ORNL-2106 - the Molten Salt Energy Technologies Web Site
ORNL-2106 - the Molten Salt Energy Technologies Web Site
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 />
.