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