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Countercurrent Air-Water Flow in a Scale-Down Model of a Pressurizer Surge Line

DOI: 10.1155/2012/174838

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Abstract:

Steam generated in a reactor core and water condensed in a pressurizer form a countercurrent flow in a surge line between a hot leg and the pressurizer during reflux cooling. Characteristics of countercurrent flow limitation (CCFL) in a 1/10-scale model of the surge line were measured using air and water at atmospheric pressure and room temperature. The experimental results show that CCFL takes place at three different locations, that is, at the upper junction, in the surge line, and at the lower junction, and its characteristics are governed by the most dominating flow limitation among the three. Effects of inclination angle and elbows of the surge line on CCFL characteristics were also investigated experimentally. The effects of inclination angle on CCFL depend on the flow direction, that is, the effect is large for the nearly horizontal flow and small for the vertical flow at the upper junction. The presence of elbows increases the flow limitation in the surge line, whereas the flow limitations at the upper and lower junctions do not depend on the presence of elbows. 1. Introduction The mid-loop operation is to be conducted during plant refueling and maintenance of a PWR (Pressurized Water Reactor). In this operation, the reactor coolant level is kept around the primary loop center, and decay heat is removed by RHR (Residual Heat Removal) systems. If the loss of cooling systems such as RHR and/or other cooling systems takes place, cooling water in the reactor core may be heated up to boil and the top of the fuel assembly can be exposed to the air. In such an event, reflux cooling by the steam generators (SG) is regarded as one of the possible and effective core cooling methods. The reflux cooling is a way of core cooling by making use of water condensed in SGs. The steam generated in the reactor core and water condensed in the SG form a countercurrent flow in the hot leg. The authors therefore measured CCFL (Countercurrent Flow Limitation) characteristics in a scale-down model of a hot leg using air and water [1] and reported that CCFL can be accurately evaluated based on a one dimensional momentum balance for air-water two-phase flow [2]. In addition to this CCFL, the steam generated in the reactor core and water condensed in the pressurizer due to heat transfer to the vessel wall may also form a countercurrent flow in a surge line which connects the hot leg and the pressurizer. The ROSA-IV/LSTF (Rig-of-Safety-Assessment No. 4/Large Scale Test Facility) experiment [3], which simulated the loss of RHR systems during mid-loop operation, reported that

References

[1]  N. Minami, D. Kataoka, A. Tomiyama, S. Hosokawa, and M. Murase, “Countercurrent gas-liquid flow in a rectangular channel simulating a PWR hot leg (1) flow pattern and CCFL characteristics,” Japanese Journal of Multiphase Flow, vol. 22, no. 4, pp. 403–412, 2008 (Japanese).
[2]  N. Minami, M. Murase, D. Nishiwaki, and A. Tomiyama, “Countercurrent gas-liquid flow in a rectangular channel simulating a PWR hot leg (2) analytical evaluation of countercurrent flow limitation,” Japanese Journal of Multiphase Flow, vol. 22, no. 4, pp. 413–422, 2008 (Japanese).
[3]  H. Nakamura, J. Katayama, and Y. Kukita, “Loss of residual heat removal (RHR) event during PWR mid-loop operation: ROSA-IV/LSTF experiment without opening on primary loop pressure boundary,” American Society of Mechanical Engineers, Fluids Engineering Division (Publication) FED, vol. 140, pp. 9–16, 1992.
[4]  K. Takeuchi, M. Y. Young, and A. F. Gagnon, “Flooding in the pressurizer surge line of AP600 plant and analyses of APEX data,” Nuclear Engineering and Design, vol. 192, no. 1, pp. 45–58, 1999.
[5]  L. E. Hochreiter, S. V. Fanto, L. E. Conway, and L. K. Lau, “Integral testing of the AP600 passive emergency core cooling systems,” Journal of Power and Energy, vol. 207, no. 4, pp. 259–268, 1993.
[6]  J. N. Reyes, “Scaling Analysis for the OSU AP600 Integral Systems and Long Term Cooling Facility,” OSU-NE-9204, 1992.
[7]  G. B. Wallis, One Dimensional Two-Phase Flow, McGraw Hill, New York, NY, USA, 1969.
[8]  S. Levy, Two-Phase Flow in Complex Systems, Wiley Interscience, 1999.
[9]  G. F. Hewitt and G. B. Wallis, ASME Multi-Phase Flow Symposium, ASME, Philadelphia, Pa, USA, 1963.
[10]  N. Minami, D. Nishiwaki, T. Nariai, A. Tomiyama, and M. Murase, “Countercurrent gas-liquid flow in a PWR hot leg under reflux cooling (I) air-water tests for 1/15-scale model of a PWR hot leg,” Journal of Nuclear Science and Technology, vol. 47, no. 2, pp. 142–148, 2010.
[11]  H. J. Richter, G. B. Wallis, K. H. Carter, et al., “Deentrainment and Countercurrent Air-Water Flow in a Model PWR Hot-Leg,” NRC-0193-9, U.S. Nuclear Regulatory Commission, 1978.
[12]  A. Ohnuki, “Experimental study of counter-current two-phase flow in horizontal tube connected to an inclined riser,” Journal of Nuclear Science and Technology, vol. 23, no. 3, pp. 219–232, 1986.
[13]  A. Ohnuki, H. Adachi, and Y. Murao, “Scale effects on countercurrent gas-liquid flow in a horizontal tube connected to an inclined riser,” Nuclear Engineering and Design, vol. 107, no. 3, pp. 283–294, 1988.
[14]  F. Mayinger, P. Weiss, and K. Wolfert, “Two-phase flow phenomena in full-scale reactor geometry,” Nuclear Engineering and Design, vol. 145, no. 1-2, pp. 47–61, 1993.
[15]  P. B. Whalley, Boiling Condensation and Gas-Liquid Flow, Oxford University Press, New York, NY, USA, 1987.
[16]  J. M. Delhaye, M. Giot, and M. L. Riethmuller, Thermohydraulics of Two-Phase Systems for Industrial Design and Nuclear Engineering, Hemisphere, New York, NY, USA, 1981.

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