Open Access Article
Felix Leven
a,
Mavin Geyerab,
Elisabeth Hutha,
Corina Andronescu
b and
Rainer Ostermann
*a
aTechnische & Makromolekulare Chemie, Westfälische Hochschule, August-Schmidt-Ring 10, 45665 Recklinghausen, Germany. E-mail: rainer.ostermann@w-hs.de
bTechnische Chemie III, Universität Duisburg Essen, Carl-Benz-Straße 199, 47057 Duisburg, Germany
First published on 15th May 2026
The tedious and time-consuming solvent exchange during aerogel production was sped up using a standard Soxhlet extractor. Optimizing the setup with a vent and molecular sieve allowed to save up to 80% of the production time compared to batchwise extractions while maintaining state-of-the-art samples of silica and polyurethane aerogels, i.e. MTMS aerogels with a thermal conductivity of 15 mW m−1 K−1 and PU aerogels with 17 mW m−1 K−1 and good mechanical properties even after freeze-drying, which is generally more stressful than supercritical drying. The syntheses had to be carried out in high-boiling solvents, but adaptation and optimisation were made possible rapidly due to the method developed.
Improvements for solvent exchange have received little attention to date and is hardly mentioned in a recent critical review that highlights all other challenges in aerogels.20 In life cycle analyses, solvent exchange and consumption was identified as the major problem in aerogel sustainability.21 In 2021, Schwan et al. described the use of a peristaltic pump and zeolites in comparison to classic static exchange on RF aerogels.22 Typically, the solvent exchange in the laboratory is accelerated via artificially generated convection (shaker), increased temperature and a large excess of the target solvent.
Frequent changing of the solution increases the concentration gradient and also helps with rapid exchange. All these parameters are part of a classic Soxhlet extraction (SE). The Soxhlet extractor was invented by Franz von Soxhlet in 1879 and was originally used to extract fats from solids.23–25 Soxhlet extraction was used in connection with aerogels to wash out intentionally adsorbed substances.26,27 In 2021, we described a solvent exchange with simultaneous extraction of gelators for polyolfine aerogels, but without scientifically investigating this aspect.28 In this paper we describe the use of Soxhlet extractors for solvent exchange in aerogel synthesis, the necessary conditions and advantages using the example of silica systems and PU materials. We describe these two different systems to illustrate the flexibility of the method. The materials were selected based on their properties and their scientific relevance in the field of aerogels. The aim is to show that high quality aerogels for research purposes can be produced and analysed in a shorter period of time.
2-Octanone, 2-nonanone, cyclohexanone, propylene carbonate, potassium sorbate, ethylene glycol, triethylene glycol, cyclohexane, acetic acid (1 M), ammonia water 25% (for analysis), benzene and methanol were purchased from VWR Chemicals (Radnor, Pennsylvania, USA). 3,3′,5,5′-Tetraethyl-4,4′-diaminodiphenylmethane and benzyl alcohol (BzOH) are supplied by Sigma Aldrich (St. Louis, Missouri, USA). M20 and Lu3300 were provided by BASF (Ludwigshafen, NRW, Germany). Methyltrimethoxysilane (97%) was purchased from ABCR (Karlsruhe, Germany) and tert-butanol (tBuOH) (99%) from S3 Chemicals (Bad Oeynhausen, Germany).
To prepare the MTMS aerogel, 3.34 mL MTMS was mixed with 0.166 mL acetic acid and hydrolysed for 1 hour with stirring. 5.27 mL BzOH was added and stirred for a further hour. The stirrer was then removed and a defined amount (1.0; 1.5; 1.75 mL) of 25% ammonia water was added, the reaction vessel was closed and shaken for 5–10 seconds to ensure homogeneous distribution before gel formation took place. To simplify handling, the solutions can be pre-cooled to reduce the reaction speed and thus allow more time for homogeneous distribution. After 3 hours, the resulting gel is aged at 60 °C for 6 days, as ammonia is slow catalyst.32 It is recommended to have only a small gas space above the sample or to use shielding gas. The aged gel must now undergo a solvent exchange and then be dried.
In order to be able to extract several samples at the same time without them lying directly on top of each other, it is recommended to build a sample holder with grids so that the solvent can flow around the individual samples. Depending on the design, this also makes it easier to insert and remove the solvogels from the chamber. Glass beads can be used to reduce the dead volume in order to realise a faster exchange. The sample should be shielded by a grid to avoid external stress. For the use of hydrophilic solvents, the glass beads can also be replaced by 3 Å molecular sieves to keep the sample free of water. This is particularly useful when working with tBuOH. For better mixing in the chamber, a tube can be inserted via the reflux condenser to inject dry air or N2 gas close to the sample. The flow accelerates the exchange, but also cools the liquid, which is why the gas flow should be set only as high as necessary to have some bubbles per minutes to “agitate” the solvent. Moreover, a small tube can be introduced in the siphon of the Soxhlet as a “vent”: when the solvent level in the chamber falls below the vent, gas enters the siphon and the drain of solvent is stopped. This is not absolutely necessary, as there is always a saturated solvent atmosphere above the sample during the distillation process, but it improves the exchange. In the event of interruptions, it also provides effective protection against superficial drying of the sample.
The purpose of solvent exchange via Soxhlet extraction is to save a significant amount of time compared to batch exchange. This applies not only to the production of individual samples, but also to the manual work involved in the laboratory. Basically, the exchange rate with a suitable solvent depends on several factors, with the sample geometry having by far the greatest influence. If we consider a typical cylindrical sample body where the diameter is greater than the height, the diffusion distance over half the sample height is the speed-limiting factor. If the diameter is smaller than the height, the radius of the sample determines the exchange speed. This problem occurs in every diffusion-driven exchange, but must be considered more intensively in Soxhlet due to the desired time reduction. The exchange rate in the gel body of the sample depends mainly on concentration gradients and the temperature (Fick's first law).33 The concentration gradient to the exchange solvent is kept as high as possible in the chamber by regularly draining and overlaying with fresh solvent. This behaviour follows Nernst's distribution law, which is why exchange with more frequent small Soxhlet cycles is more suitable than large chambers that are renewed less frequently.34 For this reason, the use of filling bodies to reduce the dead volume is recommended. The solubility of the solvents in each other and the diffusion rate are both directly dependent on temperature. This not only enables faster exchange, but also allows the exchange of liquids that are not or hardly soluble in each other under normal conditions. An example of this is the exchange of trichlorobenzene for tBuOH. Since the solvent in the chamber cools slowly at high residence times, a short cycle time is also preferred here. Fig. 2 shows a false-color image of a Soxhlet setup during extraction.
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| Fig. 2 False-colour image of a Soxhlet extraction with tBuOH (without mixing using gas, filled shortly before drainage) (a) very low heating rate (b) normal heating rate. | ||
As can be seen in the figure, a temperature gradient forms in the chamber. In the case of low boiling speed (a), the resulting temperature in the sample area is 14 K lower than in normal operation (b). The temperatures displayed refer to the surfaces and do not indicate the actual values in the Soxhlet, but they do provide a good indication. The use of a diffuse gas stream for mixing can be both advantageous and disadvantageous. Although mixing ensures a better concentration gradient around the sample and improves temperature distribution, if the gas flow is too high, it can also act as active cooling, which is counterproductive. Although it is possible in principle to introduce preheated gas, this is very costly, especially in our setup, where the gas hose is fed through the cooler. The use of a sufficiently low flow rate (some bubbles per minutes) seems to be a good compromise. Another option would be a magnetic stirrer under the sample, but this is not possible in a standard Soxhlet with filling bodies.
As described above, a high number of cycles is advantageous, which is why a small chamber volume is preferable. This conflicts with the simultaneous exchange of as many samples as possible. For this reason, the use of packing material and a bypass/valve in a larger Soxhlet setup makes sense. In the optimized setup shown earlier (Fig. 1), the samples are spatially separated from each other and surrounded by liquid on grids. Direct stacking results in non-flushed areas, which behave analogously to a single large sample body and are therefore subject to the diffusion limitations described above. The upper sample is also protected by a grid in front of the packing. If several samples are stacked in this way, the installation of a vent is preferable. When the liquid overflows, only enough solvent is drained off to ensure that the top sample is always covered with solvent. For a single sample, the volume from the siphon's backflow and the trailing solvent is usually sufficient for this purpose. Since the vent only occupies part of the siphon, the solvent also flows downwards, thus evenly washing all samples.
In this work, solvent exchange experiments were mainly carried out with cyclohexane and tBuOH, as both are well suited for the gels used and for freeze drying. Like many other silica formulations, the MTMS gels used contain water, which forms an azeotropic mixture with tBuOH and must be removed. The mixture boils at 79.91 °C, 101.3 kPa and contains 88.24 w% tBuOH.35 Heterogeneous azeotropic batch distillation with cyclohexane could be integrated into the Soxhlet, but is very difficult to implement. For this reason, an attempt was made to add 3 Å molecular sieve to the chamber. While the balls in the still pot are quickly destroyed by the boiling solvent and stirring, they simultaneously act as water absorbers and fillers in the chamber above the sample. The minimum amount of molecular sieve required can be calculated based on the water content of the samples and the solvent used. TGA measurements of used molecular sieve have shown that it was able to adsorb about 11.2 w% water in its nanopores. The macroporous portion (6.8 w%) is occupied by the azeotrope and therefore does not contribute to the drying process. Since recovering these small quantities from the molecular sieve does not make sense, this solvent is lost in the process. An analysis of all substances introduced into the process showed that 96% of the material used could be recovered with manageable effort.
In order to compare the solvent exchange in a Soxhlet extractor with an agitated batch exchange, various samples were prepared and the progress of the exchange was checked every 30 minutes via GC-MS. PU solvogels with a height of 1 cm and a diameter of 2.8 cm were exchanged against tBuOH (with 0.1% benzene as internal standard). In the batch, 10 times the amount of solvent was added, samples were taken in the first 8 hours, and after a total time of 24 hours, the solvent was replaced with new solvent. The exchange was completed after 4 days. The Soxhlet exchange was used for 8 hours with a still pot containing 150 mL of solvent. Fig. 3 shows the exchange process of the solvogels based on the accumulated amount of extracted synthesis solvent.
The measurements of the Soxhlet extraction are subject to strong fluctuations, but show a clear trend towards complete replacement. The problem with Soxhlet sampling is that a sample can only be taken after a cycle has been completed, as otherwise the light distillate is depleted by boiling and the concentration is measured incorrectly. Although the aim was to achieve sampling that was as uniform as possible, some fluctuations cannot be prevented. Sampling in batch experiments is less critical. Here, only residual solvent from the previous exchange can be identified as a relevant source of error. In batch exchange, a gradual progression can be observed, which slowly approaches the theoretical distribution equilibrium, i.e. about 10% of the initial concentration. In the closely monitored 8-hour segments, this equilibrium is not reached in the samples, but after one day the equilibrium is almost attained. In the third exchange step, the exchange is 99% complete. Depending on the gel, drying is already possible at this point, but in most cases a residual amount of ≪1% synthesis solvent is required, which is only achieved after the fourth exchange. PU aerogels containing propylene carbonate (PC) were also produced using solvent mixtures. During extraction with tBuOH, PC is less easily washed out than 2-nonanone, which means that four exchange steps are always necessary (figure in SI (Fig. S4)).
To test the minimum time for Soxhlet exchange and taking into account that theoretically the diffusion time should increase quadratically with the diffusion distance, MTMS aerogels with a thickness of 5.5 mm and a diameter of 48 mm were produced and extracted for different lengths of time. Fig. 4 shows the course of the thermal conductivities which are very sensitive to residual solvent after SE with cyclohexane and tBuOH for different extraction times. Since an exchange time of 8 hours is sufficient for a sample height of 10 mm (5 mm diffusion path), it should theoretically be possible to exchange a sample with a height of 5 mm in 2 hours which was the case for tBuOH. Since cyclohexane is the poorer solvent for the reactants used, a longer extraction time is generally required for complete exchange. Here, an exchange time of at least 12 hours is necessary for reproducible good results. In the case of tBuOH, an exchange time of more than 5 hours does not lead to any significant improvements. In principle, freeze drying from cyclohexane should be gentler due to its less polar structure, but the removal of water with molecular sieves in tBuOH produces comparably good results. The slightly better measured values after complete exchange with cyclohexane are within the margin of measurement accuracy.
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| Fig. 4 Thermal conductivity of MTMS aerogels after SE with cyclohexane and tBuOH for different times after freeze drying. | ||
The time savings are particularly evident when comparing a conventional solvent exchange followed by supercritical drying with SE followed by freeze drying. Fig. 5 shows the production time for PU and MTMS aerogels from synthesis to the finished aerogel. Most importantly solvent exchange is shortened from more than 4 days to less than 1 day (red bar). Also, in freeze drying the solvent exchange to liquid CO2 can be omitted, saving another 5 days in our setup which is not optimized and may be faster in other setups. Similarly, the time required for gel ageing was not minimized, with MTMS 6 days and PU 1 day. In all cases, the method described greatly saves up to 80% of the time for solvent exchange and thereby accelerates research progress, especially for the development and optimisation of formulations.
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| Fig. 5 Aerogel production times in batch vs. Soxhlet exchange – SCD supercritical drying, FD: freeze drying. | ||
The densities of the samples were adjusted using the amount of aqueous ammonia used. Supercritical drying results in the lowest shrinkage (<1%), which is why the densities of the aerogels are slightly lower. With freeze drying, the volume decreases slightly more depending on the solvent used. For cyclohexane and tBuOH a shrinkage of 2 ± 2% was observed. Regardless of this, comparable thermal conductivities can be achieved regardless of the drying method. The minimum thermal conductivity is achieved in samples with a density of 175–200 mg cm−3. In this range, the stronger Knudsen effect outweighs the increase in solid-state thermal conductivity in the aerogel. Shore A0 measurements were performed on the aerogels to classify their mechanical properties. Fig. 7 shows the measured Shore hardness as a function of density depending on the drying method.
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| Fig. 7 Shore hardness A0 of MTMS aerogels over the density of samples dried from different solvents. | ||
Table 1 shows the specific surface areas of the MTMS aerogels measured using nitrogen sorption from SI Fig. S10.
| SCD (CO2) | FD (cyclo-hexane) | FD (t-BuOH) | |
|---|---|---|---|
| Surface area [m2 g−1] | 728 | 718 | 707 |
| Density [g cm−3] | 0.176 | 0.192 | 0.187 |
The mechanical stability of the samples shows a linear correlation to density, which is to be expected. Freeze drying from tBuOH and supercritical drying from MeOH yield similarly good results. Although cyclohexane should be well suited for drying, the samples obtained are significantly less stable than aerogels with similar densities that were dried using other methods. To better understand this phenomenon, SEM images of the bulk structure of the gels were taken. Fig. 8 shows selected SEM images of the prevailing aerogel structures.
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| Fig. 8 SEM images of MTMS aerogels at different magnifications (A = tBuOH FD; B = cyclohexane FD; C = MeOH SCD). | ||
All samples show a uniform microstructure in the nanometre range.
The macroscopic image of the cyclohexane sample shows the greatest difference in the structures examined. In contrast to the others, these lines show a preferred direction at the fracture edges. When the sample is broken, needle-like splinters form along these edges, which run vertically through the sample.
Reference tests with batch-exchanged samples show the same behaviour. Considering that cyclohexane is a poor solvent for the reactants of the synthesis, we suspect that they are not completely washed out and accumulate locally within the exchange and freezing process, thereby reducing bulk stability.
This hypothesis is supported by the fact that the samples also show a horizontal line at half height, exactly where the diffusion fronts meet during exchange. Furthermore, the preferred direction shifts to an almost radial behaviour at the outer edges of the sample. Aerogels that have previously been exchanged with their synthesis solvent or another solvent suitable for the reactants do not exhibit this behaviour.
Fig. 9 shows images of various samples and fracture edges. As can be seen in image C, the fracture edges with preferred orientation can also be seen with the naked eye. The orientation changes at the right edge of the sample. The supercritically and thereby most gently dried sample in image A shows higher translucency than the freeze-dried samples where the microstructure apparently coarsened and lower surface area was obtained in BET analysis. The contact angle of water is between 150° and 162° for all samples (example image D).
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| Fig. 9 Images of MTMS aerogels (A = MeOH SCD; B = tBuOH FD; C = cyclohexane FD; D = water contact angle of B. | ||
The solvogels and aerogels were also subjected to thermal analysis. Aerogels are thermally stable up to 300 °C and the organic part begins to decompose at higher temperatures (TGA under nitrogen atmosphere (see SI Fig. S5)). DSC measurements on solvogels have shown that the solvents used for freeze-drying are subject to a freezing point depression due to the capillary effects of the pores.36 The freezing point of tBuOH drops from 26 °C to 4.5 °C, and that of cyclohexane from 7 °C to −9 °C (example see SI (Fig. S6 and S7)). Freeze drying was carried out at −55 °C to ensure that the samples were completely frozen.
The samples that were exchanged for cyclohexane in the Soxhlet show greater shrinkage than comparable materials that were dried using tBuOH or supercritical drying. While drying with cyclohexane results in a volume loss of 10 ± 2%, the other samples show shrinkage of <5%. For this reason, comparably produced samples show different densities after drying. As can be seen from the density range of tBuOH-replaced samples, the hardness of PU aerogels also correlates linearly with density (SI Fig. S9). For supercritically dried samples and freeze-dried samples from t-BuOH, the Shore A hardness can be adjusted linearly from 50 to 70 at densities of 140 to 170 g cm−3. Due to the shrinkage of the samples dried with cyclohexane, the density shifts upwards without any improvement in hardness.
During the production of PU aerogels, reactive groups may remain, which can make the structure more polar. The use of tBuOH as an exchange agent has the advantage that these react and ensure that a hydrophobic surface is present. In a few cyclohexane-exchanged samples that were not saturated with a primary alcohol, slightly hydrophilic behaviour was observed. The subsequent water absorption led to local collapse of the bulk structure and, in the long term, to xerogel formation. In general, the samples show a contact angle of 140°–150° and cannot be visually distinguished from the purchased reference material, nor between supercritical and freeze drying. The specific surface area 50–80 m2 g−1.
Regarding thermal conductivity, the best results were achieved with a density of approximately 145 mg cm−3. Table 2 shows the thermal conductivity of selected samples.
| Sample | Thermal conductivity [mW m−1 K−1] | Density [mg cm−3] |
|---|---|---|
| SE tBuOH FD | 17.4 ± 1 | 141 ± 5 |
| SE cyclohexane FD | 19.0 ± 1 | 183 ± 5 |
| SCD | 16.8 ± 1 | 145 ± 5 |
Within the limits of measurement accuracy, supercritical drying delivers results equivalent to those obtained by freeze drying from tBuOH. The insulating performance of the samples produced corresponds to that of the reference material (BASF's SLENTITE (18 mW m−1 K−1)).10
For example, choosing the right system is crucial for solvent exchange. Cyclohexane could be used for solvent exchange of benzyl alcohol, but it is not a suitable solvent for the reactants and any by-products and oligomers that may be present, leading to instable domains in the aerogel and thus poor mechanical properties, therefore tBuOH is the better choice. Similarly, during solvent exchange in PU gels tBuOH ensures a hydrophobic surface simultaneously. In principle, there are few necessary rules that must be followed for Soxhlet extraction. The solvents must simply be separable by distillation (difference in boiling points should be at least 50 K), miscible at the temperature in the chamber, suitable for the reactants, and the target solvent must be suitable for subsequent drying. Based on this, the method should be adaptable to many aerogel systems and speed up their development.
From an ecological and economic point of view, the use of Soxhlet exchange is debatable. On the one hand, it is possible to work with small amounts of solvent, which can be recycled relatively easily and saves a lot of time. On the other hand, the method presented here is relatively energy-intensive compared to batch exchange with subsequent reprocessing. Including solvent recovery, the Soxhlet exchange is almost twice as energy-demanding as the batch method (see SI for example calculation).
In terms of the samples produced, it was demonstrated that it is possible to adapt recipes to high-boiling solvents for gel formation and exchange into low-boiling solvents for (freeze) drying without any problems. The obtained materials are comparable in quality to the state of the art: MTMS aerogels with thermal conductivities of down to 15 mW m−1 K−1 and PU aerogels down to 17 mW m−1 K−1 were produced in various sizes.
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