Ai-Ling
Chen
a,
Hai-Rong
Yu
a,
Xiao-Jie
Ju
a,
Rui
Xie
a,
Wei
Wang
a and
Liang-Yin
Chu
*ab
aSchool of Chemical Engineering, Sichuan University, Chengdu, Sichuan 610065, China. E-mail: chuly@scu.edu.cn; Fax: +86 28 8546 0682; Tel: +86 28 8546 0682
bState Key Laboratory of Polymer Materials Engineering, Collaborative Innovation Center for Biomaterials Science and Technology, Sichuan University, Chengdu, Sichuan 610065, China
First published on 30th May 2014
A simple and portable device equipped with poly(N-isopropylacrylamide-co-benzo-18-crown-6-acrylamide) (P(NIPAM-co-B18C6Am)) hydrogel is developed for visual detection of Pb2+ ions. The device consisted of a compartment for incorporating the hydrogel, a flow channel and an indicating liquid chamber with colored solution, and a dense and elastic polyethylene (PE) membrane to separate the hydrogel and the colored solution. The device works like a mercury thermometer, in which the P(NIPAM-co-B18C6Am) hydrogel and the PE membrane act as the Pb2+ sensor and actuator and the colored liquid column in the flow channel acts as the indicator. The volume of P(NIPAM-co-B18C6Am) hydrogel changes in response to Pb2+ concentration at a certain temperature due to the formation of B18C6Am/Pb2+ host–guest complexes, and the volume change of the hydrogel causes elastic deformation of the PE diaphragm, which pushes out the colored solution from the liquid chamber into the flow channel to form a liquid column. Therefore, the Pb2+ concentration can be detected quantitatively by simply and easily measuring of the liquid column length. The device shows excellent sensitivity towards Pb2+ ions. The detection performances of the proposed devices are satisfactorily stable and repeatable. This simple and portable device enables visual detection of Pb2+ concentration without the help of electrical amplification or spectroscopic measurements.
The chemical and biological sensors based on the stimuli-responsive hydrogels have attracted an extensive attention in the detection of lead ions. Up to now, hydrogel-based sensors have mostly focused on microcantilever sensors,13 crystalline colloidal array reflection,14–18 fluorescence,19,20 and so on.21,22 The key to microcantilever sensors is to coat the microcantilever with stimuli-responsive hydrogel. The microcantilever undergoes bending deflection upon exposure to solutions containing Pb2+ as the result of a swelling of the hydrogel, and thus the Pb2+ concentration can be detected by measuring the deflection of the microcantilever.13 However, microcantilever deflection is usually measured by the optical beam deflection method, which requires accurate and expensive instruments. Optical sensors such as polymerized crystalline colloidal arrays and hydrogel diffraction gratings also have some limitations. For example, the polymerized crystalline colloidal arrays attach recognition agents (crown ether, single-stranded adapter) to the hydrogel, which can capture Pb2+ ions to cause the hydrogel to swell or shrink.14–18 As a result it can actuate a lattice constant change that shifts the diffraction wavelength in proportion to Pb2+ concentration. As for hydrogel diffraction gratings, the detection of Pb2+ ions is carried out by monitoring the variation of diffraction efficiency of the gratings when exposed to Pb2+ solutions.22 Optical sensors need spectral analysis which should be carried out by using spectrometer and other precision instruments. Fluorescent sensors detect the target analytes by changing the fluorescence intensity.19 A hydrogel-based fluorescent sensor has been developed for visual detection of Pb2+ by immobilizing a DNA probe in the hydrogel, which shows a yellow-to-green fluorescence change in the presence of Pb2+.20 However, it is hard to accurately recognize the colour change by naked eyes. Moreover, DNA probe is difficult to be stored. Therefore, it is desired and necessary to develop a easy method for quantitative detection of lead without any help of electrical amplification or spectroscopic measurement.
Here, we report a simple and portable hydrogel-based device for visual detection of Pb2+. The structure construction and the Pb2+ detection mechanism of the proposed device is schematically illustrated in Fig. 1. The device consists of a block of poly(N-isopropylacrylamide-co-benzo-18-crown-6-acrylamide) (P(NIPAM-co-B18C6Am)) hydrogel, a upper poly(dimethylsiloxane) (PDMS) module, a lower PDMS module, and a dense and elastic polyethylene (PE) membrane to separate the upper and lower PDMS modules (Fig. 1a). The upper PDMS module is consisted of an indicating liquid chamber and a flow channel, and the lower PDMS module has a compartment for holding hydrogel and through-holes in the bottom of the module (Fig. 1a). The PDMS modules are fabricated by the well-known soft lithography method. A block of P(NIPAM-co-B18C6Am) hydrogel is cut and embedded into the compartment in a shrunken state at 65 °C. Then, the PDMS modules and PE membrane are assembled, and methylene blue solution is injected into the indicating liquid chamber (Fig. 1b, c, f and g). The through-holes in the bottom of the lower PDMS module are designed for intaking Pb2+ ions into the hydrogel (Fig. 1c). When crown ether units capture Pb2+ and form B18C6Am/Pb2+ host–guest complexes,23,24 the volume phase transition temperature (VPTT) of the P(NIPAM-co-B18C6Am) hydrogel can shift from a low temperature to a higher temperature due to the repulsion among charged complex groups and the enhancement of hydrophilicity of the hydrogel.25,26 When the ambient temperature is set at a certain temperature between the two VPTT values, the P(NIPAM-co-B18C6Am) hydrogel can change from a shrunk state to a swollen state in response to recognizing Pb2+. Compared with P(NIPAM-co-B18C6Am) linear copolymers26 or gating membranes with grafted P(NIPAM-co-B18C6Am) copolymers,27–29 the crosslinked P(NIPAM-co-B18C6Am) hydrogels provide better mechanical strength and flexibility for Pb2+ response and can be used as sensors and actuators by changing their volume, shape or mechanical properties.30 The volume change of the hydrogel can be transduced into the movement of the colored solution in the flow channel with the help of the elastic diaphragm.31,32 The volume change of the hydrogel causes elastic deformation of the PE diaphragm, which pushes out the colored solution from the liquid chamber into the flow channel to form liquid column (Fig. 1d and e). Thus, the Pb2+ concentration can be detected quantitatively by measuring the liquid column length. To verify the efficiency and performance repeatability of the proposed device, we first equip the device with a block of thermo-responsive poly(N-isopropylacrylamide) (PNIPAM) hydrogel, which is much more cheaper and easier to be fabricated than the P(NIPAM-co-B18C6Am) hydrogel and used to detect temperature. Then, the device is equipped with P(NIPAM-co-B18C6Am) hydrogel and used to detect the Pb2+ concentration. The detection performance of the device is satisfactorily stable and repeatable. The results verify that the proposed simple and portable device in this study is an efficient and reliable device for visual detection of Pb2+.
Then, a block of PNIPAM hydrogel is cut and embedded into the compartment in a shrunken state at 50 °C. The performance of the device is examined by immersing the lower PDMS device with PNIPAM hydrogel in deionized water at different temperatures. The PE membrane is deformed as the volume of hydrogel changes, which pushes out the colored solution from the chamber into the flow channel. The end of the flow channel is covered with a paraffin film to prevent the evaporation of the colored solution before the detection. Effects of hydrogel sizes on the changes in liquid column length (ΔL) are investigated. The liquid column length (ΔL) in the flow channel is measured with a calibrated scale by naked eyes. Three hydrogel sizes (10 × 5 × 1, 12 × 8 × 1 and 12 × 8× 2, unit: mm) are studied and the optimum size is chosen for subsequent experiments. To investigate the repeatability and stability of the change in the column length of colored solution, the ΔL values in deionized water at 25 °C (<VPTT) and 40 °C (>VPTT) are measured alternately and repeatedly. Furthermore, the same device is used to repeatedly measure the ΔL values at various desired ambient temperatures in the range from 20 to 40 °C. Finally, different devices of the same construction and the same dimension are prepared and used to examine the reproducibility of the proposed device.
K+ and Na+ are chosen as the reference ions to investigate the selectivity of the device to different cations. We test the device with different concentrations of Pb2+ in the presence of excess Na+ or K+ at 24 °C.
Fig. 3 shows the photographs of PNIPAM-hydrogel-based device in deionized water at different temperatures. The column length of the colored solution in the flow channel changes in response to the environmental temperature. A calibrated scale is fixed at the bottom of the device. The change in column length is obvious, which can be observed by naked eyes without any help of optical or electronic instruments.
Fig. 4 shows the reproducibility and performance stability of the PNIPAM-hydrogel-based device for detecting temperature. No matter how large the PNIPAM hydrogel in the device is, the temperature detection performance with the device is reproducible and stable (Fig. 4a). However, the larger the hydrogel size is, the more obvious the thermo-responsive change of the liquid column (ΔL). Therefore, the hydrogel size of 12 × 8 × 2 mm is chosen for the subsequent experiments. Fig. 4b shows the result of the temperature dependence of ΔL in the same device upon repeatedly heating up and cooling down the temperature of deionized water. The ΔL value reduces when environmental temperature increases from 20 to 40 °C and rises when environmental temperature decreases from 40 to 20 °C, and the four curves can overlap very well. Fig. 4c shows the temperature dependence of ΔL in two different devices with the same construction and the same dimension. The two curves also overlap with each other very well. In addition, the tendency of the temperature-dependent ΔL value agrees well with the thermo-responsive volume change behaviors of PNIPAM hydrogel shown in Fig. 2. The results confirm that the proposed device possesses a good reproducibility and performance stability.
Fig. 6 shows the detection performance of Pb2+ using the P(NIPAM-co-B18C6Am)-hydrogel-based device. Temperature dependence of change in the column length in Pb2+ solutions with different concentrations (ΔLPb2+) is shown in Fig. 6a. The tendency of the ΔLPb2+ curves agrees well with the Pb2+-responsive volume change behaviors of P(NIPAM-co-B18C6Am) hydrogel shown in Fig. 5. Fig. 6b shows a three-dimensional diagram of ΔLPb2+ as a function of both Pb2+ concentration and temperature, and Fig. 6c shows the corresponding contour diagram. With the contour diagram of ΔLPb2+ as a function of both Pb2+ concentration and temperature, the Pb2+ concentration can be conveniently and quickly determined if environmental temperature and the ΔLPb2+ have been measured.
Different ion solutions containing some obstructive ions (e.g., Na+, K+) are used to confirm the selectivity of the device to detect Pb2+. Fig. 6d shows the effect of interference ions on the change in the column length (ΔL) at 24 °C. Excess Na+ (40 mM) or K+ (40 mM) causes nearly no obvious change of the ΔL whether they are in the pure water or in the Pb2+ solutions with different ion concentrations. Due to the binding constant between Pb2+ and benzo-18-crown-6 (logK = 3.19 in water at 25 °C) is much higher than K+ (log
K = 1.74 in water at 25 °C) and Na+ (log
K = 1.38 in water at 25 °C),24 the benzo-18-crown-6 is highly selective to forming complexes with Pb2+. The results verify that the visual detection of Pb2+ by the device is not interfered by the presence of certain interference metal ions.
![]() | (1) |
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Fig. 7 Temperature dependence of change in the column length of the P(NIPAM-co-B18C6Am) hydrogel-based device in deionized water (ΔLw). (a) The indicating liquid column variation (ΔLw) as a function of temperature of deionized water. (b) Comparison of the calculated ΔLw value from eqn (1) and the experimental ΔLw value. |
A comparison of the calculated ΔLw value from eqn (1) and the experimental ΔLw value is shown in Fig. 7b. Obviously, the experimental data fit well with the calculated data, and the relative error is less than 3%.
Because the P(NIPAM-co-B18C6Am) hydrogel exhibits both thermo-responsive and Pb2+-responsive properties, the relationship between Pb2+ concentration and the change in the column length should be established at certain temperature. An index is defined as the Pb2+-responsive column length variation, which is calculated from ΔX = ΔLPb2+ − ΔLw, where ΔLPb2+ is the measured column length and ΔLw is calculated from eqn (1). Fig. 8a shows the Pb2+-concentration dependence of the ΔX value at different temperatures, in which the curves are very close in the temperature range from 22 to 28 °C. Fig. 8b shows the relationship between Pb2+ concentration and the ΔX value at 24 °C. The relationship between Pb2+ concentration and the ΔX is in accordance with the cubic polynomial, which can be described with the eqn (2):
C24 = 0.0092ΔX3 − 0.2514ΔX2 + 2.5567ΔX + 0.104 | (2) |
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Fig. 8 Detection of Pb2+ concentration with the P(NIPAM-co-B18C6Am)-hydrogel-based device and eqn (2). (a) The indicating liquid column variation ΔX (ΔX = ΔLPb2+ − ΔLw) as a function of Pb2+ concentration at different temperatures. (b) The relationship between the Pb2+ concentration and the ΔX value at 24 °C. (c) Comparison of the calculated Pb2+ concentration from eqn (2) at 24 °C with the experimental Pb2+ concentration. |
A comparison of the calculated Pb2+ concentration from eqn (2) and the experimental Pb2+ concentration at 24 °C is shown in Fig. 8c. Obviously, the experimental data fit well with the calculated data and the relative error is less than 2%.
Because the Pb2+-concentration-dependent ΔX curves are very close in the temperature range from 22 to 28 °C, the relationship between Pb2+ concentration and the ΔX value at different temperatures in this temperature range can be expressed with a general eqn (3):
C = aΔX3 + bΔX2 + cΔX + d | (3) |
T (°C) | a | b | c | d | R 2 |
---|---|---|---|---|---|
22 | 0.0089 | −0.2347 | 2.4213 | 0.0997 | 0.9961 |
24 | 0.0092 | −0.2514 | 2.5567 | 0.1040 | 0.9993 |
26 | 0.0082 | −0.2315 | 2.4713 | 0.2461 | 0.9971 |
28 | 0.0085 | −0.2400 | 2.5590 | 0.1920 | 0.9980 |
In a word, with measured column length in the device, the Pb2+ concentration can be accurately calculated with eqn (1) and (3).
Due to the intrinsic nature of the P(NIPAM-co-B18C6Am) hydrogel, there are still some limitations of the current device in terms of operational and functional parameters such as temperature and concentration, requiring further developments. The optimal temperature range of the current device for detecting Pb2+ is from 20 to 36 °C. Because the salting-out effect of increased amount of anions in solutions would counteract the swelling of the P(NIPAM-co-B18C6Am) hydrogel to some extent,36,37 and the P(NIPAM-co-B18C6Am) hydrogel begins to shrink when Pb2+ concentration is larger than 30 mM,26 so the upper limit of the current device for Pb2+ detection is about 30 mM. The lower limit of the current device for Pb2+ detection is about 1 mM at present stage, which can be further extended by improving the Pb2+-responsive characteristics of the hydrogel, improving the sensitivity of the elastic diaphragm, or reducing the dimension of the flow channel, etc.
This journal is © The Royal Society of Chemistry 2014 |