Copper is FCC with r
=0.157nm. We can calculated ao
and \![]()
q = 0.5o = 0.0087 rad
dislocation spacing in the symmetrical tilt boundary, is D = b/q
![]()
We have e=ln(1+e), e=ln (le/lo)
and


Since
, We can write
or ![]()
Substituting this value of
in the Hall-Petch
relation ![]()
We have
or ![]()
0.1mm =100mm and the thickness of the specimen is 0.1mm.The grain size is the same dimension as the thickness. So, the 100mm would be not considered truly polycrystalline material because only a few grain boundaries could be find in the section of the specimen. For the Dum’s foils, the “truly polycrystalline” increase as grain size decrease.

, this equation is a
lineal equation:
The slope of the plot
of ln sy vs. ln
D would yield the value of n, which would be the exponent for D, n=-0.45.
We have n=2
(a)The grain size should be ![]()
and 
(b) The grain diameter is ![]()
(a) The magnification of the picture in the textbook is
, Using the lineal
intercept method, we draw two test lines, each 70mm. The number of intercepts
on the test line is 32. The mean lineal intercept is
and
![]()
(b) Using the
ASTM method, the number of the grains in 1 in2 at 115X is 27. Then
the number of the grains in 1in2 at 100x is:
and ![]()
![]()
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