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VGB POWERTECH 7 (2021) - International Journal for Generation and Storage of Electricity and Heat

VGB PowerTech - International Journal for Generation and Storage of Electricity and Heat. Issue 7 (2021). Technical Journal of the VGB PowerTech Association. Energy is us! Optimisation of power plants. Thermal waste utilisation.

VGB PowerTech - International Journal for Generation and Storage of Electricity and Heat. Issue 7 (2021).
Technical Journal of the VGB PowerTech Association. Energy is us!
Optimisation of power plants. Thermal waste utilisation.

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<strong>VGB</strong> PowerTech 7 l <strong>2021</strong><br />

Verification <strong>of</strong> SPACE code based on an MSGTR experiment at the ATLAS-PAFS facility<br />

Non-dimensional Collapsed water level (-)<br />

2.0<br />

1.8<br />

1.6<br />

1.4<br />

1.2<br />

1.0<br />

0.8<br />

0.6<br />

SG Level <strong>for</strong> PAFS operation<br />

0.4<br />

SG collapsed water level<br />

Exp. (SG-1) SPACE code (SG-1)<br />

0.2<br />

Exp. (SG-2) SPACE code (SG-2)<br />

0.0<br />

0.0 0.2 0.4 0.6 0.8 1.0<br />

Non-dimensional Time (-)<br />

Non-dimensional Mass flow rate (-)<br />

1.0<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0.0<br />

Mass flow rate <strong>of</strong> PAFS line<br />

Exp. (Steam supply line)<br />

Exp. (Return water line)<br />

SPACE code (Steam supply line)<br />

SPACE code (Return water line)<br />

-0.2<br />

0.0 0.2 0.4 0.6 0.8 1.0<br />

Non-dimensional Time (-)<br />

Fig. 9. Comparison result <strong>of</strong> SG collapsed water level.<br />

Fig. 10. Comparison result <strong>of</strong> PAFS line mass flow rate.<br />

1.3<br />

1.0<br />

Non-dimensional Collapsed water level (-)<br />

1.2<br />

1.1<br />

1.0<br />

0.9<br />

Collapsed water level in PCCT<br />

Exp.<br />

SPACE code<br />

0.8<br />

0.0 0.2 0.4 0.6 0.8 1.0<br />

Non-dimensional Time (-)<br />

Non-dimensional Temperature (-)<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0.0<br />

Fluid temperature <strong>of</strong> PAFS line<br />

Experiment PAFS model Default option<br />

Steam supply Steam supply Steam supply<br />

Return water Return water Return water<br />

-0.2<br />

0.0 0.2 0.4 0.6 0.8 1.0<br />

Non-dimensional Time after PAFS opseration (-)<br />

Fig. 11. Comparison result <strong>of</strong> PCCT water level.<br />

Fig. 12. Comparison result <strong>of</strong> fluid temperature at PAFS line after PAFS<br />

operation.<br />

lation result is consistent with the experimental<br />

results. Following the PAFS operation,<br />

the pressure in an intact SG-2 drastically<br />

decreased due to the cooling by PAFS;<br />

the SG-2 depressurization trend is similar<br />

to the core cooling rate trend.<br />

F i g u r e 9 shows a comparison <strong>of</strong> the SG<br />

collapsed water levels in the experiment<br />

<strong>and</strong> in the SPACE calculation. The water<br />

level <strong>of</strong> broken SG-1 increased <strong>and</strong> reached<br />

the full water level. By contrast, that <strong>of</strong><br />

an intact SG-2 decreased rapidly <strong>and</strong><br />

reached a set point <strong>of</strong> the PAFS operation.<br />

As the PAFS signal was triggered, the PAFS<br />

operation valve automatically opened, <strong>and</strong><br />

the main steam from the SG-2 flowed<br />

into the steam supply line. As shown in<br />

F i g u r e 10 , the mass flow peaked, <strong>and</strong><br />

then natural circulation flow was <strong>for</strong>med.<br />

The mass flow rate in the case <strong>of</strong> SPACE calculation<br />

was consistent with the experimental<br />

result. The main steam from the<br />

steam supply line flowed into the condensation<br />

tubes, <strong>and</strong> the condensate circulated<br />

through the return water line to the economizer<br />

<strong>of</strong> the steam generator. After the<br />

PAFS was actuated, the water level also increased<br />

due to the thermal expansion, as<br />

shown in F i g u r e 11 .<br />

3.2.4 Wall condensation heat transfer<br />

model <strong>for</strong> PCHX<br />

The wall condensation heat transfer rate in<br />

PCHX is one <strong>of</strong> the dominant factors <strong>for</strong> determining<br />

the PAFS cooling capability.<br />

There<strong>for</strong>e, the many precedent studies related<br />

to condensation in PCHX were per<strong>for</strong>med.<br />

The wall condensation models<br />

were incorporated into the SPACE code<br />

heat transfer package. For pure steam condensation,<br />

like the problem addressed in<br />

this paper, the same model used in RE-<br />

LAP5/MOD3.3 was selected as a default<br />

model. The maximum value among Nusselt’s<br />

[14], Shah’s [15], <strong>and</strong> Chato’s [16]<br />

correlations is used to consider the geometric<br />

<strong>and</strong> turbulent effects. The experimental<br />

correlation <strong>for</strong> PAFS is also included in the<br />

wall condensation model as an option in<br />

SPACE code [17]. Based on the calculation<br />

results mentioned in chapter 3.2.1, this<br />

model was applied. In this section, the default<br />

model <strong>and</strong> experiment correlation<br />

model <strong>for</strong> PAFS were compared to confirm<br />

the prediction ability <strong>of</strong> SPACE code <strong>for</strong><br />

PCHX cooling per<strong>for</strong>mance. Chen’s model,<br />

which is the default option in SPACE code,<br />

is applied to the outside <strong>of</strong> PCHX [18].<br />

The fluid temperature after PAFS operation<br />

is shown in F i g u r e 1 2 . The calculation<br />

result shows that the fluid temperature on<br />

the return water line is higher than the experiment,<br />

<strong>and</strong> that the default option case<br />

is highest. That means that the calculation<br />

results which were obtained using the default<br />

option <strong>and</strong> the PAFS model underestimated<br />

cooling per<strong>for</strong>mance. However, the<br />

calculation using the PAFS model was<br />

more accurate than the default option.<br />

4. Conclusions<br />

In this study, a MSGTR experiment with<br />

the PAFS operation per<strong>for</strong>med by KAERI<br />

was simulated using the SPACE code. This<br />

study focused on verifying the prediction<br />

capability <strong>of</strong> the SPACE code <strong>for</strong> MSGTR<br />

accidents, which is one <strong>of</strong> the multiple fail-<br />

83

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