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Chapter 8 Safety Evaluation of PWR Plants

During the time from the end of coolant blowdown to arrival of the water injected into the core, heat removal capability in the reactor core is especially reduced; and the temperature of the fuel cladding increases near the fuel pellet temperature. But when the reactor core begins to be reflooded, the core is cooled by steam generated in the core and a mixed flow of the steam and drops of water entrained by the steam occurs, and the temperature of the fuel cladding gradually decreases.

Throughout the above progress of the accident, the maximum temperature of the fuel cladding is kept less than about 1027X3 and the amount of zirconium-water reaction is kept less than about 3.6% at the maximum portion, which meets the limit values of 1200°C and 15% oxidation required by the “Guide for Evaluation of the Performance of the Emergency Reactor Core Cooling System of Light Water Power Reactors/'

Furthermore, the release of radioactive materials is within the extent that undue risk of radiation exposure to the general public in the vicinity of the facility is avoided.

  1. Steam Generator Tube Rupture

For this event, a rupture of a steam generator heat transfer tube at power operation and consequent leakage of primary coolant to the secondary side of the steam generator is postulated If no remedial action is taken against the event, primary coolant leakage to the secondary side of the steam generator will continue, and the radioactive

materials contained in the steam of the secondary side are continuously released to the atmosphere through a steam relief valve and the exhaust line of a condenser vacuum pump.

However, a number of measures are provided for mitigation of such development of the situation and early termination of the event

They are as follows.

(D Radiation monitors are installed in the blowdown piping of the steam generators and on the exhaust line of the condenser vacuum pump to generate alarms in case a high level of radioactivity is detected.

  1. The reactor is automatically tripped by the following signals from the reactor protection systems:

  • Low reactor pressure

  • High over- temperature AT

  1. If the leakage of reactor coolant continues, the ECCS is actuated by the following signals, and the boric acid water from the refueling water storage tank and boron injection tank is injected into the core:

•Coincidence of low reactor pressure and low pressurizer water level

•Low reactor pressure

Figure 8.3.2 shows the analytical results of reactor power, reactor pressure, secondary system pressure and amount of primary coolant leakage in case of an instantaneous rupture of a heat transfer tube. The event development with time is as follows.

(D The reactor is automatically tripped by the

120 r-

100 - | 80 -

60 -

s

§ 40 -

nt

20 -

0 -

Time (min)

Figure 8.3.2 Steam generator tube rupture (• indicates the initial value)

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NSRA, Japan

“High over-temperature AT“ signal generated about 5 minutes after the occurrence of the accident. As a result, the secondary system pressure rises rapidly at a turbine trip following the reactor trip ((D in Figure 8.3.2).

  1. The reactor pressure decreases along with leakage of the reactor coolant, but the emergency core cooling system is actuated by the signal “coincidence of low reactor pressure and low pressurized water level" 7 minutes after the initiation of the accident, and the boric acid water of the refueling water storage tank is injected into the reactor, resulting in increase of reactor pressure again ((2) in Figure 8.3.2).

  2. The pressure of the secondary system increases for a time as a result of turbine trip, but the pressure increase is suppressed by actuation of the main steam safety valve and other equipment, and then the steam pressure is maintained around the pressure set point of the secondary steam relief valve.

  3. The operator isolates the failed steam generator about 30 minutes after the initiation of the accident, and then by operating a steam relief valve in the intact steam generator, the temperature of the primary system is decreased ((3) in Figure 8.3.2). Furthermore, by operation of the pressurizer relief valve approximately 40 minutes after the accident initiation ( @ in Figure 8.3.2), the pressure of the reactor coolant system is decreased to the failed steam generator secondary pressure. By closing of

the pressurizer relief valve at that time, the reactor coolant pressure increases again, but the ECCS is stopped about 44 minutes after the accident initiation ( (5) in Figure 8.3.2). By about 50 minutes after the accident start, the coolant pressure decreases to the failed steam generator secondary side pressure, and leakage of coolant to the secondary system is terminated.

Throughout the above progress of the accident, release of radioactive materials into the atmosphere is within the extent that the undue risk of irradiation exposure to the general public in the vicinity is avoided and fuel integrity is secured by the minimum DNBR not decreasing below the allowance limit

  1. Dose Evaluation in Accidents

As described above, in many cases of accidents a failure of barriers to prevent release of radioactive materials outside the plant is postulated. Since that is the case for accidents, unlike “abnormal transient during operation” in which no failure of fuel, nor failure of barriers enclosing the reactor coolant is predicted, radioactive material might possibly reach general public in the vicinity of the facility through the failure of the barriers

Table 8.3.1 shows examples of safety evaluation for a 3-loop PWR plant regarding radiation exposure to the public at the boundary of the facility for postulated “accidents."

Table 8.3.1 Evaluation of dose in accidents (Examples for a 3-loop plant)

Effective Dose Equivalent (mSv)

Radioactive Gas Waste Facility Rupture

Approx. 0.53 (Rare Gas 1.5 x 10HBq Approx.)

Steam Generator Tube Rupture

Approx. 1.7 Rare Gas 4.4 x 10HBq Approx.

Iodine 9.2 x 1010Bq Approx.

Fuel Assembly Drop

Approx. 0.026 Rare Gas 6.0 x 1012Bq Approx.

Iodine 8.1 x 1010Bq Approx.

Loss of Reactor Coolant

Approx. 0.60 Rare Gas 4.4 x 1013Bq Approx.

Iodine 2.4 x 10nBq Approx.

Control Rod Ejection

Approx. 0.29 Rare Gas 2.0 x 1013Bq Approx.

Iodine 1.5 x 1010Bq Approx.

[Note] Rare gas is converted to y ray energy of 0.5Mev; iodine is 1-131 equivalent

NSRA, Japan

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