Articles
  • Characterization of NiFe2O4/Ce0.9Gd0.1O1.95 composite as an oxygen carrier material for chemical looping hydrogen production
  • Jong Ha Hwanga and Ki-Tae Leeb,c,*

  • aDepartment of Mineral Resources & Energy Engineering, Jeonbuk National University, Jeonbuk, 54896 Republic of Korea
    bDivision of Advanced Materials Engineering, Jeonbuk National University, Jeonbuk, 54896 Republic of Korea
    cHydrogen and Fuel Cell Research Center, Jeonbuk National University, Jeonbuk, 54896 Republic of Korea

Abstract

We investigated NiFe2O4/Ce0.9Gd0.1O1.95 (GDC) composites as oxygen carrier materials for chemical looping hydrogen production (CLHP). CLHP is a promising technology to simultaneously capture carbon dioxide and produce hydrogen from fossil fuels. We found that increasing GDC content increased the amount of the hydrogen production of NiFe2O4/GDC composites. Moreover, the oxygen transfer rate for the re-dox reaction increased significantly with increasing GDC content. GDC may affect the reaction kinetics of NiFe2O4/GDC composites. The finely dispersed GDC particles on the surface of NiFe2O4 can increase the surface adsorption of reaction gases due to the oxygen vacancies on the surface of GDC, and enlarge the active sites by suppressing the grain growth of NiFe2O4. The NiFe2O4/15wt% GDC composite showed no significant degradation in the oxygen transfer capacity and reaction rate during several re-dox cycles. The calculated amount of hydrogen production for the NiFe2O4/15wt% GDC composite would be 2,702 L/day per unit mass (kg).


Keywords: Chemical looping hydrogen production, oxygen carrier material, re-dox reaction, oxygen transfer capacity, oxygen transfer rate

introduction

With the depletion of petroleum resources and the global warming phenomenon, interest in developing alternative energy sources is increasing. Hydrogen is known as a clean energy source because it emits only water during combustion and has high energy density [1-4]. Therefore, the development of efficient hydrogen production technology is becoming increasingly popular. As the use of fossil fuels increases, the emission of carbon dioxide is also increasing. Carbon dioxide contributes significantly to the greenhouse effect [5]. Therefore, various carbon capture and storage (CCS) technologies have been developed to reduce carbon dioxide emissions [6-8].
Chemical looping hydrogen production (CLHP) is a technology capable of capturing carbon dioxide at a concentration of 99% or more and simultaneously producing hydrogen at a concentration of 99% or more from fossil fuels [9-13]. While other hydrogen production technologies, such as the reforming of hydrocarbon fuel, requires the membrane separation process to obtain pure hydrogen from syngas, CLHP does not require a hydrogen separator, a pressure swing adsorption (PSA), or a carbon dioxide capture device, resulting in high efficiency.
A CLHP system consists of an air reactor, fuel reactor, and steam reactor, as shown in Fig. 1. In the air reactor, the metal (Me) reacts with oxygen in the air to become metal oxide (MeO).
 
2Me (s) + O2 (g) → 2MeO (s) (exothermic reaction)
                                                                                           (1)
 
In the fuel reactor, the fuel such as CH4 reacts with the metal oxide (MeO). The metal oxide is reduced to metal (Me) and the fuel is burned to discharge carbon dioxide and water.
 
4MeO (s) + CH4 (g) → 4Me (s) + CO2 (g) + 2H2O (g)
(endothermic reaction)                                       (2)
 
In the steam reactor, the metal (Me) reacts with water to form metal oxide (MeO) and generate hydrogen.
 
Me (s) + H2O (g) → MeO (s) + H2 (g)
(exothermic reaction)                                                             (3)
 
In the above reactions, the metal oxide undergoing the re-dox reaction is called an oxygen carrier material. The transition metal oxide is usually used as an oxygen carrier material for CLHP. In the CLHP process, the oxygen carrier material plays an important role not only in transferring the oxygen required for combustion, but also in splitting water to produce hydrogen. Therefore, it is very important to develop high-performance oxygen carrier materials with high oxygen transfer rates, high oxygen transfer capacities, and excellent catalytic activity for water splitting. Oxides of Cu, Ni, Mn, and Sn have been used as oxygen carrier materials in CLHP. Among these metal oxides, Fe-based oxygen carrier materials have the advantages of high oxygen transfer capacity, low carbon deposition, lack of environmental harm, and low cost [14-16]. However, a conventional Fe-based oxygen carrier material such as Fe2O3 experiences grain growth with re-dox cycling, leading to a decrease in the surface area and consequent reduction of conversion efficiency [17]. It has been reported that the NiFe2O4 spinel phase at high temperatures exhibited higher oxygen transfer capacity and stability than individual Fe2O3 [18, 19]. Although NiFe2O4 exhibits oxygen carrying stability with a high oxygen transfer capacity during re-dox cycling, it still has slow re-dox reaction kinetics compared to conventional oxygen carrier materials.
To improve the re-dox reaction kinetics of NiFe2O4, in the present work we added gadolinium-doped ceria (GDC, Ce0.9Gd0.1O1.95) as a promoter to improve the oxygen transfer rate. It is well known that GDC has oxygen storage capability due to its formation of oxygen vacancies, and GDC has thus been widely used as a catalyst [20, 21]. Therefore, the addition of GDC may enlarge the reaction site. The present report describes our systematic investigation of the effects of GDC as a promoter upon the oxygen transfer properties of NiFe2O4/GDC composite oxygen carrier materials for CLHP.

Fig. 1

Schematic of CLHP system.

experimental procedure

NiFe2O4 powder was synthesized by a solid-state reaction method. Stoichiometric amounts of NiO (Alfa Aesar, UK) and Fe2O3 (Alfa Aesar, UK) were mixed by ball milling in ethanol for 48 h, followed by calcination in air at 1,200 °C for 3 h. To make NiFe2O4/GDC composite oxygen carrier materials, the calculated amount of commercial GDC (Ce0.9Gd0.1O1.95, Kceracell Co. Ltd., Korea) powder was mixed with the synthesized NiFe2O4 powder by a ball milling process. NiFe2O4/GDC composite powders with various amounts of GDC (0, 5 10, 15 wt %) were prepared by ball milling with zirconia balls for 24 h in ethanol, and the resulting mixtures were dried at 150 °C for 12 h.
Phase analysis was carried out by means of X-ray diffraction analysis (XRD; MAX-2500, Rigaku, Japan) using a Cu Kα radiation source. Diffraction patterns were recorded at the scan rate of 4°/min in the 2θ range of 20° to 80°. The composition of the reduced sample was confirmed by X-ray flourescence spectrometer (XRF; PW2404, Philips, USA). The valence state of Fe in the sample was analyzed by X-ray photoelectron spectroscopy (XPS; AXIS Ultra DLD Kratos, UK) with monochromatic Al Kα. The morphological changes during the re-dox cycle were monitored using a field emission scanning electron microscope (FE-SEM; SN-300, Hitachi, Japan).
Temperature programed reduction (TPR) and temperature programed oxidation (TPO) were carried out with gas chromatography (GC; YL6100GC, Youngin, Korea) to analyze the reduction and oxidation of NiFe2O4/GDC composite oxygen carrier materials depending on the temperature. The temperature was increased from room temperature to 900 °C at a heating rate of 3 °C/min. 5% H2/Ar and 10% H2O/Ar were used as the reducing and oxidizing gases, respectively. The re-dox cycling tests were also carried out with GC. The temperature was raised to 900 °C at 10 °C/min in an Ar atmosphere and maintained for 12 h. When the temperature reached 900 °C, 5% H2/Ar for reduction and 10% H2O/Ar for oxidation were alternately poured for 1 h. Ar was purged between each reduction and oxidation step for 1 h.
The oxygen transfer properties of the NiFe2O4/GDC composite oxygen carrier materials based on the re-dox reaction were evaluated by means of thermal gravimetric analysis (TGA; TGA-N1000, Shinko, Korea) at 900 °C. 5% H2/Ar and air were used as the reducing and oxidizing gases, respectively. Between each reduction and oxidation step, the reactor was purged with Ar for 3 min to prevent mixing of the reducing and oxidizing gases.

results and discussion

The XRD patterns of the NiFe2O4 samples synthesized and reacted with various gases are shown in Fig. 2. NiFe2O4 powder synthesized at 1,200 °C for 3 h in air was formed in a single phase of spinel without any detectable impurity, and the diffraction peaks matched well with those of NiFe2O4 (JCPDS No. 00-010-0325). Since the product gases for CH4 are H2O and CO2, as described in Eq. (2), oxygen carrier materials are exposed to a CO2-rich atmosphere in the fuel reactor. As shown in Fig. 2, no carbonate phases such as NiCO3 or FeCO3 were observed after the reaction with CO2. Therefore, NiFe2O4 was not influenced by CO2 in the fuel reactor at 900 °C. Meanwhile, the NiFe2O4 powders reacted with H2 and CH4 at 900 °C for 1 h showed a single phase of (Ni,Fe) alloy. In the case of CH4, carbon peaks due to a methane cracking reaction (CH4 → C + 2H2) were detected.
To confirm the re-dox mechanism of NiFe2O4, phase analysis was carried out after reduction in H2 followed by oxidation in air or H2O. The (Ni,Fe) alloy, which was the NiFe2O4 sample reduced in H2, did not return to NiFe2O4 after re-oxidation in air, as shown in Fig. 3. If the (Ni,Fe) alloy was a stoichiometric compound such as NiFe2, the re-oxidized (Ni,Fe) alloy sample must have been a single phase of NiFe2O4. However, the sample re-oxidized in air showed two phases of NiFe2O4 and Fe2O3. Therefore, the (Ni,Fe) alloy was formed in the Fe-rich composition such as NixFe2 (0 < x < 1). This can be confirmed by the XRF data, as shown in Table 1. It has also been reported that Ni can be volatilized in the presence of H2O at high temperatures [22].
The reduction of NiFe2O4 took place as a stepwise process, and the following pathway is suggested: NiFe2O4 → Ni-Fe2O3 → Ni-Fe3O4 → Ni-FeO → Ni-Fe [23]. Based on the composition and phase analysis, the reduction mechanism of NiFe2O4 at 900 °C can be described as follows.
 
NiFe2O4 (s) + H2 (g) → xNi (s) + Fe2O3 (s)
+ H2O (g) + (1-x)Ni (g)                                             (4)
Fe2O3 (s) + 1/3H2 (g) → 2/3Fe3O4 (s) + 1/3H2O (g)
                                                                                                        (5)
 
2/3Fe3O4 (s) + 2/3H2 (g) → 2FeO (s) + 2/3H2O (g)
                                                                                                        (6)
 
2FeO (s) + 2H2 (g) → 2Fe (s) + 2H2O (g)                                                                          (7)
 
Therefore, the overall reduction reaction in H2 is as follows.
 
NiFe2O4 (s) + 4H2 (g) → xNi (s) + 2Fe (s) + 4H2O (g)
+ (1-x)Ni (g)                                                                         (8)
 
= NiFe2O4 (s) + 4H2 (g) → NixFe2 (s) + 4H2O (g)
+ (1-x)Ni (g)                                                                         (9)
 
When NixFe2 was oxidized in air, the products were NiFe2O4 and Fe2O3 as shown in Fig. 3. Therefore, the reduced NiFe2O4 (NixFe2) reacted with oxygen in the air to induce the oxidation reaction as follows.
 
xNi (s) + x/2O2 (g) → xNiO (s)                                                                                                     (10)
 
2Fe (s) + O2 (g) → 2FeO (s)                                                                                                         (11)
 
2FeO (s) + 1/3O2 (g) → 2/3Fe3O4 (s)                                                                                (12)
 
2/3Fe3O4 (s) + 1/6O2 (g) → Fe2O3 (s)                                                                               (13)
 
The overall oxidation reaction in air is as follows.
 
xNi (s) + 2Fe (s) + (3+x)/2O2 (g) → xNiO (s)
+ Fe2O3 (s)                                                                                         (14)
 
= NixFe2 (s) + (3+x)/2O2 (g) → xNiFe2O4 (s)
+ (1-x)Fe2O3 (s)                                                                    (15)
Meanwhile, it has been reported that reduced nickel oxide or metallic nickel are difficult to oxidize by steam due to thermodynamic limitations [14,19,23,24]. Therefore, most of the reduced nickel ferrite can only be oxidized to be a mixture of Fe3O4 and Ni under steam. This result corresponds to the existence of Fe3O4 and Ni phases in our sample oxidized in H2O, as shown in Fig. 3. In the steam reactor, NixFe2 reacted with H2O to induce the oxidation reaction as follows.
 
xNi (s) → xNi (s)                                                                                                                                     (16)
 
2Fe (s) + 2H2O (g) → 2FeO (s) + 2H2 (g)                                                                          (17)
 
2FeO (s) + 2/3H2O (g) → 2/3Fe3O4 (s) + 2/3H2 (g)
                                                                                                        (18)
 
The overall oxidation reaction in steam is as follows.
 
xNi (s) + 2Fe (s) + 8/3H2O (g) → xNi (s) + 2/3Fe3O4 (s)
+ 8/3H2 (g)                                                              (19)
 
= NixFe2 (s) + 8/3H2O (g) → xNi (s) + 2/3Fe3O4 (s)
+ 8/3H2 (g)                                                                           (20)
 
When the oxygen carrier material oxidized in the steam reactor flowed into the air reactor, un-reacted Ni and Fe3O4 became fully re-oxidized by oxygen as follows.
 
xNi (s) + x/2O2 (g) → xNiO (s)                                                                                                     (21)
 
2/3Fe3O4 (s) + 1/6O2 (g) → Fe2O3 (s)                                                                               (22)
 
The overall re-oxidation reaction in air after the oxidation in steam is as follows.
 
xNi (s) + 2/3Fe3O4 (s) + (1+3x)/6O2 (g) → xNiO (s)
+ Fe2O3 (s)                                                                           (23)
 
= xNi (s) + 2/3Fe3O4 (s) + (1+3x)/6O2 (g) →
xNiFe2O4 (s) + (1-x)Fe2O3 (s)                            (24)
 
XPS analysis was also performed in order to verify the valence state of Fe in NiFe2O4 before and after the oxidation reaction at 900 °C for 1 h. The XPS spectra obtained for the various atmospheres are shown in Fig. 4. The binding energies of Fe 2p3/2, Fe 2p3/2 satellite, and Fe 2p1/2 in Fe2O3 are 711.0, 718.8, and 724.6 eV, respectively [25]. The peak positions of Fe 2p3/2, Fe 2p3/2 satellite, and Fe 2p1/2 in NiFe2O4 in this study were observed at 711.0, 719.1, and 724.3 eV, respectively, which indicates that the valence state of Fe in NiFe2O4 is 3+. Moreover, Dey et al. reported that the deconvolution of the Fe 2p peak of the NiFe2O4 into two components correspond to the octahedral 2p3/2 and 2p1/2 peaks, and the tetrahedral 2p3/2 and 2p1/2 peaks [26]. The results are consistent with this study and indicate the absence of Fe2+ component and confirmation of the oxygen stoichiometric compound. Alternatively, in the case of the sample oxidized in 10% H2O/Ar, the peaks of Fe2+ (Fe 2p3/2) and Fe2+ (Fe 2p1/2) were identified at 710.2 and 723.7 eV, respectively. These results correspond to the peak positions of Fe3O4 [25], indicating that the valence state of Fe in the sample oxidized in 10% H2O/Ar is a mix of 2+ and 3+. Interestingly, the peak positions of Fe 2p3/2, Fe 2p3/2 satellite, and Fe 2p1/2 in the sample re-oxidized in air are identical to those of Fe2O3 and NiFe2O4.
The reduction and oxidation properties of NiFe2O4/GDC composite oxygen carrier materials were determined by H2-TPR and H2O-TPO, as shown in Fig. 5. It has been reported that Fe2O3 exhibits a three-step reduction mechanism, with one reduction peak at a lower temperature (360-415 °C) corresponding to the reduction of Fe2O3 → Fe3O4, and two broad reduction peaks at 500-750 °C and 800-900 °C corresponding to reduction steps of Fe3O4 → FeO and FeO → metallic Fe, respectively [27-29]. It has been also reported that the H2-TPR pattern of bulk NiO consists of one broad peak in the range of 327 to 677 °C with a maximum peak at 409 °C. The results in the present study (Fig. 5a) were in good agreement with the previous works, which indicates that the established reduction mechanism is plausible. In particular, the peak corresponding to the reduction steps of Fe3O4 → FeO shifted to the low-temperature region with increasing GDC content. Based on the H2-TPR data, it can be concluded that the reduction reactivity of the NiFe2O4/GDC composite slightly increased with increasing the amount of GDC. Similarly, based on the H2O-TPO data (Fig. 5b), it is expected that the amount of oxidation reaction as well as the oxidation reactivity of NiFe2O4/GDC composite will increase with increasing the GDC content.
The XRD patterns of NiFe2O4/GDC composites before and after H2-TPR and H2O-TPO tests are shown in Fig. 6. All the XRD peaks of the samples before H2-TPR and H2O-TPO tests (Fig. 6a) were matched with those of NiFe2O4 or GDC, with no traces of secondary peaks. On the contrary, since the reduced NiFe2O4 (NixFe2) in the NiFe2O4/GDC composites during the H2-TPR test was oxidized to be a mixture of Ni and Fe3O4 under steam during the H2O-TPO test, both Ni and Fe3O4 peaks were detected after H2-TPR and H2O-TPO tests (Fig. 6b). Interestingly, CeFeO3 was observed in the samples containing GDC. Mahmoodi et al. [30] also reported the formation of CeFeO3 in the Fe2O3-CeO2 oxygen carrier system during the re-dox cycle.
The microstructures of NiFe2O4/GDC composites before and after H2-TPR and H2O-TPO tests are shown in Figs. 7 and 8. All the samples had a porous structure before H2-TPR and H2O-TPO tests (Fig. 7a-d), and the fine GDC particles were evenly distributed over the NiFe2O4 particles (Fig. 7b-d). Notably, the NiFe2O4 sample without GDC exhibited severe agglomeration after the H2-TPR and H2O-TPO tests (Fig. 8a), while the well-dispersed GDC particles in the NiFe2O4/GDC composites (Fig. 8b-d) suppressed the aggregation of NiFe2O4 particles and maintained the porous structure.
Fig. 9 shows the amount of H2 consumption and production at 900 °C in the fuel reactor with 5% H2/Ar and in the steam reactor with 10% H2O/Ar, respectively. After the first cycle, the amount of H2 consumption decreased significantly (Fig. 9a). This indicates that the reduced NiFe2O4 (NixFe2) could not be fully oxidized to NiFe2O4 by H2O. This may be ascribed to the deactivation problem caused by the agglomeration of Ni. The oxidation-reduction reaction was limited to only a part of the agglomerated Ni surface after the first cycle. The amount of H2 production in each cycle (Fig. 9b) was similar to that of H2 consumption in the second and third cycles (Fig. 9a), while the amount of H2 consumption and production of the NiFe2O4/GDC composites in the fuel and the steam reactor, respectively, increased with increasing GDC content. This might have been due to the suppression of agglomeration by the well-dispersed GDC particles, as shown in Fig. 8.
The maximum reaction rates of the NiFe2O4/GDC composites, as shown in Fig. 10, were also similar to the amount of H2 consumption (Fig. 9a) and production (Fig. 9b) for the re-dox reaction. Because the re-dox reaction rate increased in proportion to the number of active sites where H2 or H2O could react, the maximum reaction rates for the reduction (Fig. 10a) and oxidation (Fig. 10b) increased with increasing GDC content.
We used TGA to evaluate the oxygen transfer properties of the NiFe2O4/GDC composite oxygen carrier materials based on the re-dox reaction between the fuel and air reactors. Re-dox curves of the NiFe2O4/GDC composites at 900 °C with 5% H2/Ar and air used as the reducing and oxidizing gases, respectively, are shown in Fig. 11. The empirical oxygen transfer capacity of NiFe2O4 was 24.7 wt% at the first cycle, which was similar to the theoretical value of 27.3 wt% based on Eq. (9). However, in the case of NiFe2O4 without GDC, the weight gain observed during oxidation was much smaller than the weight loss during reduction, indicating that the re-dox reaction was irreversible. This indicates that the oxygen transfer capacity of pure NiFe2O4 degraded significantly during the re-dox cycle. In contrast, the NiFe2O4/15wt% GDC composite showed a full recovery of weight during oxidation.
The oxygen transfer rate (dX/dt), referring to the change in the conversion rate per unit time, can be calculated from TGA data (Fig. 11). Fig. 12 shows the oxygen transfer rate of the NiFe2O4/GDC composite for reduction and oxidation reactions, respectively. The oxygen transfer rates for the reduction (Fig. 12a) and oxidation (Fig. 12b) reactions increased with increasing the GDC content. This suggests that GDC may affect the reaction kinetics of NiFe2O4/GDC composites. Interestingly, the oxygen transfer rate for the oxidation reaction increased significantly for the composite that included 15 wt% GDC, as shown in Fig. 12(b).
It has been reported that GDC has oxygen storage capability due to its oxygen vacancies [31,32]. It is also well known that the surface adsorption of the reaction gas improves with the amount of oxygen vacancies on the surface. Therefore, the well-dispersed fine GDC particles on the surface of NiFe2O4 can accelerate the surface adsorption of reaction gases due to the oxygen vacancies formed on the surface of the GDC. Moreover, fine GDC particles may suppress the grain growth of NiFe2O4. As a result, the specific surface area per unit volume of the NiFe2O4/GDC composite was larger than that of the pure NiFe2O4. This also increases the reaction rate in terms of the enlargement of active sites.
The primary advantage of the addition of GDC was that no significant agglomeration was observed before or after the re-dox cycle. Therefore, one can expect that an NiFe2O4/GDC composite may exhibit oxygen carrying stability during long-term cycles, based on the result of the reversible re-dox reaction and microstructural observation. Fig. 13(a) shows re-dox curve of the NiFe2O4/15wt% GDC composite at 900 °C during the 10 re-dox cycles, measured by TGA. Based on the re-dox curve, the calculated oxygen transfer capacity retention and the variation of oxygen transfer rate are shown in Fig. 13(b). In fact, in this study the NiFe2O4/15 wt% GDC composite showed no significant degradation in the oxygen transfer capacity and reaction rate after the tenth re-dox cycle, as shown in Fig. 13.

Fig. 2

XRD patterns of NiFe2O4 obtained for the various reaction gases at 900 °C for 1 h.

Fig. 3

XRD patterns of NiFe2O4 according to re-dox reaction at 900 °C for 1 h.

Fig. 4

XPS spectra of NiFe2O4 before and after the oxidation reaction at 900 °C for 1 h.

Fig. 5

(a) TPR data, and (b) TPO data of NiFe2O4/GDC composites obtained for 5% H2/Ar and 10% H2O/Ar as the reducing and oxidizing gases, respectively.

Fig. 6

XRD patterns of NiFe2O4/GDC composites (a) before and (b) after H2-TPR and H2O-TPO tests.

Fig. 7

FE-SEM images of NiFe2O4/GDC composites before H2-TPR and H2O-TPO tests: (a) 0 wt% GDC, (b) 5 wt% GDC, (c) 10 wt% GDC, and (d) 15 wt% GDC.

Fig. 8

FE-SEM images of NiFe2O4/GDC composites after H2-TPR and H2O-TPO tests: (a) 0 wt% GDC, (b) 5 wt% GDC, (c) 10 wt% GDC, and (d) 15 wt% GDC.

Fig. 9

(a) H2 consumption, and (b) production of NiFe2O4/GDC composites versus GDC in reduction reaction with 5% H2/Ar and in oxidation reaction with 10% H2O/Ar, respectively, measured by GC.

Fig. 10

Maximum reaction rate of NiFe2O4/GDC composites versus GDC content for (a) the reduction with 5% H2/Ar and (b) the oxidation with 10% H2O/Ar, measured by GC.

Fig. 11

Re-dox curves of the NiFe2O4/GDC composites at 900 °C with 5% H2/Ar and air used as the reducing and oxidizing gases, respectively, measured by TGA.

Fig. 12

Maximum oxygen transfer rate of NiFe2O4/GDC composites versus GDC content for (a) the reduction reaction with 5% H2/Ar and (b) the oxidation reaction with air, measured by TGA.

Fig. 13

(a) Re-dox curve, and (b) oxygen transfer capacity retention and rate stability of the NiFe2O4/15wt% GDC composite at 900 °C during the 10 re-dox cycles, measured by TGA.

Table 1

XRF data for the NiFe2O4 powder reduced by H2 at 900 °C for 1 h.

conclusions

This study characterizes NiFe2O4/GDC composites as oxygen carrier materials for CLHP. The re-dox mechanisms represented in the solid state in the fuel, in steam, and in the air reactor were NiFe2O4→NixFe2, NixFe2→Ni+Fe3O4, and Ni+Fe3O4→NiFe2O4+Fe2O3, respectively. Carbon dioxide could be captured from the fuel reactor and hydrogen could be produced from the steam reactor.
Both the amount and rate of hydrogen production for the NiFe2O4/GDC composites increased as the GDC content increased. Moreover, the oxygen transfer rate for both the reduction and oxidation reactions increased significantly with increasing GDC content. The positive effect of the addition of GDC may be mainly ascribed to an increase in the surface adsorption of reaction gases via the oxygen vacancies formed on the surface of the GDC, as well as the enlargement of the active sites due to suppression of the agglomeration of NiFe2O4 by the well-dispersed fine GDC particles on the surface of NiFe2O4.
In the case of the NiFe2O4/15wt% GDC composite, no significant degradation in the oxygen transfer capacity or reaction rate during the re-dox cycles was observed. Assuming that the reaction rate of hydrogen production per hour is maintained, the amount of hydrogen production for the NiFe2O4/15wt% GDC composite would be 2,702 L/day per unit mass (kg). In this regard, an NiFe2O4/GDC composite can be a promising oxygen carrier material for CLHP due to its high performance and stability. However, since the cost of the GDC is still high, trade-offs in terms of performance improvement and cost as well as industrial scalability should be considered. Therefore, it is necessary to develop a technology that can maximize performance while minimizing the content of GDC such as use of nano-composite powder.

Acknowledgements

This research was supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education (2017R1D1A1B03031541). This work was also supported by the Technology Development Program to Solve Climate Changes of the National Research Foundation (NRF) grant funded by the Korea government (Ministry of Science and ICT) (2017M1A2A2044930).

References
  • 1. K.S. Go, S.R. Son, S.D. Kim, K.S. Kang, and C.S. Park, Int. J. Hydrogen Energy 34[3] (2009) 1301-1309.
  •  
  • 2. R.D. Solunke and G. Veser, Ind. Eng. Chem. Res. 49[21] (2010) 11037-11044.
  •  
  • 3. S. Dunn, Int. J. Hydrogen Energy 27[3] (2002) 235-264.
  •  
  • 4. M. Momirlan and T.N. Veziroglu, Renew. Sust. Energ. Rev. 6[1-2] (2002) 141-179.
  •  
  • 5. IPCC, in 2014: Climate Change 2014: Synthesis Report, 2015, edited by Pachauri, R. K., Allen, M. R., Barros, V. R., Broome, J., Cramer, W., Christ, R., Church, J. A., Clarke, L., Dahe, Q., Dasgupta, P., Dubash, N. K., Edenhofer, O., Elgizouli, I., Field, C. B., Forster, P., Friedlingstein, P., Fuglestvedt, J., Gomez-Echeverri, L., Hallegatte, S., Hegerl, G., Howden, M., Jiang, K., Jimenez Cisneroz, B., Kattsov, V., Lee, H., Mach, K. J., Marotzke, J., Mastrandrea, M. D., Meyer, L., Minx, J., Mulugetta, Y., O'Brien, K., Oppenheimer, M., Pereira, J. J., Pichs-Madruga, R., Plattner, G.-K., Pörtner, Hans-Otto , Power, S. B., Preston, B., Ravindranath, N. H., Reisinger, A., Riahi, K., Rusticucci, M., Scholes, R., Seyboth, K., Sokona, Y., Stavins, R., Stocker, T. F., Tschakert, P., van Vuuren, D. and van Ypserle, J.-P., Intergovernmental Panel on Climate Change Press (2015) p.151.
  •  
  • 6. S.A. Rackley, in “Carbon Capture and Storage 2nd Edition” (Butterworth-Heinemann Press, 2017) p.22.
  •  
  • 7. D.Y.C. Leung, G. Caramanna, and M.M. Maroto-Valer, Renew. Sust. Energ. Rev. 39 (2014) 426-443.
  •  
  • 8. J. Gibbins and H. Chalmers, Energy Policy 36[12] (2008) 4317-4322.
  •  
  • 9. V.J. Aston, B.W. Evanko, and A.W. Weimer, Int. J. Hydrogen Energy 38[22] (2013) 9085-9096.
  •  
  • 10. P. Gupta, L.G. Velazquez-Vargas, and L.S. Fan, Energy Fuels 21[5] (2007) 2900-2908.
  •  
  • 11. L.F. de Diego, M. Ortiz, F. García-Labiano, J. Adánez, A. Abad, and P. Gayán, J. Power Sources 192[1] (2009) 27-34.
  •  
  • 12. M. Luo, Y. Yi, S. Wang, Z. Wang, M. Du, J. Pan, and Q. Wang, Renew. Sust. Energ. Rev. 81 (2018) 3186-3214.
  •  
  • 13. L. Protasova and F. Snijkers, Fuel 181 (2016) 75-93.
  •  
  • 14. F. Li, H.R. Kim, D. Sridhar, F. Wang, L. Zeng, J. Chen, and L.-S. Fan, Energy Fuels 23[8] (2009) 4182-4189.
  •  
  • 15. Z. Huang, F. He, Y. Feng, K. Zhao, A. Zheng, S. Chang, G. Wei, Z. Zhao, and H. Li, Energy Fuels 28[1] (2014) 183-191.
  •  
  • 16. M. Rydén and M. Arjmand, Int. J. Hydrogen Energy 37[6] (2012) 4843-4854.
  •  
  • 17. J.R. Scheffe, M.D. Allendorf, E.N. Coker, B.W. Jacobs, A.H. McDaniel, and A.W. Weimer, Chem. Mater. 23[8] (2011) 2030-2038.
  •  
  • 18. S. Yang, K. Kim, J.I. Baek, J.W. Kim, J.B. Lee, C.K. Ryu, and G. Lee, Energy Fuels 26[7] (2012) 4617-4622.
  •  
  • 19. Y.L. Kuo, W.M. Hsu, P.C. Chiu, Y.H. Tseng, and Y. Ku, Ceram. Int. 39[5] (2013) 5459-5465.
  •  
  • 20. Y.M. Choi, H. Abernathy, H.-T. Chen, M.C. Lin, and M. Liu, Chem. Phys. Chem. 7 (2006) 1957-1963.
  •  
  • 21. C. Sun, H. Li, and L. Chen, Energy Environ. Sci. 5 (2012) 8475-8505.
  •  
  • 22. G. Chen, G. Guan, Y. Kasai, and A. Abudula, Int. J. Hydro. Energy 37 (2012) 477-483.
  •  
  • 23. S. Liu, F. He, Z. Huang, A. Zheng, Y. Feng, Y. Shen, H. Li, H. Wu, and P. Glarborg, Energy Fuels 30 (2016) 4251-4262.
  •  
  • 24. K. Svoboda, A. Siewiorek, D. Baxter, J. Rogut, M. Puncochar, Chem. Pap. 61(2) (2007) 110-120.
  •  
  • 25. T. Yamashita and P. Hayes, Appl. Surf. Sci. 254 (2008) 2441-2449.
  •  
  • 26. J.K. Dey, A. Chatterjee, S. Majumdar, A.-C. Dippel, O. Gutowski, M.V. Zimmermann, and S. Giri, Phys. Rev. B 99 (2019) 144412.
  •  
  • 27. T.S.T. Saharuddin, F. Salleh, A. Samsuri, R. Othaman, and M.A. Yarmo, Int. J. Chem. Eng. Appl. 6 (2015) 405-409.
  •  
  • 28. G. Neri, A.M. Visco, S. Galvagno, A. Donato, and M. Panzalorto, Thermochim. Acta 329 (1999) 39-46.
  •  
  • 29. X. Zhu, H. Wang, Y. Wei, K. Li, and X. Cheng, J. Rare Earths 28 (2010) 907-913.
  •  
  • 30. F. Mahmoodi, S.H. Najibi, and A. Shariati, J. Am. Sci. 8[11] (2012) 453-459.
  •  
  • 31. Y.M. Choi, H. Abernathy, H.-T. Chen, M.C. Lin, and M. Liu, Chem. Phys. Chem. 7 (2006) 1957-1963.
  •  
  • 32. Z. Gu, K. Li, S. Qing, X. Zhu, Y. Wei, Y. Li, and H. Wang, RSC Adv. 4 (2014) 47191-47199.
  •  

This Article

  • 2020; 21(2): 148-156

    Published on Apr 30, 2020

  • 10.36410/jcpr.2020.21.2.148
  • Received on Jul 19, 2019
  • Revised on Feb 18, 2020
  • Accepted on Feb 24, 2020

Correspondence to

  • Ki-Tae Lee
  • bDivision of Advanced Materials Engineering, Jeonbuk National University, Jeonbuk, 54896 Republic of Korea
    cHydrogen and Fuel Cell Research Center, Jeonbuk National University, Jeonbuk, 54896 Republic of Korea
    Tel : +82-63-270-2290 Fax: +82-63-270-2386

  • E-mail: ktlee71@jbnu.ac.kr