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Within each z-plane
an equidistant sampling is defined by the
pixel difference of the screen:
,
according to the
fan projection for the static resolution:
 |
(28) |
and
 |
(29) |
with
.
According to this distances the local Nyquist frequencies for low
pass filtering are given by
resp.
. Then the low pass
filtering for the z-plane
can be done at the point
,
by the functions
![\begin{displaymath}
si\left[ \frac{x-x_{0}}{2\cdot \Delta X}\right] =\frac{\sin ...
...Delta X}\right] }{2\pi \cdot \frac{x-x_{0}}
{2\cdot \Delta X}}
\end{displaymath}](img84.gif) |
(30) |
and
![\begin{displaymath}
si\left[ \frac{y-y_{0}}{2\cdot \Delta Y}\right] =\frac{\sin ...
...Delta Y}\right] }{2\pi \cdot \frac{y-y_{0}}
{2\cdot \Delta Y}}
\end{displaymath}](img85.gif) |
(31) |
Let be
the picture in z-plane
and
resp.
very
small sampling distances. The x-y-filtering then is carried out
for the point
,
by the sum
In case a dynamic resolution is wanted
has
to be substituted by
.
The not equidistant z-Planes
for sampling are
given by equation
. The filtering function for the z-coordinate at the
point
is derived as follows:
![\begin{displaymath}
f\left( z,z_{0}\right) =si\left[ \frac{1-\frac{Z_{screen}}{z}}{2\Delta D}-i_{0}\right]
\mbox{,}
\end{displaymath}](img99.gif) |
(33) |
with
 |
(34) |
Thus the filtering sum for the smaller sampling distances
will be
 |
(35) |
according
.
This completes the description of the three dimensional filtering
operations.
Normally the object image data are given also sampled. Then the
analogue function or re-sampling function is achieved by the known
sum using si-functions.
Next: Conclusion
Up: 3dprojtn
Previous: The dynamic object resolution
2000-08-21