High-frequency circuit boards are critical in modern electronics, particularly in telecommunications, aerospace, defense, and 5G applications. Rogers Corporation provides high-performance laminates such as RO4000®, RO3000®, RO4003C™, and RT/duroid® series that combine excellent electrical stability with low-loss characteristics. However, DC and RF currents flowing through these boards generate heat, and understanding the resulting temperature rise is crucial for ensuring reliability, signal integrity, and long-term device performance.
1. Factors Influencing Temperature Rise
The temperature rise in a high-frequency PCB depends on multiple interrelated factors:
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Material Thermal Conductivity: Laminates with higher thermal conductivity dissipate heat more effectively. Rogers materials range from ~0.2 W/m·K (PTFE-based RT/duroid) to ~0.8 W/m·K (RO4000 series).
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Trace Geometry: Wider and thicker copper traces reduce resistance and improve heat dissipation.
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Current Density: Higher currents increase resistive heating (I²R losses).
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Operating Frequency: RF currents introduce skin effect and dielectric losses, further raising local temperatures.
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Environmental Conditions: Ambient temperature, airflow, and cooling methods significantly impact thermal behavior.
2. Thermal Properties of Key Rogers Laminates
| Material | Thermal Conductivity (W/m·K) | Dielectric Constant (Dk) |
|---|---|---|
| RO4000 Series | 0.62 – 0.80 | ~3.5 |
| RO3000 Series | 0.5 – 0.6 | ~3.0 |
| RT/duroid 5870/5880 | 0.20 – 0.25 | 2.2 – 2.33 |
These properties help designers select laminates that balance electrical performance, signal integrity, and thermal management for high-frequency applications.
3. Calculating Temperature Rise
A. DC Current Heating
For direct current (DC), the temperature rise can be estimated using Joule heating:
ΔT=I2⋅RA⋅k⋅t\Delta T = \frac{I^2 \cdot R}{A \cdot k \cdot t}
Where:
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II = Current (A)
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RR = Trace resistance (Ω)
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AA = Cross-sectional area of the trace (m²)
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kk = Thermal conductivity of the laminate (W/m·K)
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tt = Thermal dissipation thickness (m)
This formula allows engineers to predict ΔT and optimize trace dimensions and laminate selection for minimal heating.
B. RF Current Heating
For high-frequency applications, RF currents are affected by skin effect, which concentrates current near the conductor surface and increases effective resistance:
RRF=RDC⋅δDCδRFR_{RF} = R_{DC} \cdot \sqrt{\frac{\delta_{DC}}{\delta_{RF}}}
Where:
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δRF=ρπfμ\delta_{RF} = \sqrt{\frac{\rho}{\pi f \mu}} is the skin depth
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ρ\rho = Conductor resistivity
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ff = Operating frequency (Hz)
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μ\mu = Permeability of the conductor
The RF resistance RRFR_{RF} is then used in the Joule heating equation to calculate temperature rise under alternating current conditions.
4. Example Calculation
Consider a RO4003C PCB with a 1 oz copper trace carrying a 2 A RF current at 2 GHz:
Material Parameters:
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Thermal Conductivity: k = 0.62 W/m·K
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Skin Depth: δ ≈ 1.4 μm
Trace Parameters:
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Width: 0.5 mm
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Thickness: 35 μm
Temperature Rise Estimation:
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Calculate effective RF resistance considering skin effect.
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Apply Joule heating formula to determine ΔT.
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Confirm results with empirical measurements or simulation for high accuracy.
5. Mitigation Strategies for Temperature Rise
Designers can reduce temperature rise and improve PCB reliability using several techniques:
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Increase Trace Width or Thickness: Lowers current density and resistance.
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Use Heat Sinks or Thermal Vias: Enhances heat dissipation.
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Select High-Thermal-Conductivity Laminates: RO4000 or RO4350B for critical layers.
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Improve Ventilation: Incorporate forced airflow or optimized enclosure design.
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Use Copper Pours and Thermal Pads: Spread heat efficiently across the PCB.
6. Verification and Testing
Temperature rise estimations should always be validated through:
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Infrared Thermal Imaging: Detect hot spots in operating circuits.
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Thermocouples or RTDs: Measure temperatures at critical points.
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Load Testing: Simulate worst-case conditions to ensure thermal stability.
Empirical methods complement theoretical calculations and ensure real-world reliability.

