Kai Jiang,
Teng Fei* and
Tong Zhang*
State Key Laboratory on Integrated Optoelectronics, College of Electronic Science and Engineering, Jilin University, Changchun 130012, PR China. E-mail: zhangtong@jlu.edu.cn; feiteng@jlu.edu.cn; Fax: +86 431 85168270; Tel: +86 431 85168385
First published on 5th September 2014
A crosslinked polyelectrolyte was synthesized by reaction of lithium benzene-1,3,5-tris(olate) and terephthalic aldehyde using a one-step hydrothermal process. The structure and morphology of the resultant polymer poly(lithium benzene-1,3,5-tris(olate)) (PLBTO) were investigated by Fourier transform infrared spectrum (FTIR), thermal gravimetric analysis (TGA), scanning electron microscopy (SEM) and transmission electron microscopy (TEM). A humidity sensor based on PLBTO was fabricated and humidity sensitive properties were explored. The impedance of PLBTO sensor changed four orders of magnitude with a good linearity over a relative humidity (RH) range from 33% to 95%. The conductive mechanism of the sensor was discussed based on complex impedance plots. The results indicate the quantity of adsorption water molecules would determine the category of conductive particles, and cause the impedance change under different RH. Moreover, the PLBTO sensor showed little hysteresis, rapid response/recovery and good long-term stability, which have benefited from the crosslinked structure of PLBTO.
In this report, Friedel–Crafts alkylation has been put forward to synthesize the crosslinked polyelectrolyte by a one-step hydrothermal process. Terephthalic aldehyde acts as an external cross-linker to polymerize with the monomer lithium benzene-1,3,5-tris(olate) to obtain the crosslinked polyelectrolyte with a clear structural formula. This method can effectively overcome the shortcoming of crosslinked polyelectrolytes mentioned above. The resultant polyelectrolyte was used as a humidity sensitive material to fabricate a humidity sensor. The obtained sensor showed good linearity, little hysteresis, long-term stability and rapid response/recovery. In order to research the sensing mechanism, the complex impedance plots were explored.
The characteristic curves of humidity sensitivity were measured on a ZL-5 model LCR analyzer (Shanghai, China). The data were collected by a computer automatically through an IEEE-488 GPIB Bus (82350A GPIB, Agilent, America). Special application software was developed using the LabVIEW program development environment (Version 7.1) to govern the work of the whole system. The voltage applied in our studies was AC 1 V, and the frequency varied from 20 Hz to 100 kHz. The measuring temperature was controlled at 20 °C by air-conditioner. The atmospheres of different RH were produced by different saturated salt solutions in several chambers. Their equilibrium states stood for 33% RH (MgCl2), 54% RH (Mg(NO3)2), 75% RH (NaCl), 85% RH (KCl) and 95% RH (KNO3) at 20 °C, respectively. The uncertainty of the RH values was about ± 1%.21 The measurement system of humidity sensor is shown in Fig. 1.
Thermal stability of PLBTO is investigated by TGA as shown in Fig. 2. The TGA trace shows that PLBTO is stable by heating under N2 until 300 °C, and it retains more than 65% of its mass at 600 °C. Mass loss nearly 2% up to 150 °C owes to residual solvents (dioxane, THF, and H2O), which have not been removed during the drying procedure.
The FTIR spectra of 1,3,5-trihydroxybenzene, LBTO and PLBTO are shown in Fig. 3. The FTIR spectrum of 1,3,5-trihydroxybenzene (Fig. 3(a)) shows strong vibrational peaks at 3200, 1310 and 1162 cm−1, which illustrate the stretching of phenolic hydroxyl group. These peaks disappear in Fig. 3(b), and the new absorption peak at 864 cm−1 corresponds to the stretching of O–Li bond, which indicates hydroxyl groups were thoroughly converted.22 Seen from Fig. 3(c), the absorption peak at 2920 cm−1 is assigned to the stretching of alkyl, which indicates that LBTO is reacted with terephthalic aldehyde by elimination of water molecules. The stretching of aromatic CC shows strong vibrational peaks at 1582 and 1422 cm−1. The absorption peak at 1014 cm−1 comes from the stretching of C–O bond. The absorption peak at 864 cm−1 demonstrates the stretching of O–Li bond. The absorption peaks at 822, 759 and 533 cm−1 correspond to the stretching of C–H bond in the benzene ring. Above results demonstrate the desired PLBTO is successfully prepared.
The morphology of PLBTO film is examined with SEM as shown in Fig. 4(a). As can be seen, PLBTO film is stacked by irregular submicron particles, which is different from the reported polyelectrolytes.16 In the literature, the surface of crosslinked copolymer looks like a membranous porous structure in accordance with mostly polymers. Fig. 4(b) is the TEM image of PLBTO film. It can be seen clearly that abundant pores exist in PLBTO film probably resulting from accumulation of nanoparticles and crosslinked structure of the polyelectrolyte, which may allow free passages of water molecules.
The humidity sensor based on PLBTO is fabricated and the impedance of PLBTO sensor is measured at AC 1 V from 33% to 95% RH. In order to research the influence of working frequency on humidity sensing property of PLBTO sensor, the impedance as a function of RH is measured at different frequencies as shown in Fig. 5. The impedance of PLBTO sensor decreases remarkably with raising frequency at low RH (33%) and the difference of impedance between adjacent two curves becomes gradually smaller as RH increased. The impedance versus RH curve shows a good linearity at 100 Hz, and the impedance changes four orders of magnitude from 33% to 95% RH.
In order to further research humidity sensing properties of PLBTO films, the sensitive mechanism of PLBTO sensor is researched by complex impedance plots (CIP). CIP are measured from 20 Hz to 100 kHz at different RH as shown in Fig. 6. ReZ and −ImZ, which stand for the real and imaginary parts of the CIP, are the horizontal axis and vertical axis, respectively. Table 1 shows equivalent circuits (EC) and main conductive particles (MCP) for various RH. At low RH (33%), the CIP is an arc with large curvature radius, which looks like a straight line, and the EC can be displayed by a constant phase element (CPE).23 At this point, a few water molecules are adsorbed on the surface of PLBTO films, and the MCP are protons (H+), which migrated by hopping from site to site across the surface of film leading to comparatively high impedance.24 When the RH increases to 54%, a semicircle is observed from CIP proving EC comprised of parallel resistor (Rf) and capacitor (Cf).25 More water molecules are adsorbed, synchronously, and H+ combines with H2O to form H3O+. According to the ion transfer mechanism of Grotthuss,26 H2O + H3O+ → H3O+ + H2O, the initial and final states are the same. The energy is also equivalent, so that the easy transfer of H3O+ leads to the quick decrease of impedance. As the RH further increased to 75%, CIP consists of the most part of semicircle at the high frequency range and a short line at the low frequency range. The short line represents Warburg impedance (Zw), which is caused by the diffusion process of ions or charge carriers at the interface between sensing film and electrode.27 In this process, several serial water layers form, which make a contribution to ionization of Li+. The dissociated Li+ can contribute to conduction along with H+ and H3O+. CIP at 85% RH is also comprised of the part of semicircle and a short line (not shown here), which is similar with 75% RH. With the RH increasing to 95%, the semicircle disappears and only a line remains in CIP. Due to a great quantity of ionization of Li+, the impedance of sensor was dominated by Zw, hence film resistance can ignore.23 Moreover, film conduction mainly comes from Li+ resulted in a sharp decrease of impedance of the sensor with four orders of magnitude compared to the initial impedance.
There are some other important humidity properties such as humidity hysteresis, response/recovery time and long-time stability for humidity sensor. Humidity hysteresis, defined as the maximum difference of humidity sensor between the adsorption and desorption process, is generally used to estimate the reliability of humidity sensors.28 The humidity hysteresis plots of PLBTO sensor are shown in Fig. 7. As can be seen, the maximum hysteresis is about 4% RH at the range of 33% to 95% RH, indicating a good reliability of the humidity sensor.
Fig. 8 displays response and recovery curves of PLBTO sensor. The measurements are repeated for four cycles, and the result demonstrates good repeatability of the sensor. The time taken by a sensor to achieve 90% of the total impedance change is defined as the response or recovery time.29 The response time is about 10 s when RH ranged from 33% to 95%, and the recovery time is about 19 s when RH decreased from 95% to 33% RH. The rapid response and recovery is related to the crosslinking structure of PLBTO. Water molecules are adsorbed on the surface of films by chemisorption and physisorption.30 At low RH, the chemisorption takes place firstly then physisorption follows. Lithium ions at the surface of film combine with OH− ionized by water molecules to form the chemisorbed water layer, and the chemisorbed water layer makes a contribution to forming physisorption water layer by hydrogen bonds as shown in Fig. 9. The physisorption water layers grow with the RH increasing. The adsorption/desorption rate at physisorption water layers directly influences the response/recovery time. The crosslinking structure of PLBTO is beneficial for the transportation of water molecules, hence PLBTO sensor has a fast response and recovery.
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Fig. 9 The schematic diagram of the physisorption and chemisorption of water molecules on the film surface. |
In order to research temperature dependence of PLBTO sensor, the impedances of PLBTO sensor are measured at different temperature (from 10 to 50 °C). As shown in Fig. 10, the impedances of PLBTO sensor show little change at low humidities (33 and 54% RH) with the increase of temperature. At high humidities (75, 85 and 95% RH), the impedances of PLBTO sensor decrease a little from 10 to 50 °C due to enhanced ionization of water molecules. The results demonstrate the humidity sensing property is affected by temperature variation, but the influence is limited.
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Fig. 10 The impedances of PLBTO sensor to the RH under different temperature (10, 20, 30, 40, 50 °C). |
In order to exam the long-time stability, PLBTO sensor was put into the glass container of 95% RH for repeated measurements every 5 days for 30 days. PLBTO sensor exhibits good high humidity stability and durability owing to slight variation in impedance with the passing of time as shown in Fig. 11. The results indicate that PLBTO sensor is promising for practical application.
This journal is © The Royal Society of Chemistry 2014 |