ProtectionAcademy
1.145 min · Beginner → Intermediate

Symmetrical Components & Fault Phasors

Fortescue's transformation, and why an SLG fault puts Z₁, Z₂ and Z₀ in series.

You will be able to
  • ▸Decompose any unbalanced set of phasors into positive, negative and zero sequence
  • ▸Connect sequence networks for SLG, LL, LLG and three-phase faults
  • ▸Derive 3I₀ = 3E / |Z₁ + Z₂ + Z₀| and compute bolted fault currents
  • ▸Distinguish the effective-grounding definition (COG ≤ 80%) from the impedance test (X₀/X₁ ≤ 3, R₀/X₁ ≤ 1)
Standards
Fortescue (1918)IEEE C37.110 (context)
Intuition

Turning one hard problem into three easy ones

A balanced three-phase system is easy to analyse. Solve one phase, and the other two are the same thing shifted by 120°. Faults break that symmetry. A ground fault on phase A pulls A's voltage toward zero, leaves B and C roughly where they were, and sends current back through the earth. That is three different phasors with no shortcut.

In 1918, Charles Fortescue showed that any set of three unbalanced phasors can be written as the sum of three balanced sets:

  • Positive sequence (1): equal magnitudes, 120° apart, in normal ABC rotation. This is the "healthy" part.
  • Negative sequence (2): equal magnitudes, 120° apart, in reversed ACB rotation. It measures unbalance.
  • Zero sequence (0): three identical phasors, all in phase. It only exists when current can return through ground or a neutral.

The payoff: in static equipment (lines, cables, transformers) the three sequences don't interact with each other. Each one has its own simple single-phase circuit, its sequence network. The fault is just a rule for wiring those three circuits together.

The transformation

The Fortescue matrix

The operator a=1∠120∘a = 1\angle 120^\circ rotates a phasor by 120°. Since 1+a+a2=01 + a + a^2 = 0, it is exactly what you need to pick apart the three rotations:

[V0V1V2]=13[1111aa21a2a][VaVbVc][VaVbVc]=[1111a2a1aa2][V0V1V2]\begin{bmatrix}V_0\\V_1\\V_2\end{bmatrix}=\frac{1}{3}\begin{bmatrix}1&1&1\\1&a&a^2\\1&a^2&a\end{bmatrix}\begin{bmatrix}V_a\\V_b\\V_c\end{bmatrix}\qquad\begin{bmatrix}V_a\\V_b\\V_c\end{bmatrix}=\begin{bmatrix}1&1&1\\1&a^2&a\\1&a&a^2\end{bmatrix}\begin{bmatrix}V_0\\V_1\\V_2\end{bmatrix}

Read the second row: V1=13(Va+aVb+a2Vc)V_1=\tfrac13(V_a+aV_b+a^2V_c). Multiplying Vb by a and Vc by a² rotates a positive-sequence set so that all three phasors line up with Va. They add, and anything else tends to cancel. That is the graphical construction drawn in the right-hand plot below. Numerical relays run this same calculation on filtered phasors once per processing interval (typically every ¼ to ⅛ cycle) to produce their 46, 32Q, 67Q, 59N and 51N quantities.

Interactive lab
Symmetrical Component Synthesizer
Drag the tips of Va, Vb and Vc or load a fault preset. The relay-style decomposition updates live: three balanced sets that add up to your unbalanced one.
Presets
Phase A collapses toward zero. All three sequences appear, and V₀ is the signature of a ground fault.
Sequence magnitudes (pu)
V₁0.728V₂0.248V₀0.330
Show construction of
Phase quantities (drag me)
0°90°180°-90°Va 0.15∠-5°Vb 1.02∠-124°Vc 1.02∠124°
Building V1 = ⅓(Va + a·Vb + a²·Vc)
0°90°180°-90°Vaa·Vba²·VcΣV1
Positive (1)
0°90°180°-90°Va1Vb1Vc1
Negative (2)
0°90°180°-90°Va2Vb2Vc2
Zero (0)
0°90°180°-90°Va0
phase-a componentphase-b componentphase-c component
V₁
0.728pu ∠-0°
V₂
0.248pu ∠-179°
V₀
0.330pu ∠-179°
V₂ / V₁ unbalance
34.1%
above 2 % is worth a look
Zero sequence present (V₀/V₁ = 45 %). Something is returning through ground: a ground fault, or an open phase on a grounded system.
Fault analysis

Sequence networks and how faults connect them

Each sequence network is a Thevenin equivalent seen from the fault point. Only the positive network contains a source, the pre-fault voltage E, because generators are designed to produce balanced positive-sequence voltage. The fault type sets the boundary conditions, and those decide the wiring:

FaultBoundary conditionsNetwork connectionResult
3ΦVa = Vb = Vc = 0 (bolted)N₁ onlyI1=E/Z1I_1 = E/Z_1
SLG (A-G)Ib = Ic = 0, Va = 3Zf·IaN₁, N₂, N₀ in seriesI0=EZ1+Z2+Z0+3ZfI_0=\frac{E}{Z_1+Z_2+Z_0+3Z_f}
LL (B-C)Ia = 0, Ib = −IcN₁ ∥ N₂I1=−I2=EZ1+Z2+ZfI_1=-I_2=\frac{E}{Z_1+Z_2+Z_f}
LLG (B-C-G)Ia = 0, Vb = VcN₁ + (N₂ ∥ N₀)I1=EZ1+Z2 ∥ (Z0+3Zf)I_1=\frac{E}{Z_1+Z_2\,\|\,(Z_0+3Z_f)}

For the single-line-to-ground fault, the ground (residual) current is three times the zero-sequence current:

3I0=3E∣Z1+Z2+Z0+3Zf∣3I_0 = \frac{3E}{\left|Z_1+Z_2+Z_0+3Z_f\right|}
Interactive lab
Sequence-Network Fault Calculator
A 34.5 kV system with E = 34.5/√3 = 19.92 kV line-to-neutral, seen from the fault point. Choose a fault type and watch the three sequence networks reconnect: in series for SLG, in parallel for LL and LLG. The two POI presets are the distribution-voltage POI of the worked example. The zig-zag preset changes two things at once: the grounding bank is added and the source moves from minimum to maximum, so not all of its rise in 3I₀ comes from the bank.
Fault type
Driving-point impedances
1.08 Ω
7.69 Ω
4.61 Ω
36.14 Ω
0.0 Ω
3R_f = 0Positive N₁Z₁FN383 ANegative N₂Z₂FN383 AZero N₀Z₀FN383 A
SLG: N₁, N₂ and N₀ in series with 3R_f, so I₁ = I₂ = I₀ = E / (Z₁ + Z₂ + Z₀ + 3R_f).
Fault currents (kA)
0°90°180°-90°Ia 1.15∠-83°Ib 0.00∠0°Ic 0.00∠0°3I0 1.15∠-83°
Voltages at the fault (pu)
0°90°180°-90°Va 0.00∠0°Vb 1.36∠-140°Vc 1.36∠141°
I₁
383A
∠-82.5°
I₂
383A
∠-82.5°
I₀
383A
∠-82.5°
3I₀ (ground)
1,150A
Ia / Ib / Ic
1,150 / 0 / 0A
Bolted 3Φ reference
2,565A
fault / 3Φ = 45 %
|Vb|, |Vc| (unfaulted for SLG)
1.365, 1.360pu
limit 0.8 × √3 = 1.39 pu
COG (SLG)
78.8%
effectively grounded: ≤ 80 %
X₀ / X₁
4.70
impedance test: 0 < X₀/X₁ ≤ 3
R₀ / X₁
0.60
impedance test: R₀/X₁ ≤ 1
This fault meets COG ≤ 80 %, but the impedance ratios fail. The ratio test is what keeps COG inside 80 % for every fault resistance: try R_f of a few ohms and watch COG cross 80 %.
phase Aphase Bphase C3I₀ residual
Worked example

Ground-fault current at a 34.5 kV POI

A 74.9 MW solar plus 20 MW BESS project connects at 34.5 kV. This is a distribution-voltage POI: the plant ties directly into the utility's 34.5 kV system, so the utility supplies part of the plant's ground reference. That is not the arrangement in the larger plants of Module 0.1, where the collector sits behind the delta LV winding of the main power transformer and never sees a utility ground source. There, the plant's own grounding sources are the only zero-sequence path (see the configurations table in Module 1.2). The driving-point impedances at this POI under minimum-source conditions, before any plant grounding bank, are:

Z1=Z2=1.08+j7.69 Ω,Z0=4.61+j36.14 Ω,E=34,5003=19,920 VZ_1 = Z_2 = 1.08 + j7.69\ \Omega,\qquad Z_0 = 4.61 + j36.14\ \Omega,\qquad E=\frac{34{,}500}{\sqrt3}=19{,}920\ \text{V}

Find the bolted SLG fault current 3I₀ and compare it with the three-phase fault current. Then load the "POI as-found" preset in the calculator to check your answer.

Effective grounding: the definition and the impedance test

A system is effectively grounded when the coefficient of grounding (COG) is no more than 80 %. COG is the highest healthy-phase voltage during a ground fault, as a fraction of the normal line-to-line voltage; 80 % corresponds to an earth-fault factor of about 1.4. On a line-to-neutral base the limit is 0.8 × √3 ≈ 1.39 pu, which is where the calculator's healthy-phase readout turns red.

The impedance ratios are the conventional test that keeps COG inside 80 % for practical fault resistances (the guides' curves assume R₁ is much smaller than X₁): X₀/X₁ positive and no more than 3, and R₀/X₁ no more than 1 (the IEEE C62.92 guides). The as-found POI shows why both matter. For a bolted fault its COG is 78.8 %, just inside the limit, yet X₀/X₁ = 4.70 fails the ratio test. Add fault resistance in the calculator: between roughly 2 and 12 Ω the healthy phase rises to about 1.416 pu (COG ≈ 82 %). The ratio failure is the warning, and it is the starting point of the grounding-bank study in Module 2.2.

Beyond faults

Unbalance, open phases and V₂ limits

Sequence components aren't only for faults. Steady-state voltage unbalance is usually quoted as ∣V2∣/∣V1∣|V_2|/|V_1|. An open conductor into an ungrounded load gives equal and opposite I₁ and I₂ with no I₀. A reversed rotation shows up as pure negative sequence.

IEEE 2800-2022 uses the same language for inverter-based plants. It deals with unbalance in its continuous-operation requirements, and with negative-sequence current injection during faults in Clause 7.2.2.3.4. This course's source research also cites a negative-sequence voltage figure of about 6.7 % with a 2 s window as a ride-through condition. That figure could not be verified against the standard text, so treat it as unverified and take the actual limits from the edition and clause you are applying. The decomposer only flags unbalance above 2 % as worth a look; it deliberately doesn't draw a pass/fail line.

Key takeaways
  • Any unbalanced three-phase set is the sum of balanced positive, negative and zero-sequence sets.
  • Zero sequence needs a ground or neutral return path. Negative sequence measures unbalance or reversed rotation.
  • SLG: networks in series, so 3I₀ = 3E/|Z₁+Z₂+Z₀+3Zf|. LL: N₁ ∥ N₂. LLG: N₁ in series with N₂ ∥ N₀.
  • Effectively grounded means COG ≤ 80 % (healthy phases ≤ 0.8·√3 ≈ 1.39 pu). The impedance test is 0 < X₀/X₁ ≤ 3 and R₀/X₁ ≤ 1; a large Z₀ means low ground-fault current and high healthy-phase voltage.
  • Inverters are current sources, not voltages behind impedances, and ground relays see their branch share of 3I₀, not the total.
  • Relays measure sequence quantities directly. 3I₀ is the residual current, and 3V₀ is the broken-delta voltage.
Assessment

Knowledge check

0/8 answered
  1. Q1
    A perfectly balanced set Va = 1∠0°, Vb = 1∠−120°, Vc = 1∠120° contains:
  2. Q2
    You swap the B and C leads on a set of VTs. A relay now measures:
  3. Q3
    For a single-line-to-ground fault, the sequence networks are connected:
  4. Q4
    Why does a phase-to-phase (LL) fault produce no zero-sequence current?
  5. Q5
    With E = 19,920 V, Z₁ = Z₂ = 1.08 + j7.69 Ω and Z₀ = 4.61 + j36.14 Ω, the bolted SLG current 3I₀ is closest to:
  6. Q6
    On the same system, the bolted three-phase fault current is about 2,565 A. Why is the SLG current so much lower?
  7. Q7
    What does the operator a represent?
  8. Q8
    A relay measures 3I₀ at a feeder. In terms of phase currents, 3I₀ equals:
Mastery challenge

Derive the series connection for an SLG fault

Prove from first principles why an SLG fault places Z₁, Z₂ and Z₀ in series, then verify your numbers in the calculator.

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