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IGCAR : Annual Report - Indira Gandhi Centre for Atomic Research

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IGC<br />

<strong>Annual</strong> <strong>Report</strong> 2007<br />

expected in this row. Hence the<br />

optimum position of the<br />

thermocouple tip determined<br />

<strong>for</strong> this location will be<br />

conservative <strong>for</strong> the other inner<br />

rows. Hot water (≈ 338 K) was<br />

sent through one SA, whereas<br />

in the rest of the core, cold<br />

water was circulated. The<br />

attenuation of temperature at<br />

this thermocouple tip location<br />

by the neighbouring SAs was<br />

studied. A retractable<br />

thermocouple was inserted in<br />

this location from the CP top as<br />

shown in Fig.1. The height of<br />

the thermocouple tip above<br />

core top can be varied by<br />

traversing the thermocouple<br />

from CP top. From the<br />

statistical analysis of data the<br />

mean temperature as seen by<br />

each thermocouple was<br />

estimated. These temperature<br />

data are presented in a<br />

normalized <strong>for</strong>m to transpose<br />

the result into reactor case by<br />

substituting the prototype<br />

parameters. The normalization<br />

is done in the following<br />

manner.<br />

where,<br />

T = Mean temperature of the<br />

fluid as measured by the<br />

thermocouple mounted in CP<br />

T h = Mean temperature of the<br />

hot inlet fluid (Thermocouple<br />

mounted at the SA exit)<br />

Tc<br />

= Mean temperature of<br />

the cold inlet fluid<br />

(Thermocouple mounted at the<br />

SA exit)<br />

The normalized mean<br />

temperature ( )is<br />

plotted against the elevation of<br />

the thermocouple tip above<br />

core top <strong>for</strong> various<br />

experimental conditions. The<br />

result is presented Fig. 2. It can<br />

be seen from the above figure<br />

that normalized mean<br />

temperature is close to unity<br />

(which means the fluid<br />

temperature as measured by<br />

the thermocouple is almost<br />

equal to the SA exit<br />

temperature) at the core<br />

temperature monitoring point<br />

upto the height of 34 mm<br />

above core top in model and<br />

then it decreases gradually<br />

along the jet axis due to the<br />

increased mixing of the liquid<br />

streams. The corresponding<br />

height of the thermocouple tip<br />

in reactor is 136 mm (because<br />

the geometric scale of the<br />

model is 1:4). The normalized<br />

mean temperature is also<br />

independent of Re upto this tip<br />

elevation above core top.<br />

Fig.2 Variation in mean temperature along the jet axis (in model)<br />

ENABLING TECHNOLOGIES 127

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