9.2 Example: Inversion with Retrograde
In music, retrogade means playing backwards, beginning with the last note and ending with the first note of the original composition. However, the time allotted by parameters such as »
«, »
«, etc. can’t be inverted so intuitively; the example of a recording played backwards is not musical retrograde.
We will work with the form
Simple
. Here we can see a similarity with the inversion of
and the symmetry of retrograde:
, where
is the total »size« of the piece, measured in
. If, for example, we have a measure in common time (divided in four),
, and if
(a note that begins on
in its retrograde the same note will begin on
.
But what will happen when we have 2 notes with
and
, separated by
? That is,
1 has, for example,
and
begins at
. If we apply the symmetry
, we will have

that, in our example, is

. Then the retrograde of

begins exactly
Onsetdistance 
before the retrograde of

. However, if the duration of

2 is longer than
Onsetdistance (for example, if it is 1.5) then
Offset
will not be finished when

begins.
Therefore, we include the parameter
when we define a retrograde symmetry, and we work in the two dimensional space
. If we take two events
, first we must apply
to the parameter
of both notes, i.e.,
and
. Consider the duration of
. Then we have
. However, this transformation is intermediate, because we want to avoid overlaps. That’s why we take into account the parameter
to obtain
and
, that is
and
. This way, the overlap from
to
is completely avoided, because the retrograde of
ends at
and
1 begins at
. We define retrograde as
, that is,
![[ ] (s,0) - 1 -1 Ks = e . 0 1 .](../graphic/Co2147x.gif)
It is clear that in this example we are not considering the parameter

which is also subject to retrograde. Finally, the inversion with retrograde, as used in serial dodecafonic music, involves three parameters, that is,

,

, and

. Then we have:

and if the original

,

, and

values are

, then: