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30 Containment systems Decay power

The safety system of 4S consists of the reactor shutdown system, decay heat removal system and containment. The reactor is shutdown by insertion of a neutron absorber into the core center and lowering of the reflector which surrounds the core. The reflector is divided into six parts and managed by two hydraulic systems corresponding to 3 reflector segments. The reflector moves down by opening two scram valves of a hydraulic system which has the required redundancy. If the valve of a hydraulic system is opened during upward motion of the reflector, scram is initiated and the reflector drops. Should the neutron absorber and reflector not work, the power drops due to the negative feedback coefficient to lead the reactor to its inherent shutdown. [Pg.539]

Similar to other thermal reactor designs, there are three basic functions that are necessary to mitigate the consequences of fission product releases during a postulated accident. The functions, referred to as the 3 Cs, are control, cool, and contain. Control refers to safe reactor shutdown. Cool involves the removal of heat—from the fuel produced by the fission process (at power) or by the decay heat after reactor shutdown—and rejection of the heat to a heat sink. Contain is simply the physical means to prevent the release of radioactive material to the atmosphere by provision of containment systems. [Pg.178]

The quantity, time-dependence and composition of the volatilized substances may significantly influence the further behavior of the radionuclides as well as the progress and the products of chemical reactions occurring in the primary system and in the reactor containment. On the other hand, the volatilization of the fission products from the reactor core is able to affect the further progress of core heatup and degradation, since in the first hour after reactor shutdown the gaseous and volatile fission products contribute approximately 30% of the total decay power of the core. [Pg.496]

Figure I-8(b) shows similar results for the steam vent line break. It is observed that heat rejection through the containment wall quickly exceeds core decay power, thus demonstrating the effectiveness of the liquid pool as an ultimate heat sink for long-term control of system pressure and removal of core decay heat. It also shows the equalization between reactor vessel pressure and the containment pressure, effectively stopping the break flow. The maximum containment pressure reached is 1.1 MPa (160 psi). Figure I-8(b) shows similar results for the steam vent line break. It is observed that heat rejection through the containment wall quickly exceeds core decay power, thus demonstrating the effectiveness of the liquid pool as an ultimate heat sink for long-term control of system pressure and removal of core decay heat. It also shows the equalization between reactor vessel pressure and the containment pressure, effectively stopping the break flow. The maximum containment pressure reached is 1.1 MPa (160 psi).
The turbine plant building is similar to those of standard nuclear power plants. The containment houses the primary circuit, which is located in the lower part of the containment building. All the safety systems (low pressure safety injection system, decay heat removal system, etc.) are located inside the containment building. [Pg.221]

These isotopes are sometimes used as tracers of natural terrestrial processes and cycles. Long-lived isotopes, such as Rb and Sm are used for precise dating of geological samples. When the solar system formed it also contained several short-lived isotopes that have since decayed and are now extinct in natural systems. These include Al, Fe, Pu, Pd, and Al with a half-life of less than a million years is particularly important because it is a potentially powerful heat source for planetary bodies and because its existence in the early solar system places tight constraints on the early solar system chronology. [Pg.19]

As stated above (see Chapter II.B), LII signals also contain information about the size distribution. To compare the influence of different plasma powers on primary particle diameters, different ways of size evaluation have been accomplished. It could be shown by assuming a monodisperse distribution that the mean primary particle diameter is 31 nm for 30 kW and 33 nm for 70 kW. In contrast, under the assumption of a log-normal distribution and by applying the two-decay time evaluation, the determination yields a different result which can be seen in Figure 15. Size distributions with median sizes of 17nm and 28 nm and standard deviations of 0.39 and 0.18 for 30 kW and 70 kW were observed, respectively. This indicates that in practical production systems, the evaluation of a mondisperse distribution is not sufficient. Unfortunately, the reconstruction of particle size distributions is relatively sensitive on... [Pg.240]

It has been recognized that the Lu-Hf isotopic system in zircon is a powerful tool for deciphering the evolution of the earth s crust and mantle. " Zircon normally contains 0.5-2 wt % Hf, which results in an extremely low Lu/Hf ratio (" Lu/" Hf < 0.002) and consequently a negligible radiogenic growth of Hf due to the decay of Lu. Therefore, the Hf/" Hf ratio of zircon can be regarded as the initial value at the time when it crystaUized. LA-ICP-MS with a multiple ion collector system has also been employed to study the hafnium isotopic composition of zircon and baddeleyite standards in U-Pb geochronology. °°... [Pg.404]

Equation (54) means [31] that Eq. (52) now contains a slowly decaying (a < 1) memory function with a power law kernel so that the process is no longer Markovian and thus depends on the history of the system. Equation (52) stems... [Pg.304]

In partially chaotic flows that contain KAM tori and elliptic islands, there is only slow diffusive transport across the invariant tori. Therefore the global decay rate vanishes in the Pe —> oo (i.e. D —> 0) limit. It was found numerically that the decay rate follows a power law 7 Pe-", with an exponent in the range 0 < a < 1, while the eigenmodes in such systems are mostly localized in the non-mixing region of the flow (Giona et al., 2004 Pikovsky and Popovych, 2003). [Pg.75]

Transfer system. The principal system used to transfer fuel and other components to and from the reactor vessel is the closed loop ex-vessel machine (CLEM) shown in Fig. A.2. The CLEM loads all components into the reactor vessel and removes all components from the reactor vessel and operates only when the reactor is shutdown. Under most conditions, CLEM moves a core component pot (CCP) that contains the fresh or SNF fuel to and from the reactor vessel. In a fast reactor, the core power density is very high thus, there is significant decay heat in each SNF assembly immediately after reactor shutdown. To prevent fuel failure from overheating, the SNF is kept in sodium at all times to ensure effective cooling. This is accomplished by transferring each fuel assembly in its own pot of sodium—the CCP. CLEM is also used to transfer a variety of other components within the reactor containment. [Pg.73]

The interpretation of the saturation intensity result, Eq. (8), contains a snbtlety. In the conservative two-state system nnder discnssion, a molecule removed from the upper state by laser-stimulated emission at the rate aJe(hc/Xu) per molecule must appear in the lower state. There it itmnediately is subjected to a pump rate (per molecule) of a l j hcjX returning it to the upper state. Thus for stimulated emission to produce a reduction of the small-signal upper-state population by half, it must be at a transition rate per molecule equal to the sum of the spontaneous decay rate plus the return rate, yielding Eq. (8). This makes the saturation intensity a linear function of the pump intensity at high pump rates, the e bleaches, the small-signal gain saturates at the total inversion value AT,CTe, and the output power increases with pump rate solely through the h term in Eq. (9). [Pg.78]

CFR 50.2, "Definitions", defines station blackout as the loss of the offsite electric power system concurrent with a turbine trip and unavailability of the onsite emergency AC power system. It does not include the loss of available AC power to buses fed by station batteries through inverters or by alternate AC sources. Since many systems required for core decay heat removal and containment heat removal depend on AC power, a station blackout can result in unacceptable consequences unless AC power is restored in a timely manner or AC power is supplied from an alternate source. The issue involves the likelihood and duration of station blackout and the potential for core damage as a result. [Pg.252]


See other pages where 30 Containment systems Decay power is mentioned: [Pg.244]    [Pg.2732]    [Pg.275]    [Pg.2374]    [Pg.222]    [Pg.225]    [Pg.239]    [Pg.218]    [Pg.383]    [Pg.33]    [Pg.36]    [Pg.404]    [Pg.1169]    [Pg.1193]    [Pg.246]    [Pg.210]    [Pg.436]    [Pg.180]    [Pg.122]    [Pg.103]    [Pg.110]    [Pg.1029]    [Pg.23]    [Pg.1029]    [Pg.2374]    [Pg.1149]    [Pg.1249]    [Pg.96]    [Pg.398]    [Pg.415]    [Pg.351]    [Pg.32]    [Pg.488]    [Pg.13]    [Pg.20]    [Pg.472]    [Pg.180]   
See also in sourсe #XX -- [ Pg.18 , Pg.291 ]




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