4.4 Cable Short-Circuit Capacity
Key Takeaways
- Conductors must withstand the thermal energy of a short-circuit for the time the protective device takes to clear — CCC alone does not prove fault withstand.
- The adiabatic (or energy let-through) theme relates permissible fault current and clearing time to conductor cross-section and material constants from AS/NZS 3008.
- S² = I²t / k² (rearranged forms vary): larger cross-section S, higher k, or faster clearing (smaller I²t) improves withstand.
- Upstream protective device breaking capacity and let-through energy must be coordinated with cable withstand and installation prospective fault levels.
- Exam traps include checking only overload CCC, ignoring earth-fault loop and disconnection times, and using the wrong k for conductor/insulation combinations.
Fault heat is a different problem from continuous load heat
Current-carrying capacity (Sections 4.1–4.3) limits steady temperature under continuous load. A short-circuit dumps far higher current for a short time. Insulation and conductor metal must not reach destructive temperatures before the fuse or circuit-breaker clears.
AS/NZS 3008 provides data and methods for the short-circuit capacity of conductors — commonly taught through the adiabatic assumption: for brief faults, heat stays in the conductor (negligible heat loss during the event), so temperature rise tracks the electrical energy input.
Queensland licence and the capstone assessments expect you to recognise when a cable that "passes CCC" still fails fault withstand, especially on submains close to a MEN switchboard where prospective fault current is high.
The adiabatic relationship (teaching form)
A widely used adiabatic expression relating minimum conductor size to fault duty is:
S = √(I²t) / k
or equivalently I²t = S²k²
Where:
| Symbol | Meaning |
|---|---|
| S | Conductor cross-sectional area (mm²) |
| I | Short-circuit current (A) — often the prospective fault current used for the check, or a value coordinated with device let-through |
| t | Fault duration (s) until disconnection |
| k | Factor depending on conductor material and permissible temperature rise / insulation limits from AS/NZS 3008 |
k is not a universal constant. Copper with a given insulation temperature limit has a different k from aluminium, and initial/final temperatures assumed in the Standard matter. Always take k from the AS/NZS 3008 tables matching the cable.
Rearrangements you will use
- Minimum S for a known I and t:
S ≥ √(I²t) / k - Maximum withstand time for known S, I, k:
t ≤ (S²k²) / I² - Maximum I for known S, t, k:
I ≤ S k / √t
Worked example 1 — minimum size for a bolted fault duty
Given (illustrative): Prospective short-circuit current I = 6 000 A, protective device clears in t = 0.1 s, copper conductor with k = 115 (illustrative — verify in AS/NZS 3008 for the insulation/temperature pair).
I²t = 6000² × 0.1 = 36 000 000 × 0.1 = 3 600 000 A²s
√(I²t) = √3 600 000 ≈ 1 897
Smin = 1897 / 115 ≈ 16.5 mm²
So a 16 mm² copper conductor is borderline/inadequate on this illustrative arithmetic; 25 mm² would be the next common size that satisfies S ≥ 16.5 mm². Even if CCC derating only required 16 mm² for load, fault energy forces 25 mm².
That is the exam insight: two independent checks.
Worked example 2 — checking an existing submain
Given: Cu S = 25 mm², k = 115 (illustrative), fault I = 10 000 A.
Maximum adiabatic time:
t_max = (S²k²) / I² = (25² × 115²) / 10 000²
25² = 625; 115² = 13 225; product = 8 265 625
10 000² = 100 000 000
t_max ≈ 0.083 s
If the protective device's clearing time at 10 kA is 0.2 s, the cable fails the adiabatic check — change protection (faster device / better current-limiting), reduce fault level (design change), or increase S.
If the device is current-limiting and its published let-through I²t is used instead of the unbounded I²t from prospective current × full time, use the manufacturer's let-through data with the same S²k² ≥ I²t_let-through inequality. Licence answers should state whether prospective I with clearing time or device let-through energy was used.
Overload versus short-circuit versus earth fault
| Check | What it protects against | Typical tool |
|---|---|---|
| CCC / Iz | Continuous and overload heating | AS/NZS 3008 tables + derating |
| Short-circuit thermal withstand | Phase fault energy until clearance | Adiabatic S, k, I, t / let-through |
| Earth fault disconnection | Shock and earth-fault thermal stress on PE/PEN paths | AS/NZS 3000 disconnection times, earth-fault loop impedance, PE sizing rules |
Protective earthing conductors also need fault withstand — undersized earths that melt or vaporise leave exposed conductive parts live. Do not celebrate a fat active/neutral pair with a fragile earth.
Coordination with protective devices
Circuit-breakers and fuses differ in let-through energy. A current-limiting HRC fuse may allow a smaller conductor for the same prospective fault level than a non-limiting breaker that holds longer. Conversely, a slow device on a high fault level near the supply transformer is hostile to small cables.
Also confirm the device breaking capacity (Icu/Icn) equals or exceeds prospective fault current at its point of installation — that is device selection, but it pairs with cable withstand in any serious fault study.
Voltage drop reminder (linked constraint)
Although this section focuses on short-circuit capacity, remember a cable enlarged for fault withstand often improves voltage drop automatically. On long Queensland rural runs, voltage drop may govern before fault energy; on short submains at a CBD main board, fault energy may govern before voltage drop. Run all checks.
Practical selection sequence (complete)
- Estimate Ib, select In.
- Choose installation method → base CCC → apply multiplied derating → verify Iz ≥ In.
- Check voltage drop against AS/NZS 3000 limits for the circuit type.
- Determine prospective fault current and protective clearing time / let-through.
- Verify adiabatic withstand with correct k and S.
- Verify earth conductor fault capacity and disconnection requirements.
- Document assumptions (method, factors, fault level, k source).
Exam traps for Section 4.4
- Stopping after CCC and declaring the cable "compliant".
- Using aluminium k for a copper cable (or the reverse).
- Taking t from a random guess instead of device curves or stated exam data.
- Applying adiabatic heating to justify exceeding insulation temperature continuously (adiabatic is for short faults, not steady overload).
- Ignoring that reduced cross-section control cores or tap-offs may be the weak link on a faulted submain tee-off.
Capstone narrative example
"Consumer mains: 25 mm² Cu V-90, buried method per AS/NZS 3008, Iz after factors = 98 A, In = 80 A, OK for load. Prospective fault 12 kA; main fuse clears in 0.05 s; k from AS/NZS 3008 = …; S required = … mm²; 25 mm² adequate / inadequate. Earth conductor checked separately for the same fault duty."
Candidates who speak that language show they understand AS/NZS 3008 as a selection system, not a single ampacity poster on the workshop wall.
Master continuous rating, temperature class, derating multiplication and short-circuit adiabatic checks together, and cable selection questions on the Queensland electrical licence pathway become structured calculations instead of memorised folklore.
Why must cable selection include a short-circuit thermal withstand check in addition to current-carrying capacity?
Using the adiabatic teaching relationship S = √(I²t) / k, what happens if the fault clearing time t increases while I and k remain constant?
For an illustrative copper cable check with S = 16 mm², k = 115, and a prospective fault current of 8 000 A, which statement about adiabatic withstand time is correct in principle?
A submain passes its derated CCC check at 16 mm² copper but an adiabatic calculation using the prospective fault current and device clearing time requires at least 21 mm². What is the correct outcome?