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KURENAI : Kyoto University Research Information Repository

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decreasing period and increased with an increase in velocity and heater length<br />

for constant period. The transient non-boiling heat transfer coefficient<br />

is correlated by Eq.(12) within ±20 % . Equation(13), an analytical<br />

correlation obtained based on slug flow model, predicts the exurimental<br />

trends.<br />

(5) Two types of transient boiling were observed. In A-type boiling,<br />

the transient boiling curve coincided at higher heat flux with the steady<br />

state boiling curve and/or its extrapolation. In B-type boiling, the wall<br />

superheat remained higher than that on the steady state boiling curve and/or<br />

its extrapolation until the maximum heat flux was reached.. Under most of the<br />

experimental conditions tested, A-type boiling was observed.<br />

(6) In A-type boiling, the transient maximum heat flux increased with<br />

decreasing period and with increasing pressure,velocity and subcooling.<br />

The difference between the transient maximum heat flux and the steady<br />

state flux varied approximately as the -0.6 power of the period over the<br />

pressure, velocity, subcooling and heater size ranges of this experiment.<br />

(7) The nondimensional correlation for the transient maximum heat flux,<br />

Eq.(17), is presented for A-type boiling. Equation(17) correlates experi-<br />

mental data within ±20 % . For water at pressures from 0.1 to 5 MPa,<br />

Eq.(15) can be approximated by Eq.(18)_<br />

30

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