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Methods of earth resistivity measurement

Short answer

Wenner method: four equal-spaced electrodes, resistivity ρ = 2πaR. Schlumberger method: close potential electrodes, ρ=πc(c+d)R/d. Driven-rod method: measure rod resistance by fall-of-potential, compute ρ = 2πLR/(ln(8L/d)−1). Use AC or reversing DC to avoid polarization.

Explain different methods of earth resistivity measurement with diagrams.

Earth resistivity ρ\rho is measured to design earthing systems (substation grids, tower footings). The common methods use an earth tester that injects current II and measures voltage VV, giving R=V/IR = V/I.

1. Wenner four-electrode method

Four electrodes are placed in a straight line at equal spacing aa, driven to a depth b≪ab \ll a. Current is passed between the outer pair (C1, C2); voltage is measured between the inner pair (P1, P2).

   C1      P1      P2      C2
 --|-------|-------|-------|--
   |<- a ->|<- a ->|<- a ->|

Potential due to a point source at the surface is ρI2πr\frac{\rho I}{2\pi r}. By superposition:

V=ρI2π[(1a−12a)−(12a−1a)]=ρI2πaV = \frac{\rho I}{2\pi}\left[\left(\frac{1}{a}-\frac{1}{2a}\right) - \left(\frac{1}{2a}-\frac{1}{a}\right)\right] = \frac{\rho I}{2\pi a} ρ=2πaR\rho = 2\pi a R

Readings at increasing spacing give resistivity at increasing depth (about depth aa).

2. Schlumberger (Schlumberger–Palmer) method

The potential electrodes are kept close together (spacing dd), and the current electrodes are placed at distance cc outside each potential electrode. Only the current electrodes are moved for deeper readings, so it is faster and more sensitive for large spacings.

   C1          P1  P2          C2
 --|-----------|---|-----------|--
   |<--- c --->|<d>|<--- c --->|
ρ=πc(c+d)Rd\rho = \frac{\pi c(c+d)R}{d}

For c=d=ac = d = a this gives ρ=2πaR\rho = 2\pi aR, the Wenner case.

3. Driven-rod (three-point / variation-of-depth) method

A test rod of length LL and diameter dd is driven into the soil, and its resistance RR is measured by the fall-of-potential method using a current probe C (far away, at least 5–10 times rod length) and a potential probe P at about 62% of that distance.

  Earth tester
   E      P            C
 --|------|------------|--
   |<-0.62D->|
   |<-------- D ------->|
   test rod
ρ=2πLRln⁡(8Ld)−1\rho = \frac{2\pi L R}{\ln\left(\dfrac{8L}{d}\right) - 1}

Repeating with the rod driven deeper gives the change of resistivity with depth. It is simple and suited to small areas but measures only the soil near the rod.

Practical points

  • Take readings in several directions and at several spacings; use the dry-season (highest) value for design.
  • Use AC or reversing DC to avoid polarisation and errors from stray currents.
  • Keep test leads away from buried metal pipes and cables, which distort the readings.

✓ Answer checked by Claude Opus 5.5 (high effort)

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