Open Access Article
Mohammed Ali Dheyab
*ab,
Wesam Abdullah
a,
Sara Abdulwahab
a,
Sadeen Metib Alsarayreh
a,
Mothana Hussein Tarawneh
a,
Mutaz Mohammad Alsardi
a,
Mansour A. Alanazi
c and
Azlan Abdul Aziz
ab
aSchool of Physics, Universiti Sains Malaysia, 11800 Pulau Pinang, Malaysia. E-mail: mdali@usm.my; lan@usm.my
bNano-Biotechnology Research and Innovation (NanoBRI), Institute for Research in Molecular Medicine (INFORMM), Universiti Sains Malaysia, 11800, Pulau Pinang, Malaysia
cDepartment of Physics, College of Science, Northern Border University, Arar P. O. Box 1321, Saudi Arabia
First published on 7th January 2026
The deliberate structuring of inorganic nanomaterials through mechanical forces offers a powerful alternative to conventional synthesis, enabling solvent-free, energy-efficient, and scalable design strategies. Rather than serving only as a synthetic shortcut, force-driven processing is increasingly recognized as an architectonic tool as a means of directing matter into well-defined architectures that integrate top-down shaping with bottom-up assembly. This review develops a conceptual framework of architectonics under mechanical activation, treating external force as a design parameter that dictates structure formation across multiple length scales. Methodological platforms such as ball milling, extrusion, and hybrid force–stimuli systems are systematically assessed, alongside mechanistic insights spanning multiscale reaction pathways, computational modeling, and AI-enabled predictions. The potential of this approach to generate smart and functional interfaces is highlighted through applications in catalytic and energy conversion processes, biomedical nanomedicine, and electronic or sensing devices. Finally, we discuss current limitations particularly gaps in mechanistic understanding, predictive control, and scalability and outline future opportunities to advance force-driven architectonics as a foundation for next-generation functional inorganic nanomaterials.
Ball milling in particular has re-emerged as a powerful solid-state technique, providing the necessary mechanical energy to drive reactions rapidly and under environmentally benign conditions.7,8 Initially considered a top-down comminution process for producing micro- and nanoscale powders,2,9 milling is now innovatively adapted for bottom-up nanoparticle synthesis through chemical reactions.10,11 Mechanochemical grinding of oxides exemplifies this dual role, where simultaneous physical and chemical processes occur in coordinated patterns, yielding superior fine powders compared to conventional routes.8,12 Despite its simplicity, mechanical milling often induces amorphization and surface defects, as shown by Šepelak's observation of 2–5 nm amorphous surface layers on oxide nanoparticles,13,14 yet these very features underpin the phenomenon of mechanical activation. More broadly, mechanochemical approaches such as mechanical milling, alloying, reactive extrusion, and induced solid-state reactions offer efficient, solvent-free, and sustainable routes for producing nanocrystalline materials and functional composites.15–17 Recognized as a pillar of green chemistry, mechanochemistry has been named by IUPAC among the top ten chemical innovations shaping sustainable science,18 underscoring its relevance for modern material design. Compared with conventional wet-chemistry syntheses that generate solvent waste, involve prolonged treatment times, and require multistep drying or surfactant-assisted procedures,8,19,20 mechanosynthesis bypasses solubility limitations and reduces hazardous waste while lowering energy input and reaction time.21–24 These advantages have enabled the scalable, solvent-free synthesis of diverse nanomaterials, including oxides (TiO2, CeO2, Gd2O3) and metals such as Fe,25 as well as perovskites, catalytic systems, and superhydrophobic surfaces.15,16,20,26
In recent years, applications of mechanochemical synthesis have expanded into pharmaceuticals, ligand design, drug synthesis, graphene production, and the surface modification of nanomaterials.23,27 Importantly, soft mechanochemical strategies employing solid acids, bases, hydrated compounds, or salts have opened new opportunities for tailoring inorganic nanostructures,28 while dry synthesis routes minimize solvents or surfactants, providing significant ecological and functional benefits.29–32 The performance of noble metal nanoparticles, governed by size, shape, composition, and elemental distribution, further illustrates the critical role of mechanochemistry in advancing functional nanomaterials, as their catalytic, electronic, optical, and biomedical properties extend far beyond the aesthetic appeal that first inspired their study.33,34 Collectively, these advances position mechanochemistry as a transformative platform for nanomaterials synthesis, bridging multiscale pathways of activation and assembly with the design of smart and functional interfaces.
Nonetheless, despite these achievements, previous academic research on mechanochemical synthesis has primarily emphasized scalability, solvent-free operation, and sustainability benefits, while leaving critical gaps unaddressed. Notably, Fiss et al.35 highlighted the advantages of mechanochemical strategies in inorganic redox and ion-exchange processes, yet their analysis lacks mechanistic depth and broader sustainability metrics beyond nanoparticles and hybrid frameworks such as metal–organic frameworks (MOFs). While MOFs are classified as organic–inorganic hybrid systems, their inclusion in mechanochemical discussions is common due to their highly crystalline architectures and force-responsive porosity, which often parallel the behaviors of inorganic nanomaterials. Likewise, Auvray and Friščić6 offered valuable mechanistic insights and a systematic classification for hard and high-melting inorganic materials, but their work overlooks opportunities in nanomedicine and hybrid nanostructures. Similarly, Xu et al.16 underscored the simplicity and catalytic benefits of mechanochemical synthesis as a green alternative to conventional routes, although their discussion remains confined to catalysis, neglecting wider applications in energy storage and biomedical interfaces. In light of these deficiencies, our review aims to address the unmet need for a cross-disciplinary framework in mechanochemical synthesis of inorganic nanomaterials. We provide a coherent architectonic perspective that goes beyond catalysis and selected inorganic systems, integrating methodological platforms, mechanistic insights, and smart interface engineering. By systematically linking force-driven design to functional outcomes in catalysis, energy storage, and biomedicine, we establish mechanochemistry as a versatile architectonic tool rather than a niche synthetic route. This exclusive focus on designing smart and functional interfaces aligns with global priorities for sustainable, scalable, and multifunctional nanomaterials, offering a roadmap for future advances across chemistry, materials science, and nanomedicine.
The power of mechanochemical architectonics comes from three interconnected processes (Fig. 1). First, the intense local stresses and collisions during milling distort the crystal lattice and create defect-rich areas. These defects make it easier for ions to move and redox reactions to happen, allowing solids like metals and oxides to transform quickly at the atomic level.38 For instance, when making metal oxide nanoparticles like Fe2O3, milling causes repeated breaking and welding of particles, which increases defects and speeds up reactions that would normally require high heat, enabling them to occur near room temperature.39 Second, the constant cycle of cold welding and fracturing during milling keeps generating fresh, reactive surfaces and dynamic interfaces between solids. These tiny surfaces act like small reactors where the chemistry occurs how many of these nucleation spots form and their chemical nature ultimately shape the final product. A good example is making mixed oxides like titanium dioxide (TiO2) and cerium dioxide (CeO2) by milling: the process disperses these oxides evenly and mixes them at the nanoscale, resulting in catalysts with unique properties without needing to heat them in bulk.40 Mechanochemical milling of TiO2–CeO2 at 350 rpm for 100 min yields nanoscale composites with particle sizes ∼5 µm and enhanced oxygen sensitivity (up to 8.2 at 320 °C), demonstrating force-driven architectonics without bulk heating. Third, adding small amounts of liquid during milling (called liquid-assisted grinding) changes how energy moves and how surfaces interact. This helps guide how particles aggregate or bond on the surface, offering precise control over the assembly and functionalization of particles.38 This combination of mechanical stress, dynamic surface creation, and liquid effects makes mechanochemical architectonics a powerful method for designing and synthesizing advanced materials efficiently and in environmentally friendly ways.
Shi et al.41 demonstrate a form of nano architectonics by embedding Pt single-atoms and differently-sized Pt nanoparticles (1.5, 3.0, and 7.0 nm) onto manganese-oxide nanosheets. Although the synthesis was not purely mechanochemical, the principles of architectonics namely, vacancy filling, atomic dispersion, and interface-driven functionality are central to the material's catalytic behavior. The manganese-oxide nanosheets serve as a defect-rich scaffold, with oxygen vacancies acting as anchoring sites for Pt species. The interaction between Pt and MnO2 is not merely compositional but architectonic: it alters the oxidation state of manganese, modulates the oxygen vacancy concentration, and tunes the catalytic activity of the hybrid nanozyme. This reflects the essence of mechanochemical architectonics where structure and function co-evolve through controlled energy input and spatial design.
Despite its promise, several limitations constrain the broader adoption of mechanochemical architectonics. Reproducibility and parameter standardization remain persistent challenges: milling frequency, ball-to-powder ratio, filling factor, and jar geometry introduce nonlinear effects on energy input and product distribution, complicating cross-study comparisons. Contamination from milling media, together with uncontrolled localized heating, may obscure mechanistic interpretation and compromise functional performance. Scale-up is particularly problematic, as laboratory-scale ball mills generate heterogeneous energy distributions that are not easily replicated in continuous or industrial platforms. Furthermore, mechanistic insights are often inferred from ex situ characterizations, which risk conflating transient intermediates with end products.42
Several strategies have been proposed to address these limitations and strengthen the mechanochemical toolkit. Standardized reporting of energy metrics (e.g., J g−1 or specific impact energy) would enable quantitative comparison across studies. Media wear and contamination can be minimized through careful selection of ceramic liners and inert milling components. The systematic use of Liquid-Assisted Grinding (LAG), rather than as an ad hoc additive, allows controlled tuning of interfacial chemistry. Hybrid activation methods combining mechanical milling with thermal annealing, sonication, or photonic inputs may further decouple defect generation from morphological evolution. Most critically, real-time monitoring through acoustic emission, synchrotron X-ray scattering, Raman spectroscopy, and operando temperature–pressure probes offer the potential to resolve transient intermediates and establish direct correlations between energy input and physicochemical outcomes. The development of scalable, continuous mechanochemical reactors such as twin-screw extruders and reactive ion-milling devices, validated against batch systems with conserved energy metrics, represents an essential step toward industrial translation.43
A central mechanistic underpinning is the generation of localized, transient high-energy sites commonly referred to as “hot spots” which store strain energy and enable bond cleavage and atomic rearrangements without the need for bulk thermal activation.44 The stochastic nature of collisions and nonequilibrium energy distributions during milling open pathways inaccessible to conventional methods, resulting in accelerated reaction rates, selective product formation, and stabilization of otherwise unstable intermediates. This capacity to create dynamically evolving “smart” interfaces, where chemical state, morphology, and function are continuously reconfigured under mechanical stress, provides a rational basis for enhanced catalytic, electronic, and optical performance.45
Recent studies illustrate these dynamics with increasing clarity. For instance, the mechanochemical synthesis of MOFs such as MOF-74 proceeds through rapid formation of short-lived intermediates, with liquid additives accelerating coordination and structural reorganization. In situ powder X-ray diffraction (PXRD) has revealed that these intermediates adopt distinct coordination motifs or polymorphic forms, highlighting the structural dynamism inherent to mechanochemical pathways.46 Klimakow et al.47 highlight mechanochemical architectonics is exemplified through the solvent-free synthesis of MOFs, specifically HKUST-1 and MOF-14, using ball milling techniques. The authors demonstrate that mechanical energy can be harnessed not only to drive chemical reactions but also to sculpt the pore architecture and surface properties of the resulting materials. This approach yields high specific surface areas up to 1713 m2 g−1 comparable to the best values reported via conventional solvothermal methods, yet achieved without solvents or extensive post-synthetic treatments. Similarly, mechanochemical anion-exchange in lead(II) coordination polymers demonstrates crystal-to-crystal transformations that preserve crystallinity while enabling functional modulation, underscoring the potential of architectonics to deliver solvent-minimized, highly efficient material design strategies.48
The objectives of architectonics are realized by intentionally guiding how simple molecular or nanoscale units organize into more complex and functional architectures. Rather than relying on spontaneous assembly, architectonic design emphasizes control over interfacial interactions, defect formation, and assembly pathways, allowing structure to evolve in a predictable manner across length scales. In mechanochemical systems, mechanical force serves not only as an energy source but also as a regulating element that influences contact dynamics, surface reactivity, and kinetic pathways. Through careful adjustment of processing conditions and chemical environments, this approach enables a direct connection between architectural design and material performance.49,50 This architectonic perspective provides the foundation for treating mechanical force not merely as an energy source, but as a tunable design parameter.
Additionally, force controls how solid–solid interactions collectively evolve. The balance between fracturing and cold welding, controlled by milling intensity and ball-to-powder ratio (BPR), regulates the frequency of interface renewal and the density of nucleation sites. High BPRs accelerate composite synthesis, as demonstrated in molybdenum disilicide (MoSi2) and titanium carbide (TiC) systems where a 20
:
1 ratio completed conversion in 10 h compared to incomplete reaction at 5
:
1 even after 30 h.54 Similarly, denser milling media such as zirconium dioxide (ZrO2) or tungsten carbide (WC) deliver sharper impacts that promote rapid defect generation but can also over-fragment sensitive phases, producing amorphization or unintended contaminations.54 These trade-offs illustrate the duality of force: it can either enable rapid architectonic assembly or induce destructive over-milling.
Despite its centrality, quantitative control of force in mechanochemical synthesis remains underdeveloped. Most studies report milling parameters such as frequency, ball size, or jar material but these serve as indirect proxies rather than true measures of force. Without standardized reporting of impact energy (J g−1), collision frequency, or energy density, reproducibility across laboratories suffers, reducing mechanistic comparisons to qualitative speculation at best. For example, Belenguer et al.55 emphasized that variations in jar size, shape, ball size, and materials can dramatically influence reaction outcomes even when nominal conditions remain constant highlighting the sensitive dependency of mechanochemical reactions on experimental setup specifics. Adding to this complexity, Jafter et al.56 developed a kinematic modeling framework that demonstrates how even minor changes in planetary mill geometry (such as jar radius or sun wheel dimensions) can cause a 2–3× variation in impact energy, despite identical milling speed and ball load (Fig. 3A(a)). This variability stems from the way geometric parameters influence effective impact velocity, which directly affects energy transfer. Moreover, force distribution within the milling jar is inherently heterogeneous. Fig. 3A(b) illustrates how only a subset of particles experience sufficient impact energy to overcome activation barriers, creating localized (hot spots) while adjacent regions remain under-energized. This spatial disparity aligns with granular media models predicting wide force fluctuations due to varied contact angles and bead pack dynamics. Additionally, Fig. 3A(c) highlights how ball material density alters the filling factor even at constant mass affecting the total volume occupied and thus the energy delivery profile. These insights are particularly relevant for inorganic mechanochemical reactions, such as the synthesis of metal oxides (e.g., TiO2, ZnO) and intermetallics (e.g., MoSi2–TiC), where defect formation, phase transitions, and interface engineering are highly sensitive to localized energy input.
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| Fig. 3 (A) (a) Ball collisions during circular motion deliver mechanical energy directly to the reactant molecules. (b) The mill's illustration and the pertinent factors that affect the effective impact velocity and (c) balls have particular properties that have a direct impact on the energetics. If all ball types had the same mass, the size of the balls in the illustrations would match the relative size. Reduced with permission.56 Copyright 2024, Wily. (B) (a) Considering all directions, random collisions drive mechanochemical reactivity to form the product. (b) (Left) Activation energy drops by ∼1.2 kcal mol−1 under 2 GPa, indicating a “hot” mechanochemical species. (Right) Minimal response reflects a “cold” species; isomer orientations differ for clarity. Reduced with permission.58 Copyright 2025, American chemical society. (C) Milling-map of the samples, displaying the grounding process with different ball-impact and cumulative energy which is dependent on the rotational speed. Reduced with permission.60 Copyright 2020, Royal Society of chemistry. (D) Mechanochemical nano casting method for porous metal oxide. Adapted with permission.63 Copyright 2018, American chemical society. | ||
Moreover, force distribution within the milling environment is far from homogeneous. Particle trajectories and impact geometries create regions of intense energy concentration (hot spots) and adjacent under-energized areas (cold zones), all within the same jar. This spatial heterogeneity complicates mechanistic interpretation, as only a subset of the material may undergo defect-rich transformations while the remainder remains largely unaltered. This behavior aligns with earlier theoretical models of granular media that predict wide force fluctuations due to varied contact angles and force networks even in static bead packs.57 De Armas et al.58 quantifies how directional compressive forces mimicking ball-milling impacts affect activation energy across molecular orientations. Mechanical activation energy varied by up to 1.2 kcal mol−1 depending on impact direction under 2 GPa pressure, confirming the presence of “hot spots” where reactivity is enhanced. Conversely, the reverse reaction showed negligible mechanical response, illustrating “cold zones” with minimal activation. This anisotropic behavior validates granular media models predicting force heterogeneity due to variable contact angles and impact geometries (Fig. 3B).
A further limitation arises from the interplay between mechanical and thermal effects. At high frequencies, energy dissipation as heat can blur the distinction between mechanochemical and thermally assisted pathways, confounding mechanistic models. In polymer mechanochemistry, excessive force accelerates chain scission, undermining the very architectonic control sought in synthesis. Such examples highlight that more force does not necessarily mean better outcomes; instead, there exists an optimal force window where activation is maximized while degradation is minimized.59 In a detailed investigation of oxide nanoparticle formation, Ochirkhuyag and co-workers reported that increasing the milling speed from 200 to 600 rpm raised the average collision energy from 0.1 to 0.5 J per impact, resulting in a nearly fourfold increase in defect density and a corresponding reduction in crystallite size from 45 nm to 12 nm (Fig. 3C). In the mechanochemical synthesis, that Raman bands at ∼640 cm−1 (MnO2), ∼580 cm−1 (Mn2O3), and ∼490 cm−1 (Mn3O4) evolved systematically with milling time, where extending milling from 1 h to 6 h shifted the spectrum toward the Mn3O4-dominant profile, quantitatively confirming the collision-driven reduction pathway induced by high-energy ball milling.60 Similarly, Zhao et al.61 demonstrated that applying higher milling frequency (30 Hz vs. 15 Hz) increased the lattice strain in Fe2O3 nanoparticles from 0.12% to 0.36%, which directly correlated with a 2.7× increase in catalytic activity for CO oxidation. These results show why controlled force input is central to defect engineering and catalytic optimization. Force modulation also governs interface formation. In the mechanochemical synthesis of TiO2-based composites, Bharath and colleagues observed that varying the ball-to-powder ratio (5
:
1 to 20
:
1) accelerated reaction completion from 30 h down to 10 h, as more frequent high-energy collisions generated fresh interfaces and increased nucleation site density. In their solvent-free mechanochemical synthesis used Raman spectroscopy to track structural disorder and reduction, where the characteristic D and G bands provided direct evidence of defect generation and graphitic restoration under high-energy milling mirroring how increased collision intensity in other mechanochemical systems accelerates interface formation and reaction progression.62 Importantly, these fresh interfaces were chemically distinct from bulk surfaces, hosting under-coordinated atoms that enabled selective photocatalytic activity under visible light.
Nevertheless, excessive force can be detrimental. Xiao et al.63 reported that over-milling at 800 rpm caused amorphization in zinc oxide (ZnO) nanostructures, lowering photocatalytic efficiency by >35% compared to optimally milled samples. This underscores the need to define an optimal force window, where sufficient defect generation enhances reactivity but excessive impacts lead to structural collapse and loss of crystallinity (Fig. 3D). Operando and in situ studies now provide direct experimental validation of force-driven mechanisms. In situ synchrotron PXRD during MOF-74 ball milling reveals rapid formation of short-lived intermediates with distinct coordination motifs, where liquid-assisted grinding accelerates structural reorganization under controlled collision energies. Operando acoustic spectroscopy monitors mechanochemical reactions in real-time, tracking acoustic emission changes that correlate with reaction progress and energy input during ball milling.64 The lack of standardized force quantification in mechanochemistry remains a persistent challenge, with most studies relying on indirect parameters such as rpm, ball size, or filling ratio. Li et al.65 addressed this limitation by introducing the concept of specific energy dose (J g−1), correlating mechanical input with reaction yield across different milling platforms. In their synthesis of defective molybdenum trioxide (MoO3), TiO2, and ZnO, they demonstrated that a specific energy dose of approximately 1200 J g−1 was sufficient to induce significant oxygen vacancy formation and hydrogen doping in MoO3, yielding localized surface plasmon resonance properties. In the archetypal mechanochemical synthesis of the metal–organic framework ZIF-8 from ZnO and 2-methylimidazole, in situ synchrotron PXRD measurements revealed that the distinctive Bragg reflection intensity of the (011) plane a proxy for product crystallinity evolves markedly with milling time, showing initial formation of ZIF-8 within minutes followed by significant amorphization over ca. 30–40 min of continued milling (with complete amorphization observed at ∼30 min under certain liquid additive conditions) and retention of crystalline features up to ∼55 min with higher liquid content, demonstrating force-dependent structural kinetics directly tied to milling parameters such as liquid volume and additive concentration.66 This time-resolved intensity profiles provide quantitative evidence that prolonged mechanical impact does not simply accelerate reactions but actively alters phase stability and pathway, consistent with mechanochemical architectonic control. Beyond diffraction, in situ coupled PXRD–Raman spectroscopic studies have been used to track mechanochemical reactions in real time, providing correlated structural and vibrational data that reveal the formation and consumption of intermediate phases with clear kinetic signatures as a function of mechanical input.67
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| Fig. 4 (A) Schematic illustration of the urea synthesis process using ZrO2 milling balls and a milling jar. Reproduced with permission.72 Copyright 2025, American chemical society. (B) Illustration of the two methods used to prepare Pd/CeO2 samples: incipient wetness impregnation and planetary ball milling under controlled atmosphere. Reproduced with permission.74 Copyright 2025, American chemical society. (C) Synthesis flowchart of ZIF-90PN@MB. Reproduced with permission.61 Copyright 2025, American chemical society. (D) Schematic illustration of the mechanochemical synthesis of Na3(VOPO4)2F nanoparticles starting from NaVO3, depicting the typical synthetic process of NVPFs. Reproduced with permission.75 Copyright 2021, Nature. (E) Schematic illustration of the mechanochemical activation of halloysite nanotube-rich kaolin clay and its application as a carrier for sustainable slow-release phosphate fertilizer. Reproduced with permission.76 Copyright 2025, American chemical society. | ||
At the architectural scale, Dhokale et al.80 demonstrated the critical role of milling parameters, where 7 mm balls resulted in 30% yield, while optimizing with 34 smaller 4 mm balls improved efficiency to 44% within only 99 minutes. Similarly, Marín et al.81 highlighted the impact of planetary ball milling forces on catalytic activity, showing that an optimum velocity of 250 rpm maximized metal–support interactions compared to both lower- and higher-energy regimes, while the reaction atmosphere further modulated activity. Their comparative mechanistic insights are illustrated in Fig. 4B, contrasting incipient wetness impregnation with atmosphere-controlled ball milling in the preparation of Pd/CeO2 catalysts. In another example, Zhang et al.68 processed MoAlB through intensive milling at 1000 rpm for 12 h, generating amorphous phases and thinner nanosheets, followed by NaOH etching to obtain well-dispersed MBene (MB) sheets. The mechanistic sequence of lattice disruption and selective Al removal is shown in Fig. 4C, underscoring how milling can tailor nanoscale inorganic architectures.
In the context of energy storage, Shen et al.82 synthesized Na3(VOPO4)2F nanoparticles via high-energy ball milling, achieving ∼5 nm crystallites, in situ carbon-active composites, and ultralong cycling stability (98% over 10
000 cycles). This industrially scalable process (2 kg batches, 26
650 cells) is visualized in Fig. 4D, highlighting the multiscale transformation pathways accessed during solid-state milling. To establish that mechanochemical routes extend well beyond this single system, several additional force-driven syntheses have demonstrated similarly robust performance enhancements across diverse electrode chemistries.83 For example, solvent-free mechanochemical activation has proven highly effective for Na-ion Prussian blue analogues, where reducing reaction activation energy and promoting solid-ion diffusion trigger low-temperature solid-state transformations. He et al.84 showed that a Na-rich monoclinic NaMHCF cathode prepared entirely by milling exhibits high specific capacities, superior rate capability, and fully reversible multi-phase evolution during Na+ (de)insertion representing one of the most compelling demonstrations of mechanochemistry-enabled Na-ion storage. Recent advances in all-solid-state lithium batteries provide yet another compelling line of evidence, where mechanochemical synthesis has enabled the scalable preparation of Li3PS4-based sulfide electrolytes with room-temperature ionic conductivities above 10−4 S cm−1 and favorable mechanical deformability that enhances solid–solid interfacial contact. Importantly, aliovalent ZnO substitution yields glass-ceramic Li3PS4 with significantly improved conductivity (1.12 × 10−3 S cm−1) and increased stability against both air and lithium metal, illustrating how structural distortion and defect engineering introduced by force-driven processing can be leveraged to optimize ion-transport pathways and long-term cycling reliability.85 Complementarily, Biswas et al.86 demonstrated that planetary milling of halloysite-rich kaolin shortened tubular morphologies by ∼44% within 1 h and ∼53% within 2 h, where dry milling produced nanofragments while wet milling preserved tubular structures but still tripled surface area. As highlighted in Fig. 4E, such modifications critically regulate phosphate adsorption and release, advancing kaolin as a sustainable slow-release fertilizer carrier.
Expanding further, mechanochemical strategies have enabled solvent-free C–C bond formation using Cu-complex-functionalized polyoxoniobates with high recyclability and gram-scale applicability,87 selective mechanosynthesis of quinone derivatives with yields up to 98% through frequency and additive control,88 and the sustainable conversion of coal-derived graphene oxide into turbostratic graphene sheets with improved purity and carbon content.70 Ball milling has also been applied to metal–organic framework synthesis, where Plant-Collins et al.89 reported optimal crystallinity and hierarchical porosity in MOF-505 within 80 minutes under reduced solvent input.
Mechanochemical synthesis of MOFs has been systematically established through neat grinding (NG), LAG, and ion- and liquid-assisted grinding (ILAG). James and Friščić90 highlighted that direct milling of metal salts with organic linkers enables framework formation via force-driven solid–solid reactions, while LAG alters reaction kinetics and phase outcomes by enhancing interfacial mobility. Subsequent ILAG studies demonstrated that inorganic salt additives further regulate nucleation and polymorphism during mechanochemical MOF formation.91 Operando diffraction investigations later confirmed that these force-driven routes govern MOF crystallization under solvent-minimized conditions.92
Environmental applications benefit as well: ball-milled MoS2 exhibits enhanced peroxymonosulfate activation for antibiotic degradation due to defect engineering,93 while ultrafine biochar/Fe3O4 composites efficiently remove pharmaceutical contaminants. In the energy domain, mechanochemical synthesis underpins cathode, anode, and electrolyte development for lithium- and sodium-ion batteries, offering improved electrochemical stability and performance.94,95 Importantly, the sustainable production of ammonia under mild conditions via ball milling achieving yields of 82.5% vol. at 45 °C and 1 bar positions this platform as a compelling alternative to the Haber–Bosch process.96 Collectively, ball milling enables the synthesis of diverse inorganic nanoparticles, including metal oxides, sulfides, carbides, perovskites, and layered compounds. Compared with liquid-assisted mechanochemistry and conventional wet-chemical routes, ball-milled nanoparticles typically exhibit nanocrystalline cores, high lattice strain, and defect-rich or partially amorphous shells, imparting unique properties such as enhanced catalytic activity, accelerated ion transport, and superior interfacial reactivity.
Taken together, ball milling and grinding architectures transcend conventional solution-based approaches by coupling tunable impact forces, scalable design, and solvent-free conditions to activate multiscale pathways across molecular, crystalline, and hierarchical levels. By enabling sustainable nitrogen conversion, energy-relevant nanophase design, catalytic interface engineering, and environmental remediation, these mechanochemical strategies collectively exemplify how controlled impact dynamics create smart and functional interfaces, establishing ball milling as a cornerstone of mechanochemical architectonics.
:
ligand = 2
:
3) as a dry mixture into a twin-screw extruder, where alternating conveying and kneading zones impose intense shear and compression, driving rapid solvent-free coordination between the components. Residence times of only seconds to minutes are sufficient to produce a crystalline extrudate, while controlled barrel heating (up to 200 °C) enables a melt-phase route in which the molten ligand accelerates diffusion and framework formation, yielding ZIF-8 at throughputs of 1–4 kg h−1. Beyond throughput, extrusion enhances porosity and surface area compared to conventional methods,97,98 while life-cycle assessment of ZIF-67 confirmed orders-of-magnitude lower environmental impact relative to solvothermal synthesis, underscoring its green and sustainable character.78 Twin-screw extrusion (TSE), originally developed for polymer and food processing, has been successfully adapted to mechanochemical organic synthesis, providing a robust alternative to batch methods.4,100 Pharmaceutical applications illustrate its power: direct amidation of esters eliminates the need for stoichiometric activating agents,101 and Bolt et al.102 achieved a 100-fold scale-up of this transformation by translating from batch ball milling to continuous extrusion.
This work further demonstrated solvent-minimized synthesis of 36 amides via TSE, with optimization of rheology, grinding auxiliaries, and residence time enabling long-term operation. A 7-hour run yielded ∼500 g (1.3 mol) of amide at 80% yield, and the dynamics of both small-scale and extended campaigns are vividly depicted in Fig. 5, confirming extrusion's scalability and process stability.102
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| Fig. 5 (A) Optimal extrusion runs of amides on a 50 mmol scale. (B) A 7-hour solvent-minimized continuous extrusion synthesis of an amide, with 30-minute batches of the extrudate collected to monitor performance over time (see SI for detailed breakdown). Reproduced with permission.102 Copyright 2024, wiley. | ||
Song et al.103 extended these principles through a liquid-assisted spiral gas–solid flow (LA-S-GSF) system, enabling rapid synthesis of HP-HKUST-1 at 96% yield within 11 minutes, achieving a space–time yield of 6.9 × 104 kg per m3 per day, significantly outperforming solvothermal methods. Similarly, mechanochemical cocrystallization has produced stable pharmaceutical solids, such as ligustrazine cocrystals (TMP–MG, TMP–MG–H2O, TMP–EG, TMP–PG), with reduced hygroscopicity and reversible solid-state interconversion, highlighting their sustainable pharmaceutical potential.104
Parallel developments extend into polymer and composite systems, where mechanochemical rearrangements under extrusion and high pressure preserve nanostructural porosity (>98%) and enable scalable solar water evaporation, producing 9 L per day with a 1 m2 prototype.105 Water-assisted gel-like extrusion of PVA achieved remarkable toughness (elongation at break 504.9%) and ultralow oxygen permeability after biaxial stretching,106 while incorporation of NiO nanofillers into PP/PE composites enhanced tensile strength, elongation, and thermal stability.107 Similarly, integration of caffeine-loaded UiO-66 capsules into PA6 and PLA composites via extrusion produced matrices with ∼2.5 wt% caffeine loading and significantly improved durability relative to surface post-treatments.108
Complementing extrusion, high-pressure mechanochemistry exerts profound influence on atomic arrangements in solids, driving unique chemical and physical transformations.109,110 A persistent challenge lies in controlling which mechanical strains induce specific nuclear distortions and corresponding electronic effects.111 Recent strategies aim to tune crystal flexibility, thereby directing mechanochemical reactivity toward selective stress-responsive pathways.112 Together, extrusion and high-pressure approaches open new frontiers for transitioning mechanochemical processes from laboratory to industry, particularly for continuous solid-state synthesis.113,114 By coupling throughput, structural control, and environmental compatibility, these methodologies serve as critical enablers of multiscale mechanochemical pathways that underpin the design of smart and functional inorganic interfaces.
Hybrid mechanochemistry, wherein mechanical forces are synergistically combined with external stimuli such as temperature, light, ultrasound, plasma, or electric fields has emerged as a transformative strategy for accessing reaction pathways inaccessible to conventional solid-state processes.116,117 These thermo-, sono-, photo-, and electro-mechanochemical platforms significantly broaden the chemical reactivity landscape, enabling both enhanced performance and novel functionality.117,118 Plasma-assisted milling, for example, introduces defects into MXenes, improving their electrochemical behavior, while strain engineering under mechanochemical conditions via biaxial compression or out-of-plane tension has been shown to boost lithium-ion diffusion kinetics.118,119 Hybrid protocols also facilitate in situ functionalization of MXenes, where stimuli-activated dopants or surface groups expand their utility in smart interfaces.120,121
To contextualize these differences, Table 1 provides a comparative overview of representative mechanochemical platforms in terms of energy input characteristics, scalability, and defect control. This mechanistic shift toward stimuli-activated and dynamically functionalized surfaces highlights a fundamental contrast with conventional inorganic interfaces, which respond to mechanical loading through passive pathways dominated by defect generation, microplasticity, or frictional dissipation. Traditional interfaces rely on irreversible deformation and defect-mediated reactivity characteristic of classical ball-milling or mechanically enhanced adhesion where mechanical force merely perturbs existing bonds. In contrast, smart interfaces incorporate force-responsive motifs such as mechanophores or reorganizable coordination environments that transduce mechanical, thermal, photonic, or acoustic inputs into reversible chemical rearrangements or controlled activation events. This transition from passive defect accumulation to programmable, stimuli-coupled mechanochemical behavior underpins the adaptive reactivity observed in modern thermo-, sono-, and photo-mechanochemical systems.122,123 The fusion of ball milling with sonochemistry or photochemistry unlocks novel hybrid nanomaterials with adaptive properties.43,124 Hwang et al.125 demonstrated a mechano–chemical coupling system by integrating phospholipid copolymer vesicles within alginate hydrogels, enabling stress-induced ethylene glycol tetraacetic acid (EGTA) release at only 33–55 kPa and achieving controlled degradation. On a quantum scale, Wang et al.126 and Mittal et al.127 used the constrained geometries simulate external force (CoGEF) method, where force application narrowed HOMO–LUMO gaps and lowered reaction barriers, highlighting the predictive power of mechanochemical simulations. Similarly, Ghose et al.128 and Zhao et al.129 illustrated how external solvation and ultrasound-induced piezoelectricity, respectively, modulate mechanical rupture thresholds and reactive oxygen species (ROS) generation in Zn–bis-terpyridine and Mn–ZnO hybrids. Remarkably, Qu et al.130 reported that ball milling enabled MXene/PAbz hybridization via electrostatic and hydrogen bonding interactions, drastically reducing peak heat release rate (−69.57%) and total heat release (−54.38%), showcasing the fire-retardant promise of hybrid mechanochemistry.
| Platform | Energy input | Scalability | Defect control |
|---|---|---|---|
| Ball milling | High local energy, but heterogeneous | Moderate (batch-limited) | High defect density, limited precision |
| Extrusion | Efficient continuous energy input | High (industrial-scale) | Moderate, more uniform |
| Hybrid systems | Variable, stimulus-dependent | Moderate | Tunable and interface-specific |
Inorganic–organic hybrids can also be rapidly synthesized through silane-functionalized ball milling routes with over 90% efficiency, as reported by Amrute et al.8 The solid-state synthesis of D4SB crystals via thermally responsive grinding,131 and reversible emission switching, further underscores force–stimuli cooperation in tuning optoelectronic features. Structurally responsive systems such as MOFs display dynamic mechanochemical behaviors including bond rearrangement,132 phase transitions,133 and amorphization134 that depend on framework topology,135 defect density, and pore distribution.136 Real-time tools like high-pressure crystallography and nanoindentation elucidate these force–structure couplings,137,138 while milling experiments reveal rapid coordination bond cleavage and energy storage modulation.139 Overall, hybrid mechanochemical systems not only offer a versatile toolbox for manipulating structure–function relationships at multiple scales but also underpin the rational design of smart and responsive interfaces for advanced inorganic materials.
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| Fig. 6 (A) Schematic illustration of chirality generation in self-assembled NR superlattices via a press-and-rotate mechanical force. Reproduced with permission.146 Copyright 2022, Nature. (B) Schematic of MOF transformation via ball milling, showing framework decomposition followed by structural reconstruction. Reproduced with permission.156 Copyright 2021, American chemical society. (C) Schematic illustration of mechanochemical nanocasting synthesis of porous CeMnOx catalysts. Reproduced with permission.160 Copyright 2019, American chemical society. (D) Process of the preparation of MCO3.161 Copyright 2023, American chemical society. (E) Schematic of La (Ce,K)CoO3 lattice and redox cycles, highlighting soot oxidation via Langmuir–Hinshelwood and Mars–van Krevelen mechanisms. Reproduced with permission.162 Copyright 2022, American chemical society. | ||
Progressive energy input drives crystalline–amorphous transitions, where bulk structural transformations arise from bond disruption, densification, and framework collapse.2,147–149 Localized shell formation provides both opportunities and challenges: for instance, neat milling generates nanometer-thick amorphous shells on ZnO surfaces, enhancing interfacial reactivity but also limiting further conversion by encapsulating unreacted cores.150,151 Liquid-assisted grinding modulates this balance, as demonstrated for ZnO systems where hydrated intermediates gradually reorganize into crystalline frameworks with decreasing water content.152 Under high pressure, Zn-imidazolate frameworks undergo selective bond cleavage and structural reorganization, collapsing pore networks while preserving short-range order.149,153 Such cases underscore that mechanochemical reactivity does not simply replicate thermal pathways; rather, it introduces novel transformation routes linking defect accumulation, metastable polymorph formation, and bulk structural evolution.2,154
Mechanochemistry also provides unique avenues for coupling metal oxides and organic linkers into hybrid nanostructures. For example, solid-state reactions between ZnO and Hmim yield crystalline ZIF-8 shells encapsulating Pd nanoparticles,155 while iron oxide precursors undergo stepwise transformations from maghemite to MOF-integrated composites via neat and liquid-assisted grinding.19 Similar pathways enable metal–organic recoordination and even reconstruction of decomposed frameworks: Lee et al.156 showed that ball-milling restores crystallinity and porosity in degraded MOFs such as MOF-5, MOF-177, UiO-67, and ZIF-65 through cycles of defect generation and interfacial recoordination (Fig. 6B). These insights highlight the role of mechanical force in bridging atomic-scale bond cleavage with bulk-scale structural recovery.
Beyond oxides and MOFs, mechanochemical methods have unlocked reaction channels unattainable in solution. The generation of Grignard reagents from fluoronaphthalenes,157 the activation of benzene through Mg(I) dimers,69 and the stabilization of unusual η3-allyl–Mg coordination modes158 exemplify bond activation pathways arising directly from mechanical inputs. Likewise, lignin depolymerization under milling produces stable phenoxy radicals that reduce metal ions and initiate unconventional bond transformations.16 At higher scales, metal alloys and nitrides undergo progressive grain refinement, defect accumulation, and hot-spot-assisted diffusion, as shown for Fe–Cr–Si alloys and TiN formation.6,159 These cases emphasize that interfacial charge gradients, radical fluxes, and nanoscale strain collectively govern reactivity in ways decoupled from conventional thermal dynamics.39,97,142
Hybrid mechanochemistry further expands this framework by integrating force with external stimuli, enabling hierarchical transformations across multiple scales. Cheng et al.160 reported a nanocasting route in which lattice-level Mn incorporation into CeO2 generated mesostructured CeMnOx catalysts, achieving nearly complete NOx conversion at 150 °C and highlighting the solvent-free scalability of this process (Fig. 6C). Zhang et al.161 demonstrated that salt-assisted milling engineers hierarchical porosity in carbonates, where lattice perturbations, NaCl templating, and pore evolution converge to confine Pd nanoparticles within CaCO3 matrices (Fig. 6D). Yu et al.162 advanced the concept by designing alkali/cerium co-modified La–Co perovskites that exploit coupled atomic redox cycles, interfacial oxygen vacancy dynamics, and bulk lattice oxygen participation. In situ DRIFTS and DFT revealed synergistic Langmuir–Hinshelwood and Mars–van Krevelen mechanisms, with (Fig. 6E) illustrating how bifunctional effects in soot combustion catalysis arise from coordinated atomic, interfacial, and bulk processes.
These multiscale pathways reveal that mechanochemistry does not merely replicate thermal dynamics but opens unconventional reaction channels. However, the lack of a comprehensive quantitative framework limits predictive control over outcomes. The critical challenge remains to bridge atomic and interfacial events with bulk transformations through integrated modeling for rational design of smart interfaces.
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| Fig. 7 (A) Schematic representation of the procedure for developing proton-conducting inorganic–organic hybrids, guided by computational modeling. Reproduced with permission.166 Copyright 2023, American chemical society. (B) (a) Dataset construction for HOIP prediction, comprising 21 monovalent organic molecular cations (A-site), 19 metallic cations, and 9 representative anions across the periodic table. (b) Visualization of training (gray dots) and test (red dots) data based on tolerance factor and DFT-calculated band gap (PBE), illustrating the coverage of metals, semiconductors, and insulators within the dataset. Reproduced with permission.167 Copyright 2020, American chemical society. (C) (a) (Top) Endo adduct and its spherical representation of ΔEa,mec as a function of wall-type force directions. Some impact directions reduce the activation energy by up to −16.5 kcal mol−1, with an average 〈ΔEa,mec〉 of −3.88 kcal mol−1. (Bottom) Exo case, showing a maximum reduction of −8.9 kcal mol−1 and an average 〈ΔEa,mec〉 of −2.89 kcal mol−1. (C) (b) Comparison of activation energy variations for the endo Diels–Alder reaction (top) and the retro-DA reaction from the endo product (bottom). The mechanical effect on the retro-DA reaction is nearly negligible, as reflected in the ΔEa,mec scale. (C and D) Reproduced with permission.58 Copyright 2025, American chemical society. | ||
Complementary to these approaches, quantum chemistry calculations have revealed molecular deformation during activation, with the extreme-pressure polarizable continuum model tracking cavity volume changes under hydrostatic stress,168 while density functional theory (DFT) demonstrated how mechanical stress deforms C–C bonds, enabling thermally forbidden electrocyclic reactions.169 At the mesoscale, computational studies show that forces applied orthogonally to the reaction coordinate can significantly alter transition-state curvature,170 though no current model fully quantifies the mechanical work exerted during ball milling.
Nonetheless, recent work by Pladevall et al.171 has shown that standard DFT combined with continuum solvation and microkinetic modeling can quantitatively describe ball-milling reactions. By treating mechanochemical conditions as solution-like reactions with modified effective concentrations and dielectric constants, they reproduced experimentally observed reaction times for Diels–Alder cycloadditions and N-sulfonylguanidine formation under ball milling, and concluded that, at least for these benchmark systems, the mechanisms under milling and in solution are essentially identical and amenable to DFT-based analysis. Moreover, dispersion-corrected DFT has been directly applied to ball-milling conditions themselves, as demonstrated by Rojas-Chávez et al.,172 who computed ligand–surface interactions, surface-energy shifts, and facet stabilization in PbTe nanoparticles during high-energy milling.
Molecular dynamics further illuminate surface and interfacial pathways, exemplified by alkyl thiolate interfaces on coinage metals, where shear generates distinct metal-containing species and governs stress-driven surface-to-bulk transport.173 Fusaro et al.174 advanced this direction by developing a DFT-based framework incorporating electrostatics and solvent effects, successfully predicting ∼20 kcal mol−1 binding energies for biomolecule–gold interactions, consistent with experiments. Importantly, such mechanistic insights extend directly to nanoscale biointerfaces, as demonstrated by Triatmaja et al.,175 whose DFT-optimized docking models clarified the antibacterial mechanism of GO/ZnO/eugenol composites, revealing strong binding (−11.65 kcal mol−1) to DNA gyrase and effective ATP blockade.
To capture milling dynamics more holistically, discrete element method (DEM) and structural phase-field-crystal (XPFC) models have been employed. By incorporating ballistic terms, XPFC simulations reproduced nanoparticle nucleation and growth trends under room-temperature milling, with ligand chain length modulating the free energy landscape and predicting reduced particle sizes for longer ligands.176 Further refinement of reaction selectivity under mechanical stress has been achieved through mechanochemical algorithms. For example, diphenylfulvene/maleimide systems under isotropic wall-type forces showed preferential endo-pathway stabilization, with 〈ΔEa,mec〉 reductions of −3.88 kcal mol−1 compared to −2.89 kcal mol−1 for the exo case, offering a microscopic rationale for experimentally observed endo selectivity in mechanochemical Diels–Alder reactions (Fig. 7C(a)).58 Strikingly, retro-Diels–Alder processes remained unaltered, confirming that force biases are pathway-specific (Fig. 7C(b)). Collectively, these computational strategies from CoGEF and SDPs to DEM and XPFC demonstrate how stress can reshape potential energy landscapes, drive bond rupture (C–C, Si–O, S–Au), and rationalize transformations inaccessible by purely thermal means.
The integration of artificial intelligence (AI) has further accelerated progress, enabling optimization of mechanochemical conditions and predictive modeling with unprecedented precision. Machine learning potentials now reconcile the accuracy of quantum methods with the efficiency of classical simulations, resolving long-standing trade-offs.177 Algorithms such as XGBoost, coupled with dimensionality reduction, achieve up to 80% predictive accuracy in mechanochemical cocrystallization, outperforming conventional approaches and highlighting electrostatics and structural compatibility as AI-derived guidelines for rational solvent-free design.178 Artificial neural networks (ANNs) extend this capability, with models trained on process parameters and formulations achieving R2 > 0.99 for predicting pharmaceutical cocrystallization during ball milling. Such predictive robustness motivates hybrid models that fuse mechanistic frameworks with AI, enhancing accuracy in simulating complex multi-component systems.179 Beyond organics, computational chemistry paired with AI has successfully predicted defect energetics, binding affinities, and electronic behaviors in inorganic nanomaterials ranging from metal oxides to sulfur-based systems,159,180 underscoring cross-material generality. Together, computational modeling and AI not only decode multiscale mechanistic pathways but also enable rational control of smart functional interfaces, establishing a predictive foundation for the design of next-generation inorganic nanomaterials.
Siniard et al.183 indicated that incorporating CuCoFeNiMnOx into a CeO2 lattice using ultrasound-driven lattice engineering generates numerous oxygen vacancies, well-dispersed cations, and enhanced Ce3+/Cu+ redox centers. These characteristics facilitated ultralow-temperature CO oxidation (T50 = 100 °C, T100 = 150 °C), exceeding traditional dense HEOs. Fig. 8A demonstrates that the catalytic cycle involves lattice oxygen migration, vacancy formation, and fast oxygen replenishment, exemplifying a Mars–van Krevelen mechanism that imparts remarkable activity and stability to the HEO–CeO2 interface. Similarly, Zhang et al.161 devised a salt-assisted mechanochemical method to synthesize porous CaCO3, SrCO3, and BaCO3 in few minutes, attaining unprecedented surface areas (up to 172 m2 g−1). The Pd-loaded hierarchical CaCO3 catalyst achieved nearly total nitrobenzene hydrogenation (≥99% yield, TON = 1.3 × 104 h−1) and shown exceptional reusability throughout 11 cycles. Fig. 8B illustrates that NaCl templating during milling facilitates pore development, resulting in stable, high-surface-area interfaces conducive to effective catalysis. Furthermore, Xiao et al.184 developed an innovative method for extracting gold from anode slime without the use of solvents. This process involves KMnO4 and NH4Cl generating reactive chlorine species during milling, which oxidize metallic Au into soluble AuCl3. This approach was highly selective and yielded numerous results without employing toxic cyanide or solvent-intensive methods. This illustrates how mechanochemistry may benefit the environment through resource reutilization. Fig. 8C illustrates that the mechanical activation of KMnO4 and NH4Cl in conjunction results in the release of chlorine, facilitating the direct conversion of gold at ambient temperature. Likewise, Zhan et al.185 described a template-free mechanochemical method for synthesizing mesoporous CuOx–CeO2, with surface areas of up to 122 m2 g−1 with interconnected pores measuring 2–5 nm. The sponge-like structure maintained atomic-scale Cu2+ dispersion and improved Cu2+/Cu+–Ce3+/Ce4+ redox cycling, facilitating complete CO oxidation at around 98 °C, as illustrated in (Fig. 8D). Yang et al.186 developed a solvent-free mechanochemical approach for synthesizing Fe3O4 nanoparticles, distinguished by many oxygen vacancies and Fe2+/Fe3+ redox centers, which promote improved chemoselective reduction of nitroarenes. This catalyst, produced using ball milling and characterized by numerous flaws, exhibited over 99% selectivity, commendable turnover efficiency, and excellent reusability after 10 cycles. The engineered contact inhibited sintering, preserved the crystals, and facilitated electron mobility among them. All of them are crucial for energy-related catalytic applications. This study demonstrates how mechanochemistry can produce catalytic surfaces that are both physically robust and functionally superior.
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| Fig. 8 (A) Illustration of the synergistic HEO-assisted Mars–van-Krevelen mechanism for 0.25-HEO–CeO2. Reduced with permission.183 Copyright 2024, American chemical society. (B) Process of the preparation of MCO3 via salt-assisted mechanochemical milling and calcination. Reduced with permission.161 Copyright 2023, American chemical society. (C) Mechanism of gold conversion using KMnO4–NH4Cl through the mechanochemistry approach (MA). Reduced with permission.184 Copyright 2019, American chemical society. (D) Illustration of mechanochemical synthesis of mesoporous CuOx–CeO2 and transition-metal-doped ceria catalysts. Reduced with permission.185 Copyright 2017, American Chemical Society. | ||
Here, biomedical interfaces are approached from an inorganic-centered perspective, where organic and supramolecular elements are introduced as functional enablers to tailor surface chemistry, protection, and biointeractions of nanomaterials rather than as standalone material systems. Krupiński et al.189 introduced a mechanochemical strategy to produce sub-10 nm ZnO nanocrystals stabilized with urea ligands, demonstrating how surface chemistry can be tuned during synthesis to achieve stable organic–inorganic interfaces. A subsequent modification of β-cyclodextrin (β-CD) conferred water solubility and enhanced bioprocessability, essential conditions for the biomedical application of ZnO nanoparticles. Fig. 9A demonstrates the sequential process-from urea precursors to ZnO–urea nanocrystals and ultimately β-CD functionalization-demonstrating how mechanochemistry facilitates the synthesis of nanostructures specifically designed for biomedical interfaces, where dispersibility and compatibility are crucial. Similarly, Ma et al.190 engineered solid SiO2-sealed mesoporous silica nanoparticles to co-encapsulate TiO2 and the organic UV filter DHHB, attaining broad-spectrum protection while inhibiting ROS release and skin penetration. The coating method demonstrated stability and safety in sunscreen applications, as illustrated in Fig. 9B. Likewise, Mazaheri et al.191 illustrated a solvent-free mechanochemical method for encapsulating urea within metal–phenolic networks (MPNs), wherein tannic acid coordinated with Ti4+ during grinding to create stable hybrid matrices. As illustrated in (Fig. 9C), the resultant coatings demonstrated adjustable stability and regulated release, underscoring how mechanochemistry facilitates biocompatible and protective interfaces, akin to β-cyclodextrin-modified ZnO nanocrystals and silica-encapsulated UV filter systems.
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| Fig. 9 (A) Mechanochemical synthesis of ZnO nanocrystals from ethylzinc–ureate precursors and postsynthetic β cyclodextrin (β-CD) modification for water solubility. Reduced with permission.189 Copyright 2021, American chemical society. (B) Schematic structures and advantages of solid SiO2-sealed filter-entrapped MSNs (MSN-TiO2@SiO2 and MSN-DHHB@SiO2) and their UV protection mechanism. Reduced with permission.190 Copyright 2023, American chemical society. (C) Schematic of the mechanochemical, coordination-driven assembly of MPNs for urea crystal encapsulation. Reduced with permission.191 Copyright 2023, American chemical society. | ||
To ensure consistency with the catalysis and energy sections, this section now emphasizes direct mechanism–function relationships at the bio–nano interface. In particular, mechanochemically induced surface defects, ligand coordination modes, and hybrid architectures are explicitly correlated with biological performance metrics such as biocompatibility, oxidative stress modulation, and cellular uptake behavior. A comparative overview of mechanochemical and conventional synthesis routes is provided in Table 2.
| Aspect | Mechanochemical synthesis | Conventional synthesis | Biological mechanism–function correlation | References |
|---|---|---|---|---|
| Surface structure | Defect-rich, force-activated interfaces with tunable coordination | Thermodynamically relaxed surfaces | Controlled defects reduce cytotoxicity | 189 |
| ROS behavior | Defect passivation and solid-state ligand binding suppress ROS | Unpassivated surfaces promote ROS formation | Lower oxidative stress improves cell compatibility | 192 |
| Surface chemistry | Strong solvent-free ligand anchoring | Weak post-synthetic coatings | Enhanced dispersion and stability | 193 |
| Colloidal stability | Clean interfaces minimize aggregation | Residual solvents increase agglomeration | Reduced immune activation | 97 and 194 |
| Biocompatibility & hemocompatibility | Cleaner surfaces (no solvents), strong ligand anchoring → higher compatibility | Residual solvents, surfactants → potential cytotoxicity | Mechanochemical coatings significantly improve biocompatibility and reduce cellular stress | 195–197 |
| Drug encapsulation & release profiles | Solid-state assembly of metal–phenolic networks (MPNs) yield sustained release | Sol–gel and emulsion routes often show burst release | Mechanochemical MPNs provide controlled and stable release profiles | 191 |
The clinical relevance depends on a clearer understanding of their in vivo behavior, safety profile, and regulatory positioning. Recent studies demonstrate that solvent-free architectures, including metal–phenolic networks and ligand-passivated oxide nanostructures, display enhanced serum stability, reduced aggregation, and predictable degradation pathways, resulting in improved biodistribution and biocompatibility in vivo.198,199 The stability and safety attributes correspond closely with the current expectations of the U.S. Food and Drug Administration (FDA) and European Medicines Agency (EMA), especially for the reduction of organic solvent residues, impurity control, and reproducibility in nanomaterial production.200,201 Mechanochemistry, being a solvent-free and energy-efficient process, automatically meets numerous regulatory standards, making it a compelling option for future nanomedical production pipelines.202
Beyond conventional nanocarriers, mechanochemistry is accelerating the emergence of drug–nanomaterial composite strategies that hold significant value for pharmaceutical and clinical translation. Mechanochemical co-crystallization has enabled the formation of drug–excipient pharmaceutical co-crystals that improve solubility, dissolution kinetics, and physicochemical stability.203–205 Moreover, solid-state amorphization via high-energy milling generates amorphous drug phases that exhibit improved bioavailability and regulated release characteristics, thereby obviating the necessity for organic solvents or high temperatures.206 Collectively, these advancements underscore the capacity of mechanochemistry to produce biocompatible, stable, and therapeutically pertinent solid-state drug–nanomaterial hybrids, hence enhancing the translational potential of the mechanochemical platforms outlined in this section.
Yang et al.209 devised a more environmentally friendly mechanochemical method for producing CoAl2O4 composite pigments through the ball-milling of sea sand, CaCO3, and metal nitrates, succeeded by calcination. Fig. 10A illustrates that the CoAl2O4 nanoparticles were affixed to quartz surfaces, augmenting blue-light reflectance (∼430 nm) via interface-induced scattering. This sustainable technique diminished cobalt use while attaining superior optical stability, indicating prospective applications in colorimetric sensors, NIR-reflective coatings, and functional inks. In another study by Sarfudeen et al.210 engineered a mechanochemically manufactured triboelectric nanogenerator (TENG) utilizing ZTF-8 (a zeolitic tetrazolate framework) combined with carbon, resulting in a flexible, layered interface for energy harvesting and sensing. Fig. 10B illustrates that the TENG incorporates layers of PTFE, aluminum, ZTF-8, and carbon, which cyclically accumulate and discharge surface charge during mechanical contact and separation. This arrangement facilitates alternating electrostatic equilibrium and electron flow, yielding an output of 65 V and 4.2 µA, demonstrating exceptional responsiveness to human motion. Qin et al.211 fabricated Se-doped MoS2/ZnO heterostructures by a mechanochemical approach, incorporating both substitutional and interstitial selenium atoms to improve NH3 detection at ambient temperature. The dual-site doping enhanced charge transfer, surface reactivity, and heterojunction integrity, yielding a sixfold increase in sensitivity, a detection limit of 25 ppb, and expedited reaction and recovery times. Hidalgo-Rosa et al.212 employed multiconfigurational ab initio calculations to elucidate the luminescence quenching mechanism in nitroaromatic-responsive lanthanide MOFs, demonstrating that strong host–guest electronic coupling perturbs the antenna-to-metal energy-transfer pathway. Theoretical analysis revealed that π–π interactions and analyte-induced destabilization of the ligand triplet state suppress Tb3+ sensitization, resulting in efficient turn-off luminescence behavior and high sensing selectivity toward nitro compounds.
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| Fig. 10 (A) Schematic diagram of the preparation of CoAl2O4 composite pigments via a CaCO3-assisted mechanochemistry method followed by calcination. Reduced with permission.209 Copyright 2022, American chemical society. (B) (a) Schematic diagram of the proposed ZTF-TENG device architecture, in which ZTF-8 acts as the triboelectric positive material and PTFE as the negative counterpart, layered with carbon and aluminum electrodes for flexible operation. (b) Schematic of the contact–separation mechanism, illustrating charge generation and electron flow during device operation. Reduced with permission.210 Copyright 2024, American chemical society. | ||
The inherent simplicity of mechanochemistry masks persistent issues: processes often proceed on a trial-and-error basis due to the absence of a comprehensive predictive framework,9 and current models including hot spot and magma–plasma theories remain qualitative, failing to integrate mechanical energy into thermodynamic formalisms. Existing nanoparticle growth models from dilute solutions cannot be directly applied to solid-state systems,176 and no current theory adequately describes the spatiotemporal evolution of nucleation or nanocrystalline precipitates. Consequently, rational design remains limited, and reaction selectivity is frequently undermined by unintended side reactions.215 These challenges are compounded by the restricted scope of mechanochemical transformations, as reactions requiring precise temperatures, pressures, or solvent participation often fall beyond the reach of mechanical activation.144,215
Practical synthesis also faces substantial barriers. Multistep and solvent-intensive methods raise toxicity concerns and limit suitability for biomedical applications,19,216 while poor control over size, shape, and surface chemistry continues to limit reproducibility and targeted functionality.217 Magnetic nanoparticle synthesis exemplifies these challenges, as hazardous multistep methods, difficulties in reducing poorly soluble oxides, aggregation, and reduced Curie temperatures compromise reproducibility and nanoscale stability.218 Similarly, AgNP synthesis suffers from agglomeration, contamination, and poor stability, reducing antimicrobial activity.29 For magnetic framework composites, limited studies and scarce biomedical evaluations further restrict comprehensive assessment of their potential.19 Strontium-based semiconductors also remain hindered by low precursor solubility and stable adduct formation, which compromise their targeted electronic properties.69 Highly soluble oxides such as B2O3 require sublimation or physical separation techniques due to poor by-product removal using conventional washing.219 More broadly, end products are frequently contaminated by milling media, jars, or container abrasion,181,220 which, alongside difficulties in tuning porosity, morphology, and uniformity, restricts the optimization of functional interfaces.
From a processing perspective, power ball milling has been widely employed for iron oxide synthesis,221 yet limitations in particle size control, post-processing, and contamination remain acute. Even in successful demonstrations, such as magnetite nanoparticle synthesis via prolonged milling,222 metallic impurities persisted. Knowledge on salt precursor reduction into noble metal nanoparticles remains scarce,33 and diffusion-limited mass transfer further constrains reproducibility. Moreover, mechanochemical grafting often leads to reduced surface area, pore diameter, and pore volume, while increasing silane loadings diminish silylation efficiency and limit uniform functionalization.8 Although polymer mechanochemistry holds promise, its extension to regulate heterogeneous catalysis a domain critical for industrial relevance has not yet been realized.223
Scaling laboratory processes to industrial production introduces further complexities. High-energy milling requires extensive optimization to balance quality, efficiency, and safety, while uncontrolled variables such as dust generation, noise, and equipment hazards demand stringent safety protocols.144 The energy-intensive nature of high mechanical forces also raises concerns over sustainability, operational costs, and environmental impact when reliant on non-renewable sources.215 Although mechanochemistry has advanced industrial use in pigmentation,224 catalysis,225 and wastewater treatment,226 its broader adoption remains limited. Moreover, systematic evaluation using sustainability metrics such as atom economy and waste reduction remains underutilized, with only a few applications in MOFs and nanoparticles.35 From a pharmaceutical manufacturing perspective, GMP compatibility of mechanochemical processes is platform-dependent. Continuous technologies, particularly twin-screw extrusion, are inherently more GMP-aligned due to enclosed operation, improved process control, and established pharmaceutical validation, whereas batch ball milling remains challenged by contamination risks and batch-to-batch variability, motivating a shift toward inert, enclosed, and continuous or hybrid reactors.
Taken together, these limitations underscore the dual challenge mechanochemistry faces: fundamental gaps in understanding multiscale reaction pathways227 and practical obstacles in reproducibility, scalability, and interface tuning. Without bridging the divide between atomic-scale mechanisms and process-level control, the full potential of mechanochemical architectonics in constructing smart and functional interfaces will remain unrealized.
The future of mechanochemical research will also benefit from hybrid strategies that couple mechanical energy with thermal, light-based, or electromagnetic inputs, thereby enabling greater control over nanostructure formation and reaction selectivity.159 Similarly, integrating mechanochemical methods with colloidal synthesis holds promise for overcoming current shape-control limitations, particularly in noble metal nanostructures, where anisotropy and tunability are crucial for applications in catalysis, sensing, and biomedicine.33,232 The next phase of research should therefore prioritize precise size, shape, and composition control during synthesis, supported by deeper investigation into parameters such as ball-to-powder ratio, milling time, and post-milling heat treatments, including the influence of salt matrices and ion–surface interactions.34,39,233 Developing strategies for soft-mechanochemical processing remains particularly critical for controlling size, shape, and agglomeration compared with more established non-soft approaches.39
In parallel with these broader technological advances, mechanochemistry enables clearly defined opportunities in nanomedicine and hybrid architectures. Force-driven synthesis supports solvent-free fabrication of inorganic–organic and biohybrid interfaces with enhanced stability, defect-mediated bioactivity, and controlled surface chemistry, enabling systematic development of multimodal bioimaging platforms, therapeutic nanozymes, and adaptive biomedical interfaces.
Beyond nanoparticles, mechanochemistry provides outstanding opportunities to access stoichiometric variations of inorganic compounds and synthesize ordered frameworks such as MOFs with tunable porosity, thereby advancing crystal engineering, adsorption, and separation technologies.97,234,235 Mechanochemical methodologies have also demonstrated the ability to generate inorganic complexes and reactive species inaccessible by solution routes, with notable examples including kilogram-scale synthesis of Al(III) and In(III) salen and salophen complexes, which underscores the potential for industrial upscaling.13,14 Such approaches can dramatically reduce reaction times from days to minutes, further enhancing energy efficiency for complex main-group and transition-metal compounds.236 Recent advances in solvent-free C–C and C–N couplings exemplify how mechanochemistry can reshape sustainable industrial and pharmaceutical production,69 while the growing exploration of bioconjugates involving proteins and monosaccharides points to future applications in supramolecular assembly and biointerfaces.237
The integration of real-time in situ monitoring with computational modeling, coupled with advanced synchrotron X-ray diffraction and Raman spectroscopy, provides new opportunities to unravel mechanochemical mechanisms with unprecedented resolution.35,227 Such efforts will be complemented by the emerging concept of reversible mechanochemical reactions, which enables the exploration of equilibrium processes under mechanically driven conditions.238 Life cycle assessment methodologies tailored to mechanochemistry offer a further opportunity to benchmark environmental performance against conventional routes, facilitating industrial adoption.239 At the same time, advancing theoretical models and simulations to describe mass and energy transfer across different scales remains a pressing need for bridging laboratory insights with industrial process design.240 Critically, the industrial translation of mechanochemistry requires optimization of equipment design, milling rates, and energy inputs, ensuring scalability while maintaining sustainability advantages.144,241,242 Mechanochemical routes have already demonstrated significant potential to scale catalyst synthesis toward industrial levels while simultaneously reducing hazardous waste generation and energy consumption.242 Future studies should therefore exploit mechanochemistry to design nanostructured catalysts with enhanced stability and selectivity, enabling applications in renewable energy and environmental remediation beyond traditional chemical production.144,181 The emerging practice of integrating mechanochemistry with complementary electrochemical and photochemical methods further expands the scope of multifunctional pathways, opening new directions for energy storage, conversion, and sustainable environmental technologies.144,243
Altogether, these opportunities establish mechanochemistry not merely as a cost-effective and sustainable synthetic tool, but as a transformative paradigm for designing multiscale inorganic architectures and smart functional interfaces. By uniting green chemistry, computational modeling, real-time monitoring, and hybrid processing strategies, mechanochemistry is poised to shape the next generation of advanced nanomaterials with unprecedented precision, functionality, and scalability.
Case studies spanning catalysis, energy systems, biomedicine, and electronics affirm mechanochemistry's potential to deliver application-specific nanomaterials with superior performance, tunability, and sustainability. Nonetheless, challenges persist in achieving reproducibility, real-time mechanistic insight, and precise control over size, composition, and morphology. Future progress will hinge on integrating in situ diagnostics, multiscale computational modeling, and AI-guided synthesis to establish predictive control. Furthermore, coupling mechanochemical methods with electrochemical, photochemical, and bioinspired pathways promises to expand functionality while adhering to principles of green chemistry. Altogether, mechanochemical architectonics emerges not merely as a synthetic strategy but as a forward-looking materials design philosophy, poised to shape the next generation of inorganic nanotechnologies for sustainable and multifunctional applications.
| AI | Artificial Intelligence |
| ANNs | Artificial Neural Networks |
| BPR | Ball-to-Powder Ratio |
| CoGEF | Constrained Geometries Simulate External Force |
| DEM | Discrete Element Method |
| DFT | Density Functional Theory |
| GO | Graphene Oxide |
| HER | Hydrogen Evolution Reaction |
| HKUST | Hong Kong University of Science and Technology (MOF family) |
| LAG | Liquid-Assisted Grinding |
| MOFs | Metal–Organic Frameworks |
| MXenes | Two-Dimensional Transition Metal Carbides/Nitrides |
| NMR | Nuclear Magnetic Resonance |
| NR | Nanorods |
| PAD | Push–Pull Protonated Atomic Distance |
| PLA | Polylactic Acid |
| PVA | Polyvinyl Alcohol |
| ROS | Reactive Oxygen Species |
| TSE | Twin-Screw Extrusion |
| WC | Tungsten Carbide |
Supplementary information (SI) is available. See DOI: https://doi.org/10.1039/d5mr00116a.
| This journal is © The Royal Society of Chemistry 2026 |