Long-Term Reliability of High-Frequency Circuit Materials and Printed Circuit Boards
As complexity and density increase, the long-term reliability of RF/microwave circuit components becomes more challenging to characterize. Printed Circuit Boards (PCBs) comprise numerous active and passive components, whose performance can vary over time and with operating environment temperatures. Additionally, PCB substrate materials, such as dielectrics, copper foil conductors, solder mask inks, and final finishes, may change over time, influenced by environmental conditions. Higher frequencies may experience changes in electrical performance over time, such as power and efficiency losses. These effects can occur in both short-term and long-term scenarios, often driven by thermal effects, particularly when operating in high-temperature environments.
Short-term exposure to high temperatures, such as during PCB assembly reflow soldering, typically does not affect the electrical performance of circuit materials or PCBs. However, when temperatures exceed the Relative Thermal Index (RTI) of the circuit materials or the Maximum Operating Temperature (MOT) of the PCB, electrical performance can be impacted. If temperatures rise above the decomposition temperature (Td) of the circuit materials, even for a few minutes, electrical performance may degrade. RTI is a parameter determined by temperature measurements, representing the highest temperature at which a circuit material can maintain one or more key properties without degradation. MOT is a circuit-level parameter certified by Underwriters Laboratories (UL), applicable to the entire PCB, including the dielectric and conductor layers. While both parameters indicate maximum temperatures, RTI pertains to the circuit material itself, whereas MOT applies to the completed PCB’s highest operating temperature. A circuit’s MOT will not exceed the RTI of its base material, as UL will not issue a circuit MOT higher than the material’s RTI.
High-frequency circuit laminate materials consist of dielectric materials and copper foil conductors, based on thermoplastic or thermoset materials. Thermoplastic materials are typically soft or flexible, while thermoset materials are harder and more rigid. Thermoplastic materials can be heated to melting or reflow temperatures, but thermoset materials cannot. At sufficiently high temperatures, thermoset materials will decompose.
Thermoplastic materials used for RF/microwave/millimeter-wave PCBs are often based on polytetrafluoroethylene (PTFE). While other materials can be used alone or in combination with PTFE for high-frequency circuit substrates, many RF/microwave/millimeter-wave PCBs incorporate PTFE in some form. Thermoset materials used for RF/microwave/millimeter-wave PCBs are generally hydrocarbon resins or polyphenylene ether (PPE or PPO) polymer resins, known for their dimensional stability and cost advantages.
PTFE-based thermoplastic circuit materials are highly regarded for their stability and minimal changes in electrical performance during long-term use and exposure to high temperatures. Conversely, circuits made from thermoset materials, such as those based on hydrocarbon or PPE resins, experience changes in electrical performance over time and temperature, with the extent of these changes dependent on the specific composition of the circuit material.
For nearly pure PTFE circuit materials, like Rogers Corporation’s RT/duroid® 5880 laminates, electrical performance remains highly stable over long-term use and at elevated temperatures (above room temperature or 25°C). For materials combining PTFE with other substances to adjust the dielectric constant (Dk) or provide performance needed for specific circuits (e.g., in millimeter-wave frequencies), the performance over time and temperature can vary due to the additional materials used. For instance, Rogers Corporation’s RO3003™ material, a PTFE-based circuit material with ceramic fillers and other additives, is designed for automotive radar and millimeter-wave frequency applications. As shown in Figure 1, it exhibits different aging characteristics compared to nearly pure PTFE materials.
As depicted in Figure 1, both materials show minimal thermal aging effects, with changes in Dk (relative dielectric constant, εr) of less than 1%. Initially, both materials exhibit a decrease in Dk, related to drying the materials at a high temperature of 150°C. Although both materials are low in moisture absorption, they carry some moisture at the microscopic level before testing. As moisture is driven out of the materials at high temperatures, Dk decreases. The PTFE formulation in RO3003 laminates is more complex than that in RT/duroid 5880, reacting differently to high temperatures and drying effects. However, for long-term aging at 150°C, the Dk change of less than 1% for both materials is considered highly robust.
Compared to thermoplastic materials, thermoset materials show greater changes in Dk under long-term high-temperature exposure. However, the extent of Dk change is closely tied to the specific composition of the thermoset material, and the reasons for Dk changes in thermoset materials differ significantly from those in thermoplastic materials.
The natural reaction of thermoset circuit materials to high temperatures is oxidation. While slow at room temperature, oxidation accelerates at higher temperatures. Oxidation of thermoset substrates is limited to the depth of oxygen penetration, with surface reactions changing as more oxides accumulate until the oxidation process halts. The rate of oxidation and the depth of oxide penetration in thermoset materials depend on the material’s composition. Various types of antioxidants (AOs) can be included in the formulation to slow the oxidation process, with the effectiveness of these antioxidants varying depending on the specific material composition.
Figure 2 compares two thermoset hydrocarbon laminates, one with poor oxidation performance and the other with an optimal AO content for minimizing oxidation effects and providing robust long-term aging performance. The benefits of adding AOs are evident in the stability of Dk changes over time. Figure 2 data is derived from high-temperature Dk changes over time, measured using a fixed-band stripline resonator method in the X-band. Test materials were fully exposed to the environment, and the data shown were extrapolated to longer times using the Arrhenius equation. This accelerated aging method estimates long-term thermal aging effects without extended testing durations. The test data compare a hydrocarbon laminate with Rogers Corporation’s RO4835™ circuit material, known for its long-term stable anti-aging performance. The RO4835 material maintains the same electrical properties as RO4350B™ laminates. For reference, the time scale in Figure 2 shows that 1.0E+05 hours equates to 11.4 years.
▲ Figure 1: Long-Term Aging of Dielectrics in RT/duroid 5880 and RO3003 Laminates
▲ Figure 2: Long-Term Aging of Thermoset Hydrocarbon Circuit Materials at 25°C
The Dk testing for this aging experiment is based on the X-band fixed-band stripline resonator test method defined in IPC-TM-650 2.5.5.5c, used to assess changes in Dk. The test frequency is 10GHz, and the copper foil on the test samples needs to be fully etched away, leaving only the dielectric material. When aging evaluations are performed on circuit materials in circuit form, the aging effects differ because the copper layer can protect the dielectric material from oxidation. The degree of protection depends on the different structures shown in Figure 3.
▲ Figure 3: Simple Cross-Sectional View Showing Different RF Structures and How Oxidation (Yellow) Penetrates Thermoset Dielectric Materials
▲ Figure 4: Comparison Between Bare Dielectric Material (Fully Etched) and 50 Ω Microstrip Line Circuits on 20-mil RO4350B Laminate (Std) and 20-mil RO4350B LoPro Laminate (LoPro)
The description in Figure 3 approximately illustrates how oxidation forms on dielectric materials. An oxide layer forms on the exposed substrate surface, with some oxide reaching beneath the copper foil conductor. In other words, most oxidation occurs on the material’s surface, and as the oxidation gradient accumulates, a small amount of oxidation will penetrate below the surface, although this sub-surface oxidation diminishes over time.
Circuit material parameters such as Dk and dissipation factor (Df) increase in the presence of oxidation. Several factors determine the extent to which oxidation affects the RF/microwave/millimeter-wave electrical performance of circuit materials. Thinner dielectric circuits are more significantly affected due to the proportion of oxidation relative to the entire dielectric material.
The impact of oxidation on RF/microwave/millimeter-wave circuit structures varies depending on the electromagnetic (EM) fields within the circuit. For example, in microstrip lines, most EM fields are between the bottom of the signal conductor and the top of the ground layer, with strong edge fields around the signal conductor. The signal is affected by substantial oxidation. While microstrip lines may not exhibit significant oxidation effects, these effects can be detected at high millimeter-wave frequencies. The impact is less on thicker microstrip circuits compared to thinner ones.
As shown in the position of the signal conductor, stripline structures are generally unaffected by oxidation (Figure 3). However, for edge-coupled microstrip circuits, where the coupling fields are at the surface and slightly below the substrate, intersecting with the oxide layer, oxidation degrades RF/microwave/millimeter-wave performance. At millimeter-wave frequencies, oxidation can also significantly impact ground coplanar waveguide (GCPW) circuits on thin substrates.