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Influence of the aromatic surface on the capacity of adsorption of VOCs by magnetite supported organic–inorganic hybrids

María de las Nieves Piña*, María Susana Gutiérrez, Mario Panagos, Paulino Duel, Alberto León, Jeroni Morey, David Quiñonero and Antonio Frontera*
Department of Chemistry, Universitat de les Illes Balears, Crta. de Valldemossa km 7.5, 07122 Palma de Mallorca, Spain. E-mail: toni.frontera@uib.es

Received 14th June 2019 , Accepted 31st July 2019

First published on 5th August 2019


Abstract

It has been recently evidenced that hybrid magnetic nanomaterials based on perylene diimide (PDI) dopamine and iron oxide nanoparticles are useful for the adsorption and determination of volatile organic compounds (VOCs). However, NDI compounds are expensive and difficult to handle compared to smaller size diimides. Therefore, in this manuscript a combined experimental and theoretical investigation is reported including the analysis of the effect of changing the aromatic surface on the ability of these magnetite supported organic–inorganic hybrid nanoparticles (NPs) to adsorb several aromatic and non-aromatic VOCs. In particular, two new hybrid Fe3O4NPs are synthesized and characterized where the size of organic PDI dopamine linker is progressively reduced to naphthalene diimide (NDI) and pyromellitic diimide (PMDI). These materials were utilized to fill two sorbent tubes in series. Thermal desorption (TD) combined with capillary gas chromatography (GC)/flame detector (FID) was used to analyze both front and back tubes. Adsorption values (defined as % VOCs found in the front tube) were determined for a series of VOCs. The binding energies (DFT-D3 calculations) of VOC–Fe3O4NP complexes were also computed to correlate the electron-accepting ability of the arylene diimide (PDI, NDI or PMDI) with the adsorption capacity of the different tubes. The prepared hybrids can be easily separated magnetically and showed great reusability.


Introduction

Volatile organic compounds (VOCs) are inherent to modern human life. For instance, they are used as markers in medicine1 and industry.2 Moreover, they are used as indicators for the presence of other substances. The investigation of VOCs is intensive in many areas like environmental research,3 medicine,4 and even in military applications.5 The analysis and quantification of VOCs is needed to control the quality of biomaterials6 and they are also used as markers of microbial contamination in the case of bacteria and fungi.7 Moreover, VOCs are also normally used as markers in food industry for controlling the quality of raw materials.8

Regrettably, the number of endogenic pollutants and their sources continuously rises. Therefore, it is very important to actively monitor pollutants that are generated not only from agricultural but also from personal care products and pharmaceuticals, such as birth control pills, painkillers and antibiotics.9–11 Consequently it is even more important to investigate new methodologies and develop low cost techniques for the monitoring of air,12 since VOCs are ubiquitously present in our indoor daily lives. In fact, humans are constantly exposed to smells from many sources (fragrances, furnishings, cleaners, disinfectants, printers, glues, etc.). VOCs are then considered essential to assess the quality of the air in indoor environments.13–15

For several decades, studies on application of gas sensors for detection of VOCs have been carried out.16 There are several types of chemically sensitive sensors for VOCs, including metal oxides, conducting polymers, sensors based on acoustic wave propagation, etc.17 Nowadays electronic noses with a large number of resistive sensors based on statistical methods are used to facilitate the recognition of VOCs. The commercially available electronic noses are built with conducting polymer and metal oxide sensors.18 A serious drawback of this type of sensors19 is the signal degradation over time and the complex composition of the sampling matrices.20 Some enhancement is achieved by utilizing multiple sensors20c or sensor arrays integrated on a multimodal sensing platform21 that facilitates a precise detection in real-time.22,23 The progress in micromachining and nanotechnology allows building sensors of small size.24 As a matter of fact, the utilization of nanomaterial improves the sensing performance and facilitates the generation of new multisensing arrays.25,26 There is a growing interest in the utilization of different types of nanomaterial for the design of new diagnostic tools. The main advantages of these materials are the high surface/volume ratio, fast response time and easy recovery and reutilization.27 For instance, Li et al.28 have reported the utilization of polythiophene nanostructured for the detection of VOCs that exhibited enhanced discrimination compared to standard diagnostic tools.

Compared to other materials, the main advantages of iron oxide (Fe3O4) magnetic NPs follow: (i) economic and easy to handle and prepare; (ii) versatile via functionalization and (iii) very easy to recuperate by means of an external magnetic field.29 As a matter of fact, it has been recently demonstrated that hybrid nanomaterials30 consisting of chitosan-coated magnetite nanocomposite are very convenient catalysts because of their reusability. The main advantage of these catalysts is the presence of magnetite core since it allows an easy recovery and reuse in catalytic reactions. Therefore, their use is convenient in the sense of reuse and sustainability with the environment.31 In fact, our group has recently used a PDI-dopamine derivative to functionalize hybrid nanoparticles (Fe3O4NP), which were utilized to fill sorbent tubes. These tubes were used and reused more than 200 times for the adsorption and quantification of aromatic VOCs.32

In this new investigation, the possibility of using smaller and cheaper substitutes of PDI (see Scheme 1) is explored, which are pyromellitic diimide (PMDI) 1 and naphthalene diimide (NDI) 2 to adsorb and quantify a series of VOCs. The results are compared with those obtained using the PDI-dopamine derivative. It is worth mentioning that dopamine containing pyromellitic diimide has been successfully used for the molecular recognition of electron rich guests.33 The interaction energies of the VOCs with compounds 1–3 were initially computed by using theoretical calculations (DFT-D3). Moreover, sorbent tubes filled with the three hybrid nanoparticles were built. Then a simple analytical method based on thermal desorption (TD) coupled to gas chromatography (GC) and FID detection was used and validated for the determination of the VOCs tested herein (compounds 4–12, see Scheme 1). The two families of VOCs selected (aromatic and non-aromatic) present an increasing size aliphatic chain as substituent. The sorbent tubes were filled with PDI, NDI and PMDI-based magnetite supported organic–inorganic hybrids and their ability to adsorb the VOCs was determined and compared. The different affinities showed by the hybrid nanoparticles for the adsorption and quantification of the VOCs was also compared with the DFT calculations that are in agreement with the experimental results. The increasing number of C–H⋯π interactions on going from compound 4 to 8 are responsible for the higher adsorption of the VOCs and the alkyl chain grows.


image file: c9ra04490f-s1.tif
Scheme 1 PMDI (1), NDI (2) and PDI (3) derivatives used to functionalize the Fe3O4NP. VOCs 4 to 9 used in this study.

Methods

The synthesis and characterization of the PMDI-Fe3O4 nanoparticles used herein have been carried out using the methodology described in the literature by others.34 The synthesis and characterization of the PDI-Fe3O4 hybrid nanoparticles have been previously described by us.32 Reagents and solvents required for the synthesis of the new NDI–Fe3O4 nanoparticles were purchased from Sigma-Aldrich and used without further purification. The magnetic nanoparticle functionalization reactions were carried out in a Biotage Initiator Classic Microwave Synthesizer microwave reactor with a power of 400 W. The magnets used in magnetic decantation are NdFeB magnets, with an N52 magnetic degree. The functionalized nanoparticles are thermally stable up to 450 °C, therefore they are suitable for utilization in the experiments detailed below, since the maximum temperature used in the adsorption–desorption apparatus is 375 °C. Remarkably, no degradation of the magnetic nanoparticles even after 200 repetition of the experiment is observed. The VOC analytes were purchased from Sigma-Aldrich and Fluka (Buchs, Switzerland) and their purity was higher than 98% in all cases. The solvent was purchased from Scharlau (chromatographic quality). The glass tubes (6 mm of diameter and 90 mm length) and the unsilanized glass wool were purchased from Supelco (Bellefonte, PA, USA).

Synthesis of naphthalendiimide-dopamine (NDI-DA)

1 mmol of 1,4,5,8-naphthalentetracarboxylic dianhydride is dissolved in 25 mL of DMF, in a round-bottomed flask, with a 2 mL of Et3N. After total solution, 2 mmol of dopamine hydrochloride dissolved in DMF were added. The reaction mixture was brought to constant reflux for 2 hours. After the reaction, most of the DMF was removed in a rotary evaporator, and then 100 mL of cold H2O were added to precipitate the product. Before that, the solid was filtered under vacuum, washed with cold water (3 × 10 mL) and air-dried. As a result, the final product was obtained with a good yield (80%). Molecular weight: 538.51 g mol−1. Melting point: >200 °C. 1H-NMR: (DMSO-d6) δ: 8.83 (s, 4H), 8.67 (s, 4H), 6.65 (m, 6H), 4.18 (t, 4H) and 2.75 (t, 4H) ppm. 13C (DMSO-d6) δ: 162.44; 145.22; 143.79; 130.45; 129.30; 126.28; 119.26; 115.96; 115.64; 41.82 and 32.81 ppm. FTIR (KBr): 3386, 2968, 1699, 1654, 1336 and 768 cm−1.

Functionalization of nanoparticles with NDI-DA

One drop of 1 M NaOH and 1 mL of FeNP (10 mg mL−1) were added to a solution of 0.025 mmol of NDI-DA in 4 mL of H2O. The mixture was sealed in a 5 mL microwave flask, sonicated with an ultrasound for 5 minutes and then introduced in a microwave reactor at 120 °C and 3 bar for 30 minutes. The resulting mixture containing the functionalized FeNPs was decanted magnetically and washed firstly with 5 mL of ethanol and secondly with 5 mL of H2O. The final product was dispersed in 10 mL of H2O at a concentration of 1 mg mL−1. FTIR (KBr): 3475, 3381, 2924, 2852, 1704, 1656, 1581, 1455, 1337, 1243, 1170, 1119, 1028, 880, 769, 692 and 599 cm−1. BET specific surface area: 79.07 m2 g−1. Potential Z (ζ) (H2O, 25 °C): −38.3 mV. Average diameter (SEM): 60.46 nm. Hydrodynamic diameter (Dh) (H2O, 25 °C): 300.6 nm (see ESI for further details, including SEM micrographic images, DLS size distribution and zeta potential of all hybrid nanoparticles used in this work).

Standard solutions

For each VOC used in this study freshly prepared stock standard solutions on the day of use were stored at 4 °C in darkness in 1.5 mL flasks. The standard solutions were prepared using these mother solutions by using methanol as diluent. The concentrations of the standard solutions were: 0.140, 0.280, 0.420, 0.560, 0.700, 0.840 and 0.98 μL VOC/μL with a final volume of 1000 μL. The quantity injected was 2 μL of standard solution of 0.7 μL VOC/μL (1.4 μL VOC) for the determination of the percentage of retention.

Tubes filled with magnetite supported organic–inorganic hybrids

A single tube was used for the generation of the calibration plots and two tubes connected in series were used to calculate the percentage of retention of the analyte in the functionalized nanoparticles. 450 mg of hybrid nanoparticles were introduced in each tube and a periodical test was done to both tubes to check that were able to give the same analytical result when doped with the same quantity of a given VOC. After total desorption, a verification that both tubes are perfectly clean was carried out. Before the first use, a thermal cleaning was performed using the following protocol: 250 °C for 20 min, 300 °C for 20 min, 330 °C for 20 min, 350 °C for 20 min and 375 °C for 20 min under a flow rate of dry N2 of 70 mL min−1. For successive experiments, pre-conditioning for 20 min at 375 °C was used. After conditioning, they were immediately sealed with Swagelock end caps fitted with PTFE ferrules and stored in closed plastic boxes filled with desiccant material. Samples used for the doping and desorption experiments were freshly prepared immediately after the preparation of the tubes. The commercial doping device supplied by the instrument manufacturer was employed for the doping of the tubes. A manual injection under a flow rate of dry N2 of 100 mL min−1 of the VOC was carried out. This is done through a Swagelock adapter (stainless steel) that connects the tube without any possibility of leakage. The constant N2 flow guarantees the homogeneity of the sample through the sorbent. For the sake of reproducibility, 1 μL of VOC solution was always used and a doping time of 5 min was applied. During the first minute, the syringe was kept in the injector in order to maintain the flux unperturbed.

Analytical instrumentation and procedure

The VOC analyses were carried out using a manual injection (Unity 2 model, Markes) thermal desorption (TD) coupled to a gas chromatograph with a FID detector (6890A model, Agilent Technologies). The first step is an initial pre-desorption during 0.1 min and a flux of 20 mL min−1. Subsequently, a primary desorption is performed at 300 °C during 10 min, with a split of 4 mL min−1. During this time period, the analyte that was previously adsorbed in the tube is concentrated in a criofocusing trap that contains 30 mg of Tenax TA, and kept at −30 °C. Afterwards, the trap is quickly heated from −30 °C to 300 °C and kept at the final temperature during 10 min and, thus, the secondary desorption takes place. In this step the analyte is sent to the gas chromatograph using a split with a flux of 7 mL min−1 and finally injected to a capillary column (DB-624, 60 m × 0.25 mm × 1.4 μm, Agilent Technologies) through a line at 200 °C. The oven temperature was initially set at 40 °C during 1 min and progressively increased (rate of 6 °C min−1) until 230 °C. This final temperature is maintained during 5 min. The carrier gas was premium quality N2 with a flux of 1 mL min−1 approximately.

Theoretical details

The geometries and energies of all complexes included in this study were computed at the BP86-D3/def2-TZVPP level of theory. The complexes were fully optimized and they are true minima. The BP86 functional was employed with the latest available correction for dispersion (D3),35 since it is needed to describe adequately the π-stacking interactions. This level of theory is a good compromise between the size of the systems and the accuracy of the results.36 The calculations have been carried out by utilizing the program TURBOMOLE version 7.0.37 The plots of the MEP surfaces were generated using the van der Waals surface (0.001 a.u. isosurface).

Results and discussion

Preliminary MEP analysis

As a starting point the MEP (Molecular Electrostatic Potential) surfaces of PDI, NDI and PMDI molecules (see Fig. 1) were computed. For the three compounds, the MEP values in some selected points of the surface are indicated. It can be observed that the MEP values are more positive at the imidic rings varying from +79 for NDI and PMDI to +54 kJ mol−1 for PDI. The MEP values over the central rings are also positive, +37 kJ mol−1 for PDI and PMDI and +29 kJ mol−1 for NDI. Regarding the aromatic VOCs (not shown in the Fig. 1), all of them present large and negative MEP values over the center of the ring. In case of benzene the MEP value is −86 kJ mol−1 and the rest of aromatic ring exhibit the same value, which is slightly more negative (−90 kJ mol−1) in agreement with the weak electron donating nature of alkyl substituents. These preliminary analysis anticipates that benzene should have lesser affinity than the rest of aromatic VOCs. Moreover, any difference between the alkyl substituted benzenes should be due to interaction with the alkyl chain since the π-staking should be equivalent. For the aliphatic VOC, it is expected that the π-acidic surface will have affinity for the negative O atoms, although it is also possible to envisage C–H⋯O interactions since the MEP surfaces of PDI, NDI and PMDI molecules exhibit positive values in the molecular plane close to the C–H bonds (see Fig. 1).
image file: c9ra04490f-f1.tif
Fig. 1 MEP surfaces of aromatic diimides 1–3 used in the study. Energies at selected points of the surface (0.001 a.u.) are given in kJ mol−1.

Energetic study

In order to study the affinity of compounds 1–3 to VOCs 4–12, an energetic and geometric analysis of the complexes using DFT-D3 calculations were carried out. Different conformations and binding modes for the interaction of 1–3 with the VOCs were considered. The geometries obtained of the energetically most favourable complexes for the binding of compound 8 (as representative model of aromatic VOC) with the three receptors used in this work are given in Fig. 2. The complexes of the other aromatic VOCs are similar to those found for 8. In all cases (Fig. 2) the DFT calculations indicate that the π–π stacking complexes are the most favourable binding modes, with equilibrium distances (3.22–3.33 Å) that are in the range of strong donor–acceptor π–π interactions. Moreover, two aliphatic H-atoms also point to surface of the receptor, thus further contributing to the stabilization of the assemblies. In receptor 1 the C–H bonds are located over a five membered ring, in compound 2 over a six-membered ring and in 3 over two fused six-membered ring. Therefore, they are expected to be stronger in 3 compared to 2 and 1 because the π-system is more accessible in the former. These results suggest that the ancillary C–H⋯π interactions likely modulate the interaction energies in addition to the dominant π-stacking interaction. The binding energies are gathered in Table 1. As anticipated by the MEP analysis, among the aromatic VOCs, the benzene exhibits the lowest interaction energy for the three receptors 1–3.
image file: c9ra04490f-f2.tif
Fig. 2 (a–c) Optimized geometries of 1[thin space (1/6-em)]:[thin space (1/6-em)]1 complexes between VOC 8 and the different π-acidic surfaces (PDI, NDI and PMDI) at the PB86-D3/def2-TZVPP level of theory.
Table 1 Interaction energies (ΔE in kJ mol−1) of complexes between receptors 1–3 and VOCs 4–12 at the PB86-D3/def2-TZVPP level of theory. The adsorption is the percentage of VOC retained in the front tube. See Scheme 1 for the structure of VOCs
VOC ΔE, adsorption
1 2 3
a The presence of VOC was not detected in the front tube (see main text).
4 −40.1, 59 ± 5% −45.1, 64 ± 5% −45.1, 65 ± 5%
5 −47.6, 62 ± 5% −49.3, 68 ± 5% −57.3, 76 ± 5%
6 −49.7, 69 ± 5% −57.7, 74 ± 5% −57.7, 75 ± 5%
7 −51.8, 70 ± 5% −59.8, 78% ± 5% −59.4, 77% ± 5%
8 −52.3, 70 ± 5% −59.8, 80 ± 5% −63.1, 89 ± 5%
9 −22.9, —a −36.4, —a −30.9, —a
10 −43.5, 67 ± 5% −48.5, 69 ± 5% −38.9, 63% ± 5%
11 −49.3, 70 ± 5% −55.2, 75 ± 5% −60.3, 82% ± 5%
12 −55.6, 75 ± 5% −58.9, 81 ± 5% −62.3, 86 ± 5%


Moreover, a general trend is that the interaction energy increases as the size of the alkyl chain does. The strongest complex is established between the butylbenzene and the PDI receptor. For the aliphatic VOCs, similar trends are observed. The interaction energies increase as the size of the alkyl chain increases. Moreover, the interaction energies are in general stronger for receptor 3 apart from methyl and ethyl acetate where the PDI receptor 2 forms stronger complexes. Receptor 1 presents the weakest interaction energies in line with the smallest π-surface.

The complexes of NDI receptor 2 with the non-aromatic VOCs are represented in Fig. 3. Apart from complex 9@2, the lp–π interaction is established with the most π-acidic imidic ring. The methyl group of acetate is located outside the π-surface of PDI moiety is such a way that one C–H bond points to the O-atom of the imide group (see blue dashed lines in Fig. 3). On the contrary, the alkyl chain is located over the π-system establishing an increasing number of C–H⋯π interactions on going from methyl to butyl, thus explaining the larger binding energies observed for VOCs 11 and 12. In addition, it can be observed that the lone pair (lp)–π interaction distance between the oxygen atom of the carbonyl group and the 6-membered imidic ring of the NDI is identical in the complexes of VOCs 10, 11 and 12 (measured from the O atom to the mean plane). Consequently, this geometric features confirms that the differences in the binding energies are due to the C–H⋯O and C–H⋯π interactions. Apart from the smallest VOC 9, the interaction energies gathered in Table 1 are similar for both aromatic and non-aromatic VOCs, therefore adsorbent material based on hybrid PMDI/NDI/PDI–Fe3O4NPs should be equally efficient for the aromatic and non-aromatic VOCs of these particular families.


image file: c9ra04490f-f3.tif
Fig. 3 Optimized complexes of NDI 2 with methylacetate (a) and ethyl acetate (b), propylacetate (c) and butylacetate (d) at the PB86-D3/def2-TZVPP level of theory. The lone pair (lp)⋯π interactions are indicated as dashed lines. The interaction energies are also indicated.

Table 1 gathers the quantity of VOC adsorbed by the sorbent tubes based on hybrid PMDI/NDI/PDI–Fe3O4NPs. The details of how these values were obtained are detailed below. At this point, it is worthy to emphasize that for the aromatic VOCs the percentage of adsorption versus the interaction energies was represented. Remarkably, a good correlation between the adsorption and the interaction energies (R2 = 0.9045 see Fig. 4) was found. Such correlation strongly supports the proposed binding mode of the VOCs with the π-surface of the receptors and represents a direct correlation between the interaction energies of the π-stacked complexes and the experimental adsorption data.


image file: c9ra04490f-f4.tif
Fig. 4 Regression plot of % quantity of VOC adsorbed and the interaction energies for the aromatic VOCs interacting with receptors 1–3.

Synthesis of the magnetite supported organic–inorganic hybrids, fabrication of the sorbent tubes and adsorption–desorption experiments

For the synthesis of the magnetite supported organic–inorganic hybrids the protocol available in the literature was reproduced.29–33 Moreover, the synthetic protocols for the starting products perylenediimide-dopamine (PBI-DA) and pyromellitic diimide-dopamide (PMDI-DA) ligands are also available in the literature. The new naphthalendiimide-dopamine (NDI-DA) ligand was synthesized in good yield (80%) by adding two equivalents of dopamine hydrochloride to one equivalent of 1,4,5,8-naphthalentetracarboxylic dianhydride in N,N-dimethylformamide (DMF). Subsequently, the conjugation of the NDI-DA ligand with the magnetite was performed using the microwave-assisted heating method37 since our group has previously demonstrated for PDI-DA and PMDI-DA ligands that it increases significantly the covalent functionalization of the nanoparticle.38

A series of three different sorbent tubes were prepared (glass tubes of 6 mm of diameter and 90 mm of length) filled with 450 mg of the three different hybrid nanoparticles used in this work. In addition, unsilanized glass wool was placed at both ends of the tubes. Subsequently, the adsorption ability of the sorbent tubes filled with the three different hybrid Fe3O4NPs (see Scheme 2) to collect the VOCs 4–12 was studied. The procedure has been recently described our group and involves two basic steps. The first one is the utilization of one sorbent tube which is doped with different concentrations of VOCs for the generation of the working concentration range and also the calibration plots (see ref. 20 for a comprehensive description). The calibration plots and working ranges are given in the ESI. The second step is the calculation of the adsorption capacity of the tubes. That is, two sorbent tubes connected in series (using a Swagelock-PFA union) are used, as represented in Fig. 5. Each tube is filled with 450 mg of hybrid nanoparticles, and for each experiment, a known quantity of VOC (from 0.120 to 0.130 mg) was injected, which is larger than the upper limit of the working range used for the generation of the calibration plots. The individual analysis of the back tube allows to measure the quantity of VOC that has not been adsorbed in the front tube. The results given as % VOC in the front tube are gathered in Table 1 and the absolute values are given in Table 2.


image file: c9ra04490f-s2.tif
Scheme 2 Schematic representation of the sorbent tubes and magnetite supported organic–inorganic hybrids studied in this work.

image file: c9ra04490f-f5.tif
Fig. 5 Schematic representation of the tubes connected in series. The quantitative analysis of back tube allows to quantify the amount of VOC adsorbed in the front tube.
Table 2 Retention times (min), milligrams of injected VOC, milligrams of VOC in the back tube
VOC RT (min) Injected VOC (mg) VOC in back tubea (mg)
a Data from three independent experiments.b Calibration plots are not reproducible likely due to the low adsorption of this particular VOC.
4@1 13.7 1.226 0.502 ± 0.025
4@2 13.7 1.226 0.441 ± 0.023
4@3 13.7 1.226 0.429 ± 0.020
5@1 17.5 1.214 0.461 ± 0.023
5@2 17.5 1.214 0.387 ± 0.020
5@3 17.5 1.214 0.290 ± 0.014
6@1 20.7 1.212 0.379 ± 0.019
6@2 20.7 1.212 0.315 ± 0.016
6@3 20.7 1.212 0.303 ± 0.015
7@1 23.7 1.207 0.362 ± 0.018
7@2 23.7 1.207 0.265 ± 0.013
7@3 23.7 1.207 0.277 ± 0.013
8@1 26.8 0.120 0.349 ± 0.017
8@2 26.8 0.120 0.241 ± 0.012
8@3 26.8 0.120 0.134 ± 0.007
9@1 9.7 0.130 b
9@2 9.7 0.130 b
9@3 9.7 0.130 b
10@1 12.2 0.126 0.416 ± 0.021
10@2 12.2 0.126 0.391 ± 0.019
10@3 12.2 0.126 0.467 ± 0.023
11@1 15.5 0.124 0.369 ± 0.018
11@2 15.5 0.124 0.311 ± 0.015
11@3 15.5 0.124 0.219 ± 0.011
12@1 18.7 0.123 0.309 ± 0.015
12@2 18.7 0.123 0.235 ± 0.012
12@3 18.7 0.123 0.173 ± 0.009


It is worth mentioning the same experiments and same protocol were carried out using the sorbent tubes packed with the non-functionalized magnetic nanoparticles, that is without the PMDI/NDI/PDI unit. As expected, the adsorption capability of the magnetic nanoparticles decreased drastically, ranging from 40 to 60% of adsorption reduction. More importantly, no significant differences for the adsorption capacity of the magnetic NP for the different aromatic VOCs were observed, thus evidencing the important and differential feature of the π-acidic surfaces in the hybrid nanoparticles interacting with the VOCs. This result strongly agrees with the correlation found for the absorption of VOCs and the interaction energies. Moreover, several works devoted to molecular recognition based on PMDI/NDI/PDI receptors have also correlated the π-acidity of their aromatic surfaces with their ability to recognize a variety of electron rich guests.39

The comparison of the % VOC found in the front tube for the three different hybrid nanoparticles shows that the NDI can be a convenient aromatic receptor for the construction of adsorption tubes since it is more economic and easier to use compared to PDI. In the case of the simplest PMDI, the percentage of adsorption is reduced in almost the 20% for some VOCs (for instance butylbenzene) and consequently its utilization for the construction of sorbent tubes is not recommended.

Conclusions

In conclusion, the capability of functionalized Fe3O4 magnetic nanoparticles to adsorb aromatic and aliphatic VOCs have been demonstrated in this work. Three different aromatic surfaces (PMDI, NDI and PDI) have been used to decorate the nanoparticles and analyze how the adsorption capacity is affected. DFT-D3 calculations were also performed that evidenced a strong correlation between the adsorption capacity of the magnetite supported organic–inorganic hybrids and the interaction energies of the π-stacked complexes, which strongly supports the binding mechanism.

This investigation also demonstrates that the NDI is a good candidate to construct hybrid materials to be used for the construction of sorbent tubes and utilized for the quantification of aromatic and aliphatic VOCs. Quite remarkably, these sorbent tubes can be desorbed and reused more than 200 times without losing their properties. The utilization of mixtures of the three hybrid nanoparticles is under investigation to analyze possible synergetic effects.

Conflicts of interest

There are no conflicts to declare.

Acknowledgements

The MINECO/AEI of Spain (project CTQ2017-85821-R, FEDER funds) is acknowledge for financial support and the CTI (UIB) for computational facilities. The SCT (UIB) is also acknowledged for their support in the utilization of the instrumentation used herein. M. S. Gutiérrez acknowledges her PhD scholarship from CONACyT (Consejo Nacional de Ciencia y Tecnología de México), P. Duel acknowledges his PhD scholarship from GOIB (Govern de les Illes Balears).

Notes and references

  1. C. Turner, VOC Analysis by IFT-MS, GC-MS, and Electronic Nose for Diagnosing and Monitoring Disease, in Volatile Biomarkers, ed. A. Amann and D. Smith, Elsevier, 2013, ch. 18, pp. 343–357 Search PubMed.
  2. D. James, S. M. Scott, A. Zulfiqur and W. T. O'Hare, Microchim. Acta, 2005, 149, 1–17 CrossRef CAS.
  3. (a) A. Bieganowski, G. Jozefaciuk, L. Bandura, L. Guz, G. Lagod and W. Franus, Sensors, 2018, 18, E2463 CrossRef PubMed; (b) L. Guz, G. Lagod, K. Jaromin-Glen, Z. Suchorab, H. Sobczuk and A. Bieganowski, Sensors, 2015, 15, 1–21 CrossRef CAS PubMed.
  4. H. Zhou, D. Luo, H. Gholam Hosseini, Z. Li and J. He, Sensors, 2017, 17, E1073 CrossRef PubMed.
  5. H. K. Patel, The electronic nose: Artificial olfaction technology (Biological and medical physics, Biomedical Engineering), New Delhi, India, Springer, 2014 Search PubMed.
  6. (a) F. Ayari, E. Mirzaee-Ghaleh, H. Rabbani and K. Heidarbeigi, Int. J. Food Prop., 2018, 21, 1670–1679 CrossRef CAS; (b) X. Zhang, Z. Cheng, L. Ma and J. Li, Food Chem., 2017, 227, 55–63 CrossRef CAS PubMed.
  7. (a) J. Gebicki and B. Szulczynski, Measurement, 2018, 116, 307–313 CrossRef; (b) E. Kaminski, L. M. Libbey, S. Stawicki and E. Wasowicz, Appl. Microbiol., 1972, 24, 721–726 CAS.
  8. (a) H. Jelen and E. Wasowicz, Food Rev. Int., 1998, 14, 391–426 CrossRef CAS; (b) R. Rusinek, M. Gancarz, M. Krekora and A. Nawrocka, J. Food Sci., 2019, 84, 51–58 CrossRef CAS PubMed.
  9. (a) X. Zheng, Z. Yan, P. Liu, J. Fan, S. Wang, P. Wang and T. Zhang, Bull. Environ. Contam. Toxicol., 2019, 102, 731–740 CrossRef CAS PubMed; (b) M. Sarker, B. M. Bhadra, P. W. Seo and S. H. Jhung, J. Hazard. Mater., 2017, 324, 131–138 CrossRef CAS PubMed.
  10. M. Yasukawa, S. Mishima, M. Shibuya, D. Saeki, T. Takahashi, T. Miyoshi and H. Matsuyama, J. Membr. Sci., 2015, 487, 51–59 CrossRef CAS.
  11. (a) M. Shestakova and M. Sillanpää, Chemosphere, 2013, 93, 1258–1267 CrossRef CAS PubMed; (b) M. Yang, X. Zhang, Q. Liang and B. Yang, Water Res., 2019, 158, 322–337 CrossRef CAS PubMed.
  12. (a) P. S. Thorne, Environ. Health Perspect., 2007, 115, 296–297 CrossRef CAS PubMed; (b) E. S. Snow, F. K. Perkins, E. J. Houser, S. C. Badescu and T. L. Reinecke, Science, 2005, 307, 1942–1945 CrossRef CAS PubMed.
  13. (a) Y. Guo, C. Holton, H. Luo, P. Dahlen and P. C. Johnson, Groundwater Monit. Rem., 2019, 39, 43–52 CrossRef CAS; (b) I. Azzouz, Y. G. Habba, M. Capochichi-Gnambodoe, F. Marty, J. Vial, Y. Leprince-Wang and T. Bourouina, Microsyst. Nanoeng., 2018, 4, 17093 CrossRef CAS.
  14. A. Ribes, G. Carrera, E. Gallego, X. Roca, M. J. Berenguer and X. Guardino, J. Chromatogr. A, 2007, 1140, 44–55 CrossRef CAS PubMed.
  15. G. Churkina, F. Kuik, B. Bonn, A. Lauer, R. Grote, K. Tomiak and T. M. Butler, Environ. Sci. Technol., 2017, 51, 6120–6130 CrossRef CAS PubMed.
  16. M. Gancarz, A. Nawrocka and R. Rusinek, J. Food Sci., 2019 DOI:10.1111/1750-3841.14701.
  17. A. Szczurek, B. Krawczyk and M. Maciejewska, Chemom. Intell. Lab. Syst., 2013, 125, 1–10 CrossRef CAS.
  18. (a) M. Gancarz, J. Wawrzyniak, M. Gawrysiak-Witulska, D. Wiacek, A. Nawrocka and R. Rusinek, Int. Agrophys., 2017, 31, 317–325 CAS; (b) A. Kubiak, T. Wenzl and F. Ulberth, J. Sci. Food Agric., 2012, 92, 2200–2206 CrossRef CAS PubMed.
  19. B. Bonn, J. Kreuzwieser, F. Sander, R. Yousefpour, T. Baggio and O. Adewale, Climate, 2017, 5, 78 CrossRef.
  20. (a) J. Miao, C. Chen, L. Meng and Y. S. Lin, ACS Sens., 2019, 4, 1279–1290 CrossRef CAS PubMed; (b) A. H. Jalal, F. Alam, S. Roychoudhury, Y. Umasankar, N. Pala and S. Bhansali, ACS Sens., 2018, 3, 1246–1263 CrossRef CAS PubMed; (c) B. Liu, W. Zhao, Q. Jiang, Z. Ao and T. An, Sustainable Mater. Technol., 2019, 21, e00103 CrossRef CAS.
  21. (a) Y. Paska and H. Haick, ACS Appl. Mater. Interfaces, 2012, 4, 2604–2617 CrossRef CAS PubMed; (b) A. H. Jalal, Y. Umasankar, P. J. Gonzalez, A. Alfonso and S. Bhansali, Biosens. Bioelectron., 2017, 87, 522–530 CrossRef CAS PubMed; (c) A. Romain, J. Nicolas, M. Pardo and G. Sberveglieri, AIP Conf. Proc., 2009, 1137, 443 CrossRef CAS.
  22. J. Dieffenderfer, H. Goodell, S. Mills, M. McKnight, S. Yao, F. Lin, E. Beppler, B. Bent, B. Lee, V. Misra, Y. Zhu, O. Oralkan, J. Strohmaier, J. Muth, D. Peden and A. Bozkurt, IEEE J. Biomed. Health. Inf., 2016, 20, 1251–1264 Search PubMed.
  23. S. Yao, P. Swetha and Y. Zhu, Adv. Healthcare Mater., 2018, 7, 1700889 CrossRef CAS PubMed.
  24. (a) R. A. Kadir, R. A. Rani, A. S. Zoolfakar, J. Z. Ou, M. Shafiei, W. Wlodarski and K. Kalantar-zadeh, Sens. Actuators, B, 2014, 202, 74–82 CrossRef; (b) H.-J. Kim and J.-H. Lee, Sens. Actuators, B, 2014, 192, 607–627 CrossRef CAS; (c) J. Devkota, P. R. Ohodnicki and D. W. Greve, Sensors, 2017, 17, 801 CrossRef PubMed; (d) V. Semwal, A. M. Shrivastav, R. Verma and B. D. Gupta, Sens. Actuators, B, 2016, 230, 485–492 CrossRef CAS; (e) A. H. Jalal, Y. Umasankar and S. Bhansali, ECS Trans., 2016, 72, 25–31 CrossRef CAS.
  25. (a) A. H. Jalal, F. Alam, S. Roychoudhury, Y. Umasankar, N. Pala and S. Bhansali, ACS Sens., 2018, 37, 1246–1263 CrossRef PubMed; (b) N.-H. Kim, S.-J. Choi, D.-J. Yang, J. Bae, J. Park and I.-D. Kim, Sens. Actuators, B, 2014, 193, 574–581 CrossRef CAS.
  26. R. Vishinkin and H. Haick, Small, 2015, 11, 6142–6164 CrossRef CAS PubMed.
  27. Y. Y. Broza and H. Haick, Nanomedicine, 2013, 8, 785–806 CrossRef CAS PubMed.
  28. B. Li, G. Sauvé, M. C. Iovu, M. Jeffries-EL, R. Zhang, J. Cooper, S. Santhanam, L. Schultz, J. C. Revelli, A. G. Kusne, T. Kowalewski, J. L. Snyder, L. E. Weiss, G. K. Fedder, R. D. McCullough and D. N. Lambeth, Nano Lett., 2006, 6, 1598–1602 CrossRef CAS PubMed.
  29. K. A. López, M. N. Piña, D. Quiñonero, P. Ballester and J. Morey, J. Mater. Chem. A, 2014, 2, 8796–8803 RSC.
  30. M. Mohammadikish and H. Hashemi, J. Mater. Sci., 2019, 54, 6164–6173 CrossRef CAS.
  31. M. N. Pina, P. Rodriguez, M. N. Gutierrez, D. Quiñonero, J. Morey and A. Frontera, Chem.–Eur. J., 2018, 24, 12820–12826 CrossRef PubMed.
  32. M. S. Gutiérrez, P. Duel, F. Hierro, J. Morey and M. N. Piña, Small, 2018, 14, 1702573 CrossRef PubMed.
  33. D. Singh and J. B. Baruah, Cryst. Growth Des., 2011, 11, 768–777 CrossRef CAS.
  34. J. K. Nath and J. B. Baruah, CrystEngComm, 2015, 17, 8575–8595 RSC.
  35. S. Grimme, J. Antony, S. Ehrlich and H. Krieg, J. Chem. Phys., 2010, 132, 154104–154119 CrossRef PubMed.
  36. (a) M. Kazmi, A. Ibrar, H. S. Ali, M. Ghufran, A. Wadood, U. Flörke, J. Simpson, A. Saeed, A. Frontera and I. Khan, J. Mol. Struct., 2019, 1197, 458–470 CrossRef CAS; (b) A. Gogoi, A. Das, A. Frontera, A. K. Verma and M. K. Bhattacharyya, Inorg. Chim. Acta, 2019, 493, 1–13 CrossRef CAS; (c) S. Ganguly, A. Bauza, A. Frontera and A. Ghosh, Inorg. Chim. Acta, 2019, 492, 142–149 CrossRef CAS; (d) D. Dutta, S. M. Nashre-ul-Islam, U. Saha, A. Frontera and M. K. Bhattacharyya, J. Mol. Struct., 2019, 1195, 733–743 CrossRef CAS; (e) G. Mahmoudi, S. K. Seth, F. I. Zubkov, E. López-Torres, A. Bacchi, V. Stilinović and A. Frontera, Crystals, 2019, 9, 323 CrossRef; (f) R. Pons, C. Ibáñez, A. B. Buades, A. Franconetti, A. Garcia-Raso, J. J. Fiol, A. Terrón, E. Molins and A. Frontera, Appl. Organomet. Chem., 2019, 33, e4906 CrossRef; (g) M. Kumar, L.-H. Wu, M. Kariem, A. Franconetti, H. N. Sheikh, S.-J. Liu, S. C. Sahoo and A. Frontera, Inorg. Chem., 2019, 58, 127760–127774 Search PubMed.
  37. R. Ahlrichs, M. Bär, M. Hacer, H. Horn and C. Kömel, Chem. Phys. Lett., 1989, 162, 165–169 CrossRef CAS.
  38. M. S. Gutiérrez, M. N. Piña and J. Morey, RSC Adv., 2017, 7, 19385–19390 RSC.
  39. (a) C. Wang, F. N. Miros, J. Mareda, N. Sakai and S. Matile, Angew. Chem., Int. Ed., 2016, 55, 14422–14426 CrossRef CAS PubMed; (b) Y. Zhao, N. Sakai and S. Matile, Nat. Commun, 2014, 5, 3911 CrossRef CAS PubMed; (c) Y. Zhao, Y. Domoto, E. Orentas, C. Beuchat, D. Emery, J. Mareda, N. Sakai and S. Matile, Angew. Chem., Int. Ed., 2013, 52, 9940–9943 CrossRef CAS PubMed; (d) N.-T. Lin, A. Vargas Jentzsch, L. Guenee, J.-M. Neudoerfl, S. Aziz, A. Berkessel, E. Orentas, N. Sakai and S. Matile, Chem. Sci., 2012, 3, 1121–1127 RSC.

Footnote

Electronic supplementary information (ESI) available: SEM micrographic images, DLS size distribution and zeta potential of all hybrid nanoparticles used in this work. 1H-NMR and 13C-NMR spectra of the imide-dopamine compounds and IR spectra of all compounds used in this manuscript. See DOI: 10.1039/c9ra04490f

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