Xiaolong Yu,
Xiaoyan Yuan,
Yunhui Zhao and
Lixia Ren*
School of Materials Science and Engineering, Tianjin University, No. 92 Weijin Road, Tianjin 300072, China. E-mail: lxren@tju.edu.cn; Fax: +86-22-27403233; Tel: +86-22-27403233
First published on 19th October 2015
Paramagnetic polymers based on PEI have been synthesized and characterized. Studies on the structure and property relationship showed that the magnetic property was affected by the molecular weight, ferric content and linear or branched structures of the resultant magnetic PEIs. Interestingly, the magnetic susceptibility had a linear relationship to the ferric content. The resultant polymers showed a magnetic response to an external magnetic field, and have great potential in magnetic separation, magnetic switching as well as controlled delivery.
Recently, paramagnetic ionic liquid containing tetrahalogen iron(III) anion, such as tetrachloroferrate (FeCl4−), was obtained by Hayashi and Hamaguchi through mixing quaternized ammonium salt with iron(III) halide.20 The paramagnetic ionic liquid showed magnetic response which has potential in magnetic control and separation.21,22 Furthermore, paramagnetic poly(ionic liquid) containing FeCl4− and tetrabromoferrate (FeBr4−) was synthesized and used as catalyst for Friedel–Crafts alkylation reactions by Döbbelin et al. in 2011.23 The pyridine based magnetic block copolymer was prepared via post-modification of pyridine with FeCl4−, and the nanostructured magnetic thermoset material was obtained by blending such magnetic block copolymer with epoxy resin.24
Since quaternized nitrogen cation could be complexed with iron(III) halide, polymers with quaternizable nitrogen have the potential to become (para)magnetic materials. Polyethyleneimine (PEI), known as the polymer with the most abundant amino groups and the highest cationic-charge-density potential, could be the best candidate for preparing magnetic polymers. What's even better, PEI has attracted tremendous attention of researchers due to its unique physical and chemical properties. Boussif et al.25 reported that PEI could function as a highly efficient vector for delivering oligonucleotides and plasmids both in vitro and in vivo, and hence could be an outstanding core for carriers in gene therapy. And PEI became the second polymer gene transfection reagent after poly-L-lysine.26 Beyth et al. immobilized cross-linked quaternary ammonium PEI in medical composite resin and the antibacterial activities of such compound was studied.27,28 Hu et al. grafted PEI to single-walled carbon nanotube, which was used as a substrate for cultured neurons and found that it promoted neurite outgrowth and branching.29 By impregnating PEI in a series of mesoporous silica materials, Son et al. improved its CO2 adsorption property and discovered that the CO2 adsorbing performance of these materials was influenced primarily by their pore size.30 Vinogradov et al. employed PEI as a structure-directing agent to obtain organized mesoporous CuO–Al2O3 composite.31 Although many impressive works have been done in the field of PEI related applications, to our best knowledge, the PEI related magnetic polymer is barely reported.
Magnetism is very helpful in magnetic control, especially in separation, recycling of catalyst or agent via external magnetic field. Bringing in magnetism seems promising to obtain multifunctional materials. Since every third atom of PEI is a quaternizable nitrogen, it is feasible to prepare PEI based magnetic polymers through quaternization and iron halides complexation. Meanwhile, due to the high nitrogen density, PEI based magnetic polymers could display good paramagnetic property. Furthermore, PEI is commercially available and low-cost, which makes it possible for preparation of PEI based magnetic polymers in big scale. In this work, PEI based magnetic polymers were prepared via quaternization, ion exchange and FeCl3 complexation. In attempt to obtain optimum paramagnetic property, molecular weight, linear or branched chain structures as well as FeCl4− (ferric) content were discussed in detail.
:
N+ of ca. 1
:
1, and the FeCl3 solution was added into QPEI solution and stirred at 50 °C for 16 h. The resultant mixture was evaporated and redissolved in acetonitrile followed by precipitation in excessive amount of diethyl ether for three times. Brown colored solid product was obtained through centrifuge and followed by vacuum drying. Yield: 98%. All other groups of MPEI was synthesized likewise. All experiments were reproducible.
000 Oe to 10
000 Oe at 298 K. Thermogravimetric analysis (TGA) was conducted on a Pyris 1 TGA (Perkin-Elmer System), ramping from 25 °C to 1000 °C at a rate of 20 °C min−1 under the protection of nitrogen.
The QPEIs were studied via 1H-NMR. As shown in Fig. S1,† compared with original PEI, the signals assigned for QPEIs were shifted to a lower field because of the electron withdrawing effect of nitrenium ion in quaternized ammonium unit. And, with increasing of quaternization percent (Pq), the signals down shifted a lot. However, it is difficult to calculate the Pq from 1H-NMR. Pq of the QPEIs was calculated from elemental analysis (EA) by comparing the molar ratio of C/N according to eqn (1).
| Pq = (r − m)/(M − m) × 100% | (1) |
Detailed characterization of QPEIs was shown in Table 1. For PEIs with the molecular weight of 10k, by changing the reaction time from 1 h to 100 h, the Pq can be controlled from 26% to 84% gradually, thus the QPEIs with gradient Pq were prepared. And, QPEIs with different molecular weight of linear PEI, branched PEI while maintain the similar Pq of ca. 60% were synthesized successfully.
| Code | Mna [×103] | Timeb [h] | C/Nc | Pqd [%] |
|---|---|---|---|---|
| a Molecular weight of purchased PEI.b Reaction time for quaternization.c C/N molar ratio obtained from elemental analysis.d Quaternization percent calculated from EA analysis.e Quaternized QPEI based on linear PEI.f Quaternized QPEI based on branched PEI. | ||||
| QPEI1e | 10 | 1 | 2.52 | 26 |
| QPEI2e | 10 | 3 | 2.77 | 38 |
| QPEI3e | 10 | 10 | 3.07 | 53 |
| QPEI4e | 10 | 60 | 3.25 | 63 |
| QPEI5e | 10 | 100 | 3.71 | 84 |
| QPEI6e | 1.8 | 48 | 3.18 | 63 |
| QPEI7e | 0.6 | 48 | 3.31 | 66 |
| QPEI8f | 10 | 60 | 3.19 | 60 |
The corresponding MPEIs were obtained by complexing QPEIs with FeCl3 at the conversion of ca. 100% via the similar procedures reported.32 Since the unreacted FeCl3 is soluble in diethyl ether, and the product can be purified by precipitating in diethyl ether for several times. Those MPEIs with linear and branched chain structure, different molecule weight (0.6k, 1.8k, 10k) and different ferric content were also synthesized following the similar procedures. Due to the paramagnetic property of FeCl4− anion, the MPEIs can not be characterized by 1H-NMR. However, according to literature, Raman spectrometer at 300 K was used to examine the presence of FeCl4− anion in the magnetic polymers.20 As shown in Fig. 1, all of the MPEIs showed signals at 341 cm−1, which represents the Cl–Fe–Cl vibration in FeCl4− anion and demonstrates the successfully complex of FeCl4− to QPEI. The broadness of the signal in MPEI1 might be related to the low Pq of FeCl4−. Table 2 shows the characterization of MPEIs, by controlling the Pq of QPEIs, the ferric content (CFe) of MPEIs could be tuned to study the effect of ferric content on the magnetism.
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| Fig. 1 Raman spectra of PEI based magnetic polymers. Code MPEI1–MPEI8 was corresponded to code MPEI1–MPEI8 in Table 2. | ||
| Code | Mna [×103] | CFeb [wt%] | Susceptibility [×10−6 emu g−1] |
|---|---|---|---|
| a Molecular weight of purchased PEI.b Ferric content of MPEIs, that is the weight percent of Fe element in MPEI.c MPEI based on linear PEI.d MPEI based on branched PEI. | |||
| MPEI1c | 10 | 14 | 10.7 |
| MPEI2c | 10 | 16 | 20.6 |
| MPEI3c | 10 | 18 | 29.9 |
| MPEI4c | 10 | 19 | 36.3 |
| MPEI5c | 10 | 20 | 41.6 |
| MPEI6c | 1.8 | 19 | 36.4 |
| MPEI7c | 0.6 | 19 | 33.6 |
| MPEI8d | 10 | 19 | 27.9 |
All the synthesized MPEIs showed magnetic response to neodymium magnet. Take MPEI1 as example, the MPEI1 particle was moved under the direction of neodymium magnet in ethanol since MPEI is not soluble in ethanol (Fig. 2). Furthermore, a video of MPEI1 particles moved under the attraction of neodymium magnet was supplied in ESI† to illustrate the magnetic response of the resultant MPEIs at room temperature in detail. The MPEI “walked” under the attraction of neodymium magnet directly, and fell down to the bottom under the force of gravity when withdraw the magnet. Such polymers have great potential in magnetic switching, magnetic separation, magnetic control as well as controlled release.
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| Fig. 2 Magnetic response of MPEI1 polymer in ethanol solution under the attraction of neodymium magnet. | ||
For further study of the synthesized MPEIs, the magnetic properties of MPEI were also examined using the SQUID method. The results were shown in Fig. 3 and Fig. 4. For all MEPIs with different molecular weight, ferric content and linear or branched structures, linear relationship between magnetic moment and magnetic field was observed, which showed a paramagnetic behavior for such MPEI polymers. The magnetic susceptibility of MPEIs was summarized in Table 2. For linear MPEIs at the PEI molecular weight of 10k, the magnetic susceptibility increased with increasing of CFe, as the ferric content changed from 14% to 20%, the susceptibility increased from 10.7 × 10−6 emu g−1 to 41.6 × 10−6 emu g−1 correspondingly. A positively correlated relationship between CFe and susceptibility of linear 10k PEI based MPEIs at 300 K was founded (inset in Fig. 3). The susceptibility of MPEIs increased linearly with the increasing of ferric content. This is probably because that MPEIs with higher ferric content had a larger magnetic unit density which led to higher magnetic susceptibility value under an applied external magnetic field. It seems that with a higher ferric content, the susceptibility should be higher. And by controlling the ferric content, the magnetic susceptibility could be tuned easily. However, for MPEIs based on QPEI, the maximum ferric content at Pq of 100% is just 21%. From this aspect, the polymers with higher weight percent of quaternized nitrogen should be a better candidate in design and synthesis of magnetic polymers.
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| Fig. 3 SQUID magnetization of magnetic polymers based on linear 10k PEI at 300 K. Code MPEI1–MPEI5 was corresponded to those in Table 2. | ||
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| Fig. 4 SQUID magnetization of magnetic polymers with different molecular weight and chain structure at 300 K. Code MPEI4–MPEI8 was corresponded to those in Table 2. | ||
Fig. 4 shows the relationship between magnetic moment and susceptibility for MPEIs with different PEI molecular weight (linear 0.6k, 1.8k, 10k and branched PEI) at similar quaternization percent (ca. 60%). The linear MPEIs showed similar paramagnetic property with very close magnetic susceptibility value (Table 2), which suggested that the molecular weight has less effect on the magnetic susceptibility. The magnetic susceptibility of branched MPEI (μ = 27.9 × 10−6 emu g−1) was smaller than those of linear MPEIs with similar ferric content, which is probably because branched structure is not avail to forming ordered arrangement of the polymer chain and magnet unit FeCl4− and thus decrease the magnetic susceptibility.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c5ra18175e |
| This journal is © The Royal Society of Chemistry 2015 |