Min
Hsiao
a,
Shih-Hsiu
Chen
a,
Jheng-Yi
Li
a,
Po-Hsuan
Hsiao
a and
Chia-Yun
Chen
*ab
aDepartment of Materials Science and Engineering, National Cheng-Kung University, Tainan 701, Taiwan. E-mail: timcychen@mail.ncku.edu.tw
bHierarchical Green-Energy Materials (Hi-GEM) Research Centre, National Cheng Kung University, No. 1 University Road, Tainan 701, Taiwan
First published on 24th May 2022
Rapid, reliable, and sensitive colorimetric detection has been regarded as a highly potential technique for visually monitoring the cation ions. Yet, insight into detection kinetics and quantitative analysis for colorimetric sensing of sodium ions has rarely been revealed. Herein, in-depth kinetic investigations of colorimetric detection using surface-modified Au-nanoparticle (AuNP) probes were performed for interpreting the correlation of salt concentration, reaction duration, and light absorbance. To envision these undisclosed issues, modification of AuNP surfaces with ascorbic acid was found to be highly essential for boosting the detection sensitivity due to adjusting the zeta potential of AuNP colloids towards a slightly positive value. Next, modeling the light absorbance of AuNPs under various aggregation circumstances was employed, which visually elucidated the color change so that it was visible to the naked eye, due to the intense field localization on the edges of aggregated AuNPs. In addition, the involved activation energy of AuNP aggregation was found to follow the first-order Arrhenius formula, with the extracted value of 22.5 kJ mol−1. Finally, quantitative visualization of colorimetric Na+ ion sensing was realized, and the experimental relation was obtained for explicitly determining the unknown concentration of Na+ ions in a visual manner.
In recent years, there has been extensive exploration on methods of analysis of sodium ions (Na+), and methods such as thermometric titration, atomic absorption spectroscopy, chromatography, and inductively coupled plasma mass spectrometry have been employed.3–5 However, the above-mentioned methods require either expensive apparatus or complicated analysis. Moreover, practical detection remained time-consuming, with no available method to allow simple readout of the data with the naked eye. For this aspect, colorimetric methods possess the advantages of simplicity without the requirements for either complicated instrumentation or much knowledge of the electron or energy transfer involved in electrochemical or fluorescent systems, which could satisfactorily meet the requirements for practical use.
The strategy for realizing the colorimetric detection of metal ions is based on the effect of localized surface plasmon resonance (LSPR), which is a remarkable characteristic of gold nanoparticles (AuNPs), and describes the optical phenomenon produced by light waves confined within metallic particles smaller than the wavelength of the incident light.6–8 When nanoparticles interact with incident light, surface electrons are excited by electromagnetic radiation and form surface plasmons, which spectrally reflect the maximum light absorption due to collective oscillations as the wavelength corresponds to resonant frequency.9
In 2016, detection of sodium ions was demonstrated using AuNPs as sensing probes for evaluating the concentration of Na+ ions by colour change.10 While the idea has been adopted to examine the hydration level in artificial sweat, the underlying critical kinetic dependence on reaction temperature and response time has not yet been revealed. In addition, Na+ ion detection can be also realized with a plasticized PVC-based cation-selective optode system,11 whereas the developed system strictly relied on the complicated synthesis of an ionophore-doped plasticized PVC membrane. Na+ ions in serum can also be detected based on the G-quadruplex conformation strategy with an achievable detection limit of 0.6 μM,12 but, thus far, there have been no further discussions on environmental influences such as reaction temperature, pH, and illumination circumstances.
Recently, gold nanomaterials were used as colorimetric probes for analysing sodium chloride in seawater, although further explorations of sensitivity dependence on analyte radius and charge have not been reported.13 Very recently, the employment of a microfluidic colorimetric analysis system for detecting sodium benzoate was presented, where the involved colour variation was modelled with linear expression with respect to the analyte concentration featuring the sound determination coefficient of R2 = 0.997.14 Unfortunately, it was necessary for the colorimetric reaction to be initiated at 120 °C, which is a major disadvantage for its practical utilization.
In the current study, explorations of colorimetric Na+ ion detection were carried out while taking into account the radius and charge of target analytes, pH environment, and temperature dependence using surface-functionalized AuNP probes. From in-depth kinetic examinations of AuNP aggregation phenomena, we derived information regarding the experimentally determined activation energy that accounted for the capabilities of visual Na+ ion detection. In addition, we further discuss the quantitative modelling of light absorbance, analyte concentration, and reaction duration.
All these microstructural findings indicated the presence of FCC crystals of the synthesized AuNPs, which corresponded well to the results of the XRD analysis. In addition, the chemical states of as-prepared AuNPs were investigated with XPS analysis,18,19 as presented in Fig. 1c. The dominant peaks associated with the Au 4f7/2 and 4f5/2 signals were found in spectral identification, indicating the successful reduction of HAuCl4 precursors mediated with trisodium citrate as the reducing agent. The comparably weak Au3+ signals correlated with 4f7/2 and 4f5/2 orbitals were also displayed in the resulting photoelectron spectrum, which might have originated from the existence of a small portion of Au3+ complex or residual HAuCl4 precursors.
Additionally, by functionalizing AuNPs with ascorbic acid, abrupt variation of surface features was found from FTIR characterizations, as shown in Fig. 1d. The measured spectra of AuNPs prior to and after functionalization by ascorbic acid are displayed, where the substantial enhancement of absorption dips spectrally as 1753–1686 cm−1 and 1140–1109 cm−1, which corresponds to the CO and C–O vibration modes that exist in the functionalized AuNPs, respectively, and serves as evidence of the successful modification of the AuNP surfaces.20
To investigate the morphological transition of colloidal AuNPs in the presence of Na+ ions, TEM characterizations of bare AuNPs (Fig. 2a), mixed AuNPs/NaCl (10 mM) for 10 s (Fig. 2b), and AuNPs/NaCl (60 mM) for 10 s (Fig. 2c) were examined. The dispersive nature of AuNPs can be attributed to the existence of negative charges on AuNP surfaces that caused the repulsive force between neighbouring AuNPs, as evidenced in Fig. 2a, where the involved surface charges and dispersion stability are discussed later. With the addition of 10 mM Na+ ions, dramatic agglomeration of AuNPs occurred by breaking the natural repulsion barrier. These findings were further elucidated by DLS measurements, which showed that the average dimension of AuNP clusters varied from 15.74 nm (Fig. 2d) to 20.80 nm (Fig. 2e).21 It should be noted that insufficient Na+ ions caused the broad distribution of cluster size, which was due to the coexistence of agglomeration and separation states of the AuNPs. At higher concentrations of Na+ ions (60 mM), complete agglomeration of AuNPs is visible in the TEM image, as shown in Fig. 2c, where the cluster size significantly increased to 75.12 nm, as calculated in Fig. 2f.
The involved variation of colloidal phenomena is interpreted in Fig. 2g. The electrostatic repulsion between neighbouring AuNPs because of the negative surface charges was the force that maintained their dispersion in the tested solutions. With regard to the associated interaction between AuNPs responding to the variation in cluster size, there existed three main interactive forces affecting the stability of colloidal AuNPs: van der Waals force, electrostatic repulsion, and steric repulsion.22–24 Above all, the stability of colloids composed of charged particles can be conceptually explained by the Derjaguin–Landau–Verwey–Overbeek (DLVO) theory.25 According to the DLVO theory, the colloidal stability is determined by the balance between the van der Waals attraction forces and the electrostatic repulsion forces, where the former correlates with an attraction of intermolecular forces generated by electric dipoles, and the latter is due to the electric double layer repulsion between neighbouring AuNPs. Accordingly, the sum of the two interactions dominantly manipulated the colloidal stability of dispersing AuNPs.22,24
Examinations to determine the average zeta potential of AuNP probes with the addition of different concentrations of Na+ ions are displayed in the ESI.† They indicate that the average zeta potential of the bare AuNPs without surface modification was approximately −87.7 mV. The correlated value of AuNPs treated with ascorbic acid shifted to −58.2 mV because of the obvious reduction of the negative charges on the AuNP surfaces, whereas they remained well-dispersed in the aqueous solutions. Additionally, when adding Na+ ions, the negative surface charges were gradually suppressed, and, in turn, induced the aggregation of AuNPs due to a reduction in the diffusion double layer's thickness with increasing ionic strength, as explained by the electrical double layer theory.26
Furthermore, we attempted to introduce surface functionalization with ascorbic reagents to slightly shift the energy balance of particle colloidality toward reducing the particle spacing. This could accelerate the detection of Na+ ions to achieve increased sensitivity. A colorimetric table for detecting Na+ ions from AuNP probes without surface functionalization, which resulted in suppressed detection rates, is presented in the ESI.†
The optical characteristics of the AuNP probes in the presence of Na+ ions are displayed in Fig. 3a. Systematic investigations of light-absorption spectra upon varying the detection durations from 0 to 900 s in the presence of a similar salt concentration of 45 mM were monitored. In the case of 0 s, i.e., dispersed solutions of bare AuNPs, the maximum absorbance of surface-modified AuNP probes was centred at 525 nm, which was attributed to the LSPR effect of AuNPs responding to the strong light absorption contributed by the collective oscillation of free electrons. The spectral position of light absorbance shifted to a long wavelength regime when Na+ ions were introduced, and, therefore, the absorption peak was red-shifted from approximately 600 nm (30 s) to 690 nm (600 s). Additionally, the absorbance intensities were decreased accordingly, which originated from the agglomeration of AuNPs. This was followed by a reduction in AuNP density, which reflected a decrease in the number of active sites that could absorb the incoming light.
The measured absorption spectra under various Na+ concentrations were further modelled with the finite-difference time-domain (FDTD) calculation (Fig. 3b),27–29 where different aggregation conditions of AuNPs were considered to spectrally fit the measured data for providing the elucidative picture of correlated LSPR effects, as detailed in the ESI.† A similar shift in the absorption spectra associated with aggregation conditions of AuNPs (simulated results) in correlation with the duration of AuNP/Na+ interaction (experimental results) verified that the in situ microscopic phenomena could be qualitatively monitored with FDTD calculation. It should be noted that the slightly broader absorption spectra were calculated as compared to measured data, which could be attributed to the instrumental limitation of detecting all the scattering lights with the finite size of the aperture in the UV/Vis spectrometer.
To explore the spatial distribution of light-absorption sites when LSPR effects were encountered under various conditions of AuNP agglomeration, the field mappings of AuNPs at the wavelength of the central absorption peak were monitored, as shown in Fig. 3c. The comparative results clearly indicated that the field distributions were resonantly localized at regions of AuNP surfaces under isolated, well-dispersed states (Fig. 3c), and at the edges of overlapping regions of neighbouring AuNPs (Fig. 3d–f), while the intensity of the field localization in the case of the latter seemed to be substantially greater than that of the former.
These features explained the phenomena observed with the naked eye, where the present colour of the AuNP indicators became darker (from red to purple to dark grey) as greater numbers of AuNPs were aggregated even though the overall absorption intensities were reduced, as evidenced in the measured and calculated spectra (Fig. 3a and b). Examinations of average zeta potential indicated that the main mechanism for AuNP aggregation could be attributed to the shift of the average zeta potential toward the positive regime when adding Na+ ions, which subsequently caused the instant color variations of AuNPs, depending on the extent of AuNP aggregation.
To explore the potential sensing capability of AuNP probes functioning as colorimetric indicators, visual examination of Na+ ion detection is presented in Fig. 4a.30,31 The color of the AuNP solutions gradually changed from red to purple, and even to dark grey, due to the obvious agglomeration of the AuNPs. It should be noted that the involved colorimetric detection could be repetitively utilized by transforming the aggregation state to the recovery of dispersed conditions, as demonstrated in the ESI.†
The reaction times of colour variations decreased as the salt concentrations were increased. Furthermore, the minimum concentration that could be visually detected through the naked eye was found to be approximately 30 mM, which only required 30 s to reach an obvious colour change. The time required for visual detection was unambiguously decreased while the tested salt concentration was increased. The colour change of the AuNPs remarkably decreased to less than 5 seconds at 60 mM, providing an instant and reliable detection strategy for sodium salts.
To further quantitatively visualize the colour change, the corresponding colour distributions in the presence of various salt concentrations were numerically displayed with the standard CIE colour space,30 as shown in Fig. 4b. X and Y values, corresponding to the normalization of the tri-stimulus values in the two-dimensional spatial domain of colour space, clearly indicated that the trends of time-dependent colour variation in the presence of different salt concentrations were distinct. Specifically, the approximately straight and steeply curved variations of X and Y values in the chromaticity diagrams in the case of low (30 mM, left diagram) and high (45 mM, right diagram) salt concentrations with respect to the elongation of reaction time are displayed in Fig. 4b.
These results provide an intuitive vision of the dynamic change of indicator colour depending on the salt concentration and reaction time, which were in good agreement with the colorimetric table shown in Fig. 4a. In addition to the employment of CIE colour space, the commercially used RGB colour model was also employed as an alternative to examine the involvement of colour change. It validated the fact that the change in red colour space with respect to reaction time was predominant in three examined color spaces that responded to the detection of salt concentration, as shown in the ESI.†
Other than that, another determinate influence relied on cation charge, where the detection of divalent cations seemed to be more kinetically favourable for the intended aggregation of AuNPs than the sensing condition of monovalent ions, where the available minimum detection of cation ions with respect to the ion radius is displayed in Fig. 5b. As a consequence, we inferred that the detected minimum concentration of AuNP probes was inversely dependent on the product of the cube of ion charge and ion radius, as summarized in Table 1 (Fig. 5c), which illustrates the underlying correlation of two analyte features impacting the aggregation of AuNPs.
Metal ions | Ion radius (pm) | (Ion charge)3 × ion radius | Detectable concentration minimum (mM) |
---|---|---|---|
Li+ | 76 | 76 | 45 |
Na+ | 102 | 102 | 30 |
K+ | 138 | 138 | 15 |
Mg2+ | 72 | 288 | 0.75 |
Ca2+ | 100 | 800 | 0.37 |
Sr2+ | 118 | 944 | 0.2 |
Cation ions with a larger radius provided additional active sites for contact with AuNPs, which resulted in greater availability for AuNP agglomeration. This steric effect in terms of larger cation radius favoured the rapid and efficient variation in colour visualized by the naked eye, thus reducing the detection minimum of cation concentration. However, the existence of additional surface charges on cation ions also facilitated the ionic interaction between negatively charged AuNPs and positively charged cation ions, which in turn benefited the detection sensitivity in the case of low cation concentration. In addition, the detection selectivity and practical applications, such as detecting residual Na+ ions on chopsticks using AuNP probes as indicators, were further examined, as shown in the ESI.†
The involved protonation of AuNPs due to the variation in environmental pH can be further evidenced by the measurement of corresponding zeta potentials, as shown in Fig. 6b. The aqueous zeta potentials shifted to higher values when the pH values were reduced under three various concentrations of sodium salt, which implies that the inherently negative polarity of AuNP surfaces with negative charges were partially identified due to encountering protonation mediation through lowering of the environmental pH values. Apart from that, the designed AuNP probes remained active and efficient under a wide pH range from 3 to 9.5 (Fig. 6a), which could meet the requirements for practical employment to detect salt. Moreover, from examining the change in the average zeta potentials under three different salt concentrations, it was observed that the corresponding values of zeta potential were maintained in a narrow range under pH = 3–9.5, where the deviations in the zeta potential were less than 16% (for salt concentration of 30.0 mM), 10% (for salt concentration of 37.5 mM), and 8% (for salt concentration of 45.0 mM), which thus validated the sensor stability for detecting Na+ ions.
To quantitatively explore the correlated thermodynamic kinetics, a plot of absorbance variation, determined by the change in the average absorbance within the wavelength of 380–780 nm and relative to reaction durations at each environmental temperature, was characterized for extracting the rate constant corresponding to the kinetic features of colorimetric phenomena, as shown in the insets of Fig. 7. The results clearly indicate the positive correlation between the temperature-dependent rate constant and environmental temperature. This provided elucidation regarding the rate-determining step for the involved colorimetric characteristics, which was colloidal aggregation accompanying the thermally driven activation energy that resulted in varying amounts of AuNP coalescence. To gain further insight into the involvement of activation energy on AuNP aggregation, the Arrhenius equation was adopted, as shown below:34
(1) |
(2) |
In addition, the slightly lower activation energy obtained in our work could be attributed to the induced agglomeration that resulted after adding Na+ ions that strengthened the ionic attraction between neighbouring AuNPs through overcoming the energy barrier that arose from collision hindrance and citrate desorption from AuNP surfaces. It was also found that the thermodynamic coalescence of two nanocrystallite NPs was recognized with a similar crystallographic facet on the atomic scale in order to remedy the involvement of surface free energy, which therefore contributed to either raising the temperature above ambient or decelerating the reaction rate.36,37 Evidently, these kinetic restrictions did not take place during the AuNP-based colorimetric detection of Na+ ions presented in this work, because the mediation of Na+ ions readily decreased the energy barrier and facilitated ionic-force-induced aggregation by shortening the self-diffusion distance of the AuNPs.
It should be noted that the optical sensing of sodium ions could be realized by other methods, including surface-enhanced Raman scattering,41 fluorescence techniques,42 and photonic diffraction.43 While their sensing capabilities were remarkably sound, the aforementioned methods require either sophisticated spectral instruments or complicated patterning fabrication that prevents their practical employment. Moreover, the developed AuNP probes for colorimetric sensing with sensitive and easily employed capabilities could be particularly utilized for on-site and instant sensing applications.
The underlying reason behind the rationality of this strategy could be associated with the fact that the spectral variations in light absorbance were quite broad, from 380 nm to 780 nm, while the reaction durations were longer than 15 min (Fig. 8d–g). Thus, similar to the treatment presented in the insets of Fig. 7, linear regression by fitting the correlation between average light absorbance and salt concentration was employed to examine the results under the variation of reaction time from 0 to 30 min, with 5 min as each interval, and where the corresponding R2 values of linear fitting with respect to the reaction duration are envisioned in Fig. 8h. Clearly, the corresponding R2 values were maintained above 0.96 regardless of detection time, which explicitly provided a reliable analysis of the light-absorption phenomena of AuNPs for detecting Na+ ions covering a large timespan. On the basis of these established models, the correlated mathematical expression was further explored via the employment of the second-order polynomial regression:
Response (light absorbance) = 0.74 + 2.1 × 10−3CNa+ − 8.5 × 10−3t − 3.3 × 10−4CNa+t − 9.9 × 10−5CNa+2 + 3.310−4t2 | (3) |
Footnote |
† Electronic supplementary information (ESI) available. See https://doi.org/10.1039/d2na00211f |
This journal is © The Royal Society of Chemistry 2022 |