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KURENAI : Kyoto University Research Information Repository

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As mentioned above, the transient boiling curve had a portion where<br />

Zhe wall superheat shifts to the right of the steady state boiling<br />

curve. A similar phenomenon is reported to have been observed in pool<br />

boiling of water [13] .<br />

I.3.2.c Transient Maximum Heat Flux<br />

Figures 19 through 27 are correlative representations of the experi-<br />

mental transient maximum heat flux vs. exponential period. Solid lines<br />

in these figures represent an empirical correlation, Eq.(17) and will<br />

be discussed later. The boundary between A-type and B-type boilings is<br />

also indicated in some of these figures by dot-dash-line. Unless bound-<br />

aries are indicated in the figure, A-type boiling is meant. Effects of<br />

period, pressure, subcooling, velocity and heater size on the transient<br />

maximum heat flux will be discussed individually.<br />

Effect of exponential period on transient maximum heat flux is given<br />

in Fig.26(a) for 0.8 mmdiam, 7 cm long heater at pressure 0.396 MPa, sub-<br />

cooling 30 K and velocity from 1.35 to 4.04 m/s. In this figure, the right<br />

hand side of the dot-dash-line is a region of A-type transient boiling and<br />

the left hand side a region of B-type. In the A-type region, the transient<br />

maximum heat flux increases with decreasing period at constant velocity,<br />

whereas,in the B-type region, the transient maximum heat flux , decreases<br />

with the period and then increases. •<br />

Effects of velocity, subcooling and pressure are seen in Figs.26(a),<br />

(b) and (c), respectively. Results thus indicate that the transient max-<br />

imum heat flux increases as the period is decreased and, for a constant period<br />

it increases with increasing velocity, subcooling and pressure.<br />

25

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