Journal of Nuclear Energy Science & Power Generation TechnologyISSN: 2325-9809

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Research Article, J Nucl Ene Sci Power Generat Technol Vol: 7 Issue: 2

Comparative Study of SBO and LOOP Accidents Severity from Core Catcher Design Point of View; Application to IR360 Nuclear Power Plant

Hasti Nasiri1, Faramarz Yousefpour2,3, Golamreza Jahanfarnia1* and Ali Pazirandeh1

1Nuclear Engineering Department, Science and Research Branch, Islamic Azad University, Tehran, Iran

2MASNA Co., Tehran, Iran

3Nuclear Science and Technology Research Institute, Tehran, Iran

*Corresponding Author : Golamreza Jahanfarnia
Nuclear Engineering Department, Science and Research Branch, Islamic Azad University, Tehran, Iran
Tel:
+98-912-3796937
E-mail: [email protected]

Received: April 03, 2018 Accepted: April 18, 2018 Published: April 23, 2018

Citation: Nasiri H, Yousefpour F, Jahanfarnia G, Pazirandeh A (2018) Comparative Study of SBO and LOOP Accidents Severity from Core Catcher Design Point of View; Application to IR360 Nuclear Power Plant. J Nucl Ene Sci Power Generat Technol 7:1. doi: 10.4172/2325-9809.1000183

Abstract

The most severe postulated events (called bounding case) should be considered for effective evaluation of system design in nuclear power plants. In this article the most severe case for evaluation of core catcher design is discussed. Among the most important boundaries for mitigation of severe accident effects, core catcher is the last one. Severe accidents are divided into two categories: Low Pressure (LP) and High Pressure (HP). From the core catcher point of view, HP accidents are more severe because the corium is evacuated to the core catcher at a higher pressure, and the possibility of failure is increased. Among the HP severe accidents, the most severe cases belong to the Station Black Out (SBO) and Loss of Offsite Power (LOOP). After Fukushima Daiichi accident, most of the published researches illustrate that SBO is the bounding case in nuclear power plant severe accidents. In this study, MELCOR code is used to compare the severity of an SBO and a LOOP for the core catcher design. The first step in this analysis is development and verification of a steady state MELCOR model of the IR-360 plant. Then, in the severe phase, the SBO and LOOP accidents are simulated using MELCOR for the IR-360 plant. Finally, the results are compared with each other. According to results it is concluded that the LOOP is more severe than the SBO from the core catcher point of view.

Keywords: Severe accident; Core catcher; LOOP; SBO; HPME; MELCOR

Introduction

In nuclear power plants (NPPs), severe accidents may lead to melting of the reactor core and reactor internal materials. The possibility of core damage and the subsequent release of radioactive materials to the environment are of a great concern to the public because it would threat the safety and health of human and environment.

Therefore, severe accident mitigation features should be developed. There are different strategies to achieve this goal. Although these strategies have generic features in common, they depend on specific reactor design. In the design phase, assessment of the design should be accomplished by analyzing every single feature in the most severe accident condition. Hence, selecting proper severe cases plays vitally important role in assessing the design. One of the common strategies is the use of a core catcher which is a core meltdown retention device for catching the melt and long-term cooling of the molten corium outside the reactor vessel.

In most of the research that has been done recently, SBO as severe accident has been analysed and studied. For example, the following can be noted. After the disaster at Fukushima Daiichi, realistic analysis SBO accident analysis has been performed to evaluate the effectiveness of severe accident management strategies. Simulation and analysis of a severe accident caused by SBO for a CPR1000 power plant using MELCOR is carried out [1].

The behavior of APR1400 coolant system studied under a long term SBO using an advanced MELCOR model in which model was elaborately reconstructed considering natural circulation simulation [2].

SBO analyzed for CNA2 NPP (a heavy pressurize water reactor) by MELCOR considering PSA level 2 requirements [3].

SBO has been selected as a reference scenario in severe accident analysis of a VVER440 design with MELCOR for in vessel retention strategy simulation [4]. MELCOR, MAAP4 and SCDAP/RELAP5 results were compared as part of an evaluation of SBO modeling [5].

However, overall reviews of published studies indicate that SBO commonly has been considered as the worst case in severe accident analyzing.

Depending on the scenario, discharge of core melt to the core catcher can occur at low pressure or high pressure of the reactor coolant system. If the vessel failure occurs with high pressure, High Pressure Melt Ejection (HPME) phenomenon occurs. Progression of the accident in the containment depends strictly on the pressure of the primary coolant system at the onset of vessel failure. The worth cases from core catcher design point of view are sequences with possibility of HPME. Hence all the accidents which lead to the reactor coolant depressurization before vessel breach such as LOCAs can be omitted from core catcher design evaluation procedure. SBO and LOOP (Loss of Offsite Power) are both accidents with loss of electrical power which can initiate high pressure scenario. The severity of the LOOP and SBO accidents for core catcher design evaluation and development are compared in present study.

SBO can initiate severe accident scenarios in which majority of the core would melt. LOOP stands for loss of non-emergency Alternating Current (AC) power assumed to result in the loss of all power of the plant, except diesel generators. SBO, on the other hand, implies loss of all offsite and onsite AC power concurrent with a turbine trip.

For this purpose, MELCOR model of IR-360 nuclear power plant was prepared. Then LOOP and SBO accidents were simulated by MELCOR for IR360 reactor.

MELCOR is a fully integrated systems accident code and includes models for simulating important thermal-hydraulic and fissionproduct phenomena which may occur during a postulated accident in a pressurized light water reactor. Several works have been performed on different issues with the MELCOR code [6]; such as:

The analysis with MELCOR performed to assess the effect of a variety of design parameters and operational procedures on a station blackout severe accident at the Peach Bottom Atomic Power Station [7]. The MELCOR code evaluation independently, using empirical data consistent with the recommendations of the Committee on the Safety of Nuclear Installations of the Organization for Economic Cooperation and Development (OECD/CSNI) validation matrix for core degradation codes [8]. A sensitivity analysis performed on the evolution of severe accidents that can be expected during a Loss of Coolant Accident (LOCA) at an Advanced Power Reactor 1400- MW (APR1400) [9]. The study focused on the impact of a direct vessel injection into the reactor down-comer in mitigation of a severe core degradation; the impact of different break locations and sizes; as well as on the timings of the key thermal-hydraulic responses of the containment spray systems, the severe degradation of the core, and evolution of the core materials. Several aspects analysed related to the source term in the Phebus FPT1 experiment, which contemplate circuit thermal-hydraulics, fission product and structural material release, vapours and aerosol retention in the circuit and containment, vertical line aerosol deposition and steam generator aerosol deposition [10].

This study shows that LOOP accident can be the worst case for core catcher design evaluation than SBO accident. The article is organized as follows. Section 2 describes general features of IR-360 and the MELCOR code model of this NPP. The main results are presented in section 3 and the main finding are summarised in section 4.

Description of Plant and Research Methodology

IR-360 nuclear power plant

IR-360 NPP is a typical pressurized water reactor under design. The thermal power of reactor is 1130 MW which is being cooled with two coolant loops. The Reactor Coolant System (RCS) consist of similar heat transfer loops connected in parallel to the reactor pressure vessel. The plant includes reactor pressure vessel (RPV), two steam generators (SG), two reactor coolant pumps (RCP), one pressurizer (PRZ) with a pressure relief tank (PRT) and pressurizer safety valves (PSV), and associated systems such as chemical and volume control system (CVCS), as well as engineered safety features design of an ex-vessel corium cooling system has been recently considered for this reactor.

The containment is equipped with a Core Catcher for molten core debris including the inventory of the core, internals, and lower reactor pressure vessel (RPV) head. Core debris trap is provided in the reactor cavity in order to decrease the amount of core debris dispersion to the upper compartment. The functional principle of the core catcher is to spread the molten core debris over a large area and stabilize it by quenching it with water from the in-containment refueling water storage tank (IRWST). The goal of this system is to eliminate the potential for containment failure by any means derived from the core melt, including the interaction between core melt and the containment structure and the effects of melt cooling (i.e., overpressurization of containment). A section view of IR-360 core catcher is shown in Figure 1. The present work is motivated by the need for severe accident analysis in support of the plant design.

Figure 1: A Section View of the Core Debris Retention and Cooling System.

MELCOR model of IR-360

The version of MELCOR used for these analyses is 1.8.6, released in (2005) [11]. One of the advantages of MELCOR code is that it represents the current state of the art in severe accident and source term analyses. All aspects of the accident are calculated simultaneously so that important feedbacks among the models are captured.

Methodology of the analyses is aligned with the procedure suggested by IAEA-SRS-No.023 (2002) [12]. A database is developed for the plant components which contains all the design data for each of the components. A general flowchart illustrating the modeling procedure is shown in Figure 2.

Figure 2: Flow-chart of basic steps in model development.

Here a summary of the model is provided and nodalization of the plant will be discussed concisely. The basic input models are given by control volume, the flow path and heat structure data which together describe the major reactor systems. Figure 3 shows the overall nodalization developed for IR-360 modeling by MELCOR. The containment of IR-360 NPP is modeled consisting of containment main compartment, annulus, environment, reactor cavity (core catcher), steam generator and other compartments of loop, upper part of vessel compartment, corridor region and In-containment Refueling Water Storage Tank (IRWST). Also, the frontline systems as listed in the accident sequence modeling of IR-360 are modeled.

Figure 3: IR-360 NPP MELCOR model nodalization.

The steady state qualification includes different checks: one is related to the evaluation of the geometrical data and of numerical values implemented in the nodalization; the other one is related to the capability of the nodalization to reproduce the steady state qualified conditions. Table 1 summarizes the calculated parameters that are crucial for the qualification of the steady state model. According to this table, the calculated values are fairly below the acceptability criteria [13] and confirm the credibility of IR-360 steady state model.

  Parameter Acceptable Error MELCOR Error MELCOR Value Design Value
1 Primary Circuit Water Volume (m3) 1% 0.4% 135.909 136.5
2 Primary Circuits Flow Rates (kg/s) 2% 0.005% 6940.37 6940.0
3 Secondary Circuits Flow Rates (kg/s) 2% 0.33% 602.0 604.0
4 Bypass Flow Rates (kg/s) 10% 0.18% 319.8 319.24
5 Hot leg Fluid Temperature (k) 0.50% 0.03% 586.92 586.75
6 Cold leg Fluid Temperature (k) 0.50% 0.04% 557.13 556.91
7 Power (MWth) 1% 0.01% 1129.9 1130.0
8 Pressurizer Pressure (MPa) 0.10% 0.0% 15.51 15.51
9 SG Secondary Pressure (MPa) 0.10% 0.08% 5.4455 5.45
10 Reactor Vessel Pressure Drop (MPa) 10% 4.0% 0.206 0.198
11 Steam generator primary Pressure Drop (MPa) 10% 3.25% 0.196 0.2026
12 Primary Coolant Flow Rate Through The SG(kg/s) 2% 0.005% 3470.18 3470.0
13 Primary & Secondary Power Balance(MW) 2% 0.018% 1128 1130
14 Pressurizer Level(m) 0.05 m 0.003 m 5.748 m 5.745 m
15 Secondary Side or Down-comer Level(m) 0.1 m 0.095 m 10.0 m 10.74 m down-comer
9.07 mBoiler

Table 1: Geometrical values and thermal-hydraulic parameters for the “steady state” qualification.

Description of accident scenarios model

Based on the results obtained by the plant PSA, two accidents were identified as the most significant to the plant core damage frequency therefore these two accidents were selected for further assessment, first one is LOOP and the other one is SBO.

In LOOP scenario which is modelled in present study with loss of AC power, Reactor Coolant Pumps (RCPs) and Main Feed-Water (MFW) pumps are tripped. Turbine stop valves are closed, as well. Reactivity is controlled via reactor trip. After loss of AC power, Emergency Diesel Generators (EDGs) are restarted successfully to supply electrical power and to restart Component Cooling Water (CCW) system. CCW cools down thermal barrier and protects the seals from being overheated and, hence, reduces rate of leakage from RCP seal. Since CCW is successfully restarted, RCP seal keep working. Emergency Feed Water System (EFWS) and Pressurizer Safety Valve (PSVs) fail to remove decay heat during the LOOP. Consequently the core melts and RPV is breached.

In SBO accident, all AC power sources including all EDGs are lost. Reactivity is controlled by reactor trip signal. In the present SBO scenario, there is no recovery for onsite and offsite powers. Also, EFW and CCW fail to remove decay heat. Failure of CCW discontinues RCPs cooling and, consequently, seal injection to RCPs is completely lost. RCP mechanical seal cannot withstand this condition and RCP LOCA occurs. The present model is set up to include 21 gpm nominal leakage rate at 15.5 MPa for each of the two loops.

The difference between LOOP and SBO scenarios which is analyzed in this paper is in the RCPs leakage. The leakage would depressurize the Reactor coolant system (RCS) due to the mass flow rate of the leakage. This can decrease the consequence of HPME at the onset of melt ejection from vessel breach.

Results

With SBO and LOOP accidents initiation, in the lack of safety systems, temperature of fuel rods increase to the melting point of fuel and clad (Figure 4). In SBO condition, without EDGs recovery power, RCP seal is lost and fuel temperature increase to the melting point sooner compared with LOOP condition. Generally, SBO is a faster transient than LOOP. Figure 3 shows peak of clad temperature in SBO with 21 gpm seal leakage of RCPs and LOOP conditions.

Figure 4: Peak clad temperature for SBO and LOOP accident.

Both SBO and LOOP are high-pressure melt ejection severe accidents. In Figure 5, reactor coolant pressure in SBO and LOOP conditions are shown. In the case of RCP seal leakage, RCS pressure decreases slightly. This can mitigate HPME in severe accident scenario. In LOOP scenario, RCS pressure change in high pressure range and HPME will be continued until the end of corium evacuation to the core catcher. This leads to increase HPME effect in core catcher.

Figure 5: Reactor coolant pressure for SBO and LOOP accident.

As the corium reaches to the lower plenum, it starts to rupture and the corium spout from the vessel into the core catcher. This can happen in the first 6 hours of SBO accident while in LOOP scenario it happens after 7.84 h. However, in LOOP accident, more corium is ejected into the core catcher. Figure 6 shows the mass of corium injected into the core catcher after vessel breach.

Figure 6: Core melt ejection through vessel breach in SBO and LOOP condition.

Inside core catcher, Molten Corium Concrete Interaction (MCCI) leads to corrosion of containment basement concrete and the mass of corroded concrete is aggregated with the corium. Mass of heavy resultant mixture in core catcher is shown in Figure 7.

Figure 7: Total mass of Heavy mixture in core catcher in SBO and LOOP condition.

The leakage from RCS decreases corium heat in SBO condition. In the absence of RCP leakage in LOOP condition, a larger amount of heat is generated in corium. Figure 8 shows heat loss to concrete in LOOP and SBO conditions. This heat goes to the ablation of concrete. More heat in the LOOP condition lead to more erosion of containment basement.

Figure 8: Heat loss to concrete for SBO and LOOP condition.

Considering the fact that total mass of corium in core catcher in LOOP accident is more than that in SBO accident, the corrosion of the containment basement concrete is more in LOOP situation in both axial and radial directions. Figures 9 and 10 show the core catcher basement erosion in axial and radial direction respectively.

Figure 9: Axial coordinate of core catcher body for SBO and LOOP condition.

Figure 10: Radial coordinate of core catcher body for SBO and LOOP condition.

MCCI have some of the products such as hydrogen and carbon mono oxide. These two products make hydrogen detonation and carbon mono oxide deflagration more probable. In LOOP accident H2 and CO are produced more than the SBO accident. Figures 11 and 12 show the mass of H2 and Co in LOOP and SBO conditions.

Figure 11: Total H2 production from MCCI in core catcher for SBO and LOOP condition.

Figure 12: Total CO production from MCCI in core catcher for SBO and LOOP condition.

Conclusion

Performance of different systems and components in nuclear power plants should be investigated in the worst cases at the design stage. Therefore, choosing the worst incident has played a strong role for this goal. The purpose of the core catcher design is to maintain the corium inside the containment and to prevent its release to the environment. In this paper, an attempt has been made to determine the worst conditions from the perspective of the core catcher design. In different accidents in severe cases, the corium evacuated to the core catcher after vessel breach. The main task of core catcher is to cool the corium and decrease the rate of the MCCI and consequently, decrease the ablation of the core catcher basement.

Despite the recent researches and studies which are published and have introduced the SBO as the worst case, this study shows that the LOOP accident is the worst case from the core catcher design aspect.

In the core catcher design, the spreading area is limited and the volume of water for the corium cooling is limited as well. In such a situation, the thickness and mass of the corium affect the corium cooling and containment basement erosion. The results show that in the LOOP case, the mass of the corium which is released to the core catcher is about 73 ton while it is about 63 ton in the SBO condition. More mass is equal to more thickness of the corium in the core catcher, and accordingly, more trouble in cooling the corium. Therefore, more MCCI will happen in the core catcher, and it leads to an increase in the rate of the core catcher basement erosion. More MCCI means an increase in the rate of H2 and CO production and increasing the possibility of hydrogen explosion, too. The most important point is the HPME, which in the LOOP case continues until the end of the corium evacuation and leads to debilitation of the core catcher structure. In the SBO case, the HPME will happen only at the onset of the vessel breach, and after that, pressure decreases slightly. These results demonstrate that the LOOP scenario should be selected for evaluation of the core catcher design as the most severe case.

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