A fault event in a medium voltage power distribution system does more than trip a breaker — it can leave an invisible but dangerous legacy inside your current transformer core: residual magnetism. Residual flux trapped in a CT core after a fault or DC offset transient directly degrades electromagnetic induction accuracy, causes premature core saturation, and can trigger false protection relay operations or dangerous under-reach during the next fault. For electrical engineers and maintenance teams responsible for substation reliability, knowing how to correctly demagnetize a CT core is not optional maintenance knowledge — it is a frontline protection system integrity task. This article details the physics of residual flux, the step-by-step field demagnetization procedure, and the selection criteria that determine whether your CT core is even susceptible to remanence in the first place.
Table of Contents
- What Is Residual Flux and Why Does It Form in CT Cores?
- How Does Residual Magnetism Affect CT Induction Performance and Reliability?
- How Do You Perform a Field Demagnetization Procedure on a Current Transformer?
- What Are Common Mistakes That Cause Demagnetization to Fail in Medium Voltage CTs?
What Is Residual Flux and Why Does It Form in CT Cores?
Residual flux — also called remanent magnetism or remanence — is the magnetic flux density that remains locked inside a CT core’s grain-oriented silicon steel structure after the magnetizing force has been removed. Understanding why it forms requires a brief look at the b-h hysteresis loop1 that governs all ferromagnetic core behavior.
When a CT experiences a fault current with a significant DC offset component, the primary current does not oscillate symmetrically around zero. Instead, it drives the core flux along the hysteresis curve into a region of high magnetic flux density2. When the fault is cleared and current drops to zero abruptly — as happens during a circuit breaker interruption — the core does not return to zero flux. It remains at the remanent flux density (Br), which for grain-oriented silicon steel can reach 60–80% of saturation flux density3 (Bsat).
Key technical characteristics of CT core remanence:
- Core material sensitivity: Grain-oriented silicon steel (used in high-accuracy CTs) has high permeability but also high remanence. Nickel-iron alloy cores exhibit even higher remanence levels.
- Air-gap cores: CTs designed with a small deliberate air gap in the core (TPY and TPZ classes per IEC 61869-2) have significantly lower remanence — typically less than 10% of Bsat — because the air gap provides a magnetic reset mechanism.
- Triggering events: DC offset fault currents, CT secondary open-circuit events, and improper demagnetization after testing are the three primary causes of significant residual flux buildup.
| Core Type | Remanence Level | IEC Class | Typical Application |
|---|---|---|---|
| Grain-oriented Si-Steel (no air gap) | 60–80% Bsat | 5P, 10P, TPS | Standard protection CTs |
| Nickel-Iron Alloy (no air gap) | Up to 90% Bsat | Class X, TPS | High-sensitivity differential protection |
| Gapped Core (small air gap) | <10% Bsat | TPY | Auto-reclose protection schemes |
| Large Air Gap Core | ~0% Bsat | TPZ | High-speed protection, transient performance |
The core type installed in your switchgear panel directly determines your remanence risk profile — and whether a demagnetization procedure is periodically mandatory or merely precautionary.
How Does Residual Magnetism Affect CT Induction Performance and Reliability?
Residual flux does not cause immediate visible failure — it is a hidden degradation mechanism that silently compromises your protection system’s reliability until the next fault event exposes it catastrophically. The impact operates through one primary mechanism: reduced available flux swing before saturation.
A CT core can only support a finite change in flux density before it saturates. The total available flux swing is:
If Br is already at 70% of Bsat due to residual magnetism, the core has only 30% of its normal flux capacity available for the next fault current transient. This means the CT saturates far earlier than its rated Accuracy Limit Factor (ALF) would suggest, producing a severely distorted secondary current waveform that protection relays cannot correctly interpret.
Practical consequences of unaddressed residual flux:
- Distance relay under-reach: Saturated CT output causes the relay to see a higher apparent impedance than actual, potentially failing to trip for in-zone faults
- Differential protection maloperation: Asymmetric saturation between CTs on opposite sides of a protected zone generates false differential current, causing unwanted tripping
- Overcurrent relay delayed operation: Distorted secondary waveform extends relay operating time beyond designed trip curves
- Energy metering errors: Even at normal load currents, a partially saturated core introduces ratio and phase angle errors exceeding Class 0.5 limits
Customer Case — Power Contractor, 35kV Substation Retrofit, Middle East: A power contractor managing a 35kV substation retrofit in Saudi Arabia reported repeated nuisance trips on a feeder differential protection scheme following a nearby bus fault. After consulting Bepto’s technical team, CT secondary waveform analysis revealed severe asymmetric saturation consistent with high residual flux in two of the six CTs in the differential zone. Following a structured demagnetization procedure on all six units, differential protection stability was fully restored — eliminating three weeks of intermittent nuisance trips that had been misattributed to relay settings.
How Do You Perform a Field Demagnetization Procedure on a Current Transformer?
The demagnetization procedure works by driving the CT core through progressively smaller hysteresis loops until the residual flux converges to near zero. There are two accepted field methods — AC voltage injection and DC current injection with reversal — each suited to different site conditions and CT designs.
Step 1: Isolate and Prepare the CT Circuit
- De-energize the primary circuit and confirm isolation with a voltage tester
- Short-circuit all unused CT secondary cores before beginning — open-circuit secondary terminals under any residual flux condition can generate dangerous induced voltages
- Disconnect the protection relay and metering burden from the secondary terminals being demagnetized
- Document the CT nameplate: rated ratio, accuracy class, knee-point voltage (Vk), and magnetizing current (Imag)
Step 2: Select the Demagnetization Method
| Method | Equipment Required | Best For | Limitation |
|---|---|---|---|
| AC Voltage Injection (Degaussing) | Variable AC source (Variac), ammeter | Standard 5P/10P silicon steel cores | Requires access to variable voltage source |
| DC Current Injection with Reversal | DC power supply, reversing switch, ammeter | TPY / gapped cores, high-inductance CTs | Requires careful current reversal sequencing |
| Dedicated CT Analyzer | CT analyzer with built-in demagnetization function | All core types — most reliable | Equipment cost; not always available on-site |
Step 3: AC Injection Demagnetization Procedure (Most Common Field Method)
- Connect a variable ac voltage source4 (Variac) across the CT secondary terminals (S1–S2)
- Slowly increase AC voltage from zero until the magnetizing current reaches approximately 120–150% of the rated knee-point magnetizing current — this drives the core into saturation, establishing a known starting point on the hysteresis loop
- Slowly and continuously reduce the AC voltage back to zero — do not stop or reverse; the reduction must be smooth and uninterrupted over 30–60 seconds
- The core flux traces progressively smaller hysteresis loops, converging to near-zero remanence as voltage approaches zero
- Measure the magnetizing current at the original test voltage — compare against the pre-demagnetization baseline to confirm flux reduction
Step 4: Verify Demagnetization Success
- Perform a CT excitation curve5 test (V-I characteristic) and compare against the factory magnetizing curve
- A successfully demagnetized core will show magnetizing current within ±5% of the factory baseline at the same applied voltage
- For protection CTs, verify the knee-point voltage (Vk) is restored to nameplate specification
- Record all test results in the substation maintenance log per IEC 61869-2 commissioning requirements
Step 5: Restore Secondary Circuits
- Reconnect protection relay and metering burden in correct polarity (S1→S2 orientation)
- Remove secondary short-circuit links only after all burden connections are confirmed
- Re-energize primary circuit and monitor CT secondary output during first load cycle
- Verify protection relay current inputs match expected values based on primary load current and CT ratio
What Are Common Mistakes That Cause Demagnetization to Fail in Medium Voltage CTs?
Demagnetization is a precision procedure — small execution errors can leave significant residual flux in the core or, worse, introduce new remanence at a different polarity. These are the most critical field mistakes observed across medium voltage substation maintenance operations.
Critical Errors to Avoid
- Stopping the voltage reduction mid-procedure: Interrupting the AC voltage sweep at any non-zero level freezes the core at a new remanence point — potentially worse than the original condition. The reduction must be continuous and uninterrupted to zero.
- Applying excessive initial voltage: Over-driving the core beyond 150% of knee-point magnetizing current risks insulation stress on the secondary winding. Always calculate the safe injection voltage limit before starting.
- Demagnetizing with secondary burden connected: Connected relay impedance alters the effective circuit inductance, preventing the core from completing full hysteresis loops. Always disconnect burden before the procedure.
- Skipping the excitation curve verification: Visual inspection cannot confirm successful demagnetization. Only a post-procedure V-I characteristic test against the factory curve provides objective confirmation.
- Ignoring adjacent CT cores in multi-core units: In dual-core CTs, demagnetizing one core can induce flux changes in the adjacent core through magnetic coupling. Both cores must be tested and demagnetized sequentially.
Post-Procedure Checklist
- ✔ Excitation curve matches factory baseline within ±5%
- ✔ Knee-point voltage restored to nameplate value
- ✔ Secondary polarity markings verified before burden reconnection
- ✔ All short-circuit links removed after burden reconnection
- ✔ Test results documented in maintenance records
Conclusion
Residual flux in a current transformer core is a silent reliability threat that fault events routinely create and maintenance teams routinely overlook. The demagnetization procedure — whether by AC voltage sweep or DC current reversal — restores the core’s full available flux swing, ensuring your protection relays operate within designed accuracy limits when the next fault occurs. For medium voltage power distribution systems where protection reliability is non-negotiable, demagnetization is not a corrective action — it is a mandatory post-fault commissioning step. At Bepto Electric, our CTs are manufactured to IEC 61869-2 with full factory excitation curve documentation, giving your maintenance team the baseline data needed to verify successful demagnetization every time.
FAQs About CT Demagnetization Procedure
Q: How do you know if a current transformer core has significant residual flux after a fault event?
A: Compare the post-fault excitation curve (V-I characteristic) against the factory baseline. A magnetizing current significantly lower than factory values at the same applied voltage indicates residual flux reducing effective core permeability — demagnetization is required.
Q: Can residual flux in a CT core cause a protection relay to fail to trip during a fault?
A: Yes. Residual flux reduces available flux swing before saturation, causing the CT to saturate earlier than its rated ALF. The resulting distorted secondary waveform can cause distance relays to under-reach and overcurrent relays to operate with excessive time delay.
Q: How often should CT demagnetization be performed in medium voltage substations?
A: Demagnetization should be performed after every significant fault event involving DC offset current, after any CT secondary open-circuit incident, and as part of scheduled commissioning following CT replacement or protection scheme modification.
Q: What is the difference between TPY and 5P class CTs regarding residual flux susceptibility?
A: TPY class CTs incorporate a small air gap in the core, limiting remanence to below 10% of Bsat — making them inherently resistant to residual flux buildup. Standard 5P class CTs have no air gap and can retain 60–80% of Bsat as remanence after a fault, requiring periodic demagnetization.
Q: Is it safe to perform CT demagnetization with the primary bus still energized in an adjacent bay?
A: The CT primary conductor must be de-energized and isolated before demagnetization. Adjacent energized bays are acceptable provided proper isolation barriers are in place per substation safety rules, but induced voltages from nearby conductors must be assessed before connecting test equipment.
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Understanding how ferromagnetic materials retain magnetism through the hysteresis cycle. ↩
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Technical definitions of flux density and its role in transformer core performance. ↩
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The physical limits of magnetic flux a transformer core can support before saturation. ↩
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How variable autotransformers (Variacs) control voltage for electrical testing. ↩
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A guide to interpreting V-I characteristic curves for instrument transformer health. ↩