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A new electroplated Ir/Ir(OH)x pH electrode and its application in the coastal areas of Newport Harbor, California
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Xiao ZHANG1, Ying YE1, Yating KAN1, Yuanfeng HUANG1, Jianjun JIA1, Yue ZHAO1, Chen-Tung Arthur CHEN1, 2, Huawei QIN3, *
Acta Oceanologica Sinica | 2017, 36(5) : 99 - 104
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Acta Oceanologica Sinica | 2017, 36(5): 99-104
A new electroplated Ir/Ir(OH)x pH electrode and its application in the coastal areas of Newport Harbor, California
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Xiao ZHANG1, Ying YE1, Yating KAN1, Yuanfeng HUANG1, Jianjun JIA1, Yue ZHAO1, Chen-Tung Arthur CHEN1, 2, Huawei QIN3, *
Affiliations
  • 1 Ocean College, Zhejiang University, Zhoushan 316000, China
  • 2 Institute of Marine Geology and Chemistry, National Sun Yat-sen University, Kaohsiung 80424, Taiwan, China
  • 3 School of Mechanical Engineering, Hangzhou Dianzi University, Hangzhou 310018, China
Published: 2017-05-01 doi: 10.1007/s13131-017-1064-5
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Resulting from the rising levels of atmospheric carbon, ocean acidification has become a global problem. It has significant impacts on the development, survival, growth and physiology of marine organisms. Therefore, a high-precision sensor is urgently needed to measure the pH of sea-water. Iridium wire with a diameter of 0.25 mm is used as the substrate, and an Ir/Ir(OH)x pH electrode is prepared by a one-step electrochemical method in a LiOH solution at the room temperature. A scanning electron microscope (SEM) observation reveals that it is coated with nanoscale particles. In laboratory tests, the electrode exhibits a very promising pH response, with an ideal Nernst slope (56.14–59.52), fast response, good stability and long life-span in tested pH buffer solutions. For a sea trial, four pH electrodes and one Ag/AgCl reference electrode are integrated with a self-made chemical sensor, and a profile detection of nearly 70 m is implemented near Newport Harbor, California on August 3, 2015. The results reflect that the pH value measured by the sensor is very close to the data given by Sea-Bird 911 plus CTD, with a difference value ranging from 0.000 075 to 0.064 719. And the sensor shows a better data matching degree in 0–40 m water depth. In addition, the high precision and accuracy of the sensor make it possible to use in the ocean observation field.

Ir/Ir(OH)x electrode  /  pH value  /  electroplating  /  Newport Harbor  /  California
Xiao ZHANG, Ying YE, Yating KAN, Yuanfeng HUANG, Jianjun JIA, Yue ZHAO, Chen-Tung Arthur CHEN, Huawei QIN. A new electroplated Ir/Ir(OH)x pH electrode and its application in the coastal areas of Newport Harbor, California[J]. Acta Oceanologica Sinica, 2017 , 36 (5) : 99 -104 . DOI: 10.1007/s13131-017-1064-5
The concentration of global CO2 has increased about 1×10–4 (36%) over the latest 250 a, from a range of 180×10–6 to 285×10–6 in the pre-industrial era (Feely et al., 2004; He et al., 2014) to 391×10–6 in 2014 (Wang et al., 2012). The growth rate of the particle pressure of carbon dioxide (${p_{{\rm{C}}{{\rm{O}}_{\rm{2}}}}}$) in the atmosphere was about 0.5% each year (He et al., 2014), threatening a continually rising ${p_{{\rm{C}}{{\rm{O}}_{\rm{2}}}}}$ level in sea water. It also results in a decline of pH values in sea water, which will make the water acidic.
To enable improved investigation of this global problem of ocean acidification, an accurate and economical sensor is badly needed to measure the pH of sea water. A properly-designed sensor could not only monitor ocean acidification effect on marine organisms and ecosystems, but also play an important role in the development of the marine services, data, information, prediction and global industry (Das and Mangwani, 2015).
In situations where glass electrodes are unsuitable or inconvenient at high temperatures or on a microscale (Cheng et al., 2011; Chen et al., 2007), metal oxide all-solid-state electrodes have shown potential to substitute for glass pH electrodes (Yao et al., 2001). Various solid-state metal oxides have been investigated for pH electrodes, such as TiO2 (Zhao et al., 2010), RuO2 (Maurya et al., 2013), PtO (Kreider et al., 1995), Ta2O5 (Gimmel et al., 1989), WO3 (Yamamoto et al., 2003; Xu and Zhang, 2010), and IrOx (Kim and Yang, 2014). Among these oxides, IrOx and RuO2 were the most prospective electrode materials based on the indication of pH sensitivity, working pH range, ion and redox interferences, and hysteresis (Fog and Buck, 1984).
Several preparation methods for the IrOx (hydrous and anhydrous) electrodes have been reported, including sputtered coating (Tarlov et al., 1990; Kuo et al., 2014), melting method (Ardizzone et al., 1981; Huang et al., 2011), electrochemical growth (Burke and Whelan, 1984; Olthuis et al., 1990), etc. The first two methods resulted in dense and poorly hydrated oxides which are referred to as anhydrous. The thickness and structure of the IrOx film were uneven and not easy to control at the high temperature. And when the electrode got cold, the film would be easily peeled off from the metal substrate as a result of different shrinkage rates of these two layers (Pan and Seyfried Jr, 2008; Han et al., 2009). The damageable characteristic made this kind of pH electrode unable to achieve the anticipated effects in measurements.
A considerable amount of research has focused on the electrochemical growth, for its deposition uniformity and controllability. Using cyclic voltammetry, an anodic iridium oxide film could be deposited in acidic solutions (Burke and Whelan, 1984), while it was a hydrous iridium oxide film in alkaline solutions (Baur and Spaine, 1998; Steegstra and Ahlberg, 2012). However, complicated preparation is an un-resolved problem.
An easily-operated preparation method is introduced in this work. LiOH solution was used as the electrolyte, to fabricate an Ir/Ir(OH)x electrode. Owing to the room temperature fabrication, this film has strong adhesion to the metal substrate. Furthermore, the thickness and structure could be easily controlled by electrochemical parameters.
The electrodes were mounted to an ocean acidification sensor. This was used for measuring the pH value of the sea water near Newport Harbor, California. Fabrication procedure, data processing, surface characterization and calibration results are summed up in this paper.
Iridium wire (99.9%, 0.25 mm in diameter) was purchased from Johnson Matthey Company, USA. Silver wire (99.9%, 0.6 mm in diameter) was obtained from the Precious Materials Company, Changzhou, China. LiOH (99.9%) and NaCl (99.8%) were from Sigma-Aldrich. pH standard buffer solutions of 4.00, 6.86 and 9.18 were prepared with potassium hydrogen phthalate (KHP, obtained from Sinopharm Chemical Reagent) which was dissolved 3.5% NaCl to simulate the salinity of sea water.
All electrochemical studies were made by CHI760D electrochemical workstation (Chenhua Company, Shanghai, China). A scanning electron microscopy (SEM; SU-70, Hitachi, Japan) was used to observe the surface structure of the electrode. Experiments were all performed at an ambient temperature [(25±1)°C].
Iridium wires of about 2–3 cm in length were ultrasonically cleaned in 5 mol/dm3 HCl and de-ionized water alternately for 10 min. To attach the electrode to the detector part on the chemical sensor, gas welding was then used to connect the Iridium wire with a silver wire.
The cyclic voltammetry (CV) method of the CHI760D electrochemical workstation was used to electroplate the Ir(OH)x film on the Iridium wire in 5% LiOH solution, scanning from 0 to 0.7 V at a rate of 50 mV/s for three cycles. In the three-electrode system, the working electrode was the Iridium wire, the reference electrode was a commercial Ag/AgCl, Cl electrode, and the auxiliary electrode was a Pt electrode.
Then the product was rinsed with deionized water and ethanol successively, and naturally dried in air. Finally, the electrode was immersed in 3.5% NaCl solution for at least 4 h for the purpose of improving the activation.
A schematic picture of the ocean acidification sensor is illustrated in Fig. 1a. It has a cylindrical shape with a length of 230 mm and a width of 73 mm (Ding et al., 2015). Titanium alloy was used to fabricate the sensor body because of its excellent high specific strength and corrosion resistance (Huang et al., 2005). The sensor was comprised of several parts: a temperature sensor, communication port and detector part outside and a circuit board for data recording and a battery inside.
Four pH electrodes and an Ag/AgCl reference electrode were all fixed on the detector part (Fig. 1b). The Ag/AgCl reference electrode was prepared by a melting method (Xie and Liu, 1998). Each electrode had a corresponding characteristic position, centered the reference electrode, to dampen the distance effects. The exposed metal rods of the probe were wrapped in two shrinkable tubes and an epoxy resin adhesive layer in sequence. In practical sea trials, a pure copper cap was screwed on the detector part, to get rid of the adhesion of sea creatures to the electrode.
Calibrations were the first step to obtain standard data. Electrodes were run in Tris (pH=8.093 6) (Bates and Erickson, 1986; Dickson, 1993a, b; Whitfield et al., 1985) and Dickson sea water (pH=7.87 60, obtained from University of California, San Diego) for 10 min, respectively. The data processing of the two calibrations will be discussed in Section 4.2.
We started from Newport Harbor of southwest California on August 3, 2015. The sea trial was conducted in the sea area near Newport Beach (Fig. 2). Newport Beach’s climate is greatly moderated by the Pacific Ocean with warm winter temperatures and cooling summer temperatures. Surface water near the beach had a maximum temperature of 24°C and a minimum temperature of 19°C (McLaughlin et al., 2007).
On the threshold of the sea trial, the electrode probes were wrapped in a semi-open cell, to slow down the water scouring. The sensor was strapped to a Sea-Bird 911 plus CTD. Then the two devices were carefully timed and both tuned to a sampling frequency of 8 Hz. When these preparations were completed, a profile detection was implemented at 33°33'28.8''N, 117°52'30.0''W (Fig. 2), by casting CTD down to near 70 m deep, and pulling it up to the deck after a while. The time for calibration, entering the sea, reaching the sea bottom and returning to the sea surface has been manually recorded in Table 1.
Data batched from the sensor were placed in an Excel spread-sheet and was named as OE64-August 3, 2015.
In the raw data table, each line corresponds to one measured data point. The header lists the name of data measured by the sensor, which contain time, counter, potential values (U1) and temperature (T).
To correct the signal intensity against equipment error, one more column was added after U1 and named as U2:
${U_2} = \left({{U_1} - {B_1}} \right)/{A_1}, $
where A1 and B1 are the slope and intercept of correcting equation. For OE64, A1=0.999 8, B1=0.228 6.
After organization as above, part of the data in the file was listed in Table 2.
Data at time of Point 2 (in Dickson sea water) and Point 3 (in Tris solution) in Table 1 were pasted into a new sheet named data-2 in Sheet 2.
The drifting curve and its calibration in Dickson sea water are shown in Fig. 3. The first relative minimum (FRM) is regarded as a reference point, and the one more column (U2) is corrected to a stable value ($ {U_2}^\prime $) with a linear fit.
The calibration in Tris solution works in the same way.
In Sheet 3, with known pH value of Dickson (pH=7.876 0) and Tris standard solutions (pH=8.093 6), the stable value ($ {U_2}^\prime $) in both Dickson and Tris should be corrected by a temperature coefficient:
${U_{25}} = {A_2}\left({25 - T} \right) + {U_2}^\prime, $
where U25 is the signal intensity at 25°C, T is the measured temperature; and A2 is the measured temperature coefficient for certain solutions, which unit is mV/°C. For Dickson, A2=–0.015 1, and for Tris, A2=–0.009 4.
Then a U-pH mapping relationship was built based on the U25 and pH25 in two standard solutions, and the slope (A3) and the intercept (B3) of this linear relationship could be calculated as follows:
${{p}}{{{H}}_{25}}{\rm{ = }}{A_3} \cdot {U_{25}} + {B_3}.$
Based on the U-pH relationship, the measured profile data in Sheet 1 could be calculated as
${{p}}{{{H}}_{in\,\,situ}} =\left({{U_2} - {B_3}} \right)/{A_3}, $
where pHin situ is the pH value at the in situ temperature.
And the pH value at 25°C was calculated as follows:
${{p}}{{{H}}_{25}}{\rm{ =}}{ pH_{in\,\,situ}} - {A_2}\left({25 - T} \right),$
where A2 is the temperature coefficient (–0.015 1 mV/°C) of sea water.
The final calculated results will be discussed in Section 5.3.
The SEM photographs of an Iridium wire and an Iridium wire coated with the Ir(OH)x film are displayed in Figs 4a and b. By comparison, it is found that the Ir(OH)x film formed by in situ electrochemical reaction was dense and compact. The electrode surface was covered by quite small particles with a diameter of 50–200 nm as shown in the photograph after 50 000 magnification. This thin film with nano-sized particles is quite possibly the major reason for the good performance of the electrode as revealed in the next section.
Potentiometric pH measurements were carried out by registering an open circuit potential of an Ir/Ir(OH)x pH electrode against an Ag/AgCl reference electrode (Prats-Alfonso et al., 2013). Figure 5 shows the linear fitting result in pH buffer solutions of 4.00, 6.86 and 9.18. The slopes between the response potential and pH were 56.14–59.52, close to the values predicted by the Nernst Equation (Huang et al., 2015). The correlation coefficients (R2) of these linear regressions were between 0.999 15 and 0.999 99.
Figure 6 shows the calibration process of four pH electrodes and an Ag/AgCl reference electrode in pH buffer solutions. The potential reading was taken for 200 s. Constant signals were obtained promptly after the electrode entered the solution. It took only 5 s to achieve a stable signal as shown in Fig. 3. Compared with the response time of 15 s as reported in the literature (Da Silva et al., 2008), the response of our pH electrodes was faster. In each calibration period of 200 s, the electrode had no obvious signal decay, nor response failure. After enlarging the calibration curve of pH=6.86 in Fig. 6, signals remained extremely stable, with an absolute potential drift of 0.4–2.9 mV and a potential standard deviation of 0.06–0.92 mV.
Accuracy is a required property in pH measurements for practical applications. Dickson sea water was taken to validate the correctness of the electrode. After calibrations in pH buffer solutions of 6.86 and 9.18, pH of Dickson sea water measured by the Ir/Ir(OH)x electrode was 7.875 1, which was in excellent agreement with the actual value (pH=7.876 0). Moreover, the accuracy of the electrode was further confirmed in sea trial results of Section 5.3.
To evaluate the long-term stability of the pH electrode, calibration experiments were performed continuously for 137 days. The Nernst slopes (k) and correlation coefficients (R2) are shown in Table 3. Good pH responses were maintained during the whole period of the life-span test, with Nernst slopes of 57.83–59.80. It indicates that the pH electrode will likely be used for more than 5 months.
The results comparison is shown in Table 4 (the average for every 10 s is shown because of the enormous amount of data). It can be seen that the results of our ocean acidification sensor (OAS) are very close to the data given by Sea-Bird 911 plus CTD (OCSD). The differences in pH values are quite small, and range from 0.000 075 to 0.064 719 pH units. It indicates our OAS can achieve the goal of high precision. Meanwhile, the relationship between the water depth and pH value of these two sensors is clearly shown in Fig. 7. The right-to-left curve is the entire cast process. The red and blue curves represent the results of OAS and OCSD, respectively. The development data trend of 0–40 m water depth demonstrates that the OAS is better than the OCSD, with closer data matching in the two phases.
A novel all-solid-state Ir/Ir(OH)x pH electrode was fabricated by a one-step cyclic voltammetry method. Prepared at the room temperature, the film combined tightly with the Iridium substrate. The SEM photographs indicated that the film was dense and compact. In the performance test, the pH electrode was characterized by ideal Nernst response (56.14–59.52 mV/pH), fast response, good stability and long life-span in pH buffer solutions.
On the basis of the advantage of its small size and easy integration, four Ir/Ir(OH)x pH electrodes and an Ag/AgCl reference electrode were integrated with a chemical sensor. It was used to measure pH values in a California sea area on August 3, 2015, along with the Sea-Bird 911 plus CTD. Processed by our own reliable method, pH values in the entire profile were calculated in Microsoft Excel. The comparison result shows a close relation between these two instruments, with a difference pH value ranging from 0.000 075 to 0.064 719. And the data matching degree of our ocean acidification sensor at 0–40 m water depth was better than that of the Sea-Bird. Therefore, high precision and accuracy are evident for our sensor.
With these features and advantages, the ocean acidification sensor with integrated Ir/Ir(OH)x pH electrodes will have broad application prospects in the field of global ocean observation.
  • The Key Laboratory Project of State Oceanic Administration for Marine Ecosystem and Biogeochemistry of China under contract No. 529101-X21601; the Foundation from Wendy Schmidt Ocean Health XPRIZE and the Southern California Coastal Water Research Project.
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Year 2017 volume 36 Issue 5
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doi: 10.1007/s13131-017-1064-5
  • Receive Date:2016-03-07
  • Online Date:2026-04-14
  • Published:2017-05-01
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  • Received:2016-03-07
  • Accepted:2016-07-27
Funding
The Key Laboratory Project of State Oceanic Administration for Marine Ecosystem and Biogeochemistry of China under contract No. 529101-X21601; the Foundation from Wendy Schmidt Ocean Health XPRIZE and the Southern California Coastal Water Research Project.
Affiliations
    1 Ocean College, Zhejiang University, Zhoushan 316000, China
    2 Institute of Marine Geology and Chemistry, National Sun Yat-sen University, Kaohsiung 80424, Taiwan, China
    3 School of Mechanical Engineering, Hangzhou Dianzi University, Hangzhou 310018, China

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表12种不同金属材料的力学参数

Family
属数
Number of
genus
种数
Number of
species
占总种数比例
Percentage of
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种数
Number of
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Percentage of total
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鹅膏菌科Amanitaceae 2 11 5.26 鹅膏菌属 Amanita 10 4.78
小菇科 Mycenaceae 2 12 5.74 丝盖伞属 Inocybe 5 2.39
多孔菌科 Polyporaceae 8 14 6.70 蜡蘑属 Laccaria 5 2.39
红菇科 Russulaceae 3 23 11.00 小皮伞属 Marasmius 6 2.87
小菇属 Mycena 11 5.26
光柄菇属 Pluteus 5 2.39
红菇属 Russula 17 8.13
栓菌属 Trametes 5 2.39
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