MAY 14, 202664 MINS READ
Cast copper pure copper electromagnetic shielding material encompasses a spectrum of alloy systems designed to optimize both electrical conductivity and magnetic permeability. The most extensively researched compositions are Cu-Fe binary alloys containing 10.0–50.0 mass% Fe, with additions of 0.001–5.0 mass% total of Ni and/or Co, and ≥10 ppm C 25. These alloys exhibit a characteristic microstructure wherein Fe-based secondary phases crystallize and precipitate within the Cu matrix, forming a heterogeneous structure that simultaneously provides high electrical conductivity (≥20% IACS) and elevated magnetic permeability (≥3.0) 2. The precipitation morphology is critical: for plate materials, Fe-based secondary phases with aspect ratios ≥5 must exist at densities of 10 or more per 0.05 mm thickness in the plate thickness direction, with average aspect ratios exceeding 20 to achieve optimal shielding performance at frequencies ≥5 MHz 13.
The phase distribution in cast copper pure copper electromagnetic shielding material is governed by the eutectic behavior of the Cu-Fe system. During solidification, the immiscibility gap in the Cu-Fe phase diagram leads to liquid phase separation, resulting in a Cu-rich matrix with dispersed Fe-rich droplets that solidify as ferromagnetic inclusions 18. The addition of Co, Ni, Mn, or Cr as dopants modifies the eutectic composition and refines the Fe-phase distribution, enhancing both mechanical workability and electromagnetic response 18. For instance, Co additions stabilize the body-centered cubic (BCC) Fe phase and increase its saturation magnetization, while Ni promotes face-centered cubic (FCC) phase formation, improving ductility without significantly compromising magnetic properties 25.
Advanced formulations incorporate trace elements to further optimize performance. Additions of 0.005–2.0 mass% total of P, Si, Ti, Mg, Ca, Zr, Cr, Al, and/or B serve as grain refiners and deoxidizers, reducing porosity in cast structures and improving mechanical integrity 2513. Zn additions (0.005–5.0 mass%) enhance corrosion resistance, particularly in humid environments, while noble metal additions (0.001–5.0 mass% total of Ag, Sn, In, Mn, Au, and/or Pt) improve contact resistance and long-term stability in electronic applications 2513. The carbon content, maintained at ≥10 ppm, plays a subtle but essential role in controlling Fe-phase nucleation and growth kinetics during solidification and subsequent heat treatment 25.
For applications requiring ultra-high purity, cast copper pure copper electromagnetic shielding material can be formulated with Cu content ≥99.96 mass%, incorporating 10–300 mass ppm of rare earth elements (Ca, Ba, Sr, Zr, Hf, Y, Sc, La, Ce, Pr, Nd, Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu) and/or chalcogens (O, S, Se, Te) 7. These high-purity materials exhibit average crystal grain sizes ≥15 μm on rolled surfaces and high-temperature Vickers hardness of 4.0–10.0 HV at 850°C, making them suitable for power electronics substrates and high-temperature shielding applications 7. Alternatively, materials with Cu content in the range of 99.9–99.999 mass% and average crystal grain sizes ≥10 μm, characterized by misorientation angles ≥40° between adjacent grains (measured by EBSD with 1 μm step size over ≥1 mm² areas), provide excellent thermal conductivity and mechanical stability for insulating substrates in electronic devices 16.
The production of cast copper pure copper electromagnetic shielding material involves carefully controlled melting, casting, and thermomechanical processing sequences to achieve the desired microstructure and properties. The initial step typically involves induction melting of high-purity copper (≥99.9% Cu) with electrolytic iron (≥99.5% Fe) and alloying elements under an inert atmosphere (Ar or N₂) to prevent oxidation 118. Melting temperatures are maintained at 1200–1400°C, well above the liquidus of the Cu-Fe system, to ensure complete dissolution and homogenization of alloying elements 18. For alloys containing reactive elements such as Ti, Zr, or rare earths, vacuum induction melting (VIM) at pressures <10⁻² Pa is preferred to minimize contamination and oxide formation 7.
Casting methods vary depending on the target product form and microstructural requirements. Continuous casting into billets or slabs is employed for large-scale production, with casting speeds of 0.5–2.0 m/min and mold temperatures controlled to 800–1000°C to promote directional solidification and minimize segregation 1. For thin-section products such as foils and tapes, strip casting or twin-roll casting techniques are utilized, producing as-cast thicknesses of 1–5 mm with rapid solidification rates (10²–10⁴ K/s) that refine the Fe-phase dispersion and reduce dendrite arm spacing to <10 μm 68. Investment casting or die casting may be employed for complex-shaped shielding components, with mold preheating to 200–400°C and controlled cooling rates to prevent cracking due to thermal stress 14.
Post-casting thermomechanical processing is critical for developing the desired microstructure in cast copper pure copper electromagnetic shielding material. Hot rolling at temperatures of 700–900°C with total reductions of 50–90% elongates the Fe-phase particles along the rolling direction, increasing their aspect ratios and enhancing magnetic permeability in the plane of the sheet 13. Intermediate annealing at 400–600°C for 1–4 hours in inert or reducing atmospheres (H₂/N₂ mixtures) relieves work hardening and promotes recrystallization of the Cu matrix while maintaining the Fe-phase morphology 25. Cold rolling to final thickness (typically 5–100 μm for foil products) further refines the microstructure and improves surface finish, with reductions per pass limited to 10–30% to prevent edge cracking 6817.
For applications requiring enhanced flexibility and resistance to repeated flexing, surface treatments are applied to cast copper pure copper electromagnetic shielding material. Electroplating of Ni coatings at 90–5000 μg/dm² on one surface of copper foil (5–15 μm thick) significantly improves resistance to copper foil breakage during folding or flexing 817. A subsequent chromium oxide (Cr₂O₃) layer at 5–100 μg/dm² (Cr mass basis) formed by chromate conversion treatment provides additional corrosion protection and maintains shielding performance over extended service life 817. The opposite surface is typically laminated with a resin layer (polyimide, polyester, or epoxy-based) to provide electrical insulation and mechanical support 3891517.
Specialized processing routes have been developed for cast copper pure copper electromagnetic shielding material with tailored surface properties. For plasma display panel (PDP) applications, copper foil surfaces are blackened to reduce reflectivity, with the blackened surface then subjected to nickel conversion treatment (0.1–5.0 mg/dm² Ni) and optional chromate treatment to stabilize the surface against chemical attack during subsequent etching processes 12. The reflectivity change of the blackened surface after copper mesh formation by etching is maintained at ≤2 to ensure consistent optical performance 12. Alternatively, fine roughening particle layers of copper or copper alloys are deposited on copper foil surfaces, followed by smoothening layers of Co, Ni, In, or their alloys to achieve high transmittance while maintaining electromagnetic shielding ability 6. These surfaces may be further treated with silane coupling agents or stainproof treatments to protect against oxidation and contamination 6.
The electromagnetic shielding effectiveness (SE) of cast copper pure copper electromagnetic shielding material arises from three fundamental mechanisms: reflection, absorption, and multiple internal reflections. Reflection occurs at the material surface due to impedance mismatch between free space (377 Ω) and the conductive material (typically <1 Ω for copper-based alloys), with reflection loss (SE_R) proportional to the ratio of material conductivity to frequency: SE_R (dB) ≈ 168 + 10log₁₀(σ_r/μ_r·f), where σ_r is relative conductivity, μ_r is relative permeability, and f is frequency in Hz 24. For pure copper (σ_r ≈ 1.0, μ_r ≈ 1.0), reflection dominates at low frequencies (<1 MHz), providing 80–100 dB attenuation 18. However, as frequency increases, skin depth (δ = √(2/ωμσ), where ω = 2πf, μ is permeability, and σ is conductivity) decreases, reducing the effective shielding volume and necessitating absorption mechanisms 213.
Absorption loss (SE_A) in cast copper pure copper electromagnetic shielding material is governed by eddy current dissipation and magnetic hysteresis losses within the material volume: SE_A (dB) ≈ 131.4·t/δ, where t is material thickness and δ is skin depth 413. For Cu-Fe alloys with 10–50 mass% Fe, the presence of ferromagnetic Fe-phase particles significantly increases μ_r (3.0–50.0 depending on Fe content and morphology), reducing skin depth and enhancing absorption, particularly at frequencies ≥5 MHz where magnetic losses become dominant 2513. The aspect ratio and spatial distribution of Fe-phase particles critically influence absorption: elongated particles with aspect ratios ≥20 aligned parallel to the incident electromagnetic field maximize eddy current path length and hysteresis loss, achieving absorption losses of 40–60 dB in the 10–100 MHz range for 50–100 μm thick foils 13.
Multiple internal reflections (SE_M) contribute additional attenuation when the material thickness is comparable to or greater than the skin depth, with SE_M (dB) ≈ 20log₁₀|1 - exp(-2t/δ)|, becoming significant (>10 dB) when t/δ > 3 4. For cast copper pure copper electromagnetic shielding material, the total shielding effectiveness is approximately SE_total ≈ SE_R + SE_A + SE_M, with reflection and absorption terms dominating in most practical scenarios 2413. Experimental measurements on Cu-Fe alloys (30–95 wt% Cu, 5–70 wt% Fe) embedded in resin matrices demonstrate shielding effectiveness of 50–70 dB across the 1–100 MHz frequency range, with peak performance at 10–50 MHz where both conductivity and permeability contribute optimally 14.
The frequency-dependent behavior of cast copper pure copper electromagnetic shielding material is further influenced by the dielectric properties of any resin binder or substrate. For composite formulations containing 70–98 wt% of dendritic copper fillers (0.1–50 μm length) and flaky copper fillers (0.1–50 μm diameter) dispersed in resin binders, the volume resistivity of the cured composite ranges from 10⁻⁵ to 10⁻³ Ω·cm, providing effective shielding (30–50 dB) while maintaining processability for screen printing or spray application 14. The dendritic morphology of copper fillers creates percolation networks at lower filler loadings (typically 40–60 vol%) compared to spherical particles, reducing composite viscosity and enabling thinner coatings (10–50 μm) with equivalent shielding performance 14.
For low-frequency applications (<1 MHz), where magnetic field shielding is critical, cast copper pure copper electromagnetic shielding material formulations incorporate iron fibers (20–30 wt%) and silver-coated copper particles (10–20 wt%) in polyvinyl chloride (PVC) resin matrices (50–60 wt%) with coupling agents (5–8 wt%) to enhance interfacial bonding 4. This composite architecture achieves shielding effectiveness of 60 dB at 1 MHz, decreasing to 50 dB at 100 MHz, demonstrating superior low-frequency performance compared to pure copper foils (30–40 dB at 1 MHz) 4. The iron fibers provide high permeability (μ_r ≈ 100–1000) for magnetic field absorption, while the silver-coated copper particles ensure electrical continuity and minimize contact resistance 4.
Cast copper pure copper electromagnetic shielding material finds extensive application in plasma display panels (PDPs) and other flat-panel displays, where it serves dual functions of electromagnetic interference suppression and optical transparency enhancement. Copper foil composites with thicknesses of 5–15 μm, laminated to transparent resin films (polyethylene terephthalate or polycarbonate, 25–100 μm thick), are patterned by photolithography and etching to form fine mesh structures with line widths of 10–30 μm and aperture ratios of 70–90% 36915. The mesh geometry is optimized to provide shielding effectiveness >40 dB at frequencies >30 MHz (the primary emission band of PDP discharge) while maintaining visible light transmittance >85% 612. Surface treatments, including Ni conversion (0.1–5.0 mg/dm²) and chromate passivation, stabilize the copper mesh against corrosion during panel assembly and service, with reflectivity changes limited to ≤2 after etching to ensure consistent optical performance 12.
The manufacturing process for PDP shielding materials involves joining multiple copper foil composites in the longitudinal direction to produce continuous rolls suitable for large-area panel fabrication 3915. Overlapped joints between composites are bonded with epoxy adhesives containing flexibility-imparting rubbers (nitrile-butadiene, natural rubber, styrene-butadiene, or acrylic rubber) to prevent deformation during winding and lamination 3915. The adhesive overlap length is precisely controlled to 1–6 mm to balance joint strength (≥5 N/cm peel strength) with flexibility (≥180° bend without cracking) 3915. This joining technology enables production of shielding materials in widths up to 1500 mm and lengths exceeding 1000 m, meeting the scale requirements of modern PDP manufacturing lines 915.
In printed circuit board (PCB) applications, cast copper pure copper electromagnetic shielding material is employed as ground planes, shielding layers, and electromagnetic compatibility (EMC) structures to prevent crosstalk between high-speed signal traces and to contain radiated emissions from active components 81417. Copper foils with thicknesses of 9–70 μm (corresponding to 1/4 oz to 2 oz copper weight) are laminated to FR-4, polyimide, or liquid crystal polymer (LCP) substrates using epoxy or acrylic adhesives, with peel strengths ≥1.0 N/mm required for reliable via formation and component assembly 817. For flexible PCBs and wearable electronics, ultra-thin copper foils (5–12 μm) with Ni/Cr surface treatments are laminated to polyim
| Org | Application Scenarios | Product/Project | Technical Outcomes |
|---|---|---|---|
| POSCO | Electromagnetic interference suppression in consumer electronics, automotive electronics, and telecommunications equipment requiring broad-spectrum shielding. | Cu-Fe Alloy Powder EMI Shielding Material | Achieves 50-70 dB shielding effectiveness across 1-100 MHz frequency range using copper-iron alloy powder (30-95 wt% Cu, 5-70 wt% Fe) embedded in resin matrix, with minimized manufacturing process and reduced cost. |
| KOBE STEEL LTD | High-frequency electromagnetic shielding applications in power electronics, RF equipment, and wireless communication devices operating above 5 MHz. | Cu-Fe-based Copper Alloy for EMI Shielding | Provides electrical conductivity ≥20% IACS and magnetic permeability ≥3.0 with shielding effectiveness exceeding 60 dB at frequencies ≥5 MHz through optimized Fe-based secondary phase precipitation in Cu matrix (10.0-50.0 mass% Fe). |
| JX NIPPON MINING & METALS CORPORATION | Plasma display panels and flat-panel displays requiring transparent electromagnetic shielding with optical performance maintenance. | Copper Foil Composite for PDP Shielding | Achieves >40 dB shielding effectiveness at >30 MHz with >85% visible light transmittance using fine mesh copper structures (10-30 μm line width) with Ni/Cr surface treatments for enhanced durability and flexibility. |
| FURUKAWA CIRCUIT FOIL CO. LTD. | PDP electromagnetic shields and transparent conductive applications requiring particle-free surfaces and long-term reliability. | Electromagnetic Shielding Copper Foil with Surface Treatment | Delivers superior electromagnetic shielding ability and high transmittance through fine roughening particle layers of copper/copper alloy with smoothening layers of Co/Ni/In, preventing particle shedding while maintaining surface stability. |
| MITSUBISHI MATERIALS CORPORATION | Power electronics substrates, high-temperature electromagnetic shielding, and insulating substrates in electronic devices requiring thermal conductivity and mechanical stability. | High-Purity Copper Material for Power Electronics | Exhibits high-temperature Vickers hardness of 4.0-10.0 HV at 850°C with average crystal grain size ≥15 μm and Cu content ≥99.96 mass%, incorporating 10-300 ppm rare earth/chalcogen elements for enhanced thermal stability. |