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سجل التغييرات الكاملالمحرّك 1.18.3

AC Resistance, Skin Effect & Trace Loss

المسارات والنحاس

The AC resistance of a real trace, the loss it produces, and the frequency where the laminate takes over from the copper.

هذه الصفحة غير مترجمة بالكامل بعد. الأجزاء غير المترجمة معروضة بالإنجليزية.

المدخلات

ملف اللوحة

Fills Copper weight وDielectric constant (Dk) from your board profile.

1 oz/ft² of finished copper is 34.8 µm
oz
For stripline, the plane-to-plane spacing
From the laminate datasheet. You get a warning if it is far from the working frequency.
Hz
10 GHz
Hz
5 GHz
Ask the fab which foil. If unknown, use the loss band, not one number.
From the channel budget, after connectors, vias and package
dB
°C

النتائج

1 ناجحة
Loss over the routed length IL
3.079dB
ناجح

المعيار: loss over 254 mm at 5 GHz ≤ the 10.0 dB allowance, at the rough end of the band
Attenuation at the stated frequency α
0.3079dB/in
AC resistance per unit length Rac

23.4× the DC value
57.85Ω/m
Crossover, conductor equals dielectric f×
4.941GHz
كل النتائج (10)
Skin depth δ
934.6nm
DC resistance per unit length Rdc
2.477Ω/m
Roughness factor K

at most 2
1.160
Conductor loss over this length
1.536dB
Dielectric loss over this length
1.543dB
Loss over this length, smooth copper

the smooth end of the band
2.867dB
Reach for the allowance

32.5 inches at this frequency
824.9mm
Frequency at which the copper is two skin depths thick
14.42MHz
Characteristic impedance used Z0

same model as Controlled Impedance & Delay
48.18Ω
Effective permittivity used εeff
2.784
Loss over 254 mm at 5 GHz is 3.08 dB, inside the 10.0 dB allowance even at the rough end of the band.

Trace loss alone does not decide whether a link works. Reflections, crosstalk and the receiver equaliser matter too, and none are modelled here. Confirm with a channel simulation.

Roughness puts the loss over this length between 2.87 dB (smooth) and 3.08 dB. The Hammerstad correction caps conductor loss at twice the smooth-copper value, so it cannot represent rougher foil.

Conductor and dielectric loss are equal at 4.941 GHz. Below it, widen the trace or use smoother foil; above it, the laminate matters most.

Roughness is entered as RMS. Fabs often quote Rz, Ra or a foil class instead, which are different. If yours is not RMS, use the whole band.

conductor, smoothconductor, with roughnessdielectrictotal

إلى أي حد نعرف هذا الرقم

من أين تأتي الطريقة
  • Wheeler (1942)
  • Hammerstad and Jensen (1980)
  • Hammerstad and Bekkadal

Wheeler, Formulas for the Skin Effect, Proceedings of the IRE (1942) المعادلة

Hammerstad and Jensen, Accurate Models for Microstrip Computer-Aided Design (1980) المعادلة

Hammerstad and Bekkadal, A Microstrip Handbook, University of Trondheim معايرة على قياسات

صادقة ضمن
  • Dielectric constant (Dk) 1 to 20

Dielectric constant (Dk) The impedance model was fitted for ordinary laminate permittivities. Outside that range it is not reliable enough to differentiate.

مدى دقتها
Dielectric loss is exact for stripline.

For microstrip the √ε_eff form leaves out the filling factor, so it overstates dielectric loss somewhat, on the safe side. Conductor loss uses Wheeler’s rule, which reproduces the exact coaxial result. Foil roughness and the loss tangent at your frequency move the answer most, so roughness is shown as a band and the verdict uses its rough end.

عملياً يهيمن على عدم اليقين مدخل واحد: Foil roughness, RMS. ضيّقه يضِق معه الجواب.

يُقاس مقابل

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المقطع العرضي

المبدأ

Trace loss has two parts. Copper loss rises with the square root of frequency as the skin depth shrinks; dielectric loss rises linearly. The frequency where they cross decides the fix: below it, a wider trace and smoother foil; above it, a better laminate.

Skin depth
δ=ρπfμ0\delta = \sqrt{\frac{\rho}{\pi f \mu_0}}
2.09 µm in annealed copper at 1 GHz (ρ = 1.724 × 10-8 Ω·m).
Surface resistance
Rs=πfμ0ρ=ρδR_s = \sqrt{\pi f \mu_0 \rho} = \frac{\rho}{\delta}
Wheeler’s incremental inductance rule
R=Rsμ0 ∂L∂nR = \frac{R_s}{\mu_0}\,\frac{\partial L}{\partial n}
L is the external inductance per unit length, and n is how far every conductor surface recedes into its own conductor. For coax it gives Rs/(2πa) + Rs/(2πb) exactly, so the ground return is included.
Conductor attenuation
αc=K R2Z0\alpha_c = \frac{K\,R}{2 Z_0}
nepers per metre; multiply by 8.6859 for decibels.
Hammerstad roughness correction
K=1+2πarctan⁡(1.4(Δδ)2)K = 1 + \frac{2}{\pi}\arctan\left(1.4\left(\frac{\Delta}{\delta}\right)^{2}\right)
Dielectric attenuation
αd=πfεeff tan⁡δc0\alpha_d = \frac{\pi f \sqrt{\varepsilon_{eff}}\,\tan\delta}{c_0}
Equivalently 2.31 dB/in per GHz × √εeff × tan δ.
The DC blend
R(f)=Rdc2+Rac2R(f) = \sqrt{R_{dc}^{2} + R_{ac}^{2}}
Only smooths the curve through the transition; read nothing from its shape there.
  • δ\deltaskin depth
  • RsR_ssurface resistance, ohms per square
  • Δ\Deltafoil roughness, RMS
  • KKHammerstad roughness factor, between 1 and 2
  • αc\alpha_cconductor attenuation
  • αd\alpha_ddielectric attenuation
  • εeff\varepsilon_{eff}effective permittivity of the line
  • Z0Z_0characteristic impedance, from the same model as the impedance page
تفاصيل إضافية

A simple strip formula, ρ/(δw), misses the current crowding to the edges and underside of the trace, and the loss in the return plane. Wheeler’s rule captures both.

Roughness. Hammerstad needs only the RMS roughness and caps the effect at 2×. The Huray model needs parameters fabs rarely publish, and helps only once fitted to measured S-parameters for that foil.

Not included: reflections at via stubs, connectors, AC coupling capacitors and package transitions; fibre weave; crosstalk. This is a matched, uniform line.

References: Wheeler (1942), incremental inductance rule; Hammerstad and Jensen (1980), impedance model; Hammerstad and Bekkadal, roughness correction. For a link standard’s insertion-loss limit, consult that standard.

إصدار المحرك ⁨1.18.3⁩