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Thermo-fluid experiments in KAERI for nuclear hydrogen production *Chan Soo Kim 1) , Sung-Deok Hong, Jong-Hwan Kim, Eung-Seon Kim 2) 1), 2) Hydrogen Production Reactor Technology Development Division, Korea Atomic Energy Research Instiute, Daejeon 305-353, Korea 1) [email protected] ABSTRACT A Very High Temperature gas-cooled Reactor (VHTR) can produce the high temperature heat above 850, so its applications include not only high efficient electricity but also industrial heat supply such as hydrogen production, steam reforming, and other industrial processes. The development of high temperature components of VHTR is very important because of its higher operation temperature than that of a common light water reactor and high pressure industrial process. The main advantage of VHTR is its inherent safety through the Reactor Cavity Cooling System (RCCS), which is the only ex-vessel passive safety system without additional water supply and electricity. Korea Atomic Energy Research Institute (KAERI) has focused on the development of the compact high temperature heat exchangers for nuclear hydrogen production and the demonstration of the passive safety of VHTR. This paper presents the thermos-fluid experiments for the high temperature heat exchangers and the passive safety for nuclear hydrogen production in KAERI. 1. INTRODUCTION After the Fukusima Daiichi nuclear accident, future nuclear systems are focused on a passive safety without additional external electricity. A Very High Temperature gas-cooled reactor has shown great chance for its inherent safety. Since VHTR can produce a high temperature heat above 850, its applications include not only high efficiency electricity but also industrial heat supply such as steam-methane reforming, hydrogen production, high-temperature steam production, and other industrial processes (Chang et al., 2007). Especially, hydrogen receives attention as an alternative to fossil fuel that emits green-house gas. The application area of hydrogen is not limited to the fuel-cell car but extended to the petro-chemistry industry and the iron 1) Senior Researcher 2) Principal Researcher
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Page 1: Thermo-fluid experiments in KAERI for nuclear hydrogen ... · Thermo-fluid experiments in KAERI for nuclear hydrogen production *Chan Soo Kim1), Sung-Deok Hong, Jong-Hwan Kim, Eung-Seon

Thermo-fluid experiments in KAERI for nuclear hydrogen production

*Chan Soo Kim1), Sung-Deok Hong, Jong-Hwan Kim, Eung-Seon Kim2)

1), 2) Hydrogen Production Reactor Technology Development Division, Korea Atomic Energy Research Instiute, Daejeon 305-353, Korea

1) [email protected]

ABSTRACT

A Very High Temperature gas-cooled Reactor (VHTR) can produce the high temperature heat above 850℃, so its applications include not only high efficient electricity but also industrial heat supply such as hydrogen production, steam reforming, and other industrial processes. The development of high temperature components of VHTR is very important because of its higher operation temperature than that of a common light water reactor and high pressure industrial process. The main advantage of VHTR is its inherent safety through the Reactor Cavity Cooling System (RCCS), which is the only ex-vessel passive safety system without additional water supply and electricity. Korea Atomic Energy Research Institute (KAERI) has focused on the development of the compact high temperature heat exchangers for nuclear hydrogen production and the demonstration of the passive safety of VHTR. This paper presents the thermos-fluid experiments for the high temperature heat exchangers and the passive safety for nuclear hydrogen production in KAERI. 1. INTRODUCTION

After the Fukusima Daiichi nuclear accident, future nuclear systems are focused on a passive safety without additional external electricity. A Very High Temperature gas-cooled reactor has shown great chance for its inherent safety. Since VHTR can produce a high temperature heat above 850℃, its applications include not only high efficiency electricity but also industrial heat supply such as steam-methane reforming, hydrogen production, high-temperature steam production, and other industrial processes (Chang et al., 2007). Especially, hydrogen receives attention as an alternative to fossil fuel that emits green-house gas. The application area of hydrogen is not limited to the fuel-cell car but extended to the petro-chemistry industry and the iron

1) Senior Researcher 2) Principal Researcher

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ore reduction for steel production. Nuclear hydrogen is estimated as the massive hydrogen production method without carbon dioxide emissions. Nuclear energy is one of important energy mix in Korea, which account for about 14% of total energy consumption. However, nuclear energy is used for electricity generation only whereas fossil energy is utilized for industrial, residential, and transportation as well as electricity. Due to the exhaustion of fossil fuels and reduction of carbon dioxide emission, the Korean government has the interest with expanding the application area of nuclear energy into the non-electric application. The VHTR is a useful candidate because of its wide application range and inherent safety. The Korean Government launched a nuclear hydrogen program (Lee et al., 2009) using the VHTR, which is led by Korea Atomic Energy Research Institute (KAERI). As the core outlet temperature was raised up to 950℃ for the efficient hydrogen production, key technologies were emerged to be solved. KAERI focuses on technologies such as VHTR-specialized design and analysis codes, high temperature helium experiment, passive safety experiment, high temperature material database and heat exchangers, fuel development, and thermo-chemical hydrogen production. Fig. 1 shows the nuclear hydrogen system using the VHTR and S-I process.

Figure 1 Nuclear Hydrogen Production System using VHTR

This paper presents the review of the thermo-fluid experimental researches for nuclear hydrogen production in KAERI. In the beginning, this paper introduces experimental facilities, including a small-scale gas loop, a very high temperature Helium Experimental LooP (HELP) and a Natural Cooling Experimental Facility (NACEF) constructed by KAERI. The objective, design specification and test results of the experimental facilities will be explained in detail. Future works of the experimental researches will be discussed in the conclusion.

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2. THERMO-FLUID EXPERIMENTAL RESEARCHES

The development of the high temperature components of VHTR is very important because of its higher operation temperature than that of a common light water reactor and high pressure industrial process. The main advantage of VHTR is its inherent safety through the Reactor Cavity Cooling System (RCCS), which is the only ex-vessel passive safety system without additional water supply and electricity. Since the nuclear hydrogen project stated in 2006, KAERI designed and built thermo-fluid experimental facilities for heat exchangers and passive safety. This section provides information of those facilities including design specifications and features. 2.1 Small-scale Gas Loop

The primary goal of the small-scale gas loop (Kim et al., 2011) is the integrity and feasibility test of a laboratory-scale process heat exchanger for the sulfur trioxide decomposition as shown in Fig 2. KAERI constructed the small-scale gas loop in 2007. The gas loop consists of a hot gas loop and a process gas loop. The hot gas loop simulates the intermediate loop that delivers high temperature heat above 900℃ from the VHTR core to hydrogen production system. The process gas loop simulates the decomposition of sulfuric acid into water, sulfur trioxide, sulfur dioxide, and oxygen in sulfur- iodine process, which is a thermo-chemical water-split process for hydrogen production. A laboratory-scale process heat exchanger (PHE) was installed between the two loops and tested to verify the performance of transferring the heat for the sulfur trioxide decomposition and the corrosion resistance in sulfuric acid.

Fig. 2 Flow Diagram of Small-scale Gas Loop

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The hot gas loop was designed to withstand the maximum temperature of 1000℃ and the maximum pressure of 6 MPa, and to operate with a mass velocity of 2.0 kg/min at 4.0 MPa nitrogen condition. The working fluid is nitrogen for simple high pressure gas experiments. The nitrogen loop is composed of a gas-heating system, a hot gas duct, a hybrid heat exchanger, a water-cooled printed circuit heat exchanger, a water-cooling system, a nitrogen supply system, a nitrogen purification system, and a bypass flow control valve as shown in Fig. 2. The nitrogen temperature is controlled by adjusting the power to the heaters using direct voltage controllers. The primary mass flow rate to the gas-heating system is controlled by the circulator inverter and a bypass flow control valve.

The process gas loop is designed to withstand the maximum design temperature of 950℃ at the atmospheric condition. The sulfuric acid mass flow is controlled by the acid mass flow controller or the acid feed pump. The 96wt% sulfuric acid is evaporated and de-hydrolyzed as it passes the high temperature sulfuric acid heating system. Sulfur trioxide is fractionally decomposed into sulfur dioxide and oxygen in the process heat exchanger with catalyst. Through a high temperature hybrid cooler, sulfur trioxide and steam is combined into sulfuric acid vapor and the vapor is condensed to the sulfuric acid liquid.

Fig. 3 PHE Fabrication Process

The materials for PHE require excellent mechanical properties at an elevated temperature and high pressure as well as a high corrosion resistance in sulfur dioxide / sulfur trioxide environment. KAERI has developed a new concept of PHE which adopted both hybrid heat exchanger (Kim. et al., 2008b) and surface modification technology with SiC coating and ion-beam mixing (Park et al., 2008) as shown in Fig. 3.

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The hybrid design has different flow channel shapes. The hot gas side has a flow channel of a printed circuit heat exchanger to enhance heat transfer and mechanical strength while the process gas side has that of a plate-fin type to secure a space for catalyst. The PHE is designed through the thermo-chemical design considering the kinetics of the sulfur trioxide decomposition (Kim et al., 2008a).

Experiments of the sulfuric acid loop (Hong et al, 2012) were performed in the small scale gas loop. The flow rate of 8cc/min 96wt% sulfuric acid is heated by the sulfuric acid heating superheating system and cooled down by the sulfuric acid cooler over 10 hours. After the experiment at the sulfuric acid gas condition, the modified internal surface of the process gas channel in the PHE was shown in Fig. 4. The modified surface was no change of the surface color after the test, but the color change was observed on the side surface without the surface modification.

Fig. 4 Internal Corrosion of PHE after Test

In addition, Kim et al. (2011) performed the high temperature test with a water-cooled PCHE without the link with the process gas loop at the small-scale gas loop. The high temperature test results showed that the main components had the enough performance to simulate the sulfur trioxide decomposition condition in the nuclear hydrogen production system. Especially, the gas-bearing circulator was stably operated for the long time. The gas-heating system also had enough heating ability at the high pressure condition. Kim et al.(2010, 2012) performed the feasibility tests for the hot gas temperature measurement with the Reduced Radiation Error (RRE) method. The test results showed the radiation bias effect on the hot gas temperature measurement and the feasibility of the RRE method. The dust control from the internal insulator of the heaters and the hot gas duct was required to prevent sudden flow blockage of the PCHE at the high temperature operation. The operation experience of the small scale

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gas loop provided the useful information for the design and operation procedure of the helium experimental loop in the next section.

2.2 Very High Temperature Helium Experimental Loop The Very high temperature Helium Experimental LooP (HELP) shown in Fig. 5 is

aimed at providing the component-level operation conditions for the verification tests of scale-down key components for nuclear hydrogen production. KAERI constructed HELP in 2011. The loop is designed for the verification test of a 150 kW-intermediate heat exchanger or the simulation test in a 1/6 scaled-down fuel block (Kim et al, 2013a).

Fig. 5 Flow Diagram of HELP

HELP consists of a primary loop and a secondary loop that simulate a VHTR and an intermediate loop in nuclear hydrogen production system, respectively. Two loops were designed to withstand the maximum temperature of 1000℃. Their design pressure is 9.0 MPa. The working fluid is helium as the actual coolant of VHTR. The primary loop is composed of a preheater, a high temperature heater, a hot gas duct, intermediate heat exchangers, a water-cooled shell and U-tube heat exchanger, a gas-bearing blower, a passive venting system and gas filters. Fig. 6 shows presents major components in the primary loop. Table 1 shows the design specification of the heat exchangers. The secondary loop has the same system configuration as the primary loop except a high temperature heater and a blower-outlet filter. In addition, a water-cooled printed circuit heat exchanger is installed to cool down the high temperature secondary gas from the outlet of intermediate heat exchangers. Two loops share a helium supply system, a helium purification system for oxygen and humidity removal and a water loop for a cooling tower.

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Operational tests of HELP were performed to verify its performance at the designed condition. The test showed that the blowers and the heaters sufficiently provided the component-level environment as the design performance. HELP experiments focused on the high temperature printed circuit heat exchanger. The PCHE is a candidate of intermediate heat exchanger for the VHTR application due to its high effectiveness and compactness.

Table 1 Design Specification of the Heat Exchangers in HELP

Items U-tube Heat Exchanger STS 316L PCHE Hot Side Cold Side Hot Side Cold Side

Working Fluid Helium Water Helium Water Mass Velocity 0.5 kg/s 37.27 kg/s 0.1 kg/s 1 kg/s

Tin &Tout 400C /100C 32C /37C 500C /21C 20C /80C Design P 90 bar 50 bar 90 bar 90 bar

Design DP 0.7 bar 0.7 bar 0.5 bar 0.5 bar

(b) Circulator (c) Hot gas duct

(a) High T heater (d) STS 316L PCHE (e) U-tube heat exchanger

Fig. 6 Major Components in the Primary Loop of HELP

As a first stage (2012~2013), Kim et al. (2013a, b) performed the high

temperature test with STS 316L PCHE at its design temperature. We obtained overall

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heat transfer coefficients of a stainless steel PCHE that have been corrected the heat loss from the PCHE external surfaces to the atmosphere by radiation/natural convection heat transfer. In addition, thermal expansion deformation between the inlet and the outlet of the primary side was evaluated by the laser displacement sensor. In the experimental condition above 400℃, the thermal stress was large enough to result in a plastic windingness of the nozzles of the STS 316L PCHE.

Fig. 7 800HT PCHE, STS316L PCHE, Tied Universal Expansion Joints at HELP

Fig. 8 Outlet Temperature Histories of High Temperature Heater and 2nd Pre-Heater

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As a second stage (2014~2015), we prepared a 800HT PCHE for the very high temperature test above 800℃. Four tied universal expansion joints were installed to absorb the thermal expansion of the high temperature components as shown in Fig. 7. Fig. 8 shows the outlet temperature histories of the high temperature heater in the primary system and the pre-heater in the secondary system. The picture in Fig. 8 shows an alloy617 pipe between the hot gas duct and the 800HT PCHE during the outlet temperature of the high temperature heater above 900℃. In the present, we developed and install the bench-scale alloy617 PCHE in HELP. The PCHE will be tested at very high temperature condition. The temperature will be increased in a stepwise up to 950℃.

2.3 NAtural Cooling Experimental Facility The Reactor Cavity Cooling System (RCCS), a key ex-vessel passive system of

the VHTR shown in Fig. 9, is designed to remove the residual heat in the case of accident without addition water supply and electricity. The natural heat transfer modes in RCCS include conduction, buoyancy-driven convection, and radiation. The RCCS is basically a system of duct with penetrates the power plant and envelopes the VHTR. The riser is a vertical part of the RCCS, which penetrates the reactor cavity with its end connected to the main duct work through lower and upper plenum. Air flow in the riser is induced by buoyance at the riser section passing through the reactor cavity and eventually transports the residual heat to the atmosphere.

Fig. 9 Reactor Cavity Cooling System

KAERI constructed a Natural Cooling Experimental Facility (NACEF) to evaluate

the performance of RCCS in the case of a total loss of active heat removal system. The NACEF is scale-downed to 1/4 of the PMR200 RCCS in the vertical direction and the real scale in the horizontal direction to simulate the radiation heat transfer between the

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reactor vessel and RCCS air duct (Bae et al., 2013, 2014). The NACEF as shown in Fig. 10 consists of a heater box, a plenum, and piping work. The heater box simulates the reactor cavity, which includes the ceramic heater, the heating panel, 6 riser ducts, and the reflecting panel. The ceramic heater and the heating panel simulate the core barrel and the reactor vessel, respectively. Thermal mass flow meters were installed at the outlet of the chimney to measure buoyancy-induced flow rate. . Steady-state tests with the uniform heat flux condition are in progress to establish the scaling analysis methodology for RCCS coolability demonstration (Kim et al, 2015a, b). In addition, KAERI and ANL have led the International Nuclear Energy Research Initiative to develop and confirm the scaling analysis methodology for RCCS coolability demonstration by comparative study between two reduced scale tests for RCCS.

Fig. 10 Design and Construction of Natural Cooling Experimental Facility (NACEF) 3. CONCLUSIONS

This paper reviewed thermo-fluid experimental studies related to the VHTR development for nuclear hydrogen production in KAERI. Experimental facilities constructed at KAERI were described, which are the small-scale gas loop, the helium experimental loop, and the natural cooling experimental facility. Tests performed in the facility were summarized with representative results.

The VHTR-related thermo-fluid experimental research in KAERI is still underway to contribute to design, safety, and licensing of the VHTR for hydrogen production. Future experimental studies are summarized as follows.

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-Small-scale Gas Loop : Performance test of PHE for corrosion resistance in the operating condition -HELP : Performance test of the bench-scale IHX above 900℃, characteristic test of the intermediate heat transfer system for candidate gases. -NACEF : Performance test of the RCCS at steady state and accident conditions for improved design of RCCS

ACKNOWLEDGEMENT This study was supported by Nuclear Research & Development Program of the National Research Foundation of Korea (NRF) grant funded by the Ministry of Science, ICT and Future Planning. (Grant Code: NRF-2012M2A8A2025682, NRF-2014M2A8A2064090) REFERENCES Bae, Y. Y., Cho, B. H., Hong, S. D., Kim, Y. W. (2013), “Numerical Simulation of

Convective and Radiative Heat Transfer in the PMR200 Cavity,” Proceedings of NURETH15, Pisa, Italy, May 12-17, NURETH15-091.

Bae, Y. Y., Hong, S. D., Kim, Y. W. (2014), “Scaling Analysis of PMR200 Reactor Cavity Cooling System,” Nucl. Eng. and Des., 271, 523-529.

Chang, J. H., Kim, Y. W., Lee, K. Y., Lee, Y. W., Lee, W. J., Noh., J. M., Kim, M. H., Lim, H. S., Shin, Y. J., Bae, K. K., Jumg, K. D (2007), “A Study of the Nuclear Hydrogen Production Demonstration Plant,” Nucl. Eng. and Tech., 39(2), 111-122.

Hong S. D. , Kim, C. S., Kim, Y. W., Seo, D. U., Park, G. C. (2012), “Design and Analysis of a High Pressure and High Temperature Sulfuric Acid Experimental System,” Nucl. Eng. and Des., 251, 157-163.

Kim, C. S., Hong, S. D., Kim, Y. W., Kim, J. H., Lee, W. J., Chang, J. H. (2008a), “Thermal Design of a Laboratory-scale SO3 Decomposer for Nuclear Hydrogen Production,” Int. J of Hydrogen Energy, 33, 3688-3699.

Kim, Y. W., Park, J. W., Hong, S. D., Kim, C. S., Lee, W. J., Chang, J. H. (2008b), “Development of an Innovative High Temperature Compact Heat Exchanger for the Coupling of VHTR and Hydrogen Production System,” Trans. of KNS Spring Meeting, Gyeongju, Korea, May 29-30.

Kim, C. S., Hong, S. D., Seo, D. U., Kim, Y. W. (2010), “Temperature Measurement with Radiation Correction for Very High Temperature Gas,” Proceedings of IHTC14, Washington, DC, USA, August 8-13, IHTC-23074.

Kim, C. S., Seo, D. U., Yoo, T. H., Hong, S. D. (2011), “Performance Test of Nitrogen Loop with Hybird Heat Exchanger for SO3 Decomposition of Nuclear Hydrogen Production,” Proceedings of ICAPP2011, Nice, France, May 2-5, Paper 11454.

Kim. C. S., Hong, S. D., Kim, Y. W. (2012), “Radiation-corrective Gas Temperature Measurement in a Circular Channel,” Advanced Computational Methods and Experiments in Heat Transfer, WIT Trans. Eng. Sci., 7, 157-167.

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Kim. C. S., Chae. J. S., Hong, S. D. (2013a), “Performance Test of Very High Temperature Helium Experimental Loop,” Proceedings of ICAPP2013, Jeju, Korea, April 14-18, Paper KD028.

Kim, C. S., Hong, S. D., Kim, M. H. (2013b), “Experimental Study on Stainless Steel 316L Printed Circuit Heat Exchanger at High Temperature and High Pressure Gas Environments,” Trans. of KNS Autumn Meeting, Gyeongju, Korea, Oct. 24-25.

Kim, J. H., Bae, Y. Y., Park, B. H., Kim, E. S., Kim, C. S. (2015a), “The 4th Test Results of the 1/4-scale RCCS Test Facility,” KAERI/TR-5968-2015.

Kim, J. H., Bae. Y. Y., Kim, C. S., Kim, E. S. (2015b), “The Results of the 5th Run of the 1/4-scale RCCS Performance Test Facility,” KAERI/TR-5980-2015.

Lee, W. J., Kim, Y. W., Chang, J. H. (2009), “Perspectives of Nuclear Heat and Hydrogen,” Nucl. Eng. and Tech., 41(4), 413-426.

Park, J. W., Kim, H. J., Kim, Y. W. (2008), “The Fabrication of a Process Heat Exchanger for SO3 Decomposer Using Surface-modified Hastelloy X Materials,” Nucl. Eng. and Tech., 40(3), 233-238.


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