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ORNL-2106 - the Molten Salt Energy Technologies Web Site

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ANP PROJECT PROGRESS REPORT<br />

RADIATION HEATING ON THE ART<br />

EQUATORIAL PLANE IN THE VICINITY<br />

OF THE FUEL-TO-NaK HEAT EXCHANGER<br />

H. W. Bertini<br />

The results of calculations of <strong>the</strong> radiation<br />

heating on <strong>the</strong> ART equatorial plane in <strong>the</strong> outer<br />

3 cm of <strong>the</strong> beryllium reflector and in <strong>the</strong> Inconel<br />

and <strong>the</strong> boron-containing shells on both sides of<br />

<strong>the</strong> fuel-to-NaK heat exchanger are presented in<br />

Figs. 1.2.1 and 1.2.2. The total gamma-ray<br />

heating in each region is given in Fig. 1.2.1,<br />

as well as <strong>the</strong> heating from <strong>the</strong> sources which<br />

are <strong>the</strong> main contributors to <strong>the</strong> total in each<br />

28<br />

Source<br />

No.<br />

1*<br />

2<br />

3<br />

4<br />

5<br />

6<br />

7<br />

8<br />

9<br />

10<br />

11<br />

12<br />

13<br />

14<br />

1.2. ART PHYSICS<br />

A. M. Perry<br />

shell. The encircled numbers on Fig. 1.2.1 refer<br />

to <strong>the</strong> sources described in Table 1.2.1.<br />

The data on heating in <strong>the</strong> copper-boron layer<br />

by alpha particles from <strong>the</strong> B10(n,u)Li7 reaction<br />

are plotted in Fig. 1.2.2. The heating goes to<br />

infinity at <strong>the</strong> face of <strong>the</strong> layer closest to <strong>the</strong><br />

core because <strong>the</strong> heating at various points is<br />

governed by an E, function,<br />

where h is <strong>the</strong> mean free path. The integral under<br />

<strong>the</strong> curve will be finite.<br />

TABLE 1.2.1. SOURCES OF RADIATION HEATING CONSIDERED IN CALCULATING<br />

THE RESULTS PRESENTED IN FIG. 1.2.1<br />

Source<br />

Prompt gamma rays in <strong>the</strong> fuel region of <strong>the</strong> core of <strong>the</strong><br />

reactor<br />

Decay gamma rays in <strong>the</strong> fuel region of <strong>the</strong> core of <strong>the</strong><br />

reactor<br />

Gamma rays from inelastic scattering of neutrons in <strong>the</strong><br />

fuel region of <strong>the</strong> core<br />

Capture gamma rays in <strong>the</strong> outer core shell<br />

Capture gamma rays in <strong>the</strong> reflector (average)<br />

Capture gamma rays in first Inconel shell outside of<br />

beryl1 ium reflector<br />

Boron capture gamma rays in copper-boron layer<br />

Alpha particles from <strong>the</strong> B1O(np)Li7 reaction in <strong>the</strong><br />

copper-boron layer (average)<br />

Decay gamma radiation from <strong>the</strong> fuel in <strong>the</strong> heat exchanger<br />

Gamma rays from inelastic scattering of neutrons in first<br />

9 cm of reflector (average)<br />

Capture gamma rays from delayed neutrons in <strong>the</strong> heat exchanger<br />

and Inconel shells (including <strong>the</strong> pressure shell)<br />

Capture gamma rays in <strong>the</strong> copper of <strong>the</strong> capper-boron layer<br />

Gamma rays from inelastic scattering in both core shells<br />

Capture gamma rays in <strong>the</strong> island core shell<br />

*In Fig. 1.2.1 <strong>the</strong> data for heating from sources I, 2, 3 are combined and labeled a.<br />

Source Strength<br />

28.3 w/cm3<br />

6.84 w/cm3<br />

10.1 w/cm3<br />

41.4 w/cm2<br />

-0.5 w/cm3<br />

22.5 w/cm3<br />

1.8 w/cm2<br />

42 w/cm3<br />

2.3 w/cm3<br />

0.7 w/cm3<br />

~0.1 w/cm’<br />

OS w/cm2<br />

-4 w/cm2<br />

41.4 w/cm2<br />

cs<br />

e<br />

.

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