Errata and addenda to: The role of the Boltzmann transport equation in radiation damage calculations

Prooress in Nuclear Energy, 1979, Vol. 4, p,i.

Pergamon Press Ltd. Printed in Great Britain

E R R A T A A N D A D D E N D A TO:

THE ROLE OF THE BOLTZMANN RADIATION DAMAGE

TRANSPORT EQUATION CALCULATIONS

IN

by M. M. R. WILLIAMS

Prog. Nucl. Energy, 3, 1 (1979)

The following corrections and additions should be noted: Page 8:

Equation (35) has an = sign missing after Wo(E, r, t).

Page 12:

Following equation (61), should read "where (Winterbon et al., 1970)". It is also worth noting that ~.,,(E) as defined by equation (65) is related to the conventional stopping cross section SN(E) by

Page 37:

Immediately preceding Section 9.2 add "But see modifications introduced by Winterbon and Sanders, Rad. Effects 39, 39 (1979)".

Page 38:

Equation (306) should read

O(½(l + 1)k + ½). Page 40:

Equation (320). Note that some authors define the spatial moments without n!

Page 46:

Equations (409), (411) and (412). Delete n!

1-~t &(E) = - F. ~ . ( E ) .

Equation (410). Delete hi, and change Lm to L,.

2

Page 13:

In equation (67) ,(aE) should be dE).

Page 16:

Equation (101) should be

Page 50:

Equation (438). The expression for the transport mean free path for general m is E2m

,~,(e) = 2NC. (1 - m) (1 - ~)m Page 19:

Equation (125). n, should read nj.

Page 22:

Equation (170). (x) should readf(x).

Page 24:

Equation (181). K should read K.

Page 29:

The figure is missing and should be

where

c . = ~ ~.a~(l - ~ ) ' E ~ ' . Page 52:

Equation (445). Before the first curly bracket insert the factor

Z(E, 0(E/E')) ~.(E', O(E/E'))" E

i

Section 14: A more detailed treatment of this problem is given in a forthcoming paper by I. Pazsit and M. M. R. Williams.