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JOURNAL OF SENSOR SCIENCE AND TECHNOLOGY - Vol. 33 , No. 2
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JOURNAL OF SENSOR SCIENCE AND TECHNOLOGY - Vol. 33, No. 2, pp. 63-69
Abbreviation: J. Sens. Sci. Technol.
ISSN: 1225-5475 (Print) 2093-7563 (Online)
Print publication date 31 Mar 2024
Received 30 Oct 2023 Accepted 07 Nov 2023
DOI: https://doi.org/10.46670/JSST.2024.33.2.63

Solid Electrochemical Method of Measuring Hydrogen Concentration with O2-/H+ Hetero-Ionic Junction
Chongook Park1, +
1PSS Inc. Unit 206, Building B, Techno 4-ro, Yuseong-gu, Daejeon, Republic of Korea

Correspondence to : +copark@kaist.ac.kr


This is an Open Access article distributed under the terms of the Creative Commons Attribution Non-Commercial License(https://creativecommons.org/licenses/by-nc/3.0/) which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.
Funding Information ▼
Abstract

A novel method for measuring hydrogen concentration is introduced, along with its working principle and a novel detection algorithm. This configuration requires no additional reference compartment for potentiometric electrochemical measurements; therefore, it is the most suitable for measuring dissolved hydrogen in the liquid phase. The sensor’s electromotive force saturates at a certain point, depending on the hydrogen concentration during the heating process of the sensor operation. This dynamic temperature scanning method provides higher sensitivity than the constant temperature measurement method.

Keywords: Solid electrolyte, Hydrogen, Sensor, Proton conductor, Oxygen ion conductor
1. INTRODUCTION

The dominant energy source changes from carbon to hydrogen someday [1]. Hydrogen detection and concentration measurement are necessary during production, storage, and transportation in this emerging hydrogen economy. Therefore, there is an ongoing need for faster, more durable, more accurate, and more selective hydrogen gas detection in various industrial areas to monitor and control hydrogen concentration. For example, monitoring the hydrogen gas concentration is important in the synthesis of chemicals such as ammonia, methanol, and rocket fuels in the Al foundry, in the welding and galvanic plating processes to avoid hydrogen embrittlement, in the detection of impending electric transformer failure, in the lighting industry to check the hydrogen impurities in krypton, xenon, and neon, and in nuclear power plants to prevent hydrogen explosions.

Many commercially available sensors have been reported for hydrogen detection. According to their operating principles, these can be classified as chemoresistive sensors [2-4], fuel cell sensors [5,6], FET sensors [7], Pd resistor sensors [8], and mixed potential sensors [9]. Each type has advantages and disadvantages and serves well in its applications. However, it may be difficult to find an appropriate hydrogen sensor in harsh environments, such as high temperatures or polluted sites. The measurement of dissolved hydrogen in hot melts or volatile industrial oils may be such a case.

Iwahara [10] first adopted a proton-conducting solid electrolyte, CaZr0.9In0.1O3-x (CZI), to build a hydrogen sensor for an Al melt. In this potentiometric configuration, hydrogen gas with a known concentration must flow into the reference compartment to detect the dissolved hydrogen in the Al melt. Later, Schwandt [11] introduced a solid-state hydrogen sensor with a solid reference to a Ti and TiHx mixture in an Al melt. This study introduced a novel solid electrochemical hydrogen sensor that operates without a flowing reference gas. To operate this sensor, a novel sensing method is devised whereby a momentary electromotive force (EMF) is detected along with its temperature while the sensor is being heated for a given hydrogen concentration, which is called the dynamic temperature scanning method (DTSM) here.

1.1 Operating Principle

The newly developed structure of the hydrogen measuring cell can be written as

-H2, Pt CaZr0.9In0.1O3-xHy∥YSZPt, Air O2(+)(1) 

The oxygen ions are in equilibrium with the oxygen at the Pt/YSZ electrode via Eq. 2 and combine with protons in the proton conductor to form a so-called water potential at the YSZ (yttriastabilized zirconia)/CZI (CaZr0.9In0.1O3-δ) interface as in Eq. 3. At the working electrode, hydrogen in the gas phase and protons on the CZI surface maintained equilibrium with the electrons in Pt, as expressed in Eq. 4.

12O2+2e-Pt=O2-YSZ(2) 
2H+CZI+O2-YSZ=H2O(3) 
H2=2H+CaZr0.9In0.1O3-δ+2e-Pt(4) 
H2+12O2=H2O(5) 

According to the Nernst relation, the EMF of electrochemical Cell 1 can be represented as: E = –∆G/2F

E=-ΔGH2Oo2F-RT2Fln⁡aH2OPH2PO21/2(6) 

where ∆GoH2O J/mol [20], F, aH2O, PH2, and P1/2O2 are the standard Gibbs free energy of water formation, Faraday constant, activity of water at the YSZ/CZI interface, hydrogen partial pressure at the measuring electrode, and oxygen partial pressure at the reference electrode, respectively.

The reference electrode can be either a Pt/YSZ electrode simply exposed to open air or contained in a closed chamber that is hermetically sealed and filled with a metal and metal oxide mixture, such as CuO/Cu2O and Ni/NiO, to maintain a constant oxygen pressure.

The water activity at the CZI/YSZ interface was experimentally measured by changing both temperature and hydrogen environment with the known value of ∆GoH2O [12]. They demonstrated almost constant values within the tested ranges of temperature and hydrogen concentration, as illustrated in Fig. 1. However, the thermodynamic activity of water in the proton conductor could not be fixed [13]. Water is believed to be formed at the YSZ/CZI interface, which is determined by the oxygen ions in the YSZ and protons in the CZI. They are tightly bonded and resistant to small perturbations. Further studies on this interface are required. Therefore, for constant aH2O and pO2 =0.21, Eq. 6 can be simplified as


Fig. 1. 
Change of water potential at interface with hydrogen pressure at different temperatures

E=E0'+RT2Fln⁡PH2(7) 

where E'0 corresponds to (-∆GoH2O/2F-RT/2F In aH2O+RT/4F In PO2). Because ∆Go=∆Ho-T∆So, E'0 would be a function of temperature. It experimentally demonstrates a small dependence on temperature with a slope of -2.46 × 10-4, as illustrated in Fig. 2 [14], which is close to the thermodynamically calculated value (=∆SoH2O/2F) of -2.89 × 10-4. Consequently, the cell EMF can be expressed by Eq. 8.


Fig. 2. 
E'0 as function of temperature.

E=A+BT+CTIogpH2(8) 

where A, B, and C are sensor constants. According to Eq. 8, the EMF is a function of the temperature and hydrogen pressure. Thus, hydrogen concentration can be calculated by substituting the measured temperature and EMF into Eq. 8 with known sensor constants A, B, and C.

1.2. General Gas Response of Sensor

The sensor responds quite well to changes in hydrogen gas concentration from 0.1% to 10% H2 in nitrogen for a wide temperature ranging from 650 to 800 oC in the laboratory test as illustrated in Fig. 3(a). Plotting the EMF vs according to Eq. 8 for a given temperature exhibited good Nernstian behavior with an almost theoretical slope, as illustrated in Fig. 3(b).


Fig. 3. 
EMF response of Cell 1 at temperature ranging from 650 to 800 o]C: (a) transient behavior and (b) EMF vs logarithm of hydrogen partial pressure.

2. EXPERIMENTAL

A heterojunction sensor was fabricated by attaching a CZI pellet to the tip of a YSZ tube, as illustrated in Fig. 4(a). The vertical furnace was maintained at the desired temperature and a known concentration of hydrogen gas was introduced from the bottom, as illustrated in Fig. 4(b). As soon as the gas environment stabilized in a quartz tube placed inside the furnace, the sensor was immersed in a quartz tube to measure the EMF and temperature of the sensor with a data logger (Agilent 34970A). The typical behavior of the EMF and temperature of the sensor is illustrated in Fig. 4(c), where the temperature is on the right side and the EMF is on the left side. From a series of measurements, we obtained data for the corresponding hydrogen concentration, for example, Ei, Ti, and %H2.


Fig. 4. 
(a) hetero ionic junction Sensor, (b) sensor testing set-up and (c) data acquisition

2.1 Mathematical Understanding of Response

As indicated in Eq. 8, the output from Sensor E is a function of T and log[H2] with three constants: A, B, and C. Assuming a known hydrogen concentration, Eq. 8 becomes a function of T and is expressed as

E=A+Clog⁡H2+B/CT=A+B'T(9) 

where log[H2] is no longer a variable but a constant. Thus, depending on the hydrogen concentration, the EMF followed a different dotted line in the E vs. T plot, as illustrated in Fig. 7(a). The isohydrogen concentration line (dotted line) increased with the hydrogen concentration. Similarly, for Constant T, Eq. 8 can be rearranged as a function of log[H2] as follows.


Fig. 7. 
(a) E vs T and (b) E vs x(=log[H2]+B/C)


Fig. 8. 
Sensor EMF as function of T and -x

E=A+CTlog⁡H2+B/C(10) 

For simplicity, if log[H2]+B/C is set to x, Eq. 10 becomes a first-order linear equation of E=A+C′x where C′= C{log[H2]+B/ C}. Accordingly, it gives isothermal lines (dotted) on which the EMF varies with hydrogen concentration at a given temperature, as illustrated in Fig. 7(b). As the temperature increases, the isothermal lines decrease.

In summary, the 3D shape of the sensor output EMF in Eq. 8 may be expressed as a twisted plane in the T-x space, where the projection to the E-T plane gives Eq. 7, and the projection to the E-x plane (-x is utilized here for convenience) becomes Fig. 7(b). All the EMFs measured from the hetero-ionic junction sensor were placed on this twisted plane. The projections of the measured data into the E-T and E-x spaces give the linear lines in Figs. 7(a) and (b), respectively.

2.2 Phenomenological Understanding of Response

When the sensor was immersed in the heated vertical furnace, the sensor’s temperature (right axis) increased; accordingly, the EMF (left axis) varied. Typical EMF and temperature behaviors are presented in Fig. 9. This is the case where the sensor is dipped in a chamber at 600 oC with a gas phase of 2%H2–98%N2. EMF starts to rise from around 250 oC, and there appears to be a jump at approximately 110 to 200–500 mV (Region I), but this depends on the environment to which the sensor is exposed. A high H2 concentration environment resulted in a larger jump than that in a low H2 concentration environment. Subsequently, at least three humps (Regions II, III, and IV) appear before the final steady-state EMF is reached. This differs from the EMF behavior obtained from the YSZ oxygen sensor, which exhibits a smoothly rising curve [15]. In a high H2 concentration environment, Region III often disappears.


Fig. 9. 
Typical EMF and temperature behaviors of sensor immersed in system in 2%H2-N2 atmosphere at 600 oC.

This phenomenon is suspected to be related to the following two-step process. In the early stage of Region Ⅱ, the oxygen and the incoming hydrogen react together to make a surface oxygen adsorbate and proton by the reaction:

12O2+H2=OOX surface +2H++2e(11) 

The proton in Reaction 11 gives an early EMF of Region Ⅱ at a temperature of around 250–400 oC. As the sensor’s temperature increases with time, two possible processes may occur that produce a measurement output in late Stages III and IV. The first possibility is that as oxygen is depleted near the CZI, the incoming hydrogen starts to react with the oxygen adsorbate in Eq. 11 to produce oxygen vacancies (Vo··) by the reaction:

OOX( surface )+H2=VO∙∙+H2O+2e(12) 

The oxygen vacancies in Reaction 12 produce Region III or IV EMF wave depending on the hydrogen concentration in the melt.

The second possibility is the equilibrium reaction at the electrode between hydrogen and the proton on CZI, as indicated in Reaction 13.

H2=2H++2e(13) 

The proton in Eq. 13 results from the oxygen vacancies formed by the substitutional reaction of In into the Zr sites in CaZrO3, as expressed in Eq. 14.

In2O3=2InZr'+3OOX+VO∙∙(14) 

These oxygen vacancies play a role in converting hydrogen gas into protons via the following reaction.

H2+Vo¨=2HO¨(15) 

where (2H)O is proton bound to oxygen vacancy.

3. RESULTS AND DISCUSSION

We ran ten sets resultsf experiments, as presented in Table 1, by immersing the sensor into the preheated furnace of Fig. 4(b) to obtain the corresponding sets of EMF and temperature for a given hydrogen concentration ranging from 2% to 9%. The measurements were performed by obtaining the EMF, Es, and the corresponding temperature, Ts, when the EMF was stabilized. In contrast, the sensor’s temperature increased upon dipping the sensor into the furnace. Here, the sensor was inserted into the furnace at two different temperatures of 600 and 650 oC to give a different heating rate.

Table 1. 
Ten sets of EMFs and temperatures measured from two different reactor conditions and changing hydrogen concentration from 2% to 9%.
Experiment Number Injected [H2] Ts(K) Es(mV)
1 2% 849 952
2 2% 888 930
3 4% 837 969
4 4% 857 966
5 5% 804 997
6 5% 866 970
7 7% 791 1019
8 7% 819 1000
9 9% 778 1033
10 9% 815 1017

Interestingly, the dataset of Tsij and Esij obtained from the DTSM lines up on a straight line in the Es vs. Ts plot, as illustrated in Fig. 10(a) and 7(a). We utilized the average value for each hydrogen concentration. Furthermore, Es vs. log[H2] demonstrated a nearly straight line, as illustrated in Fig. 10(b) and 7(b).


Fig. 10. 
(a) Es plotted on T axis and (b) Es vs log[H2]

We created more datasets and plotted them in the 3D space of E-T-log[H2], as illustrated in Fig. 11. The data points appeared to lie on a flat plane rather than a twisted plane. Our experimental conditions were so narrow that it was assumed they sat on a plane.


Fig. 11. 
Plot of (Ei,Ti, log[H2]i) in 3-D space of T-log[H2]-E

In this case, we can obtain A, B, and C analytically from Eq. 8, by solving the following differential equation:

dE/dT=K(13) 

with two boundary conditions of

E=Mlog⁡H2+L(14) 
T=αlog⁡[H2]+β(15) 

Here, K can be obtained from the experimental data in Fig. 10(a), and M and L can be obtained from Fig. 10(b). And α and β can also be obtained by plotting data on the E vs log[H2] diagram. Therefore, the hydrogen concentration can be obtained utilizing Eq. 16, as long as we clear K, M, L. α, and β from the experiment.

LogH2=(E-KT-L+βK)/(M-αK)(16) 

Fig. 12. 
(a) EMF as function of temperature for different hydrogen concentrations and (b) (Es, Ts) plotted on E-T space.

4. CONCLUSIONS

A heterojunction solid electrochemical sensor responds selectively to hydrogen gas over 400 oC. It demonstrates a stable interfacial structure of YSZ/CZI irrespective of temperature and hydrogen atmosphere and gives an output expressed as E= A + BT + CT log[H2]. Generally, the EMF behavior exhibits a jump and three humps before reaching a final value corresponding to the relevant hydrogen concentration. This may have resulted from the reaction of hydrogen with the remaining oxygen to form an oxygen adsorbate.

The configuration of the heterojunction sensor is convenient for measuring dissolved hydrogen in the liquid phase because its simple reference electrode arrangement makes a hermetically sealed chamber easy. In addition, because all components are made of stable oxide ceramics, they can withstand harsh environments. The heterojunction sensor is expected to be applied in a wide variety of areas owing to its versatility and simplicity of structure, for example, as a hydrogen sensor for leakage detection, dissolved hydrogen measurement for molten Al alloys, dissolved hydrogen gas analysis for transformer oil, etc.

Acknowledgments

This work was supported by the Daedok Innopolis R&BD Project and the MSIT as GFP/CISS 2011-0031870. I would also like to thank Prof. H. J. Yoo for the helpful discussions on the derivation of the mathematical algorithm.

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