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  1. Major Accidents and Hypothetical Accidents

  1. Assumption of Events

"Major accidents" and "hypothetical accidents" are assumed to evaluate the siting for a nuclear reactor. For this, accidents likely to escalate a release of radioactive materials are selected from the "accidents" described in Section 7.3 for this along with accidents involving a release of radioactive materials to the inside of the reactor containment and a release of radioactive materials to the outside of a reactor containment are assumed. In the case of the "major accidents", a release of the technically-conceivable maximum amount of radioactive materials is assumed, and in the case of the "hypothetical accidents", accidents with a release of the hypothetically-considered greater amount of radioactive materials are assumed.

Specifically, the following two types of "accidents" are evaluated.

  1. Accidents involving a release of radioactive materials to the inside of the reactor containment)

■ Loss of reactor coolant

  1. Accident involving a release of radioactive materials to the outside of reactor containment)

• Main steam line break

The "major accident" and the "hypothetical accident" are the same in the assumed accident type, but differ in assumed release rates of radioactive materials. Accident sequences and the release rates are described for a BWR-5 (1,100 MW) plant in the following.

  1. Loss of Reactor Coolant

With a guillotine break at one location of the recirculation piping during operation, it is assumed apart from the actual accident sequences that 2 % of the noble gases and 1 % of iodine (assuming a release from fuel-rod plenums) for the "major accident" and 100 % of the noble gases and 50 % of iodine (assuming a core meltdown) for the "hypothetical accident" of the radioactive materials accumulated in the reactor core are released.

For a 1,100 MW class BWR, the radioactivity of radioactive materials accumulated in the core is approximately 3.2 x 1019 Bq from noble gases and approximately 3.1 x 1019 Bq from iodine. While some

of the radioactive materials released inside of the containment are being removed due to effects of water spraying and deposition, they leak from the containment at a constant rate.

The release process of iodine is discussed in the following. In the case of the "major accidents", it is assumed that 1 % of iodine accumulated in the reactor core is released inside of the containment. The organic iodine is assumed to account for 10 % of the total iodine released, and the removing effect by the containment spray is ignored.

On the other hand, 50 % of the remaining 90 % inorganic iodine is assumed to deposit inside of the containment. Furthermore, the remaining inorganic iodine transfers into the liquid by the containment spray, but the ratio of the iodine in the gas to that in the liquid is assumed to be one hundredth (partition coefficient of 100).

Valve seats etc. of isolation valves can be considered as the leak paths, but it is assumed that radioactive materials in the containment leak at a constant rate of 0.5 %/d in total. The leaked radioactive materials deposit within the reactor building, but ignoring this effect, only the natural decay is conservatively assumed. Almost all of the iodine which leaked into the reactor building is removed by the standby gas treatment system, and the rest is discharged from the main exhaust stack. The release process of iodine that affects the dose to the thyroid gland is provided in Figures 7.4.1(1) and (2) as examples.

  1. Main Steam Line Break

Assuming a guillotine break of the main steam line outside of the containment, the radioactive materials contained in the main steam are released to the atmosphere until the main steam isolation valves are closed. Following that, it is assumed that the radioactive materials additionally released from the damaged fuel with depressurization of the reactor leak from the main steam isolation valves and are released to the atmosphere.

The concentration of radioactive materials contained in the main steam line when the accident occurred is equivalent to the maximum acceptable 131I concentration during operation, and the composition is a diffusion composition. The amount of halogens in the reactor coolant from

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Chapter 7 Safety Evaluation of BWR Plants

these assumptions is about 7.2 x 1013 Bq (equivalent in terms of 0.5 MeV y -ray energy). The amount of 131I additionally released from the damaged fuel with depressurization for BWRs is a value based on the operational data of preceding reactors during plant shutdown taking into account an appropriate margin (about 7.4 x 10I3Bq), and the composition of other nuclides is the equilibrium composition.

The amount of released radioactive materials from the main steam line is the same for both the "major accident" and the "hypothetical accident", but the treatment of additionally released radioactive materials during depressurization differs as follows:

  1. Transfer ratio to the suppression pool through the safety and relief valves etc., and

  2. Leak duration, etc.

Now, assuming that steam containing radioactive materials discharged before closure of the main steam isolation valves evaporates completely in the air forming a hemispherical steam plume, and this plume moves to the leeward direction at a speed of 1 m/s without dispersion, the effective dose equivalent is evaluated. On the other hand, for the additionally released radioactive materials after closure of the main steam isolation valves, they are evaluated taking into account their dispersion on the ground and a certain degree of their diffusion in the atmosphere.

The release process of iodine that affects the thyroid gland dose is provided in Figures 7.4.2 (1) and (2) as examples.

Amount of iodine in the reactor Approx. 5.4 x 10l8Bq

Release from fuel into the containment Release ratio: 1%

I

Leak from the gaseous phase of the containment Leak rate: 0.005/d

Duration of the leak: Infinite period

Amount of iodine in the reactor Approx. 4.9 x 10l8Bq t-

Release from fuel into the containment Release ratio: 50%

I

Leak from the gaseous phase of the containment Leak rate: 0.005/d

Duration of the leak: Infinite period

Iodine in the reactor building

i

Discharge from the main stack

I

Discharge from the main stack

Figure 7.4.1 (2) Iodine discharge process to the atmosphere during a loss of the reactor coolant (hypothetical accident) (131l equivalent: Adult thyroid gland)

Figure 7.4.1 (1) Iodine discharge process to the atmosphere during a loss of the reactor coolant (major accident) (™l equivalent: Infant thyroid gland)

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