Although often described as a simple number printed in datasheets, Loss Tangent is fundamentally a description of how much electromagnetic energy a dielectric material dissipates as heat.
Many engineers initially learn about dielectric constant because it affects impedance, but as frequency increases, Loss Tangent becomes exponentially more influential on real-world signal quality.
When a high-frequency signal passes through a dielectric medium, some of its energy is converted into heat due to:
molecular polarization delay
dipole relaxation
ionic conduction
orientation friction
dielectric resonance effects
Loss Tangent captures the combined effect of these mechanisms.
This leads to:
higher insertion loss (S21 degradation)
greater attenuation per inch
lower transmission efficiency
shortened maximum trace length for high-speed lanes
For example:
FR-4 materials typically have tanδ = 0.015–0.020
Mid-loss materials have tanδ ≈ 0.009
Low-loss materials reach tanδ ≈ 0.003
Ultra-low-loss RF/PTFE materials reach tanδ < 0.001
A reduction of Loss Tangent by even 0.002 can noticeably improve the eye diagram at 28 Gbps and 56 Gbps PAM-4 systems.
Loss Tangent is not constant across frequencies. Most materials exhibit rising tanδ as frequency increases, sometimes dramatically.
For example:
A material with tanδ = 0.005 at 1 GHz
may reach tanδ = 0.009 at 10 GHz
and exceed tanδ = 0.014 at 28 GHz
This is why many datasheet numbers measured at 1 MHz or 1 GHz do not reflect real PCB performance in 5G or 77 GHz radar systems.
When selecting materials for extremely high-frequency systems, PCB fabrication quality becomes as important as the material properties themselves. Manufacturers such as SQ PCB have optimized lamination control, resin systems, and micro-roughness reduction techniques to minimize both conductor loss and dielectric loss.
In high-frequency stackups—especially above 30 GHz—controlled material consistency and copper surface treatment can reduce effective Loss Tangent beyond what datasheets predict.

Loss Tangent
Understanding the physical meaning of Loss Tangent requires going beyond formulas and viewing the material as a dynamic, molecular-level system interacting with a rapidly changing electromagnetic field. At low frequencies, molecules have enough time to align with the electric field, store energy, release it, and repeat this cycle with minimal lag. However, at high frequencies—especially above several gigahertz—the electromagnetic field oscillates so rapidly that molecular dipoles can no longer keep up. This mismatch between field oscillation and dipole response is the root cause of dielectric loss and is precisely what Loss Tangent quantifies.
Below are the key physical interpretations that explain why this metric holds such dominance in modern PCB engineering.
At its core, Loss Tangent measures how inefficiently a material stores electromagnetic energy. A perfect dielectric would store energy with no dissipation. Real materials, however, dissipate part of the input energy due to the lagging behavior of dipoles and imperfect polarization mechanisms.
Three factors primarily determine this inefficiency:
Electronic polarization:
Electrons shift relative to nuclei under an electric field.
At extremely high frequencies, electron response is fast but not perfect.
Dipolar (orientational) polarization:
Molecules physically rotate to follow the electric field.
This mechanism slows dramatically at microwave frequencies.
Ionic polarization:
Ions move in response to the electric field, but their inertia creates delays.
Loss Tangent represents how much each of these polarization mechanisms fails to keep up with the applied field at a specific frequency.
Dielectric materials contain molecules with internal relaxation phenomena—time constants that describe how fast they return to equilibrium after being disturbed. These relaxation processes directly influence the magnitude of Loss Tangent.
A material with a strong relaxation peak near the operating frequency will exhibit a significant increase in Loss Tangent, causing:
higher attenuation
more severe waveform distortion
increased thermal loading
This effect becomes severe in mmWave frequencies, where many conventional materials show relaxation peaks that were irrelevant at lower frequencies.
It is at this stage that Loss Tangent overtakes dielectric constant as the far more influential factor.
The total attenuation experienced by a high-speed signal includes both conductor loss and dielectric loss. At lower frequencies, conductor loss dominates; however, as frequency continues rising:
Dielectric loss quickly becomes the primary source of signal attenuation.
This occurs because:
copper loss increases with √frequency (skin effect)
dielectric loss increases linearly with frequency
Therefore, when signals approach 20–80 GHz, the dielectric portion often surpasses copper loss even when smooth copper is used.
This is why engineers designing for mmWave systems focus heavily on selecting materials with ultra-low Loss Tangent.
Many designers assume dielectric constant alone defines propagation velocity and phase delay. However, Loss Tangent also contributes to dispersion—where different frequencies within the same signal travel at different speeds.
This phenomenon leads to:
eye diagram collapse at long trace lengths
jitter accumulation in multi-gigabit lanes
timing skew between differential pairs
resonant frequency shifts in RF circuits
Although this dispersion effect is less discussed in basic PCB training, it becomes a dominant limitation in:
28–112 Gbps SerDes
60–80 GHz radar antennas
satellite phased-array systems
Thus, Loss Tangent not only attenuates signals—it changes their phase relationships.
For decades, PCB designers were taught to prioritize dielectric constant (Dk) because it influences impedance control, routing geometry, and signal velocity. While dielectric constant certainly remains important, the shift toward multi-gigabit digital signaling, mmWave radio systems, and high-density packaging has revealed a fundamental truth:
In high-frequency design, dielectric constant shapes the path — but Loss Tangent determines whether the signal survives the journey.
In this section, we analyze why Loss Tangent has overtaken Dk as the key indicator of system-level performance.
The first distinction engineers must internalize is:
Dielectric Constant ≈ affects impedance, routing width, stackup geometry
Loss Tangent ≈ affects insertion loss, reach, waveform integrity, and S-parameter quality
Consider a differential 28 Gbps PAM-4 signal:
Even with perfect impedance control (driven by Dk),
the eye diagram may fully collapse if Loss Tangent is too high.
This is because insertion loss impacts:
signal amplitude
jitter margin
equalization requirements
error vector magnitude (EVM)
bit error rate (BER)
Thus, perfect impedance cannot compensate for poor dielectric loss.
In long-reach channels such as:
PCIe Gen5 / Gen6
56G / 112G SerDes
QSFP-DD and OSFP module interconnects
high-speed backplanes
the channel’s loss budget is the primary limiting factor. More specifically:
Each material’s Loss Tangent directly controls how far high-speed signals can travel before becoming unrecoverable.
For example:
A material with tanδ = 0.015 (typical FR-4)
may limit a 28 Gbps signal to just a few inches.
A material with tanδ = 0.004 may extend this reach several times over.
This is why system architects are increasingly specifying loss requirements rather than dielectric constant tolerances.
Selecting PCB materials for microwave and mmWave systems is far more complex than selecting materials for low-frequency digital circuits. At frequencies above 6 GHz — and certainly above 24, 28, 39, and 77 GHz — dielectric behavior fundamentally changes. In this operating range, Loss Tangent becomes the dominant specification affecting signal amplitude, phase stability, antenna efficiency, filter Q-factor, and the overall reliability of RF front-end hardware.
In this section, we examine how Loss Tangent shapes material choices across different applications and frequency bands, while also discussing the hidden factors engineers must understand before committing to a specific laminate family.
In mid- to high-frequency RF design, attenuation increases rapidly with frequency. This is because dielectric loss grows linearly with frequency, making it impossible for higher frequencies to “survive” on high-loss substrates.
Typical comparisons:
| Material Type | Approx. Loss Tangent (10 GHz) | Example Use Case |
|---|---|---|
| Standard FR-4 | 0.015–0.020 | Low-frequency digital & power |
| Mid-loss FR-4 | 0.008–0.012 | Entry-level RF (1–3 GHz) |
| Low-loss Hydrocarbon/Glass | 0.003–0.005 | 6–18 GHz RF front-ends |
| PTFE-based | 0.0009–0.0025 | 24–77 GHz radar, mmWave, satellite |
| Ceramic-filled PTFE | 0.0004–0.0015 | High-Q filters, precision mmWave |
At mmWave frequencies, even a minor increase in Loss Tangent can double or triple insertion loss.
This is why Loss Tangent is a non-negotiable parameter in high-end RF systems.
In antennas operating at 24, 28, 39, 60, and 77 GHz, efficiency is directly tied to how much of the signal energy is:
radiated into free space
vs.
absorbed by the dielectric
A high-Loss Tangent substrate:
reduces antenna gain
broadens radiation patterns unintentionally
increases thermal dissipation
decreases effective radiated power (ERP)
shortens system detection range (critical for radar)
This is why PTFE or ceramic-filled laminates dominate mmWave radar and satellite antenna boards.
Even a difference of 0.001 in Loss Tangent can alter antenna gain by more than 1 dB at high frequencies — a massive amount in RF design.
Dielectric resonators and microstrip filters rely on the ability of the circuit to store and release electromagnetic energy efficiently. Loss Tangent defines whether this stored energy decays quickly (low Q) or slowly (high Q).
A high Loss Tangent substrate causes:
broader filter skirts
increased insertion loss
reduced stopband rejection
frequency drift with temperature
increased phase noise in oscillator loops
Therefore:
FR-4 → almost unusable above ~3 GHz for filters
Hydrocarbon laminates → usable up to 6–18 GHz
PTFE/Ceramic PTFE → required for 24–80 GHz high-Q structures
If an engineer attempts a 77 GHz filter on FR-4, the circuit will barely function — almost all energy is lost before the resonator completes a full cycle.
In phased-array systems — widely used in radar, satellite communication, and 5G base stations — phase accuracy is critical. Steering angle, beam sharpness, side-lobe levels, and tracking precision all depend on maintaining consistent phase across multiple elements.
Loss Tangent directly influences:
phase error due to dispersion
temperature-driven phase shift
feed network stability
inter-element mismatch
At 77 GHz, even tiny variations in Loss-Tangent between layers or boards can cause:
beam pointing errors
degraded angular resolution
reduced target detection accuracy
This is another reason mmWave arrays almost always rely on low-tanδ PTFE composites.
Engineers sometimes focus solely on the Loss Tangent value, ignoring the fact that dielectric thickness strongly affects attenuation.
Thicker dielectrics = longer field penetration path = more energy lost.
For mmWave designs:
100 μm materials produce significantly less loss than 200–300 μm
ultra-thin substrates improve antenna efficiency
thinner materials reduce dispersion
thin laminates also reduce dielectric heating
This is why many radar modules use prepregs as thin as 75–100 μm.
Loss Tangent and dielectric thickness must always be considered together — never separately.
High-frequency and high-speed PCB engineering has evolved to a point where traditional material metrics—such as dielectric constant alone—no longer capture what truly determines signal integrity and system reliability. Across digital, RF, mmWave, radar, and aerospace platforms, the Loss-Tangent has emerged as the most decisive indicator of material quality. It determines how much high-frequency energy survives propagation, how stable the phase response remains across temperature and aging, and how predictable the system behaves in real-world deployment.
This article explored the meaning and implications of Loss Tangent, including its definition, physical interpretation, and its profound influence on PCB performance. We also examined system-level impacts across multiple industries and detailed how routing, stackup, copper characteristics, manufacturing variables, and signal-conditioning strategies interact with the Loss Tangent. Importantly, we also addressed how to build a practical material-selection workflow that considers cost, manufacturability, long-term stability, and real-frequency dispersion characteristics.
My central reflection is this: engineers must move beyond the habit of treating datasheet values as fixed truths. The Loss-Tangent is not a standalone parameter—it interacts with temperature, humidity, copper roughness, lamination consistency, and the electromagnetic architecture of the system itself. True engineering excellence lies not just in choosing the lowest-loss option, but in understanding how the parameter behaves in context, how it impacts the full signal chain, and how to design mitigation strategies without inflating cost or complexity.
As data rates rise to 112 Gbps PAM-4 and 6G communication extends into mmWave and sub-THz domains, mastering the Loss Tangent becomes indispensable. The systems of the future will not be limited by logic or processing capability—they will be limited by the materials that carry the signals. Those who understand how to evaluate, optimize, and leverage Loss Tangent performance will shape the next generation of high-frequency electronics.
Transmission line test coupons—such as differential stripline, microstrip, or resonator-based structures—are fabricated alongside the PCB. These allow accurate measurement of insertion loss, phase delay, and frequency dispersion. This real-world data often differs from datasheet values, making coupon testing indispensable for high-frequency designs.
Dielectric constant determines how electromagnetic fields propagate through a material and affects impedance and phase velocity. The Loss Tangent measures how much signal energy is converted into heat during propagation. Dk influences signal speed and impedance, while Loss Tangent directly impacts signal attenuation and bandwidth integrity.
Not necessarily. While lower Loss Tangent reduces dielectric loss, other factors such as copper roughness, routing length, via transitions, and manufacturing consistency may dominate total attenuation. The best material choice depends on the system-level loss budget, not simply the lowest available Loss Tangent.
Ultra-low-loss materials often use specialized resin chemistry—such as PTFE, LCP, or ceramic-filled systems—and require more complex lamination processes. These materials maintain stable Loss Tangent across wide temperatures and high frequencies, making them essential for radar, satellite, and mmWave applications. The higher cost reflects performance stability rather than just the raw materials themselves.
The Loss Tangent typically increases with temperature due to higher molecular mobility in the resin system. For automotive radar and aerospace applications, this can alter both attenuation and phase stability. Selecting materials with tightly controlled thermal dispersion is crucial for systems requiring precise frequency performance.