atw - International Journal for Nuclear Power | 04.2019
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<strong>atw</strong> Vol. 64 (2019) | Issue 4 ı April<br />
OPERATION AND NEW BUILD 214<br />
significant cracking can be tolerated<br />
without loss of essential jet pump<br />
safety functions. There<strong>for</strong>e, it is<br />
important to evaluate the remaining<br />
structural integrity when a riser is<br />
cracked.<br />
2 Statement<br />
of the problem<br />
The development of helical cracks at<br />
the weld between the riser and the<br />
riser brace compromise the structural<br />
integrity of the jet pumps. There<strong>for</strong>e,<br />
it is very important to evaluate the<br />
critical size of a crack that could<br />
be tolerated, be<strong>for</strong>e a complicated<br />
reparation has to be introduced. It can<br />
be considered that the failure can be<br />
in the range of brittle and ductile<br />
conditions. So, a methodology which<br />
considers both conditions of failure is<br />
required.<br />
3 Materials and methods<br />
In order to obtain the critical size of<br />
the crack, the loads applied on the jet<br />
pump arrangement were evaluated.<br />
The hydrodynamic loads are included.<br />
It has to keep in mind that aging could<br />
take place as hours of operation are<br />
accumulated. For this purpose, brittle<br />
and ductile failures were evaluated<br />
with fracture mechanics and net<br />
section collapse analysis approaches,<br />
respectively. Then, these results were<br />
compared against those obtained with<br />
Failure Assessment Diagrams.<br />
The hydraulic loads considered,<br />
were the following: by cross flow, the<br />
impulse loading of the pump of the<br />
Reactor Recirculation Core (RRC)<br />
system and the vibration induced by<br />
fluid flow (fatigue). In the last case,<br />
the dynamic loads are generated by<br />
the bend located at the lower end of<br />
the riser, the ram head at the top of<br />
the riser and the mixer of the jet<br />
pump. The thermohydraulic analysis<br />
was carried out with the RELAP/<br />
SCDAPSIM code [7, 8].<br />
Another source of vibration are the<br />
dynamic loads from strong earthquakes.<br />
However, strong earth quakes<br />
are not a source of fatigue because of<br />
these events do not happen everyday<br />
at the same place. Summarizing, it is<br />
important to evaluate the impact of<br />
the dynamic loads which will take<br />
place on the structural integrity of the<br />
jet pumps.<br />
3.1 Cross flow<br />
The simplified method, described in<br />
the Part N1324.1 “Avoiding Lock-In<br />
Synchronization” of Section III of the<br />
ASME Code [9], was followed. Initially,<br />
the Vortex Shedding frequency is<br />
calculated with the following relationship.<br />
(1)<br />
Where: S is the Strouhal number<br />
and it is a function of the Reynolds<br />
number, U is the velocity of the cross<br />
flow and D is the lower diameter of the<br />
assembly of the jet pumps. The calculations<br />
show that the Vortex Shedding<br />
frequency was 10.7 Hz. In accordance<br />
with the criterion of the ASME code<br />
mentioned above, 1.3f s must be lower<br />
than the first natural frequency<br />
(26.3 Hz), in order to avoid “Lock-In<br />
Synchronization” with the first mode.<br />
So, as a conclusion, cross flow vibration<br />
resonance did not take place.<br />
3.2 Impulse loading of the<br />
pump of the external<br />
Reactor Recirculation Core<br />
(RRC) system<br />
In accordance with the open literature<br />
[10, 11, 12], the centrifugal pump<br />
of each circuit of RRC operates at<br />
1,800 RPM. As a result, its frequency<br />
is 30 Hz. The impeller of the centrifugal<br />
pump has five blades. There<strong>for</strong>e,<br />
the impulse frequency is 5 (30 Hz) =<br />
150 Hz. If this parameter is compared<br />
with the range of the first 5 natural<br />
frequencies (26.3 Hz – 67 Hz), it can<br />
be concluded that resonance in operation<br />
is not induced.<br />
3.3 Flow-Induced Vibration<br />
(fatigue)<br />
The sources of fatigue on the jet pump<br />
arrangement are the dynamic <strong>for</strong>ces<br />
and moments generated by the internal<br />
flow of water.<br />
Forces at the lower elbow of the riser:<br />
These <strong>for</strong>ces are generated by the inlet<br />
flow of water at the elbow of the riser.<br />
They were calculated by the following<br />
relationships (Figure 2):<br />
(2)<br />
(3)<br />
ρ is the water density. p 1 and p 2 are the<br />
pressures at the inlet and outlet of the<br />
bend, respectively. A 1 and A 2 are the<br />
cross sections at the inlet and outlet of<br />
the bend and θ is the angle of the<br />
bend. For a 90° elbow, the <strong>for</strong>ces<br />
are resulting. F x = 15,500 lb and<br />
F y = 15,500 lb horizontal and vertical<br />
respectively.<br />
Forces over the mixer nozzles of the<br />
jet pumps (Figure 3): This <strong>for</strong>ce is<br />
| | Fig. 2.<br />
Forces on the bend.<br />
| | Fig. 3.<br />
Forces on the bend.<br />
| | Fig. 4.<br />
Forces generated by the ram head over the riser.<br />
developed by the flow discharge,<br />
which comes from the Reactor Recirculation<br />
Core System, and is mixed<br />
with the suctioned flow of the condensed<br />
steam. The vertical <strong>for</strong>ce is:<br />
(4)<br />
ΔP is the differential pressure and A i is<br />
the cross section of the nozzle. For the<br />
jet pump assembly under study are<br />
186.7 pound/inch 2 and 26.1 inch 2 ,<br />
respectively. So, the resultant <strong>for</strong>ce is<br />
4881 pounds upwards.<br />
Forces generated by the ram head<br />
over the riser (Figure 4): The vertical<br />
loads over the riser, which are generated<br />
by both elbows of the ram head,<br />
were calculated with the following<br />
equation:<br />
(5)<br />
F y is the vertical <strong>for</strong>ce, ρ is the water<br />
density, p 1 and p 2 are inlet and outlet<br />
Operation and New Build<br />
Failure Analysis of the Jet Pumps Riser in a Boiling Water Reactor-5 ı<br />
Pablo Ruiz-López, Luis Héctor Hernández-Gómez, Juan Cruz-Castro, Gilberto Soto-Mendoza, Juan Alfonso Beltrán-Fernánde and Guillermo Manuel Urriolagoitia-Calderón