EMI Shielding Effectiveness of Metal-Coated Fabric
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At a few microns of silver the coating is a fraction of one skin depth. Nearly all the shielding is reflection, and making it thicker buys almost nothing.
Shielding Effectiveness
—dB
Total attenuation of the incident field
Loss Mechanisms
Reflection Loss
—dB
Absorption Loss
—dB
Skin Depth
—µm
Field Attenuation
—×
Bulk Resistivity
—µΩ·cm
This is the plane-wave far-field result for a continuous conductive sheet, and a fabric is not continuous — apertures at the weave, seams, closures and cable entries govern real enclosures and routinely cost tens of decibels the material itself would have delivered. Near-field magnetic shielding at low frequency follows entirely different rules and this will overstate it badly. Multiple-reflection correction is omitted, which is conservative for thick shields and optimistic where thickness is well under a skin depth. Verify by measurement to ASTM D4935 or a full enclosure test.
Using this calculator
About the EMI Shielding Effectiveness of Metal-Coated Fabric
The formula
This is the expression the tool evaluates. Every term is named underneath, with the unit it must be supplied in.
Shielding EffectivenessshieldingEffectiveness = f( surfaceResistivity, coatingThickness, relativePermeability, frequency )
Each input feeds the expression evaluated in the browser; the symbol table below names every term and its unit.
Symbols used above
Symbol
Stands for
Unit
surfaceResistivity
Surface Resistivity
Ω/sq
coatingThickness
Coating Thickness
µm
relativePermeability
Relative Permeability
µr
frequency
Frequency
MHz
shieldingEffectiveness
Shielding Effectiveness
dB
reflectionLoss
Reflection Loss
dB
absorptionLoss
Absorption Loss
dB
skinDepth
Skin Depth
µm
attenuationFactor
Field Attenuation
×
bulkResistivity
Bulk Resistivity
µΩ·cm
How the result is derived
Step by step, from the values you type to the figure on screen.
The 4 inputs are read from the form on every keystroke: Surface Resistivity, Coating Thickness, Relative Permeability and Frequency.
Each value is checked against the accepted range in the input table below. A value outside its range stops the calculation rather than producing a misleading figure — the results blank out and a message appears.
The validated values are substituted into the expression above, which resolves Shielding Effectiveness together with every supporting figure in one pass — no value is carried over from a previous entry.
The supporting outputs — Reflection Loss, Absorption Loss, Skin Depth, Field Attenuation and Bulk Resistivity — come from the same pass, so they always describe the same case as the headline figure.
Results are rounded for display only. The full-precision value is used throughout the chain, so reading a rounded intermediate figure back into the tool by hand can shift the last digit.
What each input means
Where to read each value on the floor, the unit it must be in, and the range the tool accepts.
Input
Unit
Accepted range
Default
What it means
Surface Resistivity
Ω/sq
0.001 to 100 Ω/sq
0.05
Coating Thickness
µm
0.05 to 200 µm
5
Relative Permeability
µr
1 to 1000 µr
1
Above 1 only for nickel and ferromagnetic coatings.
Frequency
MHz
0.1 to 40000 MHz
1000
What the tool returns
The headline figure and every supporting value it is built from.
Output
Unit
What it tells you
Shielding Effectiveness (headline result)
dB
Total attenuation of the incident field
Reflection Loss
dB
Absorption Loss
dB
Skin Depth
µm
Field Attenuation
×
Bulk Resistivity
µΩ·cm
Worked example
Given
Surface Resistivity
0.05 Ω/sq
Coating Thickness
5 µm
Relative Permeability
1 µr
Frequency
1000 MHz
The tool loads with this case already solved — the Shielding Effectiveness shown above is its answer. Change one value and the difference from this baseline is the sensitivity of the result to that variable.
How to use it
Work through the input groups in order — Conductive Layer and Threat. The defaults are a realistic case, so you can change one value at a time and watch what moves.
There is no calculate button. Every figure recalculates as you type or drag, which is what makes this usable for a what-if sweep rather than a single answer.
Read Shielding Effectiveness in the dark results panel — that is the headline figure, expressed in dB.
Check the supporting rows underneath (Reflection Loss, Absorption Loss, Skin Depth, Field Attenuation and Bulk Resistivity) before acting on the headline — they are where an implausible input usually shows itself first.
Reset to defaults returns every field to the reference case, which is the quickest way to check whether a surprising result came from the tool or from an input you had changed earlier.
Where this is used
Process planning — establishing Shielding Effectiveness before a trial is booked, so machine time and material in Acoustic, Thermal & Metamaterial Textiles are committed against a calculated figure rather than an estimate.
Costing and quotation — Shielding Effectiveness is an input to the cost sheet, and quoting from a worked number rather than a remembered one is what keeps a margin intact.
Troubleshooting — when the floor result drifts from plan, entering the measured values (starting with Surface Resistivity) shows how much of the gap in Shielding Effectiveness each variable explains.
Teaching and study — the accepted ranges bracket normal Acoustic, Thermal & Metamaterial Textiles practice, so moving one variable at a time shows the shape of the relationship rather than a single answer.
Assumptions and limits
This is the plane-wave far-field result for a continuous conductive sheet, and a fabric is not continuous — apertures at the weave, seams, closures and cable entries govern real enclosures and routinely cost tens of decibels the material itself would have delivered. Near-field magnetic shielding at low frequency follows entirely different rules and this will overstate it badly. Multiple-reflection correction is omitted, which is conservative for thick shields and optimistic where thickness is well under a skin depth. Verify by measurement to ASTM D4935 or a full enclosure test.
Every input is bounded to the range normal practice occupies (Surface Resistivity 0.001 to 100 Ω/sq, Coating Thickness 0.05 to 200 µm and Relative Permeability 1 to 1000 µr, and so on for the rest). Those bounds are guard rails against typing errors, not a claim that the formula fails one unit outside them.
The calculation is deterministic: the same inputs always give the same result. It carries no allowance for machine condition, operator skill, ambient conditions or lot-to-lot material variation unless an input above explicitly represents one.
Nothing is sent anywhere. The maths runs in your browser, so the numbers you type never leave the page.
Questions people ask
What do I need to know before using the EMI Shielding Effectiveness of Metal-Coated Fabric?
Have these to hand: Surface Resistivity, Coating Thickness, Relative Permeability and Frequency. With those entered, the tool returns Shielding Effectiveness immediately.
What exactly is Shielding Effectiveness?
Total attenuation of the incident field. It is reported in dB. It is derived from Surface Resistivity, Coating Thickness, Relative Permeability and Frequency, and is the figure the rest of the Acoustic, Thermal & Metamaterial Textiles calculation is built around.
Which units does this calculator expect?
Enter Surface Resistivity in Ω/sq, Coating Thickness in µm, Relative Permeability in µr and Frequency in MHz. Mixing unit systems is the most common cause of a result that looks an order of magnitude wrong — convert before typing, not after reading.
What are the other figures under the main result?
They are the intermediate quantities the calculation passes through: Reflection Loss, Absorption Loss, Skin Depth, Field Attenuation and Bulk Resistivity. They are shown because a headline number nobody can trace is a number nobody trusts — checking them against your own expectation is the fastest way to confirm the inputs were read as you intended.
Can I rely on this for a production decision?
This is the plane-wave far-field result for a continuous conductive sheet, and a fabric is not continuous — apertures at the weave, seams, closures and cable entries govern real enclosures and routinely cost tens of decibels the material itself would have delivered. Near-field magnetic shielding at low frequency follows entirely different rules and this will overstate it badly. Multiple-reflection correction is omitted, which is conservative for thick shields and optimistic where thickness is well under a skin depth. Verify by measurement to ASTM D4935 or a full enclosure test. Treat the output as an engineering estimate that narrows the trial window, not as a substitute for the trial.