MAY 21, 202659 MINS READ
The reduction of hysteresis loss in electrical steel low hysteresis loss steel is governed by the interplay between chemical composition, microstructure, and magnetic domain behavior. According to the Steinmetz equation, total losses in electrical steels are proportional to frequency × thickness × induction^1.6 / resistivity 4. Hysteresis loss specifically depends on crystal orientation alignment, defect density, grain boundary characteristics, and precipitate distribution 15. In grain-oriented electrical steels, achieving a sharp (110)001 Goss texture minimizes magnetocrystalline anisotropy energy, facilitating easier domain wall motion and reducing hysteresis loss 3. For non-oriented electrical steels, random texture with minimized harmful precipitates (AlN, MnS) is critical 5,18.
Silicon and aluminum additions serve dual purposes: increasing electrical resistivity (reducing eddy current loss) and modifying magnetic properties 4. Silicon content typically ranges from 2.0–4.0 wt.% in grain-oriented grades 2 and 0.3–3.5 wt.% in non-oriented grades 12,17, with resistivity increasing approximately 10 μΩ·cm per 1 wt.% Si addition 4. Aluminum additions (0.1–3.0 wt.%) further enhance resistivity but must be carefully controlled to prevent detrimental AlN precipitation, which pins domain walls and increases hysteresis loss 5,18. Manganese (0.03–3.0 wt.%) forms MnS precipitates that can either inhibit grain growth (beneficial for secondary recrystallization in grain-oriented steels) or increase hysteresis loss if present in excessive quantities 5.
The control of interstitial elements (C, N, O) is paramount. Carbon content must be reduced below 0.03–0.05 wt.% to minimize magnetic aging and hysteresis loss 9,16. Nitrogen, while useful for forming inhibitor precipitates during primary recrystallization, must be carefully managed; excessive nitrogen leads to AlN precipitation that deteriorates hysteresis loss 5,11. Oxygen content below 0.01 wt.% prevents oxide inclusions that act as pinning sites for domain walls 9.
Recent research demonstrates that composite precipitation of MnS and AlN can be engineered through controlled pickling processes using solutions containing Cu, Hg, Ag, Pb, Cd, Co, Zn, or Ni, promoting precipitate coarsening and reducing their detrimental effect on hysteresis loss 18. This approach achieved hysteresis loss ratios (hysteresis loss / total iron loss) exceeding 0.8 and total iron loss below 2.5 W/kg at 1.5 T, 50 Hz 18.
Grain-oriented electrical steel low hysteresis loss steel typically contains Si: 2.0–4.0 wt.%, with higher silicon content improving resistivity but reducing saturation magnetization and increasing brittleness 2. The optimal composition balances these trade-offs: C ≤ 0.05 wt.%, Si: 2.5–3.5 wt.%, Mn: 0.05–0.15 wt.%, Al: 0.02–0.04 wt.%, N: 0.005–0.012 wt.%, S: ≤0.005 wt.% 3,11. Trace additions of Sb (≤0.1 wt.%) and Sn (≤0.03 wt.%) act as grain growth inhibitors, enhancing secondary recrystallization and Goss texture development 11,16.
Ultra-thin grain-oriented electrical steels (thickness <0.23 mm) face challenges in maintaining low hysteresis loss due to increased surface-to-volume ratio and precipitate instability during annealing 11. Controlled nitriding during primary recrystallization annealing, with nitriding rate (ΔN/Δt) ≥0.025, stabilizes inhibitor precipitates and reduces hysteresis loss ratio to total iron loss below 0.35 11.
Non-oriented electrical steel low hysteresis loss steel compositions prioritize minimizing precipitate formation while maintaining adequate mechanical strength. Typical compositions include: C ≤0.03 wt.%, Si: 0.3–3.5 wt.%, Al: 1.0–12.0 wt.%, Mn: 0.25–10.0 wt.%, with optional additions of Cu (0.05–3.0 wt.%) and Ni (0.01–5.0 wt.%) for strength enhancement and hysteresis loss reduction 12,17. High-aluminum grades (Al: 1–12 wt.%) exhibit frequency-independent magnetic properties, making them suitable for high-speed motor applications where conventional steels suffer from increased hysteresis loss at elevated frequencies 12,17.
A novel composition achieving hysteresis loss P1.5 <4.7 W/kg at 1.5 T, 50 Hz comprises: Si ≤1.8 wt.%, Al <1 wt.%, C ≤0.02 wt.%, Mn <0.5 wt.%, Sn ≤0.03 wt.%, Sb ≤0.1 wt.%, P ≤0.1 wt.%, with controlled cooling from austenitic to ferritic phase to minimize precipitate formation 16. This composition achieves magnetic polarization B25 ≥1.60 T at 2500 A/m and permeability μ1.5 ≥1500, demonstrating simultaneous low hysteresis loss and high saturation magnetization 16.
Precipitate control is critical for electrical steel low hysteresis loss steel performance. AlN precipitates, typically 10–100 nm in size, pin domain walls and increase hysteresis loss 5,18. Strategies to mitigate this include:
The number density of Al-based precipitates within 50 μm of the surface critically affects hysteresis loss; reducing this density below 5×10^4 particles/mm² through controlled pickling and annealing achieves iron loss reductions of 0.2–0.5 W/kg 5,18.
The manufacturing route for electrical steel low hysteresis loss steel begins with steel slab casting, followed by hot rolling at temperatures typically 1100–1250°C to achieve thickness reductions from 200–250 mm slabs to 2.0–3.0 mm hot-rolled strips 2. For non-oriented steels, controlled cooling from austenitic temperatures (>1150°C) through mixed austenite-ferrite regions to fully ferritic structures (<1050°C) minimizes precipitate formation and optimizes magnetic properties 16.
Hot-rolled sheet annealing at 900–1100°C for 30–120 seconds homogenizes microstructure and partially dissolves precipitates 5. Pickling removes surface scale using acidic solutions (HCl, H2SO4) at pH 1.0–3.0 and temperatures 60–90°C; the addition of specific elements (Cu: 0.1–5.0 g/L, Zn: 0.1–3.0 g/L, Ni: 0.1–2.0 g/L) to the pickling solution promotes beneficial precipitate morphology changes 18.
Cold rolling reduces thickness to final gauge (typically 0.23–0.35 mm for grain-oriented, 0.15–0.65 mm for non-oriented steels) with total reductions of 80–90% 2,9. For ultra-thin non-oriented electrical steel low hysteresis loss steel (<0.30 mm thickness), achieving surface arithmetic mean roughness Ra ≤0.2 μm at 20 μm cutoff wavelength is critical; this reduces hysteresis loss by 0.3–0.8 W/kg compared to conventional surface finishes (Ra: 0.4–0.6 μm) 9.
Intermediate annealing between cold rolling passes (for multi-stage rolling) at temperatures 700–900°C for 1–5 minutes prevents excessive work hardening and maintains rollability 2. The final cold rolling pass imparts crystallographic texture that influences subsequent recrystallization behavior 3.
Final annealing is the critical step for developing optimal microstructure and magnetic properties in electrical steel low hysteresis loss steel. For grain-oriented steels, a two-stage process is employed:
For ultra-thin grain-oriented steels, controlled nitriding during primary recrystallization (nitriding rate ΔN/Δt ≥0.025, typically achieved by exposing to NH3-containing atmospheres at 750–850°C for 10–60 seconds) stabilizes inhibitor precipitates and reduces hysteresis loss ratio 11.
Non-oriented electrical steel low hysteresis loss steel undergoes single-stage final annealing at 800–1050°C for 1–10 minutes in protective atmospheres (H2, N2, or dissociated ammonia) to recrystallize the cold-worked structure and develop random texture 5,16. Rapid heating rates (>50°C/s) and short holding times minimize precipitate coarsening while achieving complete recrystallization 5.
After final annealing, surface treatments are applied to reduce core loss and provide electrical insulation. For grain-oriented electrical steel low hysteresis loss steel, tension coatings (typically phosphate-based with colloidal silica) apply tensile stress of 5–15 MPa to the steel surface, reducing 180° magnetic domain width and eddy current loss 6,8. Coating thickness ranges from 1–5 μm with thermal expansion coefficient mismatched to steel substrate 6.
Non-oriented electrical steel low hysteresis loss steel may receive intrinsically formed insulating layers of Al2O3 and/or SiO2 (thickness 10–100 μm) during final annealing in oxidizing atmospheres, providing electrical insulation while reducing scaling and improving rollability 12,17. Alternatively, organic or inorganic insulation coatings (0.5–3.0 μm thickness) are applied by roll coating or spray methods 2.
Laser irradiation is a widely adopted technique for refining magnetic domains in grain-oriented electrical steel low hysteresis loss steel, reducing eddy current loss while carefully managing hysteresis loss. The process involves scanning a focused laser beam (typically Nd:YAG or fiber laser, wavelength 1064 nm, power 50–500 W) across the steel surface perpendicular to the rolling direction at intervals of 2–10 mm 1,6,8.
The laser creates localized melting and resolidification, forming a solidified layer with thickness ≤4 μm and introducing compressive stress that subdivides 180° magnetic domains 6,8. Critical parameters include:
Optimized laser irradiation reduces core loss by 5–15% (e.g., from 0.90 W/kg to 0.78 W/kg at 1.7 T, 50 Hz) while maintaining magnetostriction below 1.5×10^-6 and noise levels below 45 dBA 6,8. Surface roughness Rz at laser-irradiated portions should be minimized (<20 μm) with concave portions having width ≤200 μm and depth ≤10 μm to prevent excessive hysteresis loss increase 6,8.
Electron beam irradiation offers advantages over laser treatment for electrical steel low hysteresis loss steel by introducing thermal strain with reduced hardening and residual stress 7,13. The process employs accelerating voltages of 100–175 kV, beam currents of 5–50 mA, and scanning speeds ≤30 m/s 13. Beam control coils and stigmameter adjust energy intensity distribution and beam diameter to optimize hysteresis loss reduction 7.
Key performance metrics achieved through optimized electron beam irradiation include:
Electron beam irradiation with charged particles having mass smaller than Fe (e.g., electrons, protons) minimizes excessive hardening compared to heavier ion beams, achieving low iron loss (<0.80 W/kg at 1.7 T, 50 Hz) while maintaining low noise characteristics 13.
Mechanical groove formation provides an alternative domain refinement approach for grain-oriented electrical steel low hysteresis loss steel. Grooves are formed on one or both surfaces at angles of 60–120° to the rolling direction with intervals of 2–10 mm, using mechanical scribing, rolling with patterned rolls, or laser ablation 1,10.
Optimal groove geometries include:
The groove bottom portion must have arithmetic mean roughness Ra ≤5.0 μm and absolute skewness |Rsk| ≤2.0 to minimize unevenness and facilitate domain wall movement, thereby reducing hysteresis loss 1. Tensile stress with maximum value 20–300 MPa acts in the rolling direction within 10–300 μm from groove side surfaces, contributing to domain refinement 10.
Properly designed grooves reduce iron loss by 6–10% while maintaining mechanical integrity and coating adhesion 1,10. Excessive groove depth or surface roughness increases hysteresis loss due to impeded domain wall motion, emphasizing the importance of precise geometric control 1.
| Org | Application Scenarios | Product/Project | Technical Outcomes |
|---|---|---|---|
| NIPPON STEEL CORPORATION | Transformer cores and power distribution systems requiring low core loss and high energy efficiency with magnetic domain refinement. | Grain-Oriented Electrical Steel Sheet with Groove Domain Refinement | Achieved reduced iron loss through controlled groove formation with Ra ≤5.0 μm and |Rsk| ≤2.0, minimizing unevenness to facilitate domain wall movement and reduce hysteresis loss by 6-10%. |
| JFE STEEL CORPORATION | Low-noise transformers and power converters requiring reduced iron loss without deteriorating acoustic performance. | Electron Beam Irradiated Grain-Oriented Electrical Steel | Optimized electron beam irradiation with accelerating voltage 100-175 kV achieves 8-12% core loss reduction and maintains hysteresis loss increase below 5% while keeping noise levels under 45 dBA. |
| NIPPON STEEL CORPORATION | High-efficiency transformers and electrical equipment operating under high flux density conditions up to 1.9 T. | Laser-Refined Low Core Loss Grain-Oriented Electrical Steel | Laser irradiation creates solidified layers ≤4 μm thick with surface roughness Rz <20 μm, reducing core loss by 5-15% (from 0.90 to 0.78 W/kg at 1.7 T, 50 Hz) while maintaining magnetostriction below 1.5×10⁻⁶. |
| POSCO Co. Ltd | Compact transformers and miniaturized power conversion systems requiring ultra-thin electrical steel with low hysteresis loss. | Ultra-Thin Grain-Oriented Electrical Steel Sheet | Controlled nitriding during primary recrystallization with ΔN/Δt ≥0.025 reduces hysteresis loss ratio to total iron loss below 0.35, achieving enhanced magnetic properties in sheets <0.23 mm thickness. |
| Salzgitter Flachstahl GmbH | High-speed electric motors and variable frequency drive systems requiring stable magnetic performance across wide frequency ranges. | High-Aluminum Non-Oriented Electrical Steel Strip | Al content 1-12% with intrinsic Al₂O₃/SiO₂ insulating layer (10-100 μm) achieves frequency-independent magnetic properties and minimized hysteresis losses, suitable for high-frequency applications. |