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Technology
Until Aspen Aerogels’ breakthroughs in drying time and material form,
aerogels were limited to the realms of intellectual curiosity and research.
Kistler
formed the first aerogels in 1931 by replacing the liquid phase in a gel with
air. These first aerogels used silica as the solid phase since gels can be formed
via polymerization of silicic acid, which is readily generated by acidic neutralization
of sodium silicate in water. In this reaction, polysilicic acid rapidly forms
a solid network structure that entrains the water to form a nanoporous gel structure
or “hydrogel.” This silica hydrogel is then repeatedly rinsed with
volumes of fresh anhydrous methanol to remove virtually all traces of water. The
contents of the gel are brought past the critical point of methanol in a high
temperature autoclave to a supercritical condition. The system is then slowly
depressurized while maintaining a temperature that prevents recondensation of
methanol within the porous silica gel structure.
Kistler demonstrated that the gel’s pore structure was maintained by
drying the gels under supercritical conditions of methanol. He argued that the
surface tension between water and the gel structure caused collapse of pores during
drying at atmospheric pressure. As he stated in his 1931 paper in Nature, “no
evaporation of liquid can occur [under supercritical conditions] and consequently
no contraction of the gel can be brought about by capillary forces at its surface.”
The inverse relationship between capillary force and pore size makes pore collapse
(with a great deal of associated shrinkage) during solvent evaporation overwhelming
for materials with pore sizes on the scale of nanometers (10-9 meters).
Removal of entrained solvent under supercritical conditions brings the liquid-vapor
surface tension within the pore structures to near zero, and thus strong capillary
forces that would collapse the pores are avoided. The result is a dried gel material
that has suffered the least amount of shrinkage, retains the highest porosity,
and has the highest pore volume and surface area practically attainable. Because
the pores are filled with air after drying, they are called “aerogels”.
Drying time for aerogels can take many days using these methods.
Most aerogels have been produced as stiff, brittle monoliths from silica gels
by carefully removing the solvent via a supercritical fluid extraction method,
leaving behind only the network structure of interconnected silica material. The
volume previously occupied by the solvent is then occupied by air, typically comprising
as much as 99.8% of the volume of the remaining solid. In other words, aerogels
have densities as low as 1/500th of the base material. Due to this unique structure,
aerogels provide from two to tens times more thermal and acoustical insulating
capacity than existing insulations per unit of material.
Despite these advantages, and the application of supercritical drying, processing
times for aerogels remained long and arduous, and costs were prohibitive. In addition,
monoliths and later forms such as beads and granules were hard to handle, and
required different installation procedures than the flexible batting materials
that dominate the insulation landscape.
In the mid to late 1990’s, Aspen Systems perfected proprietary changes
in the formulation, processing and drying of aerogels, reducing drying time to
a few hours. Besides a cost effective drying time, the aerogels were also isolated
in the form of thin, flexible blankets. The blankets were much more robust than
the monoliths and beads, and could also be easily installed like any other flexible
batting. These breakthroughs led to the formation of Aspen Aerogels, Inc. in 2001,
and the commercialization of aerogel technology for broad use.
Aspen Aerogels has created a variety of organic and inorganic/organic hybrid
aerogel formulations including those made from polydimethylsiloxane/silica, cellulose
polyurethane, polyimide, polymethylmethacrylate/silica, and polybutadiene rubber.
These materials show enhanced physical and mechanical properties relative to pure
silica aerogel.
We presently manufacture silica aerogels in volume in the form of thin flexible
blankets reinforced with fibers, with properties as shown below. For more specific
data, please check the Product Data Sheets in our Literature
Center.
In addition, a libraries worth of additional information about the properties
of aerogels, and about aerogels in general can be found at http://eande.lbl.gov/ECS/aerogels/satoc.htm.
| Thermal Conductivity |
0.011-0.013 W/m-K
at 38ºC (100ºF) and 760 torr. Conductivity decreases to 0.004 W/m-K at 10 torr. |
Constant Use Temperatures |
-273°C/-459°F to 650°C/1200°F |
| Density |
Currently available in densities
from 0.10 to 0.12 g/cm3 (6 pcf to 8 pcf). |
Surface Area |
Nominal surface areas are between
400 and 1000 m2 /gram depending on formulation. |
| Pore Size Morphology and Distribution |
Open celled structure (2-50 nm
pores) with an average pore size approximately 10 nm. |
Flexibility |
Conformable at 0.25” thickness,
drapeable at 0.125” thickness. |
| Compressive Strength |
Aerogels typically have excellent
compressive strength compared to microcellular foams and fibrous insulations. |
| Hydrophobicity: |
Unencapsulated materials will float
on pure water indefinitely and resist liquid water infiltration to at least 750
psi in static water pressure tests. |
| Acoustic properties |
At 100 m/s, aerogels have an extremely
slow speed of sound. Sound adsorption is significantly enhanced with fiber reinforcement. |
| Toxicity |
Our aerogels are based on amorphous
silica gel, which is considered safe and non-toxic. In typical handling, unencapsulated
materials will generate nuisance dust. Please click to the MSDS in our Literature
Section for more details. |
|
A
variety of dopants and reinforcing agents may be added to modify the properties
of our blankets. For example, IR opacifying agents added to silica aerogels minimize
infrared transmission across virtually the entire visible, near-IR and mid-IR
region. We have manufactured silica aerogels monoliths and blankets with thermal
conductivity (k) values as low as 0.011W/m•K (R-value of approx. 13 per
inch) at 100°F. Cooling and evacuation also improve the thermal performance
of our aerogels, with thermal performance approaching 0.001 W/m-K (R-144 per inch)
at cryogenic temperatures and under hard vacuum.
As shown in the chart on the right, aerogels offer significantly more insulating
value per unit of material than other insulations. |
| MATERIAL
|
Ambient Thermal
Conductivity
(mW/m-K) |
| Aerogel |
12 |
| Polyurethane
Foam |
21 |
| Polystyrene
Foam |
38 |
| Microporous
Silica |
19-38 |
| Fiberglass |
40 |
| Mineral Wool |
38 |
| Perlite |
40-60 |
| Calcium Silicate |
47 |
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