of AC Bridges can
    be used for measurement of either
    inductance or capacitance. We can
    measure unknown inductance by
    using MAXWELL’S INDUCTANCE
    BRIDGE.
   CONSTRUCTION:
   There are four different arms in
    which:
   First arm of the bridge contains
    series combination of resistance
    and inductance.
   Third arm consists of series
    combination of variable resistance
    and variable inductance.
   Second and fourth arm consists of
    resistances respectively.
WORKING OF THE BRIDGE


  • This coil is connected to AC supply when
    alternating current flows through the coil
    according to magnetic effect , it produces
    magnetic flux lines.

  • When these magnetic flux lines are cut by coil1
    then according to FARADAY’s LAW of
    ELECTROMAGNETIC INDUCTION emf is
    induced in coil1.This emf is called as SELF
    INDUCED emf ,denoted by E1.

  • Mathematically E1=-L1(di/dt),where L is called as
    ‘SELF INDUCTANCE OF COIL’.
WORKING OF BRIDGE (CONTINUED)

     • Similarly in this figure there are 2 different coils in which
       coil1 is connected to AC supply and coil2 gets open.

     • When AC supply is given then according to the magnetic
       effect, magnetic flux lines are produced but some of the
       magnetic lines cut by coil2and all the magnetic lines cut by
       coil1.

     • Hence according to FARADAY’S LAW emf will be induced
       in both the coils.
     •
     • The emf induced in coil1 is called as SELF INDUCED EMF
       and the emf induced in coil2 is called as MUTUALLY
       INDUCED EMF.

     • Using MAXWELL’S INDUCTANCE BRIDGE we can
       measure only SELF INDUCTANCE of coil1.
DERIVATION

       In adjacent figure ,
        parameters L1 and R1 are
        unknown parameters.
       By using MAXWELL’S
        INDUCTANCE BRIDGE
        we have to find out these
        parameters
DERIVATION
The mathematical balancing
condition of AC bridge is:

     Z1.Z4=Z2.Z3
-----(1)
Where,

Z1=(R1+jωL1)
Z2=R2
Z3=(R3+jωL3+r3)
Z4=R4
Substitute the values in eq.(1)
      R1R4+jωL1R4=
R2(R3+r3)+jωL3R2
FINAL EQUATION

 Real part---     R1R4=R2(R3+r3)
 Imaginary part---L1R4=L3R2





From these equations :
The above 2 equations are FREE FROM FREQUENCY ie the values of
unknown resistance and unknown inductance does not depend upon the
frequency of supply. So that ANY TYPE OF DETECTOR can be used
PHASOR DIAGRAM

Maxwell’s induction bridge

  • 1.
  • 2.
    INTRODUCTION  Different typesof AC Bridges can be used for measurement of either inductance or capacitance. We can measure unknown inductance by using MAXWELL’S INDUCTANCE BRIDGE.  CONSTRUCTION:  There are four different arms in which:  First arm of the bridge contains series combination of resistance and inductance.  Third arm consists of series combination of variable resistance and variable inductance.  Second and fourth arm consists of resistances respectively.
  • 3.
    WORKING OF THEBRIDGE • This coil is connected to AC supply when alternating current flows through the coil according to magnetic effect , it produces magnetic flux lines. • When these magnetic flux lines are cut by coil1 then according to FARADAY’s LAW of ELECTROMAGNETIC INDUCTION emf is induced in coil1.This emf is called as SELF INDUCED emf ,denoted by E1. • Mathematically E1=-L1(di/dt),where L is called as ‘SELF INDUCTANCE OF COIL’.
  • 4.
    WORKING OF BRIDGE(CONTINUED) • Similarly in this figure there are 2 different coils in which coil1 is connected to AC supply and coil2 gets open. • When AC supply is given then according to the magnetic effect, magnetic flux lines are produced but some of the magnetic lines cut by coil2and all the magnetic lines cut by coil1. • Hence according to FARADAY’S LAW emf will be induced in both the coils. • • The emf induced in coil1 is called as SELF INDUCED EMF and the emf induced in coil2 is called as MUTUALLY INDUCED EMF. • Using MAXWELL’S INDUCTANCE BRIDGE we can measure only SELF INDUCTANCE of coil1.
  • 5.
    DERIVATION  In adjacent figure , parameters L1 and R1 are unknown parameters.  By using MAXWELL’S INDUCTANCE BRIDGE we have to find out these parameters
  • 6.
    DERIVATION The mathematical balancing conditionof AC bridge is: Z1.Z4=Z2.Z3 -----(1) Where, Z1=(R1+jωL1) Z2=R2 Z3=(R3+jωL3+r3) Z4=R4 Substitute the values in eq.(1) R1R4+jωL1R4= R2(R3+r3)+jωL3R2
  • 7.
    FINAL EQUATION  Realpart--- R1R4=R2(R3+r3)  Imaginary part---L1R4=L3R2  From these equations : The above 2 equations are FREE FROM FREQUENCY ie the values of unknown resistance and unknown inductance does not depend upon the frequency of supply. So that ANY TYPE OF DETECTOR can be used
  • 8.