RO4003C vs RO4350B — When the Lower Df Justifies the Same Process Cost

Table of Contents

Rogers RO4003C and RO4350B are both hydrocarbon ceramic laminates in the Rogers RO4000 series. Both process on standard FR4-compatible equipment — no plasma activation, standard drill parameters, up to 3 lamination cycles, compatible with RO4450F bondply for hybrid stackups. The single meaningful difference is Df: RO4003C at 0.0027 vs RO4350B at 0.0037 — a 27% reduction in dissipation factor. This guide answers the practical question: at what frequency and trace length does this 27% Df difference produce enough insertion loss improvement to justify specifying RO4003C over RO4350B? For material stock and ordering, see Rogers PCB manufacturer.

Side-by-Side Specification Comparison

PropertyRO4350BRO4003C
Dielectric constant Dk (10GHz)3.48 ±0.053.38 ±0.05
Dissipation factor Df (10GHz)0.00370.0027 — 27% lower
Thermal conductivity0.69 W/m·K0.71 W/m·K
CTE (x,y)14 ppm/°C11 ppm/°C
CTE (z)32 ppm/°C46 ppm/°C
Tg (glass transition)280°C>280°C
Process compatibility✅ FR4-compatible, no plasma✅ FR4-compatible, no plasma
Max lamination cycles33
Available thicknesses0.101–1.524mm (8 options)0.203–1.524mm (6 options)
Bonding prepreg (hybrid stackup)RO4450FRO4450F
The Dk difference (3.48 vs 3.38) is small but not zero — it produces a slightly wider 50Ω trace on RO4003C for the same substrate thickness, and a slightly shorter electrical path for the same physical length. For most designs the trace width difference is under 0.05mm and can be ignored. For precision filter designs where electrical length determines resonant frequency, the Dk difference should be accounted for in simulation — do not assume the two materials are interchangeable without recalculating trace geometry.

RO4003C and RO4350B are not pin-compatible for a design already laid out on one material. The different Dk values produce different trace widths for the same impedance target. If you switch materials after layout is complete, the impedance will shift and the design must be re-optimized.

Side-by-Side Specification Comparison

Rogers RO4003C vs RO4350B insertion loss comparison chart showing dB per centimeter versus frequency from 1GHz to 20GHz
FrequencyRO4350B (dB/cm)RO4003C (dB/cm)Difference (dB/cm)Over 10cm path
1 GHz~0.05~0.04~0.01~0.1 dB — negligible
5 GHz~0.12~0.09~0.03~0.3 dB — small
10 GHz~0.18~0.13~0.05~0.5 dB — verify budget
15 GHz~0.24~0.17~0.07~0.7 dB — significant
20 GHz~0.32~0.23~0.09~0.9 dB — significant

The insertion loss values above are approximate for 50Ω microstrip on 0.508mm substrate with 1oz copper. The 27% lower Df of RO4003C produces a consistent loss advantage at every frequency — but the absolute dB difference scales with frequency. At 5GHz, RO4003C saves approximately 0.03 dB/cm — over a 5cm trace, 0.15 dB total. At 15GHz, the saving is 0.07 dB/cm — over 5cm, 0.35 dB. Whether these numbers are significant depends entirely on your system loss budget.

Side-by-Side Specification Comparison

Substrate ThicknessRO4350B 50Ω (1oz)RO4003C 50Ω (1oz)Difference
0.254mm~0.54mm~0.56mm~0.02mm — negligible
0.338mm~0.72mm~0.75mm~0.03mm
0.508mm~1.05mm~1.09mm~0.04mm — negligible
0.762mm~1.58mm~1.64mm~0.06mm
1.524mm~3.16mm~3.28mm~0.12mm

The trace width differences are small — under 0.1mm for all common thicknesses. For designs where trace width is not constrained by element spacing or layout density, this difference is irrelevant. For phased array feed networks where element pitch tightly constrains trace width, the 0.02–0.06mm difference may affect routability at high frequencies — confirm with simulation.

When RO4003C Is Worth Specifying

Designs above 10GHz with loss budget constraints

Below 10GHz, the absolute insertion loss difference between RO4003C and RO4350B over typical trace lengths (under 10cm) is under 0.5 dB. Most RF system budgets can absorb this without affecting performance. Above 10GHz, the difference grows — at 15GHz over a 10cm feed network, RO4003C saves approximately 0.7 dB vs RO4350B. In a receiver front-end where 0.7 dB directly degrades noise figure, this is a meaningful improvement.

Microwave bandpass filters with tight insertion loss specification

In a coupled-line or hairpin bandpass filter, the filter insertion loss in the passband is directly proportional to the substrate Df — lower Df gives lower filter insertion loss. For a filter with a specified maximum passband insertion loss of 1 dB at 10GHz, the difference between RO4350B and RO4003C may determine whether the design passes or fails the specification. This is one of the clearest cases where the Df improvement of RO4003C provides measurable benefit.

Long feed networks in phased array designs

In a phased array PCB with a corporate feed network, the cumulative loss through multiple Wilkinson divider stages adds up. A 4-stage binary divider with 10cm total feed path at 15GHz loses approximately 2.4 dB on RO4350B vs 1.7 dB on RO4003C — a 0.7 dB difference in array efficiency that translates directly to output power and EIRP. For large aperture arrays where feed network loss is a significant fraction of total loss budget, RO4003C is worth the slightly higher material cost.

When RO4350B Remains the Better Choice

  • Designs below 5GHz — the insertion loss difference is under 0.1 dB over any practical trace length, and RO4350B’s slightly lower cost is the deciding factor
  • Short traces at any frequency — if your longest RF trace is under 3cm, the absolute loss difference is too small to affect system performance
  • Thermal management priority — RO4350B (0.69 W/m·K) and RO4003C (0.71 W/m·K) have nearly identical thermal conductivity, but RO4350B’s broader thickness selection (8 options vs 6) may offer more stackup flexibility
  • Design already completed on RO4350B — switching to RO4003C requires recalculating all trace widths for the different Dk and re-running impedance verification. The performance gain must justify the redesign cost

Hybrid Stackup Considerations

Both RO4003C and RO4350B use RO4450F bondply at the Rogers-to-FR4 interface in hybrid stackups — the bonding prepreg is the same for both materials. CTE in the z-axis differs slightly (RO4003C 46 ppm/°C vs RO4350B 32 ppm/°C) — for thick multilayer boards with many thermal cycles, confirm via barrel reliability with your fabricator if switching between the two materials in an established design.

Design ScenarioRO4350BRO4003C
Below 5GHz, short traces✅ Correct choiceNo measurable benefit
5–12GHz, trace <5cm✅ Usually adequateConsider if NF is tight
5–12GHz, trace >10cmVerify loss budget✅ Lower loss worthwhile
12–20GHz, any trace lengthVerify budget — may be marginal✅ Better choice — 0.7–0.9dB/10cm advantage
Above 20GHzBoth inadequate — PTFE requiredBoth inadequate — PTFE required
PA PCB — thermal priority✅ 0.69 W/m·K0.71 W/m·K — marginally better
Filter with tight IL specCheck if budget allows✅ Lower Df benefits filter IL
Price-sensitive high volume✅ Typically slightly lower costSlightly higher — verify with supplier

RO4350B and RO4003C Both In Stock — 5–7 Day Prototype

Both materials available in standard thicknesses. FR4-compatible process, no plasma activation. TDR impedance verification every lot. RO4450F bondply for hybrid stackups. No MOQ.

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