Note
Go to the end to download the full example code.
Lumped port tuning: coaxial line#
A pre-flight check for a lumped port terminating a coaxial line: fill in the given quantities of your target model, run, and the scoreboard tells you how good the termination is — worst reflection, usable band, phase error. Edit the three knobs and re-run until the numbers meet your spec, then carry the settings over.
The measurement: a waveguide port launches the exact grid mode onto
the lumped port under test (|S11| is the termination’s
self-reflection), and a reference run of the same line with waveguide
ports at both ends provides the grid-exact phase ruler. The page
Lumped ports: investigations explains the setup and shows
which knob moves which error; every number here is a property of
your grid, so re-run whenever cross-section, resolution or band
change.
import matplotlib.pyplot as plt
import numpy as np
import magnelio as mio
from magnelio import geo, plots, ports
from magnelio.constants import ETA0
Given quantities#
What the target simulation dictates. cell is the cross-section
cell size the test mesh may not fall below — copy the size your
production mesh will actually have at the port.
r_i = 0.405e-3 # inner conductor radius [m]
r_o = 1.475e-3 # shield (dielectric outer) radius [m]
eps_r = 2.25 # solid polyethylene
f_max = 15e9 # upper band edge [Hz]
cell = 0.5 * r_i # production cross-section cell size [m]
The knobs#
The compromise you will carry into the target simulation:
gap— end gap between inner conductor and shorted end plate; sets the broadband reflection level.gap_position— where the gap starts relative to the reference plane (negative = before it); sets the phase error.z0_port—Noneuses the line impedance of the grid, as measured by the waveguide-port solver; a number (e.g. 50.0) uses that instead. Sets the low-frequency reflection floor.
gap = 0.4 * (r_o - r_i)
gap_position = 0.0
z0_port = None
Derived quantities#
closed-form line impedance: 51.67 Ohm
Measurement machinery — a uniform test grid (max = min cell
size), the plain line as phase reference, and the candidate
termination: inner conductor to the gap start, gap, shorted end
plate, lumped port bridging the gap on the axis.
def _model(length, pin_length):
model = mio.GeometryModel(background="pec")
dielectric = geo.Cylinder(
origin=(0.0, 0.0, 0.0),
radius=r_o,
height=length,
axis="z",
material=mio.Material.from_isotropic(name="polyethylene", epsilon=eps_r),
)
inner = geo.Cylinder(
origin=(0.0, 0.0, 0.0), radius=r_i, height=pin_length, axis="z", material="pec"
)
model.add(geo.Difference(dielectric, inner))
model.add(inner)
model.add_port(ports.PortWaveguide(name="wg", plane="zmin"))
return model
def _mesh(model):
return mio.Mesh.from_geometry(
model,
mio.MeshControl(min_cell_size=cell, max_cell_size=cell),
f_max=f_max,
)
ref_model = _model(L, pin_length=L)
ref_model.add_port(ports.PortWaveguide(name="far", plane="zmax"))
ref = mio.AnalysisScatteringTD(mesh=_mesh(ref_model), verbose=False).run(excited=[("wg", 0)])
z_pin = L + gap_position
z_end = z_pin + gap
model = _model(z_end, pin_length=z_pin)
mesh = _mesh(model)
z_line = mio.AnalysisScatteringTD(mesh=mesh, verbose=False).solve_ports()["wg"].z_line_num
print(f"line impedance on this grid: {z_line:.2f} Ohm ({100 * (z_line / z_formula - 1):+.1f} %)")
model.add_port(
ports.PortLumped(
name="dut",
start=(0.0, 0.0, z_end),
end=(0.0, 0.0, z_pin),
Z0=float(z0_port if z0_port is not None else z_line),
)
)
result = mio.AnalysisScatteringTD(mesh=mesh, ports=list(model.ports), verbose=False).run(
excited=[("wg", 0)]
)
mesh | feature planes
mesh | grid lines
mesh | materials
mesh | conformal cells
mesh | PEC masks
mesh | 14 x 14 x 36 cells
mesh | feature planes
mesh | grid lines
mesh | materials
mesh | conformal cells
mesh | PEC masks
mesh | 14 x 14 x 38 cells
line impedance on this grid: 47.31 Ohm (-8.4 %)
The test fixture#
A cut along the propagation direction: the waveguide port on the
left launches down the uniform line, the inner conductor stops at
gap_position relative to the reference plane, and the lumped
port under test bridges the gap to the shorted end plate.
fig, ax = plots.plot_cross_section(model, "y", 0.0, flip=True, title="Coax test fixture")
ax.set_xlim(-0.3, z_end * 1e3 + 1.0)

(-0.3, 8.802999999999999)
The scoreboard#
The phase error is polarity-normalised: the sign of a mode profile is a convention, so the error is referenced to the nearest multiple of 180° at the low end of the band.
f = np.asarray(result.f_axis)
band = f <= f_max
s11_db = result.db("wg", "wg")
err = result.phase("dut", "wg") - ref.phase("far", "wg")
err -= 180.0 * np.round(err[int(np.argmax(f >= f_max / 15.0))] / 180.0)
good = s11_db[band] < -20.0
f_edge = f[band][np.argmin(good)] if not good.all() else f[band][-1]
print("--- current settings — tune until this meets your spec ---")
print(f"worst |S11| in band : {s11_db[band].max():6.1f} dB")
print(f"|S11| < -20 dB up to: {f_edge / 1e9:6.2f} GHz")
print(f"max |phase error| : {np.abs(err[band]).max():6.2f} deg")
fig, (ax1, ax2) = plt.subplots(1, 2, figsize=(9.0, 3.6))
ax1.plot(f[band] / 1e9, s11_db[band])
ax1.set_xlabel("frequency [GHz]")
ax1.set_ylabel("|S11| [dB]")
ax1.set_title("Self-reflection")
ax1.grid(True, alpha=0.3)
ax2.plot(f[band] / 1e9, err[band])
ax2.set_xlabel("frequency [GHz]")
ax2.set_ylabel("phase error [deg]")
ax2.set_title("Phase error at the reference plane")
ax2.grid(True, alpha=0.3)
fig.tight_layout()

--- current settings — tune until this meets your spec ---
worst |S11| in band : -19.5 dB
|S11| < -20 dB up to: 14.18 GHz
max |phase error| : 28.97 deg
The cross-section with the mesh it is actually solved on — check that the gap region resolves the way your production model does.

Carry it over#
Once the three numbers meet your spec, transfer gap,
gap_position (relative to where your reference plane is) and
the port impedance into the target model. Which knob moves which
number — and why — is shown in
Lumped ports: investigations; when the cross-section,
resolution or band changes, run this page again.
Total running time of the script: (0 minutes 1.491 seconds)