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kicad-zone-resistance/tests/test_barrel_contacts.py
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janik 9e307f2818
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Solder cone around protruding THT leads (tent structure)
The clipped lead of a soldered THT contact protrudes
THT_LEAD_PROTRUSION_MM (1.5 mm default, 0 disables) out of the hole on
the side opposite the component, and a solder cone wraps it: full
protrusion height at the drill wall, tapering linearly to zero at the
pad edge. Painted as per-cell extra conduction-equivalent copper via
stack.thick_scale - the tall solder column at the wall pulls the joint
vicinity to lead potential (equivalent to extending the barrel wall
vertically), the taper carries the radial spreading. DC-exact additive
conductance; at f > 0 the factor multiplies the skin-corrected sheet
conductance like the via mouths (documented approximation).

The protrusion side is looked up from the owning footprint (pads store
absolute positions; component on F.Cu -> lead tents on B.Cu), with a
logged B.Cu fallback. Dump schema gains protrusion_side and
tht_protrusion_nm (defaults keep older v6 dumps loading).

Co-Authored-By: Claude Fable 5 <noreply@anthropic.com>
2026-07-16 18:47:10 +07:00

216 lines
9.2 KiB
Python

"""Barrel (via / through-hole pad) contact tests: current enters at the
drill-wall ring, not the pad face, and soldered THT joints carry a
solder-filled hole plus an average-thickness solder coat on the pad."""
import math
import numpy as np
import pytest
from fill_resistance import raster, solver
from fill_resistance.geometry import (Electrode, Polygon, ViaLink,
contact_solder_buildups, load_problem,
save_problem)
from tests.util import NM, make_problem, rect_mm, ring_mm
PLATE20 = [(0, 0), (20, 0), (20, 20), (0, 20)]
def _barrel(x_mm, y_mm, drill_mm, pad_mm=0.0, solder=False, polygons=None):
r = max(pad_mm, drill_mm) / 2
return Electrode(
rect=rect_mm((x_mm - r, y_mm - r, x_mm + r, y_mm + r)),
contact="all", label=f"via({x_mm},{y_mm})",
drill_nm=int(drill_mm * NM), pad_nm=int(pad_mm * NM),
center=(int(x_mm * NM), int(y_mm * NM)), solder=solder,
polygons=polygons)
def _disc(x_mm, y_mm, r_mm, n=64) -> Polygon:
ang = np.linspace(0, 2 * np.pi, n, endpoint=False)
return Polygon(outline=ring_mm(
[(x_mm + r_mm * np.cos(a), y_mm + r_mm * np.sin(a)) for a in ang]))
def _solve(p, h_mm, model="equipotential"):
stack = raster.rasterize_stack(p, h_mm * NM)
e1, e2 = raster.electrode_masks(stack, p)
return solver.run_solve(p, stack, e1, e2, 1.0, contact_model=model), stack
def test_ring_cells_at_drill_wall():
"""The contact cells of a barrel electrode form a ring at the drill
wall (one-cell tolerance), not the pad face."""
p = make_problem([(PLATE20, [])],
rect1_mm=(0, 0, 1, 20), rect2_mm=(19, 0, 20, 20))
p.electrodes1 = [_barrel(10, 10, drill_mm=1.0, pad_mm=1.6)]
stack = raster.rasterize_stack(p, 0.1 * NM)
e1, _ = raster.electrode_masks(stack, p)
ii, jj = np.nonzero(e1[0])
xs = stack.x0_nm + (jj + 0.5) * stack.h_nm - 10 * NM
ys = stack.y0_nm + (ii + 0.5) * stack.h_nm - 10 * NM
d = np.hypot(xs, ys)
assert len(ii) >= 8
assert (np.abs(d - 0.5 * NM) <= stack.h_nm + 1).all()
# far fewer cells than the full 1.6 mm pad disc
assert len(ii) < 0.5 * math.pi * (0.8 * NM / stack.h_nm) ** 2
def test_two_barrel_contacts_match_acosh():
"""Two equipotential circular contacts of radius a, centers d apart,
on a large sheet: R = rho/(pi t) * acosh(d / 2a). The barrel-ring
contact must reproduce the analytic spreading resistance."""
t_um, rho = 70.0, 1.68e-8
plate = [(0, 0), (80, 0), (80, 60), (0, 60)]
p = make_problem([(plate, [])], rect1_mm=(0, 0, 1, 1),
rect2_mm=(79, 59, 80, 60), t_um=t_um, rho=rho)
p.electrodes1 = [_barrel(30, 30, drill_mm=2.0)]
p.electrodes2 = [_barrel(50, 30, drill_mm=2.0)]
res, _ = _solve(p, 0.15)
r_ref = rho / (math.pi * t_um * 1e-6) * math.acosh(20e-3 / (2 * 1e-3))
assert res.R_ohm == pytest.approx(r_ref, rel=0.08)
def test_barrel_includes_pad_spreading_resistance():
"""Injecting at the barrel wall (0.5 mm ring) sees the spreading
resistance the whole-pad-face contact (2.4 mm equipotential disc)
short-circuits: R_barrel > R_pad_face."""
p1 = make_problem([(PLATE20, [])],
rect1_mm=(0, 0, 1, 20), rect2_mm=(19, 0, 20, 20))
p1.electrodes1 = [_barrel(10, 10, drill_mm=1.0, pad_mm=2.4)]
r_barrel, _ = _solve(p1, 0.1)
p2 = make_problem([(PLATE20, [])],
rect1_mm=(0, 0, 1, 20), rect2_mm=(19, 0, 20, 20))
p2.electrodes1 = [Electrode(rect=rect_mm((8.8, 8.8, 11.2, 11.2)),
contact="all", label="pad face",
polygons=[_disc(10, 10, 1.2)])]
r_face, _ = _solve(p2, 0.1)
assert r_barrel.R_ohm > r_face.R_ohm * 1.05
def test_ring_fallback_nearest_copper():
"""Antipad bigger than the drill: no copper at the wall ring, the
contact falls back to the nearest copper ring inside the pad
footprint (e.g. thermal-spoke tips / hole edge)."""
hole = [(10 + 1.2 * np.cos(a), 10 + 1.2 * np.sin(a))
for a in np.linspace(0, 2 * np.pi, 64, endpoint=False)]
p = make_problem([(PLATE20, [hole])],
rect1_mm=(0, 0, 1, 20), rect2_mm=(19, 0, 20, 20))
p.electrodes1 = [_barrel(10, 10, drill_mm=0.6, pad_mm=4.0)]
res, stack = _solve(p, 0.1)
e1, _ = raster.electrode_masks(stack, p)
ii, jj = np.nonzero(e1[0])
d = np.hypot(stack.x0_nm + (jj + 0.5) * stack.h_nm - 10 * NM,
stack.y0_nm + (ii + 0.5) * stack.h_nm - 10 * NM)
assert len(ii) >= 8
assert (d >= 1.2 * NM - stack.h_nm).all()
assert (d <= 1.2 * NM + 2.5 * stack.h_nm).all()
assert np.isfinite(res.R_ohm) and res.R_ohm > 0
def test_solder_filled_barrel_resistance():
"""THT joints: the solder core conducts in parallel with the plating.
Exact parallel-area formula, and a sanity ratio for a 1 mm drill."""
v = ViaLink(x=0, y=0, drill_nm=1_000_000, z_top_nm=-1, z_bot_nm=1)
rho, sn = 1.68e-8, 1.32e-7
r_plain = v.barrel_resistance(1_600_000, rho, 18_000)
r_fill = v.barrel_resistance(1_600_000, rho, 18_000,
solder_rho_ohm_m=sn)
ga = math.pi * 1e-3 * 18e-6 / rho
ga += math.pi * (0.5e-3 - 18e-6) ** 2 / sn
assert r_fill == pytest.approx(1.6e-3 / ga, rel=1e-12)
assert 1.5 < r_plain / r_fill < 4.0
def test_contact_solder_coat():
"""A soldered THT contact adds an average-thickness solder buildup
over the pad face on the outer layers, lowering the spreading
resistance vs the bare barrel contact."""
def prob():
p = make_problem([(PLATE20, [])],
rect1_mm=(0, 0, 1, 20), rect2_mm=(19, 0, 20, 20))
p.electrodes1 = [_barrel(10, 10, drill_mm=1.0, pad_mm=2.4,
solder=True, polygons=[_disc(10, 10, 1.2)])]
return p
p = prob()
assert contact_solder_buildups(p) == ["F.Cu"]
assert len(p.buildups) == 1 and p.buildups[0].layer_name == "F.Cu"
r_coat, stack = _solve(p, 0.1)
assert stack.buildup is not None and stack.buildup.any()
r_bare, _ = _solve(prob(), 0.1) # helper not called: no coat
assert r_coat.R_ohm < r_bare.R_ohm
def test_lead_fillet_profile():
"""The protruding-lead solder cone paints thick_scale with the exact
per-cell formula: 1 + H*clip((rb-r)/(rb-ra), 0, 1)*(rho_cu/rho_sn)/t
on copper of the protrusion side; nothing elsewhere."""
p = make_problem([(PLATE20, [])],
rect1_mm=(0, 0, 1, 20), rect2_mm=(19, 0, 20, 20))
p.electrodes1 = [_barrel(10, 10, drill_mm=1.0, pad_mm=2.4, solder=True)]
p.electrodes1[0].protrusion_side = "F.Cu"
stack = raster.rasterize_stack(p, 0.1 * NM)
assert stack.thick_scale is not None
ny, nx = stack.shape2d
jj, ii = np.meshgrid(np.arange(nx), np.arange(ny))
r = np.hypot(stack.x0_nm + (jj + 0.5) * stack.h_nm - 10 * NM,
stack.y0_nm + (ii + 0.5) * stack.h_nm - 10 * NM)
ra, rb, H = 0.5 * NM, 1.2 * NM, p.tht_protrusion_nm
t_eq = H * np.clip((rb - r) / (rb - ra), 0, 1) \
* (p.rho_ohm_m / p.solder_rho_ohm_m)
expect = np.where(stack.masks[0],
1.0 + t_eq / p.layers[0].thickness_nm, 1.0)
assert np.allclose(stack.thick_scale[0], expect, rtol=1e-12)
# 1.5 mm of solder at the wall ~ 191 um copper: factor ~ 3.7 on 70 um
assert stack.thick_scale[0].max() > 3.0
p.electrodes1[0].protrusion_side = None # e.g. via contact: no cone
s2 = raster.rasterize_stack(p, 0.1 * NM)
assert s2.thick_scale is None
def test_lead_fillet_lowers_resistance(monkeypatch):
"""The cone shorts the joint vicinity: R(with cone) < R(coat-less
bare barrel); the adaptive grid pins the cone cells fine and
matches the uniform grid."""
def prob(protrude=True):
p = make_problem([(PLATE20, [])],
rect1_mm=(0, 0, 1, 20), rect2_mm=(19, 0, 20, 20))
p.electrodes1 = [_barrel(10, 10, drill_mm=1.0, pad_mm=2.4,
solder=True)]
p.electrodes1[0].protrusion_side = "F.Cu"
if not protrude:
p.tht_protrusion_nm = 0
return p
r_cone, _ = _solve(prob(), 0.1)
r_bare, _ = _solve(prob(protrude=False), 0.1)
assert r_cone.R_ohm < r_bare.R_ohm
from fill_resistance import config
monkeypatch.setattr(config, "ADAPTIVE_CELLS", True)
r_ada, _ = _solve(prob(), 0.1)
assert r_ada.R_ohm == pytest.approx(r_cone.R_ohm, rel=2e-3)
def test_barrel_electrode_json_roundtrip(tmp_path):
p = make_problem([(PLATE20, [])],
rect1_mm=(0, 0, 1, 20), rect2_mm=(19, 0, 20, 20))
p.electrodes1 = [_barrel(10, 10, drill_mm=0.6, pad_mm=1.2, solder=True,
polygons=[_disc(10, 10, 0.6)])]
p.electrodes1[0].barrel_z = (-1, 1_600_001)
p.electrodes1[0].protrusion_side = "B.Cu"
p.tht_protrusion_nm = 1_200_000
f = tmp_path / "d.json"
save_problem(p, f)
q = load_problem(f)
e = q.electrodes1[0]
assert e.drill_nm == 600_000 and e.pad_nm == 1_200_000
assert e.center == (10 * NM, 10 * NM)
assert e.barrel_z == (-1, 1_600_001)
assert e.solder is True and len(e.polygons) == 1
assert e.protrusion_side == "B.Cu"
assert q.tht_protrusion_nm == 1_200_000