Advertise DC resistance only; frame f>0 as a skin-only estimate

Skin resistance is a small fraction of real AC impedance (proximity
and inductance dominate), so AC must not appear in the descriptions.
README headline, PCM/plugin metadata, pyproject, dialog note, CLI
help and the summary label now all say: skin-only lower bound on the
resistance rise, not an AC impedance simulation.

Co-Authored-By: Claude Fable 5 <noreply@anthropic.com>

README.md

@@ -1,15 +1,17 @@
 # Fill Resistance — KiCad 10 plugin
 
-Computes the **DC or AC resistance of copper zone fills and traces**
+Computes the **DC resistance of copper zone fills and traces**
 between two contacts, **single- or multi-layer**: the chosen net's fills
 (teardrops included) and tracks on the selected copper layers are
 solved as coupled finite-difference sheets linked by the net's **via
-and through-hole-pad barrels** (18 µm plating, configurable). At a user-set **frequency** the exact 1D foil/barrel
+and through-hole-pad barrels** (18 µm plating, configurable). Shows
-skin-effect correction is applied (AC results are a rigorous lower
+per-layer rasterized maps, potential, current density, and **power
-bound; see *Model & limits*). Shows per-layer rasterized maps,
+density**, and reports **per-via currents** (via ampacity!) and total
-potential, current density, and **power density**, and reports **per-via
+dissipation at a **selectable test current**. PNGs + a text summary are
-currents** (via ampacity!) and total dissipation at a **selectable test
+saved per run. An optional **skin-effect correction** (exact 1D
-current**. PNGs + a text summary are saved per run.
+foil/barrel solution at a user-set frequency) estimates the resistive
+skin rise only — it is **not** an AC impedance simulation (no proximity
+effect, no inductance; see *Model & limits*).
 
 ![Current density on a two-layer demo net](docs/img/demo-current.png)
 *Real output on a synthetic two-layer net: current from a soldered
@@ -236,10 +238,14 @@ SWIG API. Requires KiCad **10.0.1+**.
   isolated foil), and the analogous correction for the 18 µm barrel wall.
   Enter one frequency per run (e.g. a switching harmonic, with its RMS
   amplitude as the test current); suffixes `k`/`M` are accepted.
-  **Caveat:** only through-thickness crowding is modeled. Lateral
+  **Caveat:** this is **not an AC impedance simulation** — skin
-  (proximity-effect) redistribution needs a magneto-quasistatic solver
+  resistance is only a small part of real AC behavior. Only
-  and is not captured — since the resistance-driven distribution is the
+  through-thickness crowding is modeled: lateral (proximity-effect)
-  minimum-dissipation one, AC results are a rigorous **lower bound**.
+  redistribution needs a magneto-quasistatic solver and is not
+  captured — since the resistance-driven distribution is the
+  minimum-dissipation one, the f > 0 resistance is a rigorous **lower
+  bound** — and inductance, usually the dominant term of a real AC
+  impedance, is absent entirely.
   Rule of thumb for 70 µm foil: skin is negligible below ~300 kHz
   (δ = 173 µm at 142 kHz), ~+11 % at 1 MHz. At f > 0 the |J| maps are
   referenced to the skin-reduced conduction-equivalent thickness

fill_resistance/dialog.py

@@ -137,10 +137,10 @@ class _Dialog(QDialog):
         lay = QVBoxLayout(self)
         lay.addLayout(form)
         note = QLabel("Multiple layers are coupled through the net's "
-                      "via/through-pad barrels. At f > 0 the foil-thickness "
+                      "via/through-pad barrels. f > 0 applies only the "
-                      "skin effect is applied per layer; lateral (proximity) "
+                      "foil-thickness skin effect (a lower bound on the "
-                      "redistribution is not modeled, so AC results are a "
+                      "resistance rise) - not an AC impedance simulation: "
-                      "lower bound.")
+                      "proximity and inductance are not modeled.")
         note.setWordWrap(True)
         note.setStyleSheet("color: gray; font-size: 10px;")
         lay.addWidget(note)

fill_resistance/report.py

@@ -59,7 +59,8 @@ def write_summary(outdir: Path, problem: Problem, stack: RasterStack,
          + (f"{result.freq_hz:g} Hz (skin depth {result.skin_depth_um:.0f} um)"
             if result.freq_hz > 0 else "DC")),
         f"RESISTANCE:        {result.R_ohm * 1000:.6g} mOhm"
-        + (" (AC LOWER BOUND: lateral/proximity redistribution not modeled)"
+        + (" (SKIN-ONLY LOWER BOUND: no proximity/inductance - "
+           "not AC impedance)"
            if result.freq_hz > 0 else ""),
         f"VOLTAGE DROP:      {result.R_ohm * result.i_test * 1000:.4g} mV "
         f"@ {result.i_test:g} A",

fill_resistance/standalone.py

@@ -26,7 +26,8 @@ def main(argv=None) -> int:
                     help="test current [A] (default: config TEST_CURRENT_A)")
     ap.add_argument("--freq", type=parse_frequency, default=0.0,
                     help="frequency, e.g. 142k or 1.5M (default: DC). "
-                         "AC results are a lower bound (skin per foil only)")
+                         "Skin resistance only, a lower bound - not AC "
+                         "impedance (no proximity, no inductance)")
     ap.add_argument("--cell-um", type=float, default=None,
                     help="force grid cell size [um]")
     ap.add_argument("--layers", type=str, default=None,

metadata.json

@@ -1,8 +1,8 @@
 {
     "$schema": "https://go.kicad.org/pcm/schemas/v2",
     "name": "Fill Resistance",
-    "description": "DC/AC resistance of copper zone fills and traces between two contacts, single- or multi-layer with via coupling; current and power density maps.",
+    "description": "DC resistance of copper zone fills and traces between two contacts, single- or multi-layer with via coupling; current and power density maps.",
-    "description_full": "Computes the DC or AC resistance of copper zone fills and traces between two contacts (marker rectangles on User.1/User.2 and/or selected pads/vias), single- or multi-layer: the chosen net's fills and tracks are solved as coupled finite-difference sheets linked by the net's via and through-hole-pad barrels. Selected vias/THT pads inject at the drill-wall barrel, and every populated THT hole carries its full solder joint (component lead, solder fill, one-sided pad coat and protruding-lead cone) with exact pad shapes and do-not-populate flags read from KiCad, conducting in-plane as its solder plug and lead on every layer it spans. Every net pad's exact copper shape is stamped on the layers it sits on, SMD as well as through-hole, and oblong (slotted) holes are modelled as their true stadium shape rather than an approximating circle. Traces narrower than the grid become exact 1D resistor chains, and an adaptive multi-resolution grid (fine at features, coarse plane interiors, deferred-corrected) keeps large boards fast.\n\nShows per-layer rasterized maps, potential, current density and power density, reports per-via currents (via ampacity) and total dissipation at a selectable test current. At a user-set frequency the exact 1D foil/barrel skin-effect correction is applied (AC results are a rigorous lower bound). PNGs, a text summary and a re-solvable geometry dump are saved per run.\n\nNote: the first load builds the plugin's Python environment (numpy, scipy, pyamg, matplotlib, PySide6) and can take several minutes.",
+    "description_full": "Computes the DC resistance of copper zone fills and traces between two contacts (marker rectangles on User.1/User.2 and/or selected pads/vias), single- or multi-layer: the chosen net's fills and tracks are solved as coupled finite-difference sheets linked by the net's via and through-hole-pad barrels. Selected vias/THT pads inject at the drill-wall barrel, and every populated THT hole carries its full solder joint (component lead, solder fill, one-sided pad coat and protruding-lead cone) with exact pad shapes and do-not-populate flags read from KiCad, conducting in-plane as its solder plug and lead on every layer it spans. Every net pad's exact copper shape is stamped on the layers it sits on, SMD as well as through-hole, and oblong (slotted) holes are modelled as their true stadium shape rather than an approximating circle. Traces narrower than the grid become exact 1D resistor chains, and an adaptive multi-resolution grid (fine at features, coarse plane interiors, deferred-corrected) keeps large boards fast.\n\nShows per-layer rasterized maps, potential, current density and power density, reports per-via currents (via ampacity) and total dissipation at a selectable test current. An optional skin-effect correction (exact 1D foil/barrel solution at a user-set frequency) estimates the resistive skin rise only - proximity redistribution and inductance are not modeled, so this is not an AC impedance simulation. PNGs, a text summary and a re-solvable geometry dump are saved per run.\n\nNote: the first load builds the plugin's Python environment (numpy, scipy, pyamg, matplotlib, PySide6) and can take several minutes.",
     "identifier": "th.co.b4l.fill-resistance",
     "type": "plugin",
     "author": {

plugin.json

@@ -2,7 +2,7 @@
     "$schema": "https://go.kicad.org/api/schemas/v1",
     "identifier": "th.co.b4l.fill-resistance",
     "name": "Fill Resistance",
-    "description": "DC/AC resistance of copper zone fills and traces between two contacts (marker rectangles or pads), single- or multi-layer with via coupling",
+    "description": "DC resistance of copper zone fills and traces between two contacts (marker rectangles or pads), single- or multi-layer with via coupling",
     "runtime": {
         "type": "python"
     },

pyproject.toml

@@ -4,7 +4,7 @@
 [project]
 name = "fill-resistance"
 version = "1.2.1"
-description = "DC/AC resistance of copper zone fills and traces between two contacts (KiCad 10 plugin)"
+description = "DC resistance of copper zone fills and traces between two contacts (KiCad 10 plugin)"
 license = "GPL-3.0-or-later"
 requires-python = ">=3.11"
 dependencies = [