Jasmine C.
Lightfoot†‡
,
William
Battell†
,
Bernardo
Castro-Dominguez
and
Carmelo
Herdes
*
Department of Chemical Engineering, University of Bath, Claverton Down, Bath BA2 7AY, UK. E-mail: cehm21@bath.ac.uk
First published on 25th August 2025
Selective adsorption of hazardous micropollutants from water remains a critical challenge in sustainable materials design. Herein, we demonstrate a combined computational–experimental approach to rationally engineer molecularly imprinted polymers for targeted porosity, using 2,4,6-trinitrotoluene as a model template. By simulating pre-polymerisation mixtures of monomers, crosslinkers, and solvent using molecular dynamics, we capture key template–monomer interactions and predict the resulting porosity of the final polymer network. Surface area and free volume predictions from simulations show excellent agreement with experimental nitrogen sorption data across varying solvent compositions. Our findings highlight a fundamental trade-off between imprinting efficiency (favoured in acetonitrile-rich environments) and porous structure (promoted by dimethyl sulfoxide). We validate that pre-polymerisation simulations alone can accurately guide formulations toward high-performance materials, opening new pathways for computationally-driven design of porous polymeric adsorbents.
Design, System, ApplicationThis study introduces a simulation-informed strategy to guide the design of porous molecularly imprinted polymers (MIPs) based on the structural organisation of pre-polymerisation mixtures. By modelling the interactions between monomers, crosslinkers, templates, and solvents using molecular dynamics simulations, we predict the porosity of the final polymer without needing to simulate the polymerisation reaction itself. The system under investigation targets 2,4,6-trinitrotoluene (TNT), a hazardous water pollutant, serving as a template to demonstrate the interplay between chemical recognition (imprinting) and structural functionality (porosity). Our approach captures how solvent composition modulates both binding fidelity and polymer morphology, revealing a fundamental trade-off between imprinting efficiency and surface area. The ability to anticipate and control porosity computationally, prior to synthesis, has wide-reaching applications in materials for environmental remediation, sensing, and separations. This framework is generalisable to other crosslinked porous systems and significantly reduces the trial-and-error typically associated with polymer formulation, offering a practical design route for advanced functional materials. |
Molecularly imprinted polymers (MIPs) represent a powerful class of synthetic materials capable of selectively recognising target compounds through templated cavities formed during polymerisation.3 Foundational reviews and mechanism studies in molecular imprinting provide the broader context for this work, covering core design principles, stability/reusability in application, and surface-imprinting mechanisms.4–6 These engineered cavities mimic the structural and functional complementarity found in biological systems and are particularly suited for applications involving trace-level analyte detection or capture. Recent “greenificated” MIP strategies also emphasise sustainability across the materials' life cycle, underscoring the value of predictive design to minimise experimental iteration.7 However, successful MIP synthesis is highly sensitive to the pre-polymerisation formulation—including the choice of functional monomer, crosslinker, and, critically, the porogenic solvent.8–10 The latter not only influences the template–monomer interactions that determine imprinting fidelity, but also governs the final polymer's morphology and porosity, which are key to material performance. The overall synthetic strategy for generating the MIP materials is summarised in Fig. 1.
Designing MIPs with both high binding specificity and appropriate surface area remains challenging due to the complex interplay of chemical and physical interactions in the pre-polymerisation mixture. The high dimensionality of the formulation space and the lack of predictive models has meant that MIP development is often reliant on empirical, trial-and-error methods.11,12 In this context, molecular modelling has emerged as a valuable tool for rational MIP design, enabling insights into monomer–template interactions, solvent effects, and network formation tendencies.9–14 While quantum chemical methods can estimate binding energies for isolated monomer–template complexes,15,16 they typically neglect solvent influence and are limited in scope. By contrast, classical molecular dynamics (MD) simulations offer a route to explore the full pre-polymerisation environment—capturing competition, clustering, and emergent behaviour from multi-component mixtures.10,17
Previous work has demonstrated the utility of MD simulations in screening MIP formulations, particularly in the context of pharmaceutical targets.10,13 Recent studies have also model pre-polymerisation compatibility in full template–monomer–crosslinker–solvent systems for MIP design14 however, these do not attempt to predict final polymer porosity directly from pre-polymerisation snapshots or to map porogen-controlled surface area trends. This is the specific gap we address. Here, we extend our simulation-guided approach to explore how solvent composition affects the porosity of the final polymer network. Rather than simulating polymerisation explicitly—a computationally demanding task requiring reactive force fields—we propose that static snapshots of the pre-polymerisation mixture can be used to predict surface area trends. This is particularly relevant for thermosetting systems where porosity is strongly linked to the packing and arrangement of precursor molecules before curing.8,10
As a case study, we examine a MIP system targeting 2,4,6-trinitrotoluene (TNT), a nitroaromatic compound of environmental concern due to its widespread industrial and military use and associated toxicity.18 In fact, the UN estimates that 10 million hectares of land worldwide are contaminated with explosives like TNT,19 with concentrations, detected in military sites, exceeding 100 μg L−1, which is far above safe limits for drinking water (typically <2 μg L−1).18 Moreover, TNT has been widely studied as a template for MIP-based sensors,3,9 including fluorescent platforms, reinforcing its relevance as a model system,20 but prior modelling work has not addressed how porogen choice influences polymer morphology. Building on our earlier TNT–monomer interaction studies9 and recent advances in porosity prediction,10 we combine MD simulations and experimental synthesis to investigate how mixed DMSO–acetonitrile (ACN) porogens affect both template–monomer interactions and the resulting material structure. Our aim is to demonstrate that pre-polymerisation simulations can provide predictive insights into the porous architecture of MIPs, thereby guiding materials design prior to synthesis.
This dual focus on chemical binding and physical morphology aligns with emerging strategies in simulation-informed polymer engineering. We anticipate that the same pre-polymerisation-snapshot approach can inform other crosslinked porous materials (e.g., HCPs, COFs, PIMs) where solvent-driven packing dictates morphology;21–23 related simulation-guided studies in polymer porosity and transport support this transferability.24,25
Simulation boxes were constructed to model the initial formulation of a molecularly imprinted polymer targeting TNT. Each system contained 10 TNT molecules (template), 60 methacrylic acid (MAA, functional monomer), 250 ethylene glycol dimethacrylate (EGDMA, crosslinker), and 600 solvent molecules. The solvent composition was systematically varied across five ratios of dimethyl sulfoxide (DMSO) and acetonitrile (ACN): 0:
100, 25
:
75, 50
:
50, 75
:
25, and 100
:
0 (v/v). These formulations mirror those used experimentally, enabling direct comparison between predicted and measured surface area trends.
Molecular interactions were described using the OPLS-AA force field with atom types, bonded parameters, and electrostatic charges obtained from the automated topology builder (ATB).29 This combination has been validated in our previous MIP studies10 and provides a transferable framework for crosslinked monomer systems.
To ensure statistical robustness, 18 independent replicas were generated for each solvent composition, enabling ensemble averaging of structural and energetic metrics. Importantly, these simulations capture the distribution and organisation of functional monomers and crosslinkers under different solvent environments—providing a structural basis for predicting polymer morphology.
Porogen | H-bonding time (%) | |
---|---|---|
(DMSO![]() ![]() |
Ortho | Para |
0![]() ![]() |
93.0 | 95.4 |
25![]() ![]() |
90.8 | 93.7 |
50![]() ![]() |
88.8 | 92.8 |
75![]() ![]() |
85.3 | 91.2 |
100![]() ![]() |
85.7 | 90.4 |
These analyses collectively characterise the extent to which solvent composition affects template–monomer complexation and monomer clustering—both of which are known to influence the imprinting process.8–10
Surface area was evaluated using two complementary computational approaches:
Fig. 2 illustrates how solvent-accessible surface area (denoted with the dashed-blue region) was computed using spherical probe methods.
Fractional free volume (FFV) was also determined using the GROMACS freevolume utility, which computes the unoccupied volume fraction based on van der Waals radii.
By correlating these simulated structural descriptors with experimentally measured BET surface areas (see section 4), we demonstrate that pre-polymerisation MD simulations can serve as a reliable, predictive tool for tuning porosity in MIP design. This framework eliminates the need to explicitly simulate polymerisation or assess adsorption performance—instead, it provides a rapid and computationally efficient route to formulate porous, functional polymers.
Nitrogen sorption measurements were carried out using a Quantachrome Autosorb iQ instrument to assess surface area and porosity. UV-visible spectra were collected on an Agilent Cary 100 spectrophotometer to confirm template presence during synthesis. Scanning electron microscopy (SEM) imaging was performed using a Hitachi SU3900 microscope. Prior to imaging, polymer powders were sputter-coated with gold using an Edwards 150B coater.
For each formulation, TNT (220 μL of a stock solution corresponding to 10 mmol) and MAA (110 μL, 60 mmol) were first mixed in a glass vial (1,6 molar ratio). EGDMA (1.10 g, 250 mmol) and AIBN (36 mg, 2.2 mmol) were added, and the mixture was dissolved in 8 mL of solvent comprising one of five ACN:
DMSO volume ratios: 0
:
100, 25
:
75, 50
:
50, 75
:
25, or 100
:
0. Solutions were purged with nitrogen gas for 5 minutes, sealed, and polymerised at 60 °C for 24 hours in an oil bath.
The resulting polymers were dried at 90 °C for 24 hours, then ground and further processed with a ball mill to obtain fine, homogeneous powders suitable for surface area analysis and SEM imaging. Non-imprinted polymers (NIPs) were synthesised identically, excluding the TNT template.
Nitrogen adsorption–desorption isotherms at 77 K were recorded for all MIP and NIP samples after drying. BET surface areas were calculated from the adsorption branch using the standard Brunauer–Emmett–Teller method, assuming monolayer coverage of N2 on accessible surface sites.
SEM was employed to visualise the surface texture and morphology of the polymer particles. Samples synthesised at different DMSO:
ACN ratios were imaged at magnifications of 300×, 2000×, and 10
000×. The surface topography was analysed to qualitatively assess the degree of porosity and surface roughness, which correlates with the computationally estimated free volume and solvent-accessible surface areas.§
![]() | ||
Fig. 3 Chemical structure of the TNT molecule, highlighting the nitro groups in the ortho and para positions (relative to the methyl group). |
In addition to nitro–MAA interactions, TNT can, in principle, interact with MAA via its aromatic π system. A previous theoretical study of TNT complexation35 showed that the electron-deficient aromatic ring of TNT can act as a hydrogen-bond acceptor (through its π cloud) or as a π–π stacking partner. In our simulations, we observed occasional π-hydrogen interactions, where the MAA hydroxyl forms a hydrogen bond perpendicular to the face of TNT's aromatic ring. However, these interactions were minor in frequency compared to the dominant nitro-based hydrogen bonds and are not the focus of this study (though they may be of interest for future work on MIP–TNT recognition mechanisms).
As the DMSO content increased, hydrogen bonding between TNT and MAA decreased (Table 1). In pure ACN, template–monomer interactions were sustained for ∼94% of the simulation time, while in pure DMSO this dropped to ∼88%. This trend reflects competition from the porogen itself: DMSO, being a stronger hydrogen bond acceptor than ACN, more effectively interacts with MAA's hydroxyl hydrogen, displacing TNT from potential binding interactions (Fig. 4). This solvent-driven modulation of imprinting interactions confirms previous observations that porogen choice can critically impact MIP formation pathways.8–10
Additionally, MAA clustering was observed to increase in DMSO-rich environments. The aggregation of monomer units leads to decreased accessibility for both TNT and solvent molecules. Coordination analysis and RDFs revealed that in high-DMSO formulations, monomers form larger, more internally hydrogen-bonded clusters, consistent with solvophobic effects and poor solvation of MAA in DMSO.10 This self-association limits effective template complexation, suggesting that DMSO may reduce imprinting efficiency despite improving polymer morphology. To quantify this effect, we computed RDFs between the solvent acceptor atoms and the MAA hydroxyl hydrogen, data shown in Fig. 4 are for the single-solvent systems (100% DMSO and 100% ACN). The peaks near 0.17 nm indicate the presence of hydrogen-bonded solvent–MAA interactions. The larger peak for DMSO reflects stronger competition by DMSO for bonding with MAA relative to ACN. Both pure ACN and pure DMSO systems show a peak in the RDF at around 0.17–0.18 nm, corresponding to hydrogen-bonding distance. However, the peak for DMSO is higher than that for ACN, indicating that DMSO forms stronger/more frequent hydrogen bonds with MAA compared to ACN. This is consistent with DMSO's stronger competitive binding, which in turn explains the reduction in TNT–MAA hydrogen bonding as DMSO content increases.
Fig. 5 shows RDFs between MAA's hydroxyl hydrogen and the acceptor atoms of both ACN and DMSO for each solvent mixture. In both cases, the peak height decreases when going from lower DMSO content (25%) to higher DMSO content (75%), indicating fewer solvent–monomer hydrogen bonds at higher DMSO fractions. As the fraction of ACN decreases (and DMSO increases), the first peak of ACN around MAA diminishes (due to lower ACN concentration and increased competition from DMSO). One might expect the DMSO–MAA RDF peak to grow; accordingly, however, we observe that the DMSO–MAA RDF peak also decreases with higher DMSO content. This somewhat counterintuitive result indicates that beyond a certain concentration, additional DMSO does not lead to more MAA–DMSO interactions, because many of the MAA molecules are now engaged in MAA–MAA interactions (clustered) and thus less accessible even to DMSO. In other words, at high DMSO content, the monomers form self-associated clusters wherein internal MAA molecules are shielded from both TNT and solvent. This highlights DMSO's disruptive role: while it competes strongly with TNT for monomer binding, it simultaneously induces monomer clustering that limits overall hydrogen bonding in the system. The implications of this behaviour on MIP performance (in terms of binding vs. porosity) will be discussed next.
Porogen | Exp. SA | Comp. SA | ||
---|---|---|---|---|
(DMSO![]() ![]() |
(m2 g−1) | (rel.) | FreeSASA (rel.) | MeshSA (rel.) |
0![]() ![]() |
70.98 | 0.184 | 0.881 | 0.950 |
25![]() ![]() |
352.60 | 0.916 | 0.957 | 0.968 |
50![]() ![]() |
371.46 | 0.965 | 0.963 | 0.984 |
75![]() ![]() |
379.77 | 0.986 | 0.997 | 0.989 |
100![]() ![]() |
385.11 | 1.000 | 1.000 | 1.000 |
These trends were accurately predicted by pre-polymerisation molecular simulations. By analysing configurations from MD trajectories with solvent and template removed, two computational approaches—MeshSA (GCMC probing) and FreeSASA (geometric surface analysis)—independently replicated the experimental increase in surface area with rising DMSO content. For porous formulations (≥25% DMSO), simulated relative surface areas were within 4–6% of experimental values (Table 2). This strong agreement confirms the validity of using non-reactive, pre-polymerisation simulations to predict polymer morphology.
One exception was the 0% DMSO case, where simulations overestimated porosity. This discrepancy is likely due to the lack of polymer network collapse in the simulation: after solvent removal, the static polymer configuration is assumed to remain rigid, whereas in reality, polymers formed in poor porogens like ACN collapse into denser structures during curing and drying. Capturing such densification would require reactive MD or post-curing simulations, beyond the current scope.
Further supporting these findings, SEM imaging showed distinct morphological changes with porogen variation (Fig. 6). Polymers synthesized in ACN formed smooth, featureless surfaces, while DMSO-derived samples displayed granular textures with fine surface roughness consistent with microporosity. To further illustrate this solvent-dependent morphological trend, additional SEM micrographs for all intermediate formulations (MIP 2–MIP 4) are provided in Fig. S3 at three magnifications (300×, 2000×, and 10000×). These images bracket the transition from the smooth morphology of pure ACN-derived MIP 1 to the highly textured surface of pure DMSO-derived MIP 5, enabling visual correlation with the corresponding BET surface area and simulated SASA/FFV values. These visual observations correlate directly with both experimental BET data and the predicted expansion of accessible void space in the simulations (Fig. 7).
Fractional free volume (FFV) calculations from MD trajectories also revealed a linear increase with DMSO content (Table 3), from 0.194 (0% DMSO) to 0.248 (100% DMSO). This trend aligns with the molar volume difference between DMSO (∼71 cm3 mol−1) and ACN (∼53 cm3 mol−1), reinforcing the idea that solvent selection impacts monomer packing density and available void volume in the final material.
Porogen | FFV |
---|---|
(DMSO![]() ![]() |
(dimensionless) |
0![]() ![]() |
0.194 |
25![]() ![]() |
0.208 |
50![]() ![]() |
0.222 |
75![]() ![]() |
0.235 |
100![]() ![]() |
0.248 |
Across DMSO fractions, both SASA (FreeSASA/MeshSA) and FFV increase monotonically, mirroring the BET trend (Tables 2 and 3). Together with the hydrogen-bond analysis (Table 1), these data support a solvent-driven trade-off: ACN-rich mixtures favour sustained template–monomer bonding, whereas DMSO-rich mixtures favour enlarged accessible voids.
While this study did not assess rebinding performance or target removal efficiency, the structural insights gained provide a predictive framework for selecting formulations tailored to specific applications. For instance, systems requiring high surface area but tolerating lower imprinting specificity may favour DMSO-rich porogens, whereas selective sensing materials may benefit from ACN-rich environments despite lower porosity.
Simulations revealed that acetonitrile-rich environments enhance specific hydrogen bonding between the TNT template and methacrylic acid (MAA) monomer, whereas DMSO-rich mixtures promote monomer clustering and reduce imprinting efficiency. However, the inclusion of DMSO significantly increased polymer surface area and free volume, as confirmed by both BET measurements and SEM analysis. These experimental trends were quantitatively reproduced by surface area calculations and free volume estimations from solvent-stripped MD configurations, validating the use of MD as a predictive tool for morphology design.
Our approach does not model polymerisation kinetics, curing-induced densification/collapse, or template rebinding; static, solvent-stripped configurations can therefore overestimate porosity in poor-porogen cases (e.g., 0% DMSO), where network densification during curing/drying is expected. Extending the workflow to other chemistries will require force-field validation and descriptor checks tailored to those monomers/porogens; nonetheless, when solvent-driven packing dominates morphology, pre-polymerisation snapshots provide actionable guidance for porosity-directed formulation.
Importantly, our approach requires only simulations of the pre-polymerisation mixture, avoiding the need for polymerisation modelling, reactive force fields, or computationally intensive curing simulations. As such, it provides a tractable and versatile screening method for tailoring the structural properties of porous polymers based on monomer, crosslinker, and solvent composition.
Beyond MIPs, this framework is applicable to a wider range of porous materials, including hyper crosslinked polymers (HCPs), covalent organic frameworks (COFs), and polymers of intrinsic microporosity (PIMs), where solvent-induced morphological control is similarly critical.21–23 By bridging molecular-scale simulations with experimental synthesis, this work underscores the value of integrative, modelling-guided design in accelerating the development of advanced functional polymeric materials.
Footnotes |
† J. C. L. and W. B. contributed equally to this work. |
‡ Current address: The Hartree Centre, STFC Daresbury Laboratory, Warrington, WA4 4AD, UK. |
§ TNT was extracted from the MIPs following synthesis using Soxhlet extraction with refluxing methanol. While this ensured template removal for surface area consistency, no rebinding experiments were conducted, and no adsorption performance metrics were evaluated in this study. |
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