EMI, EMC, and Shielding Shielding and Enclosure Design Informational

What is the shielding effectiveness of common enclosure materials at microwave frequencies?

The shielding effectiveness (SE) of enclosure materials at microwave frequencies is dominated by the absorption loss (which depends on conductivity and permeability) and the reflection loss (which depends on the impedance mismatch between free space and the material). For solid panels thicker than a few skin depths, the SE is extremely high and the practical SE is limited by apertures, not the material. Material comparison at 1 GHz for 0.5 mm thick panels: (1) Copper (sigma = 5.8e7 S/m, mu_r = 1): skin depth = 2.1 um. Absorption = 8.686 × 500/2.1 = 2070 dB. Reflection = 71 dB. Total SE > 2000 dB (wall is not the limiting factor). (2) Aluminum (sigma = 3.8e7 S/m, mu_r = 1): skin depth = 2.6 um. Absorption = 1671 dB. Reflection = 69 dB. Total SE > 1700 dB. Excellent. (3) Steel (sigma = 1.0e7 S/m, mu_r = 200 typ): skin depth = 0.11 um. Absorption = 39,000+ dB. Reflection reduced by low sigma but enhanced by high mu. Total SE > 80 dB at 1 GHz. Excellent for both electric and magnetic fields (unlike copper/aluminum which have lower SE for magnetic fields at low frequencies). (4) Mu-metal (sigma = 1.7e6 S/m, mu_r = 20,000): skin depth = 0.003 um at 1 GHz. SE > 200 dB. But expensive and fragile; used primarily for low-frequency magnetic shielding. (5) Conductive plastic (carbon-filled or metal-plated): sigma = 1-100 S/m (much lower than metals). Skin depth at 1 GHz ≈ 0.5-5 mm. SE = 15-40 dB (just the plating or fill material). Much lower than solid metal but sufficient for many commercial EMC applications. (6) Conductive paint (silver or copper paint on plastic housing): sigma = 1e4 - 1e6 S/m. Thickness: 25-75 um. SE = 30-60 dB at 1 GHz. Applied to low-cost plastic enclosures. For most RF enclosures at microwave frequencies: any solid metal panel (aluminum, copper, steel) provides SE > 80 dB. The enclosure SE is almost always limited by apertures, not the wall material.
Category: EMI, EMC, and Shielding
Updated: April 2026
Product Tie-In: Enclosures, Gaskets, Absorbers, Filters

Enclosure Material SE

Material selection for RF enclosure shielding involves balancing SE, weight, cost, thermal conductivity, and manufacturability.

Material Properties Table

Key properties for shielding: (1) Aluminum 6061-T6: sigma = 2.5e7 S/m. Weight: 2.7 g/cm³ (light). Thermal: 167 W/m·K (good heat sinking). Cost: low. Machinability: excellent (easy CNC). Corrosion: self-passivating oxide (but non-conductive oxide can degrade SE at seams). Most common RF enclosure material. (2) Copper C110: sigma = 5.8e7 S/m (highest conductivity). Weight: 8.9 g/cm³ (heavy). Thermal: 388 W/m·K (best for heat sinking). Cost: moderate-high. Used for high-performance filter boxes, cavity filters, and waveguide. Tarnishes (requires plating or surface treatment for seam conductivity). (3) Brass (CuZn): sigma = 1.5e7 S/m. Weight: 8.5 g/cm³. Good machinability. Used for precision machined connectors and filter housings. (4) Mild steel (1008/1010): sigma = 6e6 S/m, mu_r = 100-500. Weight: 7.9 g/cm³. Excellent magnetic shielding at low frequencies. Corrosion-prone (requires plating: zinc, nickel, or tin). Used for EMI enclosures where magnetic field shielding is needed (power supply enclosures, relay housings). (5) Stainless steel 304: sigma = 1.4e6 S/m, mu_r = 1 (non-magnetic). Poor conductor (SE relies on thickness). Used where corrosion resistance is paramount (outdoor enclosures, marine environments). (6) Die-cast zinc (Zamak): sigma = 1.7e7 S/m. Weight: 6.6 g/cm³. Excellent castability for complex shapes. Used for high-volume commercial RF enclosures (routers, access points).

Non-Metal Shielding Options

For lightweight or low-cost enclosures where plastic is the base material: (1) Vacuum metallization: thin metal layer (0.5-5 um) deposited on the plastic interior. Materials: aluminum (most common), copper, or nickel. SE = 30-50 dB (limited by the thin layer and contact quality at seams). (2) Conductive paint/spray: silver, copper, or nickel-filled paint. Thickness: 25-75 um. Sheet resistance: 0.05-1.0 ohm/square. SE = 30-60 dB. Cost: moderate (material is expensive, but the process is simple). (3) Metal foil tape: copper or aluminum foil tape applied to the interior. Excellent SE (60+ dB) if properly applied with overlapping seams. Labor-intensive for production; suitable for prototypes and small quantities. (4) Conductive plastic compounds: carbon fiber, carbon black, or metal fiber filled polymers. SE = 15-40 dB depending on filler loading and frequency. Used for molded EMI enclosures in consumer electronics. (5) Metal mesh embedded in plastic: a fine metal mesh is insert-molded into the plastic part. SE = 30-50 dB. Provides structural and shielding functions in one part.

Selection Guide

For SE > 60 dB (military, medical, sensitive receivers): aluminum or copper machined enclosure with EMI gaskets at all seams. For SE > 40 dB (commercial wireless, consumer electronics): aluminum or zinc die-cast enclosure. Painted or conductive plastic with proper seam treatment. For SE > 20 dB (basic EMC compliance): conductive paint on plastic, or metallized plastic. Adequate for many FCC Part 15 Class B applications. Weight-critical applications (aerospace, handheld devices): thin aluminum (0.3-0.5 mm), carbon fiber composite with conductive mesh, or metallized plastic.

Material SE Values
δ = √(1/(πfμ₀μᵣσ)) skin depth
A = 8.686 × t/δ dB (absorption)
Copper @1GHz: δ=2.1μm, SE > 2000 dB
Aluminum @1GHz: δ=2.6μm, SE > 1700 dB
Conductive paint: SE = 30-60 dB typical
Common Questions

Frequently Asked Questions

Is aluminum or steel better for EMI shielding?

At RF/microwave frequencies (> 1 MHz): aluminum and steel both provide SE > 80 dB for solid panels. The panel material is not the limiting factor. At low frequencies (< 100 kHz): steel is better for magnetic field shielding because its high permeability (mu_r = 100-500) increases the absorption loss for H-fields. Aluminum (mu_r = 1) has very low magnetic shielding at low frequencies. For DC magnetic fields (permanent magnets, Earth field): only high-permeability materials (mu-metal, steel) provide shielding. Aluminum provides zero DC magnetic shielding. For most RF enclosures: aluminum is preferred due to lighter weight, better machinability, and lower cost. Steel or mu-metal is added selectively for low-frequency magnetic shielding if required (e.g., around a VCO or sensitive receiver where external magnetic fields cause frequency pulling).

Does wall thickness matter at microwave frequencies?

For SE through the wall: not really, as long as the wall is thicker than a few skin depths. At 1 GHz: copper skin depth = 2.1 um. A 0.1 mm (100 um) wall = 48 skin depths. Absorption = 417 dB. Even a 0.01 mm (10 um) copper foil at 1 GHz: 5 skin depths = 43 dB absorption + 71 dB reflection = 114 dB total. Beyond adequate. Wall thickness matters for: mechanical rigidity (thinner walls flex, opening seam gaps), thermal conductivity (thicker walls spread heat better), and low-frequency magnetic shielding (thicker steel walls = more absorption at low frequencies).

Can I use conductive fabric for EMI shielding?

Yes. Conductive fabrics (silver-plated nylon, copper-plated polyester, stainless steel woven fabric) provide SE of 30-70 dB depending on the weave density and metallization quality. Applications: EMI shielding tent/draping for field testing, cable shielding braid (flexible), gasket material (conductive fabric over an elastomer core), and personal radiation protection (RF-blocking garments). Limitations: the fabric SE degrades at seams and openings (same as any shielded enclosure). The surface resistance is typically 0.01-1.0 ohm/square (higher than solid metal). Washable conductive fabrics degrade after repeated laundering (the metal coating wears off).

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