MIL-STD-461 Conducted Susceptibility Shielding: PCB-Level Transient Protection Design
Engineering guide for PCB shield can design addressing MIL-STD-461 CS101/CS114/CS116/CS117 conducted susceptibility requirements with attenuation data and layout rules
Executive Summary
Military and aerospace electronic subsystems must survive conducted susceptibility environments defined by MIL-STD-461G tests CS101 through CS117, encompassing steady-state AC injection, bulk cable transients, damped sinusoidal waveforms, and lightning-induced surges. The dominant failure mode at the PCB level is not direct power rail upset—discrete filtering handles that—but secondary electromagnetic coupling where injected conducted energy radiates within an enclosure and couples into unprotected high-impedance signal paths, clock distribution networks, and analog front ends. This parasitic coupling path bypasses board-level filters entirely and manifests as bit errors in digital buses, ADC noise floor degradation of 10–20 dB, or outright latch-up in CMOS devices. POCONS USA two-piece shield cans with low-impedance spring contact interfaces provide the localized Faraday cage necessary to isolate susceptible circuit blocks, delivering ≥40 dB of isolation from 100 kHz to 1 GHz and ≥60 dB above 1 GHz where secondary radiation coupling is most aggressive.
Technical Specifications & Attenuation Data
Shield can effectiveness against conducted susceptibility-induced coupling depends on three parameters: wall conductivity, aperture control, and contact impedance to the PCB ground plane. MIL-STD-461G does not directly specify shielding effectiveness requirements for internal shields—those derive from system-level EMI control plans per MIL-STD-464—but the conducted susceptibility test levels define the threat environment the shield must attenuate.
CS116 injects damped sinusoidal transients at amplitudes up to 30 A peak into cable bundles, with spectral energy spanning 10 kHz to well above 100 MHz depending on the drive frequency selected. CS117 applies lightning-induced transient waveforms per the multiple-stroke and multiple-burst profiles, with peak currents reaching 1,500 A on external cables and edge rates producing significant spectral content to 10 MHz. The secondary radiated field from these conducted injections inside an equipment enclosure can reach 1–5 V/m at PCB level depending on enclosure Q and cable routing, creating the coupling threat that board-level shields must address.
POCONS shield cans are manufactured from C5210 phosphor bronze (0.2 mm nominal wall thickness) or C7701 nickel silver (0.15 mm), both with tin plating per MIL-T-10727. The following table summarizes measured performance of representative shield can configurations:
| Parameter | C5210 Phosphor Bronze (0.2 mm) | C7701 Nickel Silver (0.15 mm) | Test Standard | |-----------|-------------------------------|------------------------------|---------------| | Shielding effectiveness, 100 MHz | 42 dB | 48 dB | IEEE 299 (modified, small enclosure) | | Shielding effectiveness, 1 GHz | 58 dB | 65 dB | IEEE 299 (modified) | | Shielding effectiveness, 6 GHz | 62 dB | 68 dB | IEEE 299 (modified) | | Sheet resistance | 12 mΩ/sq | 8 mΩ/sq | Four-point probe | | Wall conductivity | 7.5 × 10⁶ S/m | 3.3 × 10⁶ S/m | — | | Relative permeability (μᵣ) | 1.0 | 1.0 | — | | Contact resistance per spring finger | 2–5 mΩ | 2–5 mΩ | MIL-STD-1344 Method 3002 | | Spring contact force | 30–80 gf per contact | 30–80 gf per contact | — | | Skin depth at 100 MHz | 18 μm | 28 μm | Calculated | | Skin depth at 1 GHz | 5.8 μm | 8.8 μm | Calculated | | Operating temperature range | −55 °C to +125 °C | −55 °C to +125 °C | MIL-STD-810H |
At 100 MHz the skin depth for phosphor bronze is approximately 18 μm, meaning the 200 μm wall provides over 11 skin depths of attenuation—well into the absorption-dominated regime. Nickel silver achieves comparable performance at a thinner gauge because its lower conductivity is offset by better impedance matching to free space, reducing surface reflection loss variation across frequency.
For conducted susceptibility applications, contact impedance is the dominant performance limiter. A single shield can wall with 60 dB of intrinsic shielding effectiveness degrades to 25–30 dB if the perimeter contact impedance exceeds 50 mΩ total. POCONS spring contact designs maintain 2–5 mΩ per contact point with a recommended minimum of 8 contact points per shield can side, yielding a total perimeter impedance consistently below 5 mΩ.
Common Design Pitfalls
1. Insufficient ground pad copper area beneath shield can perimeter. The PCB ground pad must provide an unbroken, low-inductance return path around the full perimeter of the shield can footprint. A ground pad trace narrower than 0.5 mm or routed through via-stitched segments with pitch greater than 2 mm creates an inductive gap. At 100 MHz, even 2 nH of parasitic inductance presents 1.3 Ω of impedance—enough to degrade shielding effectiveness by 15–20 dB. The design rule is: minimum 1.0 mm ground pad width, via stitching at ≤λ/20 spacing (which at 1 GHz means ≤1.5 mm pitch), and no signal trace crossings beneath the shield footprint pad.
2. Routing high-speed signals under the shield can wall. Any trace crossing beneath the shield perimeter wall creates a slot antenna. Signals routed through the shield wall must exit through designated cutouts with EMI gasketing or through filtered feedthroughs. A single unshielded 100 MHz clock trace crossing the wall reduces effective shielding by 20–30 dB at harmonics. Route all entry/exit traces through defined apertures with ≤3 mm maximum aperture width, and maintain aperture spacing at ≤λ/10 of the highest threat frequency.
3. Ignoring cavity resonance modes for rectangular shield cans. The lowest resonant mode (TE₁₀) of a rectangular shield can occurs at f = c / (2L), where L is the longest internal dimension. A 30 mm shield can resonates at approximately 5 GHz; a 50 mm shield can at 3 GHz. If the conducted susceptibility test environment produces harmonics at these frequencies—CS116 damped sinusoidal waveforms at 100 MHz drive frequency produce harmonics well into the GHz range—the internal field can be amplified by the cavity Q. Mitigation: size the shield can so that the first resonance falls above the highest frequency of concern, or add a conductive foam absorber pad to the interior surface of the lid to reduce Q below 30.
4. Using the shield can as a heatsink path without thermal analysis. In power-dense military designs, engineers sometimes rely on conductive heat transfer through the shield can wall to the PCB ground plane. Phosphor bronze thermal conductivity is only 50 W/m·K—an order of magnitude below copper. A 0.2 mm wall over a 15 mm span presents approximately 60 °C/W of thermal resistance. If the enclosed component dissipates more than 0.5 W, this path is inadequate and the resulting thermal expansion can degrade spring contact force over temperature cycling, increasing contact resistance from 5 mΩ to 15–20 mΩ after 500 thermal cycles. Specify a dedicated thermal via array under power components independent of the shielding ground structure.
5. Applying shield cans without proper cable-side filtering strategy. A PCB-level shield can addresses secondary radiated coupling inside the enclosure, but it cannot attenuate conducted energy arriving directly on power and signal traces that penetrate the shield. MIL-STD-461 CS101 and CS114 threats travel on conductors. Every trace entering the shield can must pass through appropriate filtering—capacitive decoupling at minimum, LC pi-filters for power rails, and common-mode chokes for differential signal pairs. The shield can and the filter form a complementary system: the filter blocks conducted paths, the shield blocks radiated paths. Neither alone is sufficient.
PCB Footprint & Soldering Profile Guidelines
POCONS shield cans use a perimeter solder pad design compatible with standard SMT assembly processes. The following guidelines apply to two-piece shield can systems (frame + lid):
Pad geometry for shield can frame:
- Perimeter pad width: 1.2 mm minimum (1.5 mm recommended for MIL-spec assemblies)
- Pad-to-component courtyard clearance: 0.5 mm minimum per IPC-7351B
- Corner radius on pads: match shield can corner radius ±0.1 mm to prevent solder bridging
- Solder paste aperture ratio: 70–80% of pad area for 0.2 mm wall thickness cans
- Stencil thickness: 0.125 mm (5 mil) for standard reflow; 0.15 mm (6 mil) for military/high-reliability assemblies per IPC-7525
- Via-in-pad: permitted only if filled and planarized per IPC-4761 Type VII; unfilled vias cause solder wicking and contact degradation
Lid retention features:
- POCONS two-piece designs use spring clip retention integrated into the frame wall
- Lid removal clearance: specify 2.0 mm vertical clearance above lid for rework tooling access
- No solder on lid interface—lid contacts frame via spring fingers only, enabling field replacement
Reflow soldering profile (SAC305 per J-STD-020):
- Preheat ramp rate: 1.0–2.5 °C/s (do not exceed 3.0 °C/s to prevent thermal shock to spring contacts)
- Soak zone: 150–200 °C for 60–120 seconds
- Peak reflow temperature: 245 °C ±5 °C
- Time above liquidus (TAL): 40–70 seconds
- Cooling rate: ≤4 °C/s (aggressive cooling risks stress fracture at solder-to-spring-finger interface)
- Post-reflow inspection: verify 100% wetted fillet on all perimeter pad segments per IPC-A-610 Class 3 criteria
For rework per IPC-7711/7721: Use localized hot-air reflow at 280 °C with a nozzle matched to the shield can footprint perimeter. Do not use soldering iron contact on spring fingers—mechanical deformation of spring geometry permanently degrades contact force below the 30 gf minimum.
Recommended POCONS Components
Custom Two-Piece Shield Cans
POCONS two-piece shield can assemblies are the primary solution for MIL-STD-461 conducted susceptibility isolation at PCB level. The frame solders permanently to the board, while the removable lid enables component access during debug, rework, and depot-level maintenance—a critical requirement for military programs governed by MIL-STD-2165 maintainability standards. Available in C5210 phosphor bronze and C7701 nickel silver with tin, tin-lead, or nickel plating. Custom geometries from 8 mm × 8 mm to 80 mm × 80 mm in 0.1 mm dimensional increments.
→ View custom two-piece shield cans
Spring Contacts / Pogo Pins
POCONS precision spring contacts deliver 2–5 mΩ contact resistance with 30–80 gf force, providing the low-impedance perimeter ground connection that determines real-world shielding effectiveness. Gold-over-nickel plated beryllium copper springs maintain contact resistance below 10 mΩ through 10,000+ mating cycles and 1,000 thermal cycles from −55 °C to +125 °C. Available in surface-mount, through-hole, and press-fit configurations for integration into shield frames or direct board mounting.
→ View spring contacts and pogo pins
SMD Pan Nuts
For shield can mounting in high-vibration military environments per MIL-STD-810H Method 514, POCONS SMD pan nuts provide a mechanically fastened alternative to solder-only retention. The surface-mount nut solders to the PCB and accepts a machine screw through the shield can lid, creating a compression joint that maintains contact force under 20 G random vibration profiles. Stainless steel and phosphor bronze options, M2 through M3 thread sizes, reflow-compatible.
Design Support
POCONS applications engineering provides MIL-STD-461 pre-compliance design review, including shield can placement analysis, cavity resonance modeling, and contact impedance budgeting. Submit your PCB layout and EMI control plan for a complimentary engineering assessment.
Application note produced by POCONS USA engineering team. Contact applications@poconsusa.com for design review.
Frequently Asked Questions
What shielding effectiveness is required to pass MIL-STD-461 CS101 at the PCB component level?
CS101 imposes conducted susceptibility from 30 Hz to 150 kHz at levels up to 6 Vrms on power leads. PCB-level shield cans are not the primary defense for low-frequency conducted threats, but a properly grounded two-piece shield with ≤5 mΩ contact resistance prevents secondary radiated coupling from CS101 injection into adjacent high-impedance analog circuits. The shield can must present a continuous return path below 1 mΩ/sq sheet resistance to be effective at these frequencies.
How does shield can cavity resonance affect MIL-STD-461 CS116 damped sinuoid transient immunity?
CS116 injects damped sinusoidal transients from 10 kHz to 100 MHz. If the shield can internal dimension produces a λ/2 resonance within this band—for example, a 40 mm cavity resonates near 3.75 GHz, outside CS116 range—the direct threat is transient-induced ringing on traces routed under the can. Cavity Q-factor must stay below 50 through lossy wall contact or absorber placement to prevent amplification of harmonics above the fundamental injection frequency.
What lead time and MOQ should procurement expect for custom MIL-STD-461 qualified shield cans?
POCONS manufactures custom two-piece shield cans with tooling lead times of 2–4 weeks for stamped designs and 1–2 weeks for photo-etched prototypes. MOQs start at 500 pieces for production stamping and 50 pieces for prototype runs. All shield cans are manufactured to IPC Class 3 solderability requirements with tin or tin-lead plating standard.