Board-Level Shielding as a Complement to Ferrite Bead and EMI Filter Strategies
Why ferrite beads and LC filters alone fail radiated EMI targets—and how PCB shield cans with low-impedance spring contacts close the gap.
Executive Summary
Ferrite beads and discrete EMI filters are the default first line of defense against conducted emissions on power rails and signal lines—but they do not attenuate radiated emissions from high-speed digital ICs, switch-mode converters, or RF oscillator sections once energy has coupled into free space or board-level cavity modes. For products targeting CISPR 25 Class 5 radiated limits (automotive), IEC 61000-4-3 immunity requirements (industrial), or MIL-STD-461G RE102 (defense), board-level metallic shielding is not optional—it is the design closure mechanism that ferrite beads cannot provide. POCONS USA's custom two-piece shield cans and precision spring contacts deliver ≥60 dB shielding effectiveness from 200 MHz to 6 GHz with contact resistance below 50 mΩ, providing the low-impedance enclosure boundary that converts a marginally passing design into a design with verified margin.
Technical Specifications & Attenuation Data
The fundamental limitation of ferrite bead filtering is modal: ferrite beads suppress common-mode and differential-mode conducted noise along a specific trace or pin. They present a frequency-dependent lossy impedance—typically peaking between 100 MHz and 600 MHz for standard NiZn formulations—that converts conducted RF energy to heat. This mechanism is effective for power supply decoupling, preventing high-frequency switching noise from propagating along VCC rails, and damping parasitic oscillations at IC outputs.
However, ferrite beads do nothing to contain radiated emissions from the IC die, bond wires, package leads, or PCB trace segments that act as unintentional antennas. A 10 mm trace segment resonates as a quarter-wave monopole at approximately 7.5 GHz and radiates efficiently across a broad bandwidth well below that frequency. No amount of conducted filtering on the supply pins will suppress the electromagnetic field emanating from the signal routing itself.
Board-level shield cans address this gap directly. A properly grounded metallic enclosure surrounding the offending circuit section provides shielding effectiveness (SE) governed by reflection loss, absorption loss, and the quality of the enclosure's ground boundary.
| Parameter | POCONS Shield Can Specification | Reference Standard | |---|---|---| | Shielding Effectiveness (200 MHz–1 GHz) | ≥60 dB | IEEE 299 / MIL-STD-285 methodology | | Shielding Effectiveness (1 GHz–6 GHz) | ≥50 dB | IEEE 299.1 (small enclosures) | | Wall Material | Tin-plated cold-rolled steel (CRS), 0.20 mm nominal | — | | Sheet Resistance | ≤1.5 mΩ/sq | ASTM B539 | | Relative Permeability (µr) | 100–200 (CRS) | Enhances absorption loss below 500 MHz | | Spring Contact Resistance (initial) | 20–30 mΩ | EIA-364-06 | | Spring Contact Resistance (after 10⁶ cycles) | ≤50 mΩ | EIA-364-09 | | Contact Normal Force | 0.3–0.8 N per contact | — | | Operating Temperature | –40°C to +125°C | AEC-Q200 aligned | | Dimensional Tolerance (stamped) | ±0.05 mm | — |
The material choice matters. Tin-plated CRS provides both high conductivity for reflection loss at GHz frequencies and ferromagnetic permeability for absorption loss at lower frequencies. For applications requiring nonmagnetic shielding—such as proximity to magnetic sensors or compass modules—POCONS also supplies tin-plated brass and copper-alloy shield cans, trading absorption loss below 500 MHz for magnetic neutrality.
Spring contacts are the critical interface between the shield can and the PCB ground plane. Each contact point must maintain low impedance across the full operating frequency range. At 2.4 GHz, a 50 mΩ contact with 0.5 nH of parasitic inductance presents approximately 7.9 Ω of impedance—still low enough to maintain enclosure integrity if contact spacing is held below λ/20 (approximately 6 mm at 2.4 GHz). POCONS spring contacts are designed with gold-over-nickel plating on beryllium copper substrates, achieving the required contact resistance while providing the mechanical compliance for repeated lid removal during prototyping and rework.
Common Design Pitfalls
1. Insufficient ground pad copper area creates an inductive return path. The PCB footprint for a shield can must provide a continuous, unbroken ground copper ring on the surface layer, connected to the internal ground plane with a via fence at ≤2 mm pitch. Engineers frequently use narrow ground traces (0.3 mm) or rely on a small number of widely spaced vias. The consequence is a high-inductance return path that degrades shielding effectiveness by 15–25 dB above 1 GHz. The mitigation is a minimum 1.0 mm wide copper pad ring with stitching vias on 1.5 mm centers, tied to an uninterrupted internal ground plane.
2. Traces or signal vias routed underneath shield can walls create slot antenna radiation. Any trace that crosses under the shield can wall perimeter acts as an excitation source for a slot antenna formed by the gap between the can wall and the ground plane. Even a single 0.15 mm trace crossing under the wall can degrade SE by 20 dB at the slot's resonant frequency. All signal routing entering or exiting the shielded zone must pass through designated entry points where filtered pads or feed-through capacitors can be placed. Route signals through gaps in the shield wall only at defined locations, and never run traces parallel to the wall edge.
3. Internal cavity resonance from oversized shield can dimensions. The shield can forms a rectangular cavity resonator. The lowest resonant mode (TE₁₀) occurs at a frequency determined by the longest internal dimension: f₁₀ = c / (2L), where L is the longest dimension and c is the speed of light. A 30 mm shield can resonates at approximately 5 GHz. If the enclosed circuit generates energy near this frequency, the cavity amplifies rather than attenuates. Mitigation involves sizing the shield can so that the lowest cavity resonance falls above the highest significant emission frequency, or partitioning the interior with divider walls to reduce the effective dimension. POCONS two-piece designs support internal divider walls for multi-compartment shielding.
4. Reflow-induced warping from asymmetric solder paste application. Shield cans with perimeter solder pads are sensitive to paste volume uniformity. Excessive paste on one side creates uneven surface tension during reflow, pulling the can off-center and producing a gap on the opposite side. A 0.1 mm gap at 5 GHz reduces local SE to near zero at that point. Use a 1:1 aperture ratio on the stencil for shield can pads, or reduce to 80% area ratio with a 0.12 mm stencil to prevent excess paste volume. Verify coplanarity of the shield can base flange to ≤0.05 mm before placement.
5. Missing thermal relief on shield can ground pads slows reflow and creates cold joints. Large ground copper pours act as heat sinks, pulling thermal energy away from the solder joint during reflow. Without thermal relief spokes on the ground pad connection to the copper pour, the solder paste may not reach liquidus, resulting in cold joints with contact resistance exceeding 500 mΩ. Use four-spoke thermal relief with 0.3 mm spoke width and 0.25 mm gap on all ground via connections within the shield can footprint. This balances thermal management during reflow against DC resistance requirements.
PCB Footprint & Soldering Profile Guidelines
Shield can PCB footprints must be designed with the following geometric parameters:
Pad Geometry:
- Perimeter pad width: 1.0 mm minimum (1.2 mm preferred for hand-rework compatibility)
- Pad extends 0.5 mm outside and 0.5 mm inside the nominal can wall position
- Courtyard clearance: 0.5 mm from shield can outer edge to nearest non-ground copper feature
- Corner pads: extend 0.3 mm beyond corner radius to ensure full wetting on can corner legs
- Ground via fence: 0.3 mm finished hole diameter, 0.6 mm pad, on 1.5 mm pitch along entire perimeter
- Paste aperture ratio: 80% of pad area for 0.12 mm stencil; 70% for 0.15 mm stencil
Two-Piece Design Footprint (POCONS Standard): For POCONS two-piece configurations, the fence (base frame) is soldered permanently, and the lid snaps or clips onto the fence. The fence footprint follows the same perimeter pad rules above. Additionally, spring contact landing pads must be provided:
- Spring contact pad: 1.0 mm × 1.0 mm square, ENIG or OSP finish
- Pad copper thickness: 1 oz minimum (35 µm) to withstand repeated contact cycling
- No solder mask over spring contact landing areas (NSMD pad definition)
- Minimum of one spring contact pad per 6 mm of shield can perimeter length
Reflow Soldering Profile (per J-STD-020 and IPC-7530 guidelines):
- Preheat ramp rate: 1.0–2.5°C/s (avoid exceeding 3.0°C/s to prevent thermal shock to CRS plating)
- Soak zone: 150–200°C for 60–120 seconds
- Peak reflow temperature: 245–250°C (SAC305 alloy), 230–240°C (SnBi low-temp)
- Time above liquidus (TAL): 45–75 seconds for SAC305; 30–60 seconds for SnBi
- Cooling rate: 2.0–4.0°C/s maximum (excessive cooling rate causes tin pest in lead-free joints)
- Shield cans should be placed after all shorter components in the placement sequence to avoid shadowing effects during reflow
Per IPC J-STD-001 Class 2/3, solder fillets on shield can perimeter tabs must show ≥75% wetting on both the pad and the tab vertical surface. Post-reflow inspection should verify no visible gaps between the can base flange and the PCB surface exceeding 0.05 mm.
For rework, follow IPC-7711/7721 procedures. Use a preheater to bring the board to 150°C before local reflow of the shield can perimeter. POCONS two-piece designs significantly reduce rework cost—the permanently soldered fence remains in place while the lid is removed by hand for component-level rework underneath.
Recommended POCONS Components
Custom Two-Piece Shield Cans POCONS custom two-piece shield cans are the primary recommendation for designs requiring post-assembly rework access, multi-zone shielding within a single board region, or compliance with automotive AEC-Q200 reliability requirements. The base fence is permanently soldered during standard SMT reflow, while the snap-fit lid provides tool-free access during debug, test, and field service. Available in CRS, brass, and copper alloy with tin, nickel, or gold plating. Custom geometries from 5 mm × 5 mm up to 80 mm × 80 mm with internal divider walls. → View Custom Two-Piece Shield Cans
Precision Spring Contacts / Pogo Pins For two-piece shield can systems, POCONS spring contacts provide the electrical continuity between the removable lid and the PCB ground plane. Gold-over-nickel plated beryllium copper construction delivers 20–30 mΩ contact resistance with 0.3–0.8 N normal force, rated for over 1 million insertion cycles. Available in surface-mount and through-hole configurations with travel ranges from 0.3 mm to 1.5 mm to accommodate board-level stack-up variation and manufacturing tolerances. → View Spring Contacts & Pogo Pins
SMD Pan Nuts For shield can mounting in applications where mechanical fastening supplements or replaces solder attachment—such as high-vibration automotive or military environments—POCONS SMD pan nuts provide a reflow-solderable threaded receptacle directly on the PCB. Combined with a screw-down shield can lid, this approach achieves the lowest possible contact impedance and mechanical retention force, suitable for MIL-STD-461G environments where solder joints alone may not meet shock and vibration requirements per MIL-STD-810. → View SMD Pan Nuts
Application note produced by POCONS USA engineering team. Contact applications@poconsusa.com for design review.
Frequently Asked Questions
Why do ferrite beads fail to suppress radiated emissions above 1 GHz?
Ferrite beads are lossy impedance elements optimized for conducted noise on traces. Above their peak impedance frequency—typically 100–600 MHz for standard NiZn compounds—their impedance drops and parasitic capacitance (0.2–0.8 pF) creates a low-impedance bypass path, allowing RF energy to couple radiatively from unshielded ICs and routing. Board-level shield cans provide 40–80 dB of radiated attenuation in the 1–6 GHz range where ferrite bead effectiveness collapses.
What contact resistance is required for effective shield can grounding?
Shield can ground contacts must maintain ≤50 mΩ per contact point across the operating life. POCONS spring contacts achieve 20–30 mΩ initial contact resistance with ≤50 mΩ after 1 million cycles, ensuring continuous low-impedance grounding that prevents slot antenna effects at shield-to-board interfaces.
Can shield cans be specified in custom geometries for non-standard PCB layouts?
Yes. POCONS manufactures custom two-piece shield cans with tolerances of ±0.05 mm in stamped or drawn configurations. Minimum order quantities start at 1,000 pieces for custom tooling, with 3–4 week lead times for initial samples. Engineering review with DFM feedback is available at no cost.