Core Losses

The complete guide to core losses (iron losses) — the power wasted as heat inside a magnetic core under AC. From hysteresis loss and eddy-current loss to the Steinmetz formula, lamination, and iron vs copper loss in transformers and motors.

Complete Learning Path — Core Losses

From what core losses are, through hysteresis and eddy-current loss, the formula and lamination, to frequency effects, iron vs copper loss and how to reduce them

What are Core Losses?

Core losses — also called iron losses — are the power turned into heat inside a magnetic core whenever it is magnetised by an alternating current. They happen in the iron of every transformer, motor and inductor.

Core loss is the sum of two parts: hysteresis loss (from repeatedly re-magnetising the material) and eddy-current loss (from tiny currents induced in the core). Because they depend on the AC flux, not the load current, core losses are present even at no load — that is why they are called a constant or no-load loss.

Core (iron) loss equals hysteresis loss plus eddy-current loss in an AC-magnetised transformer core
Core (iron) loss = hysteresis loss (B–H loop area) + eddy-current loss (induced loops), generated whenever the core carries an alternating flux.
Pc
Core (iron) loss
Ph
Hysteresis loss
Pe
Eddy-current loss
no-load
Constant with load

Pc = Ph + Pe

Total core loss = hysteresis loss + eddy-current loss

Hysteresis Loss

Hysteresis loss is the energy spent re-aligning the core’s magnetic domains every AC cycle. Because the material “remembers” its magnetisation (see the B–H curve), it takes the long way round a loop — and that costs energy as heat.

Hysteresis loss equals the shaded area of the B-H loop, the energy lost per magnetisation cycle
The area enclosed by the B–H loop is the energy lost per cycle. A fatter loop (harder material) means more hysteresis loss.

Ph = Kh f Bmn  (n ≈ 1.6–2)

Rises with frequency f and peak flux density Bm; Kh and n are Steinmetz material constants

Worked example

If frequency doubles (50 → 100 Hz) at the same peak flux, hysteresis loss:

roughly doubles (Ph ∝ f). Cut the peak flux Bm by 20% and Ph drops by about 30% (since n ≈ 1.6).

Eddy-Current Loss

A changing magnetic flux induces voltages inside the conductive core itself, driving little circulating eddy currents. These currents heat the core through its own resistance — wasted power.

Eddy currents form large loops in a solid core but tiny loops in a laminated core, cutting eddy-current loss
A solid core lets large eddy currents flow (high loss). Thin, insulated laminations confine them to tiny loops — eddy loss falls as t².

Pe = Ke f² Bm² t² / ρ

Rises with f², Bm² and lamination thickness t²; falls with core resistivity ρ

Why cores are laminated

Since Pe ∝ t², halving the lamination thickness cuts eddy loss to a quarter. That is why transformer and motor cores are stacks of thin (0.2–0.5 mm) insulated steel sheets, not solid blocks.

The Core-Loss Formula

Put both mechanisms together and you get the classic Steinmetz core-loss equation — the tool engineers use to predict and minimise iron loss.

Core loss formula Pc = Kh f Bm^n + Ke f^2 Bm^2 t^2 with every term defined
The core-loss formula and every term: frequency f, peak flux Bm, lamination thickness t, and the material constants Kh, Ke, n.

Pc = Kh f Bmn + Ke f² Bm² t²

The full core-loss equation (hysteresis term + eddy-current term)

Specific core loss — watts per kg

Manufacturers quote a material’s specific core loss in W/kg at a stated frequency and flux density (e.g. 1.1 W/kg at 50 Hz, 1.5 T) so designers can pick the lowest-loss steel for the job.

How Core Loss Grows with Frequency

The two loss terms scale differently with frequency, and that decides which material to use.

Graph of core loss versus frequency: hysteresis loss proportional to f, eddy loss to f squared, total is their sum
Hysteresis loss grows with f; eddy loss grows with f². At high frequency eddy loss dominates — so switch-mode supplies use ferrite cores.
Increase…Hysteresis PhEddy Pe
Frequency f (×2)×2 (∝ f)×4 (∝ f²)
Peak flux Bm (×2)×3 (∝ Bm1.6)×4 (∝ Bm²)
Lamination t (×2)no change×4 (∝ t²)

Iron Loss vs Copper Loss & Efficiency

A transformer or motor has two loss families: iron (core) loss and copper loss (I²R in the windings). Together they set the efficiency.

Iron loss constant with load, copper loss rising as load squared, efficiency maximum where copper loss equals iron loss
Iron loss is constant (present at any load); copper loss grows as load². Efficiency is highest where copper loss = iron loss.

η = Pout / (Pout + Piron + Pcopper)  ·  max η when Pcopper = Piron

Efficiency and the maximum-efficiency condition

Measuring iron loss: the open-circuit test

Apply rated voltage to a transformer with the secondary open. Almost no current flows, so copper loss is negligible and the wattmeter reads essentially the core loss. Copper loss is found separately from the short-circuit test.

How to Reduce Core Losses

Lower core loss means a cooler, more efficient, longer-lasting machine. Here is how engineers cut it.

Thin laminations

Stacks of 0.2–0.5 mm insulated sheets slash eddy loss (Pe ∝ t²).

Silicon steel (CRGO)

Adding silicon raises resistivity and grain-orienting narrows the B–H loop.

Ferrite for high f

Very high resistivity kills eddy loss in SMPS and RF inductors.

Amorphous & nanocrystalline

Ultra-low-loss cores for high-efficiency distribution transformers.

Lower peak flux

Design for a modest Bm — loss falls steeply with flux density.

Good core design

Mitred joints and tight stacking keep flux smooth and loss low.

Key Terms at a Glance

The essential core-loss vocabulary students and engineers search for.

Core / iron loss

Heat in the core under AC (no-load loss).

Hysteresis loss

B–H loop area × f; KhfBmn.

Eddy-current loss

Induced core currents; ∝ f²t².

Lamination

Thin insulated sheets to cut eddy loss.

Steinmetz

The core-loss equation & constants.

Copper loss

I²R in windings; grows with load².

Specific core loss

W/kg at a stated f and Bm.

Open-circuit test

Measures core loss at no load.

Frequently Asked Questions

Quick, expert answers to the questions people ask most about core losses.

What are core losses in simple words?

They are the heat wasted inside the iron core of a transformer or motor when AC magnetises it. There are two kinds — hysteresis loss and eddy-current loss — and together they are called iron loss or no-load loss.

What is the difference between hysteresis and eddy-current loss?

Hysteresis loss comes from re-magnetising the material each cycle and equals the B–H loop area times frequency. Eddy-current loss comes from circulating currents induced in the conductive core. Lamination reduces eddy loss; a better material reduces hysteresis loss.

What is the core-loss formula?

Pc = Ph + Pe = KhfBmn + Kef²Bm²t², where f is frequency, Bm the peak flux density, t the lamination thickness and n ≈ 1.6–2.

Why are cores laminated?

To break up eddy-current paths. Because eddy loss varies with the square of thickness (Pe ∝ t²), thin insulated sheets cut it dramatically compared with a solid core.

Do core losses depend on load?

No — core loss depends on the voltage and frequency (the flux), so it is essentially constant from no load to full load. That is why it is called a constant or no-load loss, unlike copper loss which rises with load.

What is the difference between core loss and copper loss?

Core (iron) loss is in the magnetic core and stays roughly constant; copper loss is the I²R heating in the windings and grows with load². Efficiency peaks where copper loss equals iron loss.

How do you measure core loss?

With the open-circuit (no-load) test: apply rated voltage with the secondary open so copper loss is negligible; the wattmeter then reads essentially the core loss.

Why do high-frequency circuits use ferrite cores?

Because eddy-current loss rises with f², steel cores would overheat at high frequency. Ferrite has very high resistivity, so eddy currents stay tiny — ideal for switch-mode supplies and RF inductors.

Conclusion & Key Takeaways

Core losses are the unavoidable heat of magnetising iron with AC — and minimising them is central to efficient power equipment.

Pc = Ph + Pe

Hysteresis + eddy.

Hysteresis ∝ f

= B–H loop area.

Eddy ∝ f²t²

So laminate the core.

No-load loss

Constant with load.

Max η

Copper loss = iron loss.

Better cores

Silicon steel, ferrite.

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