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An Experimental and Theoretical £ Investigation of Annular Steam ...

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- 24 -<br />

3.2.5. Measurements <strong>of</strong> Wave Frequency <strong>and</strong> Velocity<br />

Besides being used for the determination <strong>of</strong> the film thickness,<br />

the needle contact probes were also used to measure the<br />

frequency <strong>and</strong> velocity <strong>of</strong> the roll waves on the film. (Cf<br />

Whalley, Hewitt, Hutchinson (1973)).<br />

By means <strong>of</strong> the Hewlett Packard 3721A correlator, an autocorrelation<br />

<strong>of</strong> the signal from one needle was recorded. The<br />

correlation was then processed by a Hewlett Packard 3720A<br />

spectrum display to obtain the power spectrum <strong>of</strong> the signal.<br />

The signals from two needles, mounted 0.5 m apart, were then<br />

cross-coirrelated using the 3721A correlator.<br />

Typical examples <strong>of</strong> correlations <strong>and</strong> power spectra are<br />

shown on figs. 3.35 <strong>and</strong> 3.36.<br />

3.3. <strong>Experimental</strong> Data<br />

A summary <strong>of</strong> the experiments is given in table 3.2. This<br />

lists the test sections, the main system parameters <strong>and</strong> the<br />

measurements carried out in the experimental periods.<br />

In the table, the diabatic length L- refers to the distance<br />

between the inner sides <strong>of</strong> the power clamps. The adiabatic length<br />

L is the distance between the inner side <strong>of</strong> the upper power<br />

cl<br />

clamp <strong>and</strong> the lower end <strong>of</strong> the suction area. In the adiabatic<br />

experiments this length is identical to the total length <strong>of</strong> the<br />

test section.<br />

The majority <strong>of</strong> the data obtained are reported graphically<br />

in this section. A complete list or the data is given in tabular<br />

form in Appendix.<br />

3.3.1. Film Flow Rates<br />

The film flow rates are estimated from suction curves, which<br />

are obtained as described in sect. 3.2.2. In fig. 3.9 an example<br />

<strong>of</strong> a suction curve is shown. Two straight lines are drawn through<br />

the measuring points. The line with the slope s is assumed to<br />

represent the situation where droplets are sucked <strong>of</strong>f the core.<br />

The intersection <strong>of</strong> this line with the line in • 0 (x^ -m /m =<br />

g out g<br />

x Qut ) is assumed to represent the film flow rate m f . In this<br />

figure <strong>and</strong> in the tables the film flow rate is designated m f .<br />

The line with the slope s<br />

is assumed to represent the case<br />

where waves on the film are sucked <strong>of</strong>f. Thus the intersection

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