Enlargeability
It has often been stated that there is no limit
to the enlargement factor, since larger prints are
viewed from greater distances. Fine, if there is a
barrier preventing the viewer from approaching
closer than the intended distance, or if the intent
is obvious as in photo murals.
When, for the intended viewing conditions, and
audience, the print gives a hint of UNINTENDED lack of crispmess or
granularity, or loses its maximum visual impact,
the limit has been exceeded.
Although we like to herald the virtues of the
8x11mm Minox, and it is indeed a magnificent
machine, there is an enlargement factor for each
negative at which the characteristics of the print
will reduce the impact of the image. This break-up
is generally signaled by an increase in "fuzziness"
or an increased awareness of "granularity" or lack
of smoothness. The former is the realm of the
camera, the latter, of the film. The perception of
these factors is influenced by the viewer's vision
and experience.
The contact print (enlargement factor = 1)
provides print quality not possible with ANY degree
of enlargement. Enlargement introduces image
degradation, the degree depending on the AMOUNT of enlargement. So, all
other factors being equal, prints made by enlarging
various sized negatives TO THE SAME
DEGREE, should exhibit the same quality
characteristics. It is the AMOUNT of enlargement
that counts!
The Minox camera uses a special cartridge with an
un-perforated strip of film approximately 9.4mm
wide, as shown in the "contact proof" below. The
size of the negative image is 8mm x 11mm. The full
image shown is approximately a 14 x enlargement
with the fishing boat "Kiaora" further enlarged.
The fully enlarged boat is therefore a 120 x
enlargement which would produce a 38" x 52" full
print. This does not imply that I can make a 38" x
52" silver print directly from a
Minox negative (the grain visible in the 16x20 inch
print renders this image unacceptable at that
size), only that the information to produce the
image shown is present in this micro-negative. The
120 x enlargement is 400 pixels wide on your
screen, and represents a 1.17mm wide portion of the
11mm negative. It clearly shows the silver grain
clumps in the background hillside, the worst case,
middle gray haze in a silver print. This image was
made with a Minox IIIs and now discontinued Kodak
High Contrast Copy Film (5069), a wonderful film
with a nice spectral response and very fine grain
... about ASA 6. The camera was hand-held at
probably 1/60th of a second. The image demonstrates
the spectacular design characteristics, quality,
and depth of field of this fine 1950s camera.

The scale below the 120 x enlargement may be
used to appraise the resolving power of the
camera/film combination. I have no data about the
"official" resolving power of either film or
camera.
The 14 x enlargement was made directly from a
negative scan. The 142 x enlargement was made from
a "flatbed" scan of a 16 x 20 inch silver print
made with an Omega B-22XL, Nikkor 28mm lens, and
diffused light source.
When the 16x20 inch print is scanned at 600
samples per inch, what are thought of as "grain
clumps" (actually spaces between grain clumps on
the film), are in the range of 8 pixels across.
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