EMC Design

Shielding Effectiveness Calculator

Estimate skin depth, absorption loss, reflection loss, multiple-reflection correction, and aperture leakage for a uniform single-layer shield under a far-field plane-wave approximation.

FORMULAv1.0.0
INPUT PARAMETERS

Enter material and thickness

Uses a far-field plane-wave, uniform single-layer shield approximation; apertures may control total shielding.

CALCULATION RESULT

Calculation result

Calculated locally

Enter the parameters and run the calculation to see results and model assumptions here.

FORMULA & TRACEABILITY

Formulas and applicability

Formulas, variables, and model boundaries are published. References last reviewed on 2026-08-30.

5 formulas · 4 references
CORE EQUATIONS

Core equations

These equations directly produce the primary results and define the tool’s core model.

3
F01

Skin Depth

δ = 1 / √(πfμσ) = 1 / √(πfμ₀μᵣσ)

Characteristic depth at which field amplitude inside a conductor falls to 1/e of its surface value.

δ
Skin Depth Calculatorm
f
FrequencyHz
μ
Absolute permeability μ₀μᵣH/m
σ
ConductivityS/m
Applicability
  • Good-conductor approximation σ ≫ ωε
  • Uniform, isotropic material
F02

Absorption Loss

A = 8.686 · t / δ

Absorption attenuation in dB produced by shield thickness t relative to skin depth.

A
Absorption LossdB
t
Shield thicknessm
Applicability
  • Uniform single-layer shield
F03

Plane-wave reflection loss

R = 168 − 10·log₁₀(f·μᵣ/σᵣ)

Reflection loss at the shield interface for a plane wave, where σᵣ = σ/σ_copper.

R
Reflection LossdB
μᵣ
Relative permeability1
σᵣ
Relative conductivity σ/σ_copper1
Applicability
  • Far-field plane-wave incidence
DERIVED & CONVERSION

Derived and conversion equations

Derive units, levels, and supporting engineering quantities from the core values.

2
F04

Multiple-reflection correction

MRC = 20·log₁₀(1 − 10^(−A/10))

Correction for internal multiple reflections in a thin shield when A is small.

MRC
Multiple-reflection correctiondB
Applicability
  • A < 15 dB 时不可忽略
F05

单孔泄漏简化包络

SE_pore ≈ 20·log₁₀(λ / (2·d_max))

以最大开孔 d_max 得到远场单孔工程包络;min(本体 SE, 孔隙 SE) 仅是保守瓶颈估算,不是实际腔体的严格解。

d_max
Maximum aperture dimensionm
Applicability
  • 远场、单孔近似,d_max < λ/2
  • 不适用于多孔阵、接缝、通风板或腔体谐振的定量预测
REFERENCES

References

01NASA · NASA CR-4784, sections 5.2–5.3Design Guidelines for Shielding Effectiveness, Current Carrying Capability, and the Enhancement of Conductivity of Composite Materials1997 · 公开技术报告列出 SE=A+R+B、吸收损耗及远场平面波反射损耗形式,用于独立核对本体屏蔽计算。
02Van Nostrand · Schelkunoff, S.A., 1943 (single-layer shield theory)Electromagnetic Waves1943 · Schelkunoff theory for a uniform single-layer shield, the source of SE = A + R + MRC.
03Wiley · Ott, H.W., 2009, Ch.13 (Shielding)Electromagnetic Compatibility Engineering2009 · Chapter 13 covers absorption/reflection loss and aperture leakage, forming the basis of this tool.
04IEEE · Schulz, R.B., et al., IEEE Trans. EMC-30(3), 1988Shielding Theory and Practice1988 · 屏蔽理论综述;用于核对模型的假设与边界,不将简化单孔式误表述为实际箱体的严格解。
Engineering use notice

Results use the models and assumptions shown on this page for design estimates and pre-compliance risk review. Complex structures, dispersion, near-field coupling, and test setup can cause significant deviation.

FAQ

Frequently asked questions

What is the shielding effectiveness definition?

SE(dB) = 20·log₁₀(E_incident / E_transmitted). Via transmission-line theory it decomposes into absorption loss A, reflection loss R, and multiple-reflection correction B (Schelkunoff decomposition).

What is the absorption loss formula?

A(dB) = 8.686 · t / δ, with t the shield thickness and δ the skin depth at that frequency. Each additional skin depth adds about 8.7 dB of absorption.

Why is low-frequency magnetic field shielding hard?

At low frequencies reflection loss vanishes and skin depth is large (insufficient absorption); high-permeability materials (mu-metal, silicon steel) must divert the flux. Copper and aluminum are nearly useless for low-frequency H fields.

PRE-COMPLIANCE SUPPORT

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