The correct option is
C an R and C in parallel
Given, Bridge balance is obtained.
Voltage source is of fixed frequency.
Now at balance,
R1R2=(R3+jωL3)Z
To obtain bridge balance z should be capacitive in nature.
Case.I. z = R and C in series
⇒ z=R+1jωC
⇒ R1R2=(R3+jωL3)(R+1jωC)
⇒ R1R2=R3R+L3R ...(i)
and 0=j[ωL3R−R3ωC]
⇒ ωL3R=R3ωC ...(ii)
To obtain bridge balance we need to select
R3 and L3 as variable as source frequency is fixed. Since
R3 and L3 term is present in both equations i.e., (i) and (ii), so obtaining bridge balance is difficult.
Case.II. z = R and C in parallel
⇒ R1R2=(R3+jωL3)(RjωCR+1)
⇒ R1R2+jωCRR1R2=R3R+jωL3R
⇒ R1R2=R3R
⇒ R=R3R1R2 ...(iii)
and ωCR1R1R2=ωL3R
⇒ C=L3R1R2 ...(iv)
To obtain bridge balance we will select
R3 and L3 as variable. So, we will vary
R3 only for R and vary
L3 only for C.
Out of both cases I and II, bridge balance can be obtained but this bridge is seldon used for case I as bridge balance will be difficult.