MAY 20, 202658 MINS READ
Bulk metallic glasses are metastable amorphous solids formed by quenching molten multicomponent alloys at cooling rates sufficient to suppress crystallization 1. The critical cooling rate—the minimum rate required to bypass nucleation and growth of crystalline phases—defines the processability of a given alloy system 5. For BMGs, critical cooling rates typically range from 1 K/s to 100 K/s, significantly lower than the 10⁵ K/s required for conventional metallic glasses, enabling casting of bulk sections with thicknesses from millimeters to centimeters 7,9.
The glass-forming ability (GFA) of an alloy is quantitatively assessed through thermal parameters derived from differential scanning calorimetry (DSC). The supercooled liquid region, ΔTₓ = Tₓ − Tg (where Tₓ is the crystallization temperature and Tg is the glass transition temperature), serves as a primary indicator: alloys exhibiting ΔTₓ > 20 K demonstrate robust GFA 6,13. The reduced glass transition temperature, Trg = Tg/Tl (where Tl is the liquidus temperature), provides another criterion; Trg ≥ 0.6 correlates with high amorphous formability in Fe-based systems 9,12. Theoretical modeling of liquidus temperature depression through multicomponent alloying—incorporating refractory metals (Mo, W, Cr) and metalloids (B, C, Si)—enables rational composition design to maximize GFA while maintaining target functional properties 6,10.
Within the supercooled liquid region, BMGs exhibit viscoelastic behavior and can be thermoplastically formed under applied pressure, analogous to polymer processing 1. This unique deformation mode, absent in crystalline metals, underpins net-shape forming techniques such as blow molding and embossing. However, if cooling rates fall below critical thresholds during solidification or reheating, heterogeneous nucleation at impurity sites or mold interfaces triggers crystallization, degrading the amorphous structure and forfeiting the material's superior properties 2,5,20.
Iron-based BMGs have attracted significant interest due to their potential for low-cost production, soft magnetic properties, and high specific strength 4,6,9. Exemplary compositions contain 59–70 at.% Fe alloyed with 10–20 at.% metalloids (B, C, Si, P) and 10–25 at.% refractory metals (Mo, W, Cr, Nb) 6,9,12. A representative formulation is Fe₁₀₀₋ₐ₋ᵦ₋꜀₋ᵈ₋ₓ₋ᵧMₐNbᵦSi꜀BᵈIₓJᵧ, where M = Co and/or Ni, I includes Al, Cr, Cu, Mn, C, P, and J encompasses Ti, S, N, O, with constraints: 0 < a ≤ 46.1 wt.%, 5.4 ≤ b ≤ 12.4 wt.%, 2.2 ≤ c ≤ 4.4 wt.%, 2 < d ≤ 6 wt.%, x ≤ 2 wt.%, y ≤ 0.2 wt.% 4.
The FeNbBSi system is particularly notable for soft magnetic applications, exhibiting coercivity < 10 A/m and relative permeability > 10⁴ at 1 kHz 4. Controlled impurity levels (especially O, N, S < 200 ppm) are critical to prevent heterogeneous nucleation during casting 4. X-ray diffraction (XRD) patterns of fully amorphous Fe-based BMGs display a single broad halo centered at 2θ ≈ 44° (Cu Kα radiation), confirming absence of long-range atomic order 9,12,19. Some Fe-based BMGs are ferromagnetic at room temperature (e.g., Fe₆₀Co₈Ni₈Mo₅Zr₁₀B₁₅), while others with higher Cr or Mo content are non-ferromagnetic, enabling tailored magnetic responses 6,9.
Titanium-based BMGs offer high specific strength (strength-to-density ratio > 400 MPa·cm³/g) and excellent corrosion resistance, suitable for biomedical and aerospace applications 13,14. A general formulation is Ti₁₀₀₋ₐ₋ᵦ₋꜀₋ᵈNiₐCuᵦSi꜀Snᵈ, where 15 ≤ a ≤ 35, 4 ≤ b ≤ 15, 2 ≤ c ≤ 12, 4 ≤ d ≤ 10, and Ti content exceeds 45 at.% 13,14. Specific examples include Ti₆₀Ni₂₄Cu₈Si₄Sn₄, Ti₆₆Ni₂₂Cu₄Si₄Sn₄, and Ti₆₈Ni₂₀Cu₇Si₄Sn₆ 14. The addition of Sn (4–10 at.%) stabilizes the supercooled liquid and suppresses competing intermetallic phases, enhancing GFA 13.
Theoretical liquidus temperature calculations guide composition optimization: by balancing the enthalpies of mixing among constituent elements, substantial refractory metal content (e.g., Mo, W up to 15 at.%) can be incorporated while maintaining Tl depression necessary for bulk glass formation 6,13. Ti-based BMGs typically exhibit Tg in the range 350–450°C and ΔTₓ = 30–60 K, enabling thermoplastic forming in the supercooled liquid region 13,14.
Gold-based BMGs have been developed for ornamental and jewelry applications, offering improved tarnish resistance and mechanical durability compared to conventional gold alloys 1. These compositions leverage the intrinsic nobility of gold combined with the amorphous structure's resistance to surface oxidation and corrosion. Critical casting thickness for Au-based BMGs ranges from 0.5 to 3 mm, sufficient for watch cases, bezels, and decorative components 1. The amorphous microstructure eliminates grain boundaries, which are preferential sites for tarnish initiation, thereby extending the aesthetic lifespan of jewelry pieces 1.
BMG parts are typically produced by melting master alloys in inert atmospheres (Ar or He) and pouring the molten alloy into metallic or ceramic molds pre-cooled to extract heat at rates exceeding the critical cooling rate 3,4,18. The critical casting thickness, dc, is the maximum section dimension that can be solidified amorphously under given cooling conditions and is inversely related to the critical cooling rate: dc ∝ (Tl − Tg)/Rc, where Rc is the critical cooling rate 5,7. For high-GFA alloys (e.g., Zr-based BMGs), dc can exceed 50 mm, whereas marginal glass-formers may be limited to < 1 mm 5.
Mold material selection profoundly influences crystallization kinetics. Conventional crystalline molds (e.g., Cu, steel) present grain boundaries that act as heterogeneous nucleation sites, promoting crystallization at the mold-alloy interface 20. To mitigate this, molds can be coated with amorphous materials (e.g., amorphous silica, carbon-based coatings) to eliminate nucleation sites and improve surface finish 20. Wetting properties between the molten BMG and mold coating must be optimized: low wetting (contact angle > 90°) reduces interfacial heat transfer, potentially lowering cooling rates, while high wetting (contact angle < 90°) enhances heat extraction but may increase adhesion and demolding difficulty 20.
For large-scale BMG components exceeding the critical thickness of a single pour, multi-inlet casting techniques have been developed 3. Molten amorphous alloy is introduced simultaneously from at least two inlets into a mold cavity, and the molten streams bond in situ before solidification 3. This approach enables fabrication of bulk sections (e.g., > 10 cm diameter) by ensuring that local cooling rates remain above critical values throughout the part 3.
Additive manufacturing (AM) techniques, including selective laser melting (SLM) and layer-by-layer deposition, have been adapted for BMG fabrication to overcome geometric constraints of casting 5. In layer-by-layer construction, thin layers (50–200 μm) of BMG powder or wire feedstock are sequentially melted and solidified 5. Rapid localized heating (via laser or electron beam) followed by conductive cooling into the substrate achieves cooling rates > 10³ K/s, sufficient to maintain amorphous structure even in alloys with moderate GFA 5.
Key process parameters include laser power (100–400 W), scan speed (200–1000 mm/s), and layer thickness, which collectively determine the thermal gradient and solidification rate 5. Post-deposition annealing in the supercooled liquid region (Tg < T < Tₓ) can relieve residual stresses without inducing crystallization, provided hold times are < 10 minutes 5. AM-produced BMG parts exhibit mechanical properties comparable to cast counterparts, with tensile strengths of 1.5–2.0 GPa and elastic limits of 2% strain 5.
Marginal glass-formers and nanocrystalline precursors can be consolidated into bulk amorphous or composite articles using rapid capacitor discharge forming (RCDF) 16. In this technique, metallic glass-forming alloy powder (particle size 10–100 μm) is packed into a green body and subjected to a high-energy electrical pulse (discharge time < 1 ms, peak current > 10 kA) 16. Joule heating rapidly elevates the powder compact to temperatures between Tg and Tl, enabling viscous flow and inter-particle bonding, while the short pulse duration limits heat diffusion and maintains cooling rates above critical thresholds 16.
Alternatively, stacked amorphous foils (thickness 20–50 μm) can be consolidated by heating to the supercooled liquid region under applied pressure (10–100 MPa) and subsequently quenched 16. This method is particularly effective for producing near-net-shape components with complex geometries, as the foil stacking allows conformal filling of mold cavities 16. Consolidated BMG parts exhibit relative densities > 99% and retain > 95% amorphous fraction, as verified by XRD and DSC 16.
Flame spraying and high-velocity oxy-fuel (HVOF) spraying enable deposition of BMG coatings onto substrates with thicknesses exceeding the critical casting thickness of the alloy 11. Molten or semi-molten BMG droplets (diameter 10–50 μm) impact the substrate at velocities of 100–300 m/s, flattening into splats (thickness 1–5 μm) that solidify at cooling rates of 10⁴–10⁶ K/s, well above critical rates 11. The substrate must be maintained at temperatures sufficiently low (typically < 200°C) to extract heat rapidly from impinging droplets, thereby preserving the amorphous structure 11.
HVOF-sprayed BMG coatings exhibit hardness values of 800–1200 HV, porosity < 2%, and bond strengths > 50 MPa to metallic substrates 11. These coatings provide wear resistance, corrosion protection, and can be applied to complex geometries unsuitable for bulk casting 11. Post-spray annealing in the supercooled liquid region can densify the coating and reduce residual stresses, though care must be taken to avoid crystallization 11.
X-ray diffraction (XRD) is the primary method for confirming amorphous structure: fully amorphous BMGs produce diffraction patterns with a single broad halo lacking sharp Bragg peaks, indicative of short-range order without translational symmetry 9,19. Quantitative phase analysis via Rietveld refinement of XRD data can determine the volume fraction of residual crystalline phases (detection limit ≈ 2 vol.%) 2.
Differential scanning calorimetry (DSC) measures Tg, Tₓ, and the enthalpy of crystallization (ΔHₓ), providing insights into thermal stability and degree of amorphicity 2,13. A sharp exothermic peak at Tₓ with ΔHₓ > 50 J/g indicates substantial amorphous content, whereas multiple overlapping peaks suggest partial crystallization or phase separation 2. The glass transition is observed as a step increase in heat capacity at Tg, typically 5–15 J/(mol·K) for metallic glasses 13.
A novel non-destructive method for quantifying amorphous content employs thermal emissivity imaging 2. Specimens are irradiated with passive infrared radiation, and the emitted thermal radiation is captured using an infrared camera 2. Amorphous regions exhibit different emissivity (ε ≈ 0.3–0.4 at λ = 3–5 μm) compared to crystalline regions (ε ≈ 0.5–0.6), due to differences in electronic structure and phonon scattering 2. Image analysis algorithms assess spatial variations in emissivity, enabling mapping of amorphous fraction with spatial resolution < 100 μm 2. This technique is particularly valuable for quality control in manufacturing, as it avoids specimen destruction and can inspect large areas rapidly 2.
Tensile testing of BMGs reveals elastic moduli of 80–120 GPa, yield strengths of 1.5–2.5 GPa, and elastic strain limits of 2–2.5%, significantly exceeding those of crystalline alloys of similar composition 5,7. However, BMGs typically exhibit limited plastic strain (< 1%) in tension due to catastrophic shear band propagation 8. Compressive testing shows higher plastic strains (up to 10%) owing to the suppression of crack opening under compressive stress states 8.
Fracture toughness, KIC, of monolithic BMGs ranges from 20 to 80 MPa·m^(1/2), lower than high-toughness steels but comparable to ceramics 8. To enhance ductility, BMG matrix composites reinforced with ductile crystalline phases (e.g., β-Ti dendrites in Ti-based BMGs) or graphite particles have been developed 8. These composites exhibit fracture toughness > 100 MPa·m^(1/2) and compressive plastic strains > 15%, as
| Org | Application Scenarios | Product/Project | Technical Outcomes |
|---|---|---|---|
| Chow Sang Sang Jewellery Company Limited | Luxury jewelry and watch components including cases, bezels, and decorative elements requiring long-term aesthetic stability and corrosion resistance. | Gold-based BMG Jewelry Components | Superior tarnish resistance through amorphous structure eliminating grain boundaries; enhanced mechanical durability; critical casting thickness 0.5-3 mm suitable for ornamental applications. |
| Apple Inc. | Smartphone and laptop casings, wearable device housings, and precision consumer electronics requiring high strength-to-weight ratio and complex geometries. | Consumer Electronics Enclosures | Non-destructive thermal emissivity imaging enables rapid quality control of amorphous content with <100 μm spatial resolution; layer-by-layer additive manufacturing achieves cooling rates >10³ K/s maintaining amorphous structure; amorphous mold coatings eliminate grain-boundary nucleation sites. |
| The Regents of the University of California | Magnetic cores for transformers and inductors, high-strength structural components in automotive and aerospace, sensor applications requiring soft magnetic response. | Fe-based Amorphous Steel Alloys | Iron content 59-70 at.% with theoretical liquidus temperature optimization; soft magnetic properties with coercivity <10 A/m and permeability >10⁴ at 1 kHz; tensile strength 1.5-2.5 GPa with specific strength >400 MPa·cm³/g. |
| Crucible Intellectual Property LLC | Complex-geometry components for aerospace, medical implants, and custom tooling where traditional casting thickness limitations restrict design freedom. | BMG Additive Manufacturing Systems | Selective laser melting with controlled parameters (100-400 W laser power, 200-1000 mm/s scan speed) achieving >10³ K/s cooling rates; produces parts with tensile strength 1.5-2.0 GPa and 2% elastic strain comparable to cast BMG. |
| OCAS (ArcelorMittal R&D) | Ring-shaped magnetic cores for power electronics, distribution transformers, and high-frequency inductors requiring low core loss and high permeability. | Fe-Nb-B-Si Magnetic Core Materials | FeNbBSi composition with controlled impurities (<200 ppm O, N, S) preventing heterogeneous nucleation; bulk casting thickness >0.5 mm eliminating ribbon-winding processes; cost reduction through simplified manufacturing. |