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A.C.Bridges
By :-
Ranjal Agrawal (0105EC131087)
EC 3rd Sem.
 A.C.Bridges are those circuits which are
used to measured the unknown resistances,
capacitance and inductance.
Maxwell’s inductance Bridge
 In the Maxwell’s inductance bridge ,there
are two pure resistances used for balance
relations but on other side or arms the two
known impedances are used.
 The known impedances and the resistances
make the unknown impedances as Z1 and
Z2.Such a network is known as Maxwell’s
A.C.. Bridge. As shown in fig.
Fig.
(R1 + jwL1 )R3 = (R4 + jwL4 )R2
Maxwell’s Capacitance Bridge
 In the Maxwell’s capacitance Bridge the
positive phase angle of the inductance may
be compensated by the negative phase
angle of the capacitance impedance put in
the opposite arm.
 The unknown inductance then becomes
known in terms of the capacitance. As
shown in fig.
Fig.
R2 R4 + jwL1 R2 = R1 R3 + jwCR1 R2 R3
Anderson Bridge
 In the Anderson Bridge the unknown
inductance is measured in terms of a known
capacitance and resistance.
 This method is capable of precise measurements
of inductance over a wide range of values from
a few micro-henrys to several henrys and is the
best bridge method.
Hay’s Bridge
 It is also a modification of the Maxwell’s Wien
Bridge and is particularly useful if the phase
angle of the inductive impedance is large.
 In this case a comparatively smaller series
resistance R1 is used instead of a parallel
résistance.( which has to be of a very large
value) as shown in fig.
Fig
L3= C1 R2 R4 R3= w C1 R1 R2 R4
1+w R1 C1 1+w R1 C1
Schering Bridge
 Schering bridge used for the measurement
of capacitance and dielectric loss of a
capacitor.
 It is a device for comparing an imperfect
capacitor C2 in terms of a loss-free
standard capacitor C1. As shown in fig.
Fig.
C3 = C2 ( R1 / R2 ) R3 = R2 ( C1 / C2 )
Wien Series Bridge
 It is a simple ratio bridge and is used for
audio-frequency measurement of
capacitance over a wide range. As shown
in fig.
Fig.
R1=R2R4/R3 C1=C4(R3/R2)
Wien Parallel Bridge
 It is also a ratio bridge used mainly as the
feedback network in the wide range audio-
frequency R-C oscillators.
 It is may be used for the measurement of
the audio-frequency but it is not as
accurate as the modern digital frequency
meters. As shown in fig.
Fig.
C2 = R2 = R3
C1 R1 R4
THANK YOU

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Ac bridges

  • 1. A.C.Bridges By :- Ranjal Agrawal (0105EC131087) EC 3rd Sem.
  • 2.  A.C.Bridges are those circuits which are used to measured the unknown resistances, capacitance and inductance.
  • 3. Maxwell’s inductance Bridge  In the Maxwell’s inductance bridge ,there are two pure resistances used for balance relations but on other side or arms the two known impedances are used.  The known impedances and the resistances make the unknown impedances as Z1 and Z2.Such a network is known as Maxwell’s A.C.. Bridge. As shown in fig.
  • 4. Fig. (R1 + jwL1 )R3 = (R4 + jwL4 )R2
  • 5. Maxwell’s Capacitance Bridge  In the Maxwell’s capacitance Bridge the positive phase angle of the inductance may be compensated by the negative phase angle of the capacitance impedance put in the opposite arm.  The unknown inductance then becomes known in terms of the capacitance. As shown in fig.
  • 6. Fig. R2 R4 + jwL1 R2 = R1 R3 + jwCR1 R2 R3
  • 7. Anderson Bridge  In the Anderson Bridge the unknown inductance is measured in terms of a known capacitance and resistance.  This method is capable of precise measurements of inductance over a wide range of values from a few micro-henrys to several henrys and is the best bridge method.
  • 8.
  • 9. Hay’s Bridge  It is also a modification of the Maxwell’s Wien Bridge and is particularly useful if the phase angle of the inductive impedance is large.  In this case a comparatively smaller series resistance R1 is used instead of a parallel résistance.( which has to be of a very large value) as shown in fig.
  • 10. Fig L3= C1 R2 R4 R3= w C1 R1 R2 R4 1+w R1 C1 1+w R1 C1
  • 11. Schering Bridge  Schering bridge used for the measurement of capacitance and dielectric loss of a capacitor.  It is a device for comparing an imperfect capacitor C2 in terms of a loss-free standard capacitor C1. As shown in fig.
  • 12. Fig. C3 = C2 ( R1 / R2 ) R3 = R2 ( C1 / C2 )
  • 13. Wien Series Bridge  It is a simple ratio bridge and is used for audio-frequency measurement of capacitance over a wide range. As shown in fig.
  • 15. Wien Parallel Bridge  It is also a ratio bridge used mainly as the feedback network in the wide range audio- frequency R-C oscillators.  It is may be used for the measurement of the audio-frequency but it is not as accurate as the modern digital frequency meters. As shown in fig.
  • 16. Fig. C2 = R2 = R3 C1 R1 R4