Jun 26, 2026

The real engineering question isn't "how does this material perform at 25°C." It's "how does this material perform at the temperature it will actually see for years of continuous service" — and whether the answer to that question was ever tested at all, or just assumed. A flat line on a marketing slide is a claim. A continuous, five-point curve from a named test standard, with a stated fitting error, is data. This gap between advertised performance and real-world service becomes most consequential above 300°C — and that is exactly where most datasheets stop providing data.
Here's what most datasheets don't explain: pure silica aerogel has a well-known high-temperature weakness, and it isn't a manufacturing defect — it's basic physics.
Mean Temperature | Thermal Conductivity λ |
|---|---|
100°C | 0.022 W/(m·K) |
200°C | 0.024 W/(m·K) |
300°C | 0.028 W/(m·K) |
400°C | 0.033 W/(m·K) |
500°C | 0.043 W/(m·K) |
Compared to the sixfold conductivity increase documented for unreinforced pure aerogel between 300K and 700K, this fiber-reinforced blanket's rise from 0.022 to 0.043 W/(m·K) across the full 100–500°C range — roughly a factor of two — reflects exactly the kind of radiative-transfer suppression that reinforcement is engineered to deliver.
The thermal conductivity curve above is only part of the verified data behind this product. The structural performance figures referenced in the scenarios below — shrinkage resistance (ASTM C356), tensile strength (GB/T 17911), and vibration-induced mass loss (GB/T 34336) — come from the same third-party testing program and are introduced at the point each becomes relevant to a specific application.
Battery energy storage systems occupy one of the most safety-scrutinized corners of industrial design today. When thermal runaway occurs in a lithium-ion cell or module, the entire safety case for the installation rests on one question: does the failure stay contained, or does it propagate to the next cell, module, or unit?
What a stable high-temperature material does solve, inside that broader fire safety system, is the structural half of the problem. Passive fire barriers and thermal management layers inside a BESS enclosure need to hold their shape and stay in place under sustained extreme heat — because a barrier that shrinks, cracks, or settles away from a hot surface stops doing its job exactly when the job matters most. This is where the material-level data becomes directly relevant:
1255 kPa transverse tensile strength and 0.3% vibration-induced mass loss — the material resists tearing or shedding particulate inside a sealed enclosure, where dust and debris accumulation is its own hazard
99.7% hydrophobic structure under standby/ambient conditions — relevant to outdoor BESS installations facing humidity and condensation cycles over years of unattended standby operation, where a moisture-absorbing material degrades in ways a datasheet won't show until it's already failed in the field. This hydrophobicity comes from methyl-based surface groups, which are known in the aerogel literature to oxidize under sustained exposure above roughly 300°C in air — so the 99.7% rating should be read as a standby/ambient-condition property, not a guarantee that persists through a sustained high-temperature thermal event
That distinction matters because the backup insulation layer has its own well-documented failure mode, separate from hot-face spalling. Multilayer refractory systems — hot face, safety layer, insulation — are vulnerable to layer separation and delamination when repeated thermal cycling stresses the interfaces between layers, particularly in kilns with frequent start-stop cycles or alternative-fuel firing that produces sharper temperature swings than continuous steady-state operation. A backup insulation material that shrinks or settles under sustained heat can open exactly the kind of interface gap that industry literature identifies behind this delamination pattern — which is the general engineering principle behind why shrinkage resistance is the critical spec for this application:
Less than 0.8% shrinkage after 96 hours at 649°C is what prevents the interface gap that industry literature identifies behind this delamination pattern from forming in the first place
A1 non-combustible rating and near-zero soluble chlorides matter for kiln shells where any chloride contribution to the steel shell's corrosion budget compounds over years of continuous high-temperature service
The same shrinkage resistance and flat conductivity curve that solve the BESS and kiln backup scenarios apply directly here:
Soluble chloride below 20 ppm and full ASTM C795/C692 compliance address Corrosion Under Insulation risk on high-alloy piping, where traditional fiber insulation's moisture retention is the root cause of most CUI failures
Pure, unreinforced silica aerogel is nearly transparent to infrared radiation in the 2–8 μm range. At room temperature this doesn't matter much, but above roughly 300°C, radiative heat transfer starts to dominate, and an infrared-transparent material has little to stop it — published research on unreinforced aerogel has recorded conductivity increases of sixfold or more between 300K and 700K. Fiber-reinforced aerogel blankets, like Premium S-Grade, are specifically engineered to interrupt that radiative pathway, which is why the reinforced product's curve stays comparatively flat where unreinforced aerogel's does not.
Its high-temperature structural stability supports passive thermal barrier design, but it does not replace UL 9540A system-level fire propagation testing required for AHJ approval in most North American jurisdictions. See the BESS scenario section above for full performance boundaries and application notes.
It's an insulation material, used as backup insulation behind the refractory hot-face lining — not a substitute for fireclay, alumina, or castable refractory that directly contacts flame or molten process material. Its role is reducing heat loss and protecting the kiln shell, the same function traditional ceramic fiber or microporous board backup insulation performs.
GB/T 10294-2008, the Double-Specimen Steady-State Plate Method, on Sample ID NJ20260521A01-12 at 174 kg/m³ density. The fitted curve has a maximum error of 2.28% against the five measured data points. The full lab report is available on request.
Want the full lab report behind this curve, or a project-specific read on where your application sits relative to the data above?
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Website: www.cn-aerogel.com
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- A project-specific thermal calculation for petrochemical, power, BESS, or kiln backup insulation applications
The comparative figures cited for unreinforced silica aerogel (including the sixfold conductivity increase between 300K and 700K) are drawn from published third-party academic research on pure, unreinforced aerogel as a general material category, not from testing of any specific competitor's commercial product, and are cited for material-science context only. This article serves only as technical reference and does not constitute engineering warranty or performance guarantee. Professional thermal, structural, and fire-safety design guidance specific to your application and jurisdiction is recommended for all projects.
Hebei Woqin Co., ltd. is a professional exporter of high-performance silica aerogel insulation materials, headquartered in Shijiazhuang, Hebei Province, China. The company focuses on providing stable, energy-saving, and safe thermal solutions for global customers in petrochemical, power generation, offshore marine, new energy, and industrial manufacturing sectors.
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