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Double conductive copper foil tape · Z-axis conduction and pressure contact scheme
The engineer applied a double conductive copper foil tape between the PCB grounding pad and the metal frame. Measured with a multimeter, there is indeed conductivity between the adhesive surface and the copper foil surface, and the reading is normal. But after the equipment was assembled, the ESD test still failed and the grounding resistance was much higher than expected.
Core proposition:The problem is not with the tape itself, but with the gap between "conductivity" and "low resistance conductivity". The Z-axis conductivity of double conductive copper foil tape depends on the mutual contact of nickel particles in the adhesive layer - this contact is not metallurgical bonding like welding, but pressure contact. The actual value of vertical resistance is determined by the pressure applied during attachment, the thickness of the adhesive layer, and the distribution density of particles. If the pressure is insufficient or the adhesive layer is not fully compressed, the particles are only "close" rather than "in contact", and the vertical resistance may be several orders of magnitude higher than the specification value.
The double conductive copper foil tape consists of three layers: high-purity electrolytic copper foil layer, conductive acrylic pressure-sensitive adhesive layer, and release layer. The copper foil surface is conductive, and the adhesive surface is also conductive due to the addition of conductive particles such as nickel.
The implementation path of Z-axis conduction is that when the adhesive tape is attached between the surfaces of two conductors, the conductive pressure-sensitive adhesive layer is compressed, and the nickel particles in the adhesive layer approach each other. When the pressure is sufficient to overcome the elastic resistance of the adhesive layer, physical contact is formed between particles, constructing a vertical conductive path from the adhesive surface to the copper foil. This mechanism is similar to the Z-axis conduction principle of anisotropic conductive adhesive (ACF) - the conductive path is only established in the direction of pressure, rather than randomly diffusing within the plane of the adhesive layer.
Nickel particles serve a dual function in dual conductive tape: as conductive fillers to achieve Z-axis conductivity, while also providing magnetic shielding capability as ferromagnetic metals. Copper foil is responsible for electrical signal shielding, while nickel particles in the adhesive surface are responsible for magnetic signal shielding. The two work together to achieve complete electromagnetic shielding.
Vertical resistance is the most crucial but easily misread parameter of double conductive copper foil tape. The "≤ 0.03 Ω" on the specification sheet is usually measured under standard pressure conditions - for example, after reciprocating rolling with a roller of a specified weight. In actual construction, if only lightly pressing with fingers or not applying sufficient pressure after bonding, the vertical resistance may significantly increase.
Three key variables that affect vertical resistance:
The greater the pressure, the more fully the adhesive layer is compressed, the tighter the nickel particles are in contact, and the lower the vertical resistance. In industry practice, it is recommended to use a scraper or roller to evenly press the surface of the tape to ensure that the adhesive layer fully wets the object being pasted and compresses the conductive particles.
The thicker the adhesive layer, the greater the pressure required to bring the particles into contact. Thin adhesive layers are more likely to achieve low vertical resistance under the same pressure. The total thickness of the double conductive copper foil tape is usually between 0.06mm and 0.08mm, and the thickness of the adhesive layer needs to match the thickness of the copper foil.
A rough surface will reduce the effective contact area between the adhesive layer and the substrate, resulting in uneven local pressure distribution and higher vertical resistance. A clean and smooth surface is a prerequisite for low vertical resistance.
The adhesive surface of the single conductive copper foil tape is insulated, and current can only be conducted along the X-Y direction within the copper foil surface. The adhesive surface of the double conductive copper foil tape is conductive, and current can pass through the adhesive layer to reach the object being pasted, forming X-Y-Z three-way conduction.
| Feature | Single conductive copper foil tape | Double conductive copper foil tape |
|---|---|---|
| Copper foil surface conductivity | conduct electricity | conduct electricity |
| Adhesive surface conductivity | Non-conductive (insulating) | Conductive (containing nickel particles) |
| Current path | Only copper foil surface (X-Y direction) | Copper foil adhesive surface (X-Y-Z three directions) |
| Z-axis conduction mechanism | Nothing | Pressure contact, nickel particles in contact with each other |
| Vertical resistance | — | ≤ 0.03 Ω (under standard pressure) |
| Magnetic shielding mechanism | Nothing | Nickel particles on the adhesive surface provide magnetic shielding |
| typical scenario | Insulation surface shielding, single-sided grounding | Crossover conductive surface, double-sided conductive grounding, shielding cover seam |
The core application scenarios of dual conductive copper foil tape include: bridging the gap between two conductive casings, and the adhesive surface contacts the two casings to form a bridging path; The PCB grounding pad is connected to the metal frame to release static electricity, and Z-axis conduction completes grounding; The conductive connection between the cable shielding layer and the metal connector housing; Maintain electrical continuity at the seams between the components of the shielding cover.
| performance metrics | typical value | Testing/Remarks |
|---|---|---|
| Copper foil purity | ≥99.95%–99.98% | Advanced Institute of Technology Product Data |
| Copper foil surface resistance | ≤0.05Ω/inch | GB/T30139 |
| Vertical resistance (Z-axis) | ≤0.03Ω | Under standard pressure conditions |
| Shielding effectiveness | ≥80dB | wideband |
| Adhesive force (180 ° peel off) | 1.0–1.5kg/25mm | Depending on the thickness of the copper foil |
| Temperature resistance range | -10 ° C to 120 ° C | long-term use |
| copper thickness | 0.018mm / 0.025mm / 0.035mm / 0.050mm | Customizable as needed |
| width | 5–500mm | Customizable slitting |
The three steps of correct construction:
Selection warning:The Z-axis conductivity of double conductive copper foil tape is a pressure contact mechanism, rather than a metallurgical bonding by welding. The vertical resistance value on the specification sheet is measured under standard pressure - in actual construction, if the pressure is insufficient, the vertical resistance may be several times or even an order of magnitude higher. In scenarios with strict grounding resistance requirements, it is necessary to use rollers to fully crush and verify the conductivity effect.
The value of double conductive copper foil tape lies in its provision of a detachable and field repairable Z-axis conductivity solution - no welding equipment or high-temperature processes are required, only surface cleaning and pressure application are needed to establish an electrical connection between two conductors. But the premise of this convenience is to understand the pressure dependent mechanism of its Z-axis conduction: it is not a switch that "conducts when attached", but a pressure contact interface that "conducts when pressed".
Understanding the relationship between vertical resistance and bonding pressure, the influence of adhesive layer thickness on conductivity, and the decisive role of correct construction in the reliability of Z-axis conductivity - these are the key to upgrading double conductive copper foil tape from a "roll of tape" to an "engineering decision".
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