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Murray loop test for cable faults

Short answer

The Murray loop test locates a cable fault by forming a Wheatstone bridge with a sound core and the faulty core linked at the far end. At balance, fault distance from test end is x = [Q/(P+Q)] × 2l, where l is cable length. Fault resistance in the battery arm does not affect the result.

Explain Murray Loop test for locating short circuit fault in underground cable.

The Murray loop test is a bridge (Wheatstone principle) method to locate a short-circuit or earth fault in an underground cable. It needs one sound core running alongside the faulty core.

Connections

  • At the far end, the faulty core and a sound core are joined by a low-resistance link, forming a loop.
  • At the test end, the sound-core end (D) is connected to ratio arm PP and the faulty-core end (B) to ratio arm QQ (both variable resistors); a galvanometer G is connected across D and B.
  • A battery is connected between the junction A of PP and QQ and earth (for an earth fault), or the other core in contact (for a short-circuit fault). The fault point completes the circuit.
     A o-----[Battery]------+  Earth (sheath)
       |                    :
   +---+---+                :  fault resistance
   P       Q                :
   |       |                :
 D o--(G)--o B              :
   |       |                :
   |       +== faulty core =X========+
   |        <------ x ----->         |
   +========= sound core ============+
 Test end                 Far end (cores joined)

Theory

The loop forms a Wheatstone bridge: PP, QQ, RxR_x (faulty core from test end to fault) and RR (sound core plus faulty core from far end back to fault). At balance (G reads zero):

PQ=RRx⇒P+QQ=R+RxRx\frac{P}{Q} = \frac{R}{R_x} \quad\Rightarrow\quad \frac{P+Q}{Q} = \frac{R+R_x}{R_x} Rx=QP+Q(R+Rx)R_x = \frac{Q}{P+Q}(R+R_x)

(R+Rx)(R+R_x) is the total loop resistance =2l×r= 2l\times r (r per unit length). If both cores have the same cross-section, resistance is proportional to length:

x=QP+Q×2lx = \frac{Q}{P+Q}\times2l

where xx is the distance of the fault from the test end and ll the cable length.

Example

For a 500 m cable balanced at P=3 ΩP = 3\ \Omega, Q=1 ΩQ = 1\ \Omega: x=14×1000=250x = \frac{1}{4}\times1000 = 250 m from the test end.

Points to note

  • Fault resistance appears in the battery arm, so it does not affect the balance (only sensitivity).
  • Needs a sound core of known length; works best for low-resistance faults.
  • If the cores differ in area, convert to equivalent lengths before using the formula.

✓ Answer checked by Claude Opus 5.5 (high effort)

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