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Arrester separation for a 500 kV/μs surge

Short answer

Protective ratio at zero distance is 500/420=1.19, below 1.25. At 40 m separation transformer voltage is 420+2*500*40/300=553.3 kV. Maximum distance for BIL is 24 m; no distance meets PR 1.25.

The arrester used in a line has its spark over voltage of 420 kV. A surge having steepness of 500 kV/μs on the front reaches the arrester terminal at time t = 0 and travels towards the transformer. BIL withstand voltage of the transformer is 500 kV and the PR required for transformer protection is 1.25. (i) Check whether the transformer is properly coordinated? (ii) Compute the voltage at the transformer terminal when the arrester is kept 40 m away from transformer. (iii) What is the maximum distance allowed between the transformer and the arrester in case of this surge? Assume that the residual voltage (discharge voltage) of the arrester is equal to its spark over voltage.

A surge reaching the arrester rises at S=500S = 500 kV/μs. It travels on to the transformer, dd metres beyond, and arrives after T=d/vT = d/v. The transformer (open end) doubles it, and the reflected wave gets back to the arrester at 2T2T. From then on, the arrester voltage rises at 2S2S, so the arrester sparks over at Va=420V_a = 420 kV at time ts=Va/(2S)+Tt_s = V_a/(2S) + T. The clamping effect takes a further time TT to reach the transformer, and until then the transformer voltage keeps rising. The standard result is

Vt=Va+2Sdv,v=300 m/μsV_t = V_a + 2S\frac{d}{v}, \quad v = 300\ \text{m}/\mu\text{s}

This holds when the reflection returns before the arrester would spark over on the incident wave alone, i.e. 2T<Va/S=420/500=0.84 μ2T < V_a/S = 420/500 = 0.84\ \mus (d<126d < 126 m), which is true here.

(i) Coordination check (arrester right at the transformer)

PR=BILVa=500420=1.19PR = \frac{\text{BIL}}{V_a} = \frac{500}{420} = 1.19

The required PR is 1.25, which means the protective level must not exceed 500/1.25=400500/1.25 = 400 kV. Since 420>400420 > 400 kV, i.e. 1.19<1.251.19 < 1.25:

Not properly coordinated, even with zero separation.

(ii) Transformer voltage with the arrester 40 m away

T=40300=0.1333 μsts=4202×500+0.1333=0.553 μsVt=420+2×500×0.1333=420+133.3=553.3 kV\begin{aligned} T &= \frac{40}{300} = 0.1333\ \mu\text{s} \\ t_s &= \frac{420}{2 \times 500} + 0.1333 = 0.553\ \mu\text{s} \\ V_t &= 420 + 2 \times 500 \times 0.1333 \\ &= 420 + 133.3 = 553.3\ \text{kV} \end{aligned}

This exceeds the BIL of 500 kV, so the transformer insulation would fail. The achieved PR is 500/553.3=0.90500/553.3 = 0.90.

(iii) Maximum allowed distance

With PR = 1.25: the allowed transformer voltage is 400 kV, which is already below the arrester level of 420 kV. So no distance works (dmaxd_{max} is negative). The arrester rating must be lowered or the BIL raised.

Without margin, Vt≤V_t \le BIL = 500 kV:

420+2×500×d300≤500d≤(500−420)×3002×500=24 m\begin{aligned} 420 + 2 \times 500 \times \frac{d}{300} &\le 500 \\ d &\le \frac{(500 - 420) \times 300}{2 \times 500} = 24\ \text{m} \end{aligned}
  500 kV/us                  d
 ---------->  Arrester  ----------- Transformer
             (420 kV)               (BIL 500 kV)
ItemResult
PR at zero distance1.19 (< 1.25, not OK)
VtV_t at 40 m553.3 kV
dmaxd_{max} for PR 1.25none possible
dmaxd_{max} for VtV_t = BIL24 m

Answer: (i) not coordinated (PR = 1.19); (ii) 553.3 kV; (iii) the arrester can be at most 24 m away to keep the voltage within the BIL. With the 1.25 margin, no distance satisfies the requirement.

✓ Answer checked by Claude Opus 5.5 (high effort)

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