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Etch Factor and Line-Width Compensation on Heavy Copper

Bottom line first: when line width drifts out of control on heavy-copper boards, the cause is usually not exposure or development — it is the etch factor collapsing as copper thickness rises while the compensation coefficient still reflects 1 OZ. Separating top width from bottom width, and building compensation tables by copper thickness and pattern density, is the precondition for getting heavy copper right the first time.

Side-etch is not a defect — it is what isotropic etching does

Cupric chloride etching is isotropic: as the chemistry attacks downward it also attacks sideways. The etch factor (EF) describes that anisotropy: EF = 2 × copper thickness ÷ (top width − bottom width). Higher EF means a more vertical sidewall; lower EF means a trapezoidal section and, in severe cases, a mushroom profile with overhanging copper on top and a pinched foot below.

Under a fixed recipe, EF moves inversely with copper thickness. At 1 OZ (35 μm) a shop typically holds 3.0–4.0, giving 4–6 μm of side-etch per edge; at 2 OZ (70 μm) EF falls to 2.0–2.5; at 3 OZ (105 μm) often only 1.5–2.0. At 13 OZ, subtractive etching can no longer hold fine line width: you need segmented etching (SEP) or multiple imaging passes, and the minimum achievable line width moves up.

A frequent misread: AOI reports top width as conforming while the cross-section shows bottom width short. Top width is set by development and exposure energy, bottom width by the etch. On thin copper the gap is negligible; on heavy copper it reaches 20–40 μm — enough to shift current capacity by a class.

Build the compensation table by copper thickness, not by board

Pattern density: the second variable in the coefficient

Etch rate depends on local copper area: an isolated line refreshes the chemistry quickly and side-etches more, while a dense area depletes the bath, etches slower and comes out wider. A 10–15 μm difference between the two on the same panel is normal, not an anomaly.

Control works on three levels: dummy copper in isolated areas to reach 40%–60% local coverage; oscillating spray with staged pressure, front-to-back differential below 0.5 bar; and a bath held at 130–160 g/L copper ion and 48–52 °C by automatic dosing. Compensate edge-to-centre variation with conveyor speed, never with concentration — raising it widens side-etch across the whole line.

Bottom width is the electrical dimension: two separate accounts

Impedance is computed from bottom width plus sidewall contribution. On a 50 Ω microstrip at 5 mil line width, a 10 μm change in bottom width shifts impedance by roughly 1.5–2 Ω, or 3%–4%: inside ±8% on its own, but stacking dielectric thickness tolerance and Dk lot variation pushes it past the limit. Check the coupon against a cross-sectioned bottom width, not the design value.

Current capacity follows the cross-sectional area at bottom width. On 13 OZ at 100 A-class current, losing 20 μm removes nearly 20% of the area and pushes temperature rise up a step. Enter the measured bottom width in any IPC-2152 calculation; nominal values are systematically optimistic on heavy copper.

Acceptance: cross-section, AOI, and coupon cannot substitute for each other

Line-width accuracy on heavy copper is not something the etch step can guarantee alone: nominal dimension, compensation logic, pattern-density distribution and cross-section feedback form one closed loop, and removing any link lets parameters drift by the next lot. AIPCB.cc supports up to 44 layers, a maximum panel size of 610×1100 mm, heavy copper up to 13 OZ, line-width accuracy of ±8 μm, impedance tolerance of ±8% (±10% standard), and aspect ratio up to 20:1 (25:1 for backplanes), with 24-hour rush prototypes. For engineering and quotations, contact info@ipcba.com.cn or +86 138 2310 9230.

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