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2.1 Some theory What
is spatial frequency? Every one is familiar with the idea of Fourier
analysis of a time domain signal; that is to say, taking a continuous
time signal such as a speech pattern in which pressure is a function
of
time, and decomposing it into the sum of numerous sinusoidal harmonics
each of which has its own frequency, amplitude and phase. This is
a very useful technique not only because it allows us to consider signals
in frequency
space which is normally more intuitive but also because, for linear
systems at least, we can work out the effect of complete systems by considering
their influence on each of the input frequency components separately
and
adding them all up at the end. The same concept can be applied to
two dimensional images where the luminance is a function not only of
time but also of position
in space. Starting with the case of a static image such as a photograph
we can decompose our picture into the sum of spatial harmonics each
of which has a spatial frequency, amplitude and phase. Unlike temporal
frequency
which can be understood as individual notes played on a piano, spatial
frequency is less intuitive but can be useful to think about it as
a measure of feature size. Things with big dimensions contain low spatial
frequencies
while small things or those with sharp edges have a large high spatial
frequency content. Obviously the apparent size of something depends
on the position of the observer relative to it so spatial frequencies
are
measured as the angle subtended by one cycle of the waveform at the
observer in units of cycles per degree (cpd). For example, the fence
posts (spacing
2m) at the bottom of the garden (distance 30m) have a fundamental
spatial frequency of 0.3cpd. There are of course many higher frequencies
present
as well which are needed to define the exact shape of the posts,
the surface texture etc. It is convenient to remember that with a 57cm
viewing distance
one cycle of a 1cpd waveform measures 1cm.
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