DOI:
10.1039/C4RA02151G
(Paper)
RSC Adv., 2014,
4, 18694-18701
Study on the interaction behavior of lysozyme with lanthanide ions by flow injection chemiluminescence analysis
Received
12th March 2014
, Accepted 31st March 2014
First published on 31st March 2014
1. Introduction
The lanthanide family (Ln: La–Lu, 57–71) has a consequence of their peculiar and similar electronic configuration [Xe]4fn (n = 0–14),1 which is divided into light lanthanides (LL) from La to Eu and heavy lanthanides (HL) from Gd to Lu.2 The chemical, optical, and magnetic properties as well as all aspects of lanthanide ions (LnIII) were summarized in detail by J. C. G. Bünzli.3 Although they exist merely in nature, they play a significant role in many areas of contemporary techniques and scientific applications.4,5 For example, as catalysts, lanthanum salts and cerium oxide are used in the production of petroleum and synthetic products;6,7 NdIII, ErIII and YbIII are used in lasers and upconverting nanoparticles;8–10 and LaIII, CeIII and SmIII are applied to promote seed germination and seedling growth.11–13 EuIII, TbIII and DyIII have been utilized extensively in biological systems, and the applications range from luminescent labels of biological molecules and the detection of cellular functions in vivo to the elucidation of the structure and function of enzymes and proteins.14–16
It is well known that study on the interaction of protein with metal ions has become a hot spot in the fields of chemistry, biochemistry and clinical research.17 For example, the interaction of lysozyme with CeIII, SmIII, EuIII, TbIII, CuII, ZnII and HgII using nuclear magnetic resonance (NMR),18,19 inductively coupled plasma mass spectrometry (ICP-MS),20,21 fluorescence (FL),22,23 inductively coupled plasma-atomic emission spectrometry (ICP-AES),24 and ultraviolet and visible spectrometry (UV-Vis)25 have been reported. Nevertheless, the interaction of lysozyme with lanthanide family members from La to Lu by flow injection chemiluminescence (FI-CL) analysis has not been reported up to now.
Lysozyme, a small monomeric, low molecular weight (14.4 kDa) globular protein with 129 amino acid residues and active sites of Glu35, Trp62 and Asp52,26,27 could accelerate the electron transferring rate of excited 3-aminophthalate, and enhanced luminol CL intensity has been reported.28 In this work, using luminol as a luminescence probe, the interaction of lysozyme with LnIII was studied at nanomole levels, which provided an effective way for investigating luminescence behavior of the lanthanide family.
It was found that LnIII could quench the CL intensity of the luminol–lysozyme system; the decrement of CL intensity was linearly proportional to the logarithm of LnIII concentration in the range of 0.1–50.0 nmol L−1 with a detection limit of 0.03 nmol L−1 (3σ). At a flow rate of 2.0 mL min−1, complete determination of LnIII including sampling and washing could be accomplished in 0.5 min, giving a maximum sample throughput of 120 h−1. The possible CL mechanism of luminol–lysozyme–LnIII reaction was also studied, and the application of lysozyme with LnIII was given.
2. Materials and methods
2.1. Apparatus
The FI-CL system used in this work is shown schematically in Fig. 1. A peristaltic pump of the IFFM-E Luminescence Analyzer (Xi'an Remax Analysis Instrument Co. Ltd., Xi'an, China) was applied to deliver all streams. PTFE tubing (1.0 mm i.d.) was used throughout the manifold for carrying the CL reagents. A six-way valve with loops of 100 μL was used for sampling. The flow cell was made by coiling 15 cm of a colorless glass tube (1.0 mm i.d.) into a spiral-shape disk (2.0 mm i.d.) and placing it close to the photomultiplier tube (PMT). The CL signal produced in the flow cell was detected without wavelength discrimination, and PMT output was recorded by a PC with an IFFE-E client system. Inductively coupled plasma atomic emission spectroscopy (ICP-AES, IRIS Advantage, Thermo Scientific, America) was used as a reference technique for the comparison of the results among the samples. A water bath (HW.SY11-K6B/C, Leici, Shanghai, China) was used for controlling the temperature.
 |
| | Fig. 1 Schematic diagram of the FI-CL system for the determination of LnIII. Luminol: 2.5 × 10−5 mol L−1; lysozyme: 1.0 × 10−7 mol L−1; NaOH: 0.025 mol L−1; flow rate: 2.0 mL min−1; high voltage: −700 V. | |
2.2. Reagents
All reagents used in this work were of analytical reagent grade unless specified, and doubly deionized water was purified in a Milli-Q system (Millipore, Bedford, MA, USA) and used for the preparation of solutions in the whole procedure. Luminol (Fluka, Biochemika, Switzerland) was purchased from Xi'an Medicine Purchasing and Supply Station, China. Lysozyme (Sigma-Aldrich, St. Louis, MO, USA) was used without any further purification. Ln2O3 (99.99%) was purchased from Beijing Founde Star Science and Technology Co., Ltd (Beijing, China). Samples with different LaIII content were supplied by Dr Zhao in the College of Chemistry and Materials Science, Northwest University.
Luminol (2.5 × 10−2 mol L−1) was prepared by dissolving 0.44 g luminol in 100 mL of 0.1 mol L−1 NaOH solution in a brown calibrated flask. Lysozyme solution (1.0 × 10−4 mol L−1) was prepared by dissolving 35.00 mg lysozyme in 25 mL purified water. A series of LnCl3 stock solutions (1.0 × 10−3 mol L−1) were prepared by dissolving Ln2O3 in 12 mol L−1 HCl with subsequent heating to deplete the excess HCl and dilute with purified water.29 All working standard solutions were prepared daily from the above stock solutions by appropriate dilution as required, and the stock solutions were stored at 4 °C.
Sample preparation: five samples were weighed exactly and placed in five crucibles, and then every sample (50.0 mg) was heated at 700 °C for 4 h in muffle furnace. After that, each sample was dissolved in 12 mol L−1 HCl. Thereafter, the sample solutions were heated at 80 °C to dry. After cooling to the room temperature, each sample was prepared with purified water in a 25 mL calibrated flask. Suitable aliquots were taken and diluted with appropriate multiples for the determination of LaIII by the proposed CL and ICP-AES methods.
2.3. Molecular docking
The crystal structure of lysozyme was taken from the Protein Data Bank (PDB, http://www.rcsb.org/pdb/). The 3D conformer structure of luminol was retrieved from the National Center for Biotechnology Information and converted to PDB format by OpenBabel 2.3.2. These PDB structures of lysozyme and luminol were used for docking by AutoDock 4.2 software. Docking simulation was performed using the Lamarckian Genetic Algorithm (LGA) to search for the optimum binding energy of lysozyme with luminol. Docking parameters included AutoGrid using a box 40 Å × 40 Å × 40 Å. Luminol could therefore be completely contained in the box.
2.4. Procedures
A schematic profile of the equipment in the flow system is described in Fig. 1, and flow lines were inserted into luminol/NaOH, carrier (purified water), lysozyme and LnIII solutions at a constant speed of 2.0 mL min−1. The whole flow system was washed with purified water until a stable baseline was recorded. The luminol standard solution (100 μL) was injected into the carrier stream by an injection valve and merged with a mixture flow of lysozyme and LnIII. The mixed solution was delivered into the CL cell, producing CL emission, and detected by the PMT at a high voltage of −700 V. The concentration of LnIII could be quantified on the basis of the decrement of luminol–lysozyme CL intensity, ΔI = I0 − I, where I and I0 were luminol–lysozyme system CL signals in the presence and absence of LnIII, respectively. The temperature of working solutions was controlled by a water bath, which was kept in a certain range (T ± 0.1 °C) throughout the experiment. Since the speed of detection was rapid, the time that the solution was flowing in the tube was short and the temperature of solutions was kept constant, so during detection, the error of temperature was negligible.
2.5. The optimization of experimental conditions
The effect of luminol concentration on CL intensity was investigated at concentrations ranging from 5.0 × 10−7 to 5.0 × 10−5 mol L−1. It was found that the CL intensity increased steadily with increasing luminol concentration up to 2.5 × 10−5 mol L−1 and then tended to be stable. Thus, 2.5 × 10−5 mol L−1 was chosen as the optimum luminol concentration. Similarly, the influence of lysozyme concentration on CL intensity was tested from 1.0 × 10−9 to 1.0 × 10−6 mol L−1. The CL intensity rose drastically with increasing lysozyme concentration up to 1.0 × 10−7 mol L−1, and then increased slowly from a higher concentration. Therefore, 1.0 × 10−7 mol L−1 was chosen as the optimum lysozyme concentration in the following experiments. Because luminol reaction is more favored under basic conditions, NaOH was introduced to improve the sensitivity of the system. A series of NaOH solutions with different concentrations were tested. The CL intensity arrived at a peak with the concentration of NaOH arriving at 0.025 mol L−1, and thus, this concentration was employed in subsequent experiments.
The CL intensity was related to the flow rate and mixing tube length. The effect of flow rate on CL intensity was investigated with flow rates ranging from 0.5–5.0 mL min−1. It was found that the CL intensity increased with the augmentation of flow rate, while the CL signal was unstable at a high flow rate. As a compromise between less reagent consumption and higher sensitivity, a flow rate of 2.0 mL min−1 was recommended. The effect of mixing tube length on CL intensity was also tested with lengths from 5.0 to 20.0 cm, and it was observed that the CL intensity was strong and stable using a mixing tube of 10.0 cm. Accordingly, 10.0 cm was selected as the optimum length for the mixing tube.
The pH effect of LnIII solutions on luminol–lysozyme CL intensity was tested at pH values ranging from 4.0 to 9.0, which were adjusted by HCl or NaOH solutions. It was found that the pH effect for all LnIII solutions was the same, and as Fig. 2 shows (LaIII as an example), the remarkable increments in CL intensity were at pH values of 5.0–6.5. A lower pH affects the luminol–lysozyme CL reaction and a higher pH promotes the hydrolysis of LaIII, leading to a decrease in ΔI. Considering the sensitivity of LaIII determination, finally, a pH of 6.0 was selected in this work.
 |
| | Fig. 2 The pH effect of 10.0 nmol L−1 LaIII on the CL intensity of the luminol–lysozyme reaction. | |
2.6. The operational stability of the FI-CL system
The operational stability of the FI-CL system was tested by injecting 100 μL luminol solution into the flow system, which was further merged with the mixed solution of EuIII and lysozyme (1.0 and 10.0 nmol L−1, respectively). Then, the relative CL intensity (ΔI = I0 – I) was recorded to test the stability of the system. The experiment lasted for 5 days with the FI-CL system regularly used over 8 h per day, and the stability and precision of the FI-CL system for EuIII determination are shown in Table 1. It was found that ΔI kept stable under the fluctuation of I0, and RSDs were less than 3.0%, which showed that the system had very good stability.
Table 1 The stability test of the FI-CL system under 1.0 and 10.0 nmol L−1 EuIIIa
| Time day |
ICL blank |
RSD% |
ICL 1.0 nmol L−1 |
RSD% |
ICL 10.0 nmol L−1 |
RSD% |
| Each result is the average of seven separate determinations. |
| 1st |
352 |
1.6 |
335 |
2.5 |
308 |
2.7 |
| 2nd |
351 |
2.0 |
337 |
1.8 |
306 |
2.4 |
| 3rd |
353 |
1.9 |
338 |
2.2 |
304 |
2.5 |
| 4th |
350 |
2.1 |
339 |
2.6 |
305 |
2.3 |
| 5th |
354 |
2.3 |
336 |
2.0 |
307 |
2.5 |
3. Results and discussion
3.1. The relative CL intensity–time profile
The relative CL intensity–time profile of luminol–lysozyme–LnIII is shown in Fig. 3. The time to reach the maximum CL intensity (Tmax) for the luminol–dissolved oxygen system (curve 7) was 4.4 s, and the Tmax of the luminol–lysozyme (100 nmol L−1) system (curve 1) was 4.0 s. The maximum CL intensity (Imax) was increased from 98 to 352. It was suggested that lysozyme reacted with the luminol, leading to the enhancement CL intensity of luminol. In the presence of LaIII, EuIII, GdIII, TbIII and LuIII (5 nmol L−1), the Imax of luminol–lysozyme CL system decreased from 352 to 295, 268, 256, 247 and 193 by 8.5, 23.9, 27.3, 29.8 and 45.2%, respectively (curves 2–6). The decrement of luminol–lysozyme CL intensity was proportional to the concentration of LnIII, and the quantitative correlation equation could be obtained. It was indicated that the interaction between lysozyme and LnIII should exist and resulted in the CL intensity of luminol–lysozyme being inhibited.
 |
| | Fig. 3 Relative CL intensity–time profiles in different CL systems. Curve 1: CL intensity of luminol–lysozyme reaction; curve 2–6: CL intensity in the presence LaIII, EuIII, GdIII, TbIII and LuIII of luminol–lysozyme reaction; curve 7: CL intensity of luminol. The concentration of luminol was 2.5 × 10−5 mol L−1, the concentration of lysozyme was 1.0 × 10−7 mol L−1, and the concentrations of LaIII, EuIII, GdIII, TbIII and LuIII were 5.0 × 10−9 mol L−1. | |
3.2. The quantitative correlation equations of LnIII
Under the optimized conditions, the standard solutions of LnIII series were tested by FI-CL using the luminol–lysozyme system. It was found that the decrement of CL intensity (ΔI) was proportional to the logarithm of the concentration of LnIII over the range from 0.1 to 50 nmol L−1 with correlation coefficient R from 0.9960 to 0.9986 and obeyed the quantitative correlation equation, ΔI = A
ln
CLn + B, in which the slope A was defined as the sensitivity factor. The linear equations of the LnIII series are given in Table 2, and the calibration graphs of LaIII, SmIII, YbIII and LuIII are shown in Fig. 4. It can be seen that A(B) varied with increasing Z, among ALL from 15.39 to 18.48 and AHL from 22.20 to 29.01 with linear equations ALL = 0.55Z − 15.96 and AHL = 1.26Z − 60.70.
Table 2 Linear equations of lysozyme with LnIII
| LnIII |
ΔI = A ln CLn + B |
R |
| LaIII |
ΔI = (15.39 ± 0.02)ln CLa + (30.54 ± 0.04) |
0.9960 |
| CeIII |
ΔI = (16.52 ± 0.02)ln CCe + (34.81 ± 0.03) |
0.9971 |
| PrIII |
ΔI = (17.46 ± 0.01)ln CPr + (36.08 ± 0.01) |
0.9961 |
| NdIII |
ΔI = (17.55 ± 0.02)ln CNd + (38.46 ± 0.03) |
0.9966 |
| SmIII |
ΔI = (18.41 ± 0.03)ln CSm + (39.66 ± 0.02) |
0.9976 |
| EuIII |
ΔI = (18.89 ± 0.02)ln CEu + (43.74 ± 0.01) |
0.9971 |
| GdIII |
ΔI = (18.48 ± 0.02)ln CGd + (44.04 ± 0.03) |
0.9968 |
| TbIII |
ΔI = (22.20 ± 0.03)ln CTb + (53.34 ± 0.02) |
0.9969 |
| DyIII |
ΔI = (23.19 ± 0.01)ln CDy + (55.16 ± 0.01) |
0.9971 |
| HoIII |
ΔI = (24.63 ± 0.01)ln CHo + (57.51 ± 0.03) |
0.9986 |
| ErIII |
ΔI = (25.65 ± 0.02)ln CEr + (59.14 ± 0.02) |
0.9961 |
| TmIII |
ΔI = (26.77 ± 0.02)ln CTm + (61.18 ± 0.03) |
0.9975 |
| YbIII |
ΔI = (27.41 ± 0.01)ln CYb + (63.29 ± 0.01) |
0.9985 |
| LuIII |
ΔI = (29.01 ± 0.01)ln CLu + (65.05 ± 0.01) |
0.9981 |
 |
| | Fig. 4 The calibration graphs of LaIII, SmIII, YbIII and LuIII. | |
It is well known that the LnIII series can be divided into two subgroups by the severity of the Gd break,30,31 which is approximated in the existing diad theory.32,33 By plotting A against Z, good linear relationships for LL and HL except at the GdIII break at f7 are presented in Fig. 5. It was clear that GdIII was a break point, which agreed with the lanthanide contraction and the Gd break effect. The correlation equations of A with some physical parameters (ionic radius γ±, hydration enthalpy ΔHhyd and standard redox potential Eo) of LnIII are listed in Table 3, and the relationship curves of A vs. Z, γ±, ΔHhyd and Eo are shown in Fig. 6. It can be seen that A vs. |ΔHhyd| (the absolute value of ΔHhyd) was the best trend (the same A as a function Z), and few lines intersected at the point Gd, which indicated that HL had a bigger slope value than LL, and may be attributed to the increased polarizability caused by lanthanide contraction.34–36
 |
| | Fig. 5 Plots of sensitive factor A against atomic number Z for the LL and HL with linear equations. | |
Table 3 Correlations of A with the physical parametersa for LL and HL
| Parameters |
LL |
HL |
| Linear equations |
R |
Linear equations |
R |
| Ionic radius γ± (Å), hydration enthalpy ΔHhyd (kJ mol−1) and standard redox potential Eo (V). |
| A vs. γ± |
A = −34.6γ± + 51.8 |
0.9741 |
A = −100.0γ± + 113.5 |
0.9923 |
| A vs. |ΔHhyd| |
A = 1.7 (|ΔHhyd|) – 39.7 |
0.9518 |
A = 4.2 (|ΔHhyd|) – 128.4 |
0.9750 |
| A vs. |Eo| |
A = −33.7 (|Eo|) + 99.9 |
0.9864 |
A = −55.3 (|Eo|) + 152.7 |
0.9705 |
 |
| | Fig. 6 The linear relationships of A vs. physical parameters of LnIII. | |
3.3. The interaction parameters of lysozyme with LnIII
Utilizing the homemade FI-CL model lg[(I0 − I)/I] = n
lg
[Ln] + lg
K,37 the binding constants K and the number of binding sites n could be obtained from the plot of lg[(I0 − I)/I] against lg[Ln], and the results are listed in Table 4. The binding constants K were 105 to 106 L mol−1 level, suggesting that there existed a high binding affinity of LnIII to lysozyme, which agreed well with the binding constants K obtained by fluorescence,38–40 and the number of binding sites n were approximately equal to 1.0 and confirmed a 1
:
1 complex. It was found that the binding constants K and number of binding sites n increased with increasing Z, and the binding ability of LnIII to lysozyme increased with increasing Z, which matched with the order of sensitivity in the presence of lanthanide contraction. As shown in Fig. 7, it was clear that GdIII was a break point and the HL possessed relatively high binding ability compared with the LL, which was in good agreement with a large number of classical experimental results.41–43
Table 4 Binding parameters of lysozyme with LnIII at 288/300/310 K
| LnIII |
K × 105/L mol−1 |
n |
R |
| LaIII |
1.26 ± 0.02/1.10 ± 0.01/1.05 ± 0.02 |
0.69 ± 0.01 |
0.9897/0.9876/0.9833 |
| CeIII |
1.99 ± 0.01/1.70 ± 0.01/1.47 ± 0.01 |
0.70 ± 0.01 |
0.9898/0.9906/0.9892 |
| PrIII |
2.68 ± 0.01/2.21 ± 0.01/1.91 ± 0.01 |
0.73 ± 0.01 |
0.9952/0.9948/0.9901 |
| NdIII |
3.60 ± 0.01/2.97 ± 0.01/2.46 ± 0.01 |
0.75 ± 0.01 |
0.9990/0.9942/0.9916 |
| SmIII |
4.37 ± 0.01/3.31 ± 0.01/3.10 ± 0.01 |
0.78 ± 0.02 |
0.9855/0.9926/0.9892 |
| EuIII |
5.40 ± 0.01/4.23 ± 0.01/3.55 ± 0.01 |
0.80 ± 0.01 |
0.9854/0.9936/0.9838 |
| GdIII |
5.63 ± 0.01/4.46 ± 0.01/3.67 ± 0.01 |
0.81 ± 0.01 |
0.9929/0.9974/0.9884 |
| TbIII |
10.09 ± 0.01/7.14 ± 0.01/5.43 ± 0.02 |
0.92 ± 0.01 |
0.9882/0.9856/0.9896 |
| DyIII |
13.33 ± 0.02/9.40 ± 0.01/7.01 ± 0.02 |
0.94 ± 0.02 |
0.9843/0.9872/0.9914 |
| HoIII |
17.10 ± 0.01/11.86 ± 0.01/8.76 ± 0.01 |
0.97 ± 0.01 |
0.9952/0.9929/0.9879 |
| ErIII |
21.57 ± 0.01/14.36 ± 0.01/10.71 ± 0.01 |
1.00 ± 0.01 |
0.9917/0.9848/0.9945 |
| TmIII |
24.92 ± 0.01/16.36 ± 0.01/12.04 ± 0.01 |
1.02 ± 0.01 |
0.9857/0.9927/0.9966 |
| YbIII |
31.65 ± 0.01/20.56 ± 0.02/14.70 ± 0.01 |
1.05 ± 0.02 |
0.9987/0.9946/0.9905 |
| LuIII |
39.47 ± 0.01/24.75 ± 0.02/17.69 ± 0.01 |
1.08 ± 0.02 |
0.9849/0.9884/0.9962 |
 |
| | Fig. 7 Plots of the number of binding sites n against atomic number Z of LnIII. | |
3.4. The thermodynamic parameters of lysozyme with LnIII
According to the obtained binding constants of lysozyme with LnIII, the thermodynamic parameters (ΔH, ΔS and ΔG) at different temperatures (288, 300 and 310 K) were calculated using the Van't Hoff equation44 and summarized in Table 5. It can be seen that ΔG < 0, ΔH < 0 and ΔS > 0. The results testified the formation complex of lysozyme with LnIII was a spontaneous exothermic reaction, and the main binding force was electrostatic interaction.45 As shown in Fig. 8, the absolute value of ΔG increased with the increasing of atomic number Z and HL increased more obviously than LL, which was consistent with the effect of lanthanide contraction and the diad theory. The binding ability and the affinity of lysozyme with LnIII varied in the following sequence: LaIII to LuIII increased successively. With ion radii decreasing systematically, the electrostatic force of lysozyme with LnIII and higher binding ability for HL was achieved. It was also found that with increasing temperature, the absolute value of ΔG increased and the spontaneous reaction was more easily initiated, which indicated that high temperature was favorable for reaction.
Table 5 Thermodynamic parameters of lysozyme with LnIII
| LnIII |
T/K |
ΔG/kJ mol−1 |
ΔH/kJ mol−1 |
ΔS/J mol−1 K−1 |
| LaIII |
288 |
−28.13 ± 0.01 |
−8.55 ± 0.02 |
68.03 ± 0.01 |
| 300 |
−28.96 ± 0.02 |
| 310 |
−29.63 ± 0.01 |
| CeIII |
288 |
−29.21 ± 0.02 |
−10.10 ± 0.02 |
66.47 ± 0.01 |
| 300 |
−30.04 ± 0.02 |
| 310 |
−30.67 ± 0.01 |
| PrIII |
288 |
−29.92 ± 0.01 |
−11.39 ± 0.01 |
64.33 ± 0.02 |
| 300 |
−30.69 ± 0.01 |
| 310 |
−31.34 ± 0.02 |
| NdIII |
288 |
−30.64 ± 0.01 |
−12.82 ± 0.01 |
62.03 ± 0.01 |
| 300 |
−31.43 ± 0.01 |
| 310 |
−31.99 ± 0.01 |
| SmIII |
288 |
−31.10 ± 0.02 |
−13.39 ± 0.01 |
61.03 ± 0.01 |
| 300 |
−31.70 ± 0.01 |
| 310 |
−32.47 ± 0.01 |
| EuIII |
288 |
−31.61 ± 0.02 |
−14.23 ± 0.02 |
60.27 ± 0.01 |
| 300 |
−32.31 ± 0.01 |
| 310 |
−32.93 ± 0.01 |
| GdIII |
288 |
−31.71 ± 0.02 |
−14.39 ± 0.01 |
60.20 ± 0.01 |
| 300 |
−32.45 ± 0.01 |
| 310 |
−33.03 ± 0.02 |
| TbIII |
288 |
−33.10 ± 0.01 |
−20.90 ± 0.01 |
42.40 ± 0.01 |
| 300 |
−33.62 ± 0.02 |
| 310 |
−34.03 ± 0.01 |
| DyIII |
288 |
−33.77 ± 0.01 |
−21.62 ± 0.02 |
42.27 ± 0.01 |
| 300 |
−34.30 ± 0.01 |
| 310 |
−34.69 ± 0.02 |
| HoIII |
288 |
−34.36 ± 0.01 |
−22.52 ± 0.02 |
41.20 ± 0.01 |
| 300 |
−34.88 ± 0.01 |
| 310 |
−35.27 ± 0.01 |
| ErIII |
288 |
−34.92 ± 0.02 |
−23.65 ± 0.01 |
39.03 ± 0.01 |
| 300 |
−35.36 ± 0.01 |
| 310 |
−35.78 ± 0.01 |
| TmIII |
288 |
−35.27 ± 0.01 |
−24.58 ± 0.01 |
37.03 ± 0.01 |
| 300 |
−35.69 ± 0.02 |
| 310 |
−36.09 ± 0.01 |
| YbIII |
288 |
−35.84 ± 0.01 |
−25.86 ± 0.02 |
34.63 ± 0.01 |
| 300 |
−36.26 ± 0.01 |
| 310 |
−36.60 ± 0.01 |
| LuIII |
288 |
−36.37 ± 0.02 |
−27.11 ± 0.01 |
32.03 ± 0.01 |
| 300 |
−36.72 ± 0.01 |
| 310 |
−37.08 ± 0.01 |
 |
| | Fig. 8 Plots of the absolute value of Gibbs free energy |ΔG| against atomic number Z of LnIII at 288, 300 and 310 K. | |
3.5. The possible mechanism of luminol–lysozyme–LnIII
The possible mechanism of luminol–lysozyme–LnIII was investigated by FI-CL, fluorescence and molecule docking methods.
The possible mechanism of luminol to lysozyme: As Fig. 3 shows, the Tmax of the maximum CL intensity of luminol-dissolved oxygen system shifts from 4.4 s to 4.0 s in the presence of lysozyme with the corresponding intensity changing 3.6-fold, which demonstrated that lysozyme could accelerate the electron transfer rate of excited 3-aminophthalate and enhance the CL intensity of the luminol-dissolved oxygen system. It was found that the fluorescence intensity of 0.5 μmol L−1 luminol (λex/λem = 350 nm/425 nm) was decreased in the presence of lysozyme with its concentrations ranging from 1.0 × 10−9 to 1.0 × 10−6 mol L−1. Using the Stern–Volmer quenching equation,46 the regression equation of F0/F = 2.28 × 105Clysozyme + 1.04 (R = 0.9949) was obtained. The established equation for using a small molecule as the FL probe47 could give the binding constant K (4.2 × 104 L mol−1) and the number of binding sites n (2.18). By molecular docking, it was revealed that luminol could enter the cleft and bind to the active sites of Glu35 and Trp62 on lysozyme with binding distances of 2.2 Å and 2.4 Å.
The possible mechanism of LnIII to lysozyme: by the homemade FI-CL model,37 the obtained binding parameters (K and n) of LnIII to lysozyme were at the 105 to 106 L mol−1 level and around 1.0, which indicates that a 1
:
1 lysozyme–LnIII complex was formed with relatively high binding affinity. It has been reported that some metal ions (e.g. CuII, MnII, PbII, HgII and CoII) could bind to the active site Asp52 of lysozyme,48–50 and it was suggested that LnIII should enter the Asp52 site of lysozyme. The thermodynamic parameters at different temperatures are listed in Table 5; the data support the finding that the reaction of LnIII binding to lysozyme was a spontaneous process with electrostatic interaction.
The possible mechanisms of luminol–lysozyme–LnIII can be explained as follows: lysozyme is a globular protein with the active sites of Glu35, Trp62 and Asp52; as shown in Fig. 9, luminol binds to Glu35 and Trp62 on lysozyme to enhance the CL intensity of luminol and produce the effect of complexation enhancement of CL (CEC); and LnIII should be able to enter Asp52 on lysozyme, which could produce the effect of complexation quenching of CL (CQC).
 |
| | Fig. 9 The possible mechanism luminol–lysozyme–LnIII reaction process. The result was obtained by AutoDock 4.2 (The Scripps Research Institute) pump waste lysozyme mixing tube valve luminol/NaOH carrier LnIII flow cell detector PC. | |
3.6. Determination of LaIII in samples
The five samples were supplied by Dr Zhao's lab in our college and were complex admixtures of La with some organic ligands, and the results for the recoveries ranged from 96.4 to 102.5%, with RSDs less than 2.0%, as listed in Table 6. The same samples were also determined by ICP-AES, and it was found that the results obtained by the proposed CL method agreed well with the ICP-AES results. Comparing the two methods, it can be seen that the proposed CL method was more sensitive than ICP-AES.
Table 6 Results of determination of LaIII in samplesa
| Sample no. |
Added/found ng mL−1 |
RSD% |
Recovery% |
FI-CL μg mL−1 |
ICP-AES μg mL−1 |
| The average of five determinations. Not detected. |
| 1 |
0.0/50.8 |
0.9 |
98.6 |
50.30 ± 0.03 |
50.2 ± 1.6 |
| 50.0/100.7 |
1.0 |
| 2 |
0.0/15.5 |
1.3 |
101.5 |
15.08 ± 0.01 |
15.2 ± 1.9 |
| 15.0/30.2 |
0.9 |
| 3 |
0.0/7.1 |
1.4 |
97.8 |
7.05 ± 0.03 |
NDb |
| 7.0/13.9 |
1.3 |
| 4 |
0.0/3.1 |
1.8 |
96.4 |
2.98 ± 0.01 |
NDb |
| 3.0/6.0 |
1.2 |
| 5 |
0.0/0.5 |
1.4 |
102.5 |
0.51 ± 0.01 |
NDb |
| 0.5/1.0 |
0.9 |
4. Conclusion
The binding abilities of lysozyme to LnIII were studied by a FI-CL method for the first time, and the results showed that the reaction of lysozyme with LnIII was a spontaneous process mainly induced by an electrostatic effect, and the binding affinity increased with increasing Z of LnIII. It was found that A varied as the atomic number Z increased monotonically, and the good correlations for LL and HL in [Xe]4fn configurations were discussed and matched with the lanthanide contraction and the Gd break effect.
Declaration of interest
The authors declare there is no conflict of interest.
Acknowledgements
The authors gratefully acknowledge the financial support from the National Nature Science Foundation of China (no. 21275118) and the Open Funds from the Key Laboratory of Synthetic and Natural Functional Molecule Chemistry of Ministry of Education, China.
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