sometimes incomplete thoughts about music
[ 0 0> 1/1 F [-1 1> 3/2 C [-3 2> 9/8 G [-4 3> 27/16 D [-6 4> 81/64 A [-7 5> 243/128 E [-9 6> 729/512 B [ 1 0> 2/1 F' 0 1 2 3 4 5 6 7 8 | +------------------+ 0 |F | -1 | C | -2 | | -3 | G | -4 | D | -5 | | -6 | A | -7 | E | -8 | | -9 | B | -10| | +------------------+
this moment-of-symmetry structure repeats at the ratio 3/2 instead
of the typical 2/1, but its shape closely mimics the diatonic scale
which repeats at 2/1
[ 0 0> 1/1 B [ 2 -1> 4/3 E [ 5 -3> 32/27 A [ 8 -5> 256/243 D [-1 1> 3/2 B' +-------------------+ | |9 | D |8 | |7 | |6 | A |5 | |4 | |3 | E |2 | |1 | B|0 +-------------------+ |9 8 7 6 5 4 3 2 1 0|
if repeated each occurrence of ~2/1 instead of 3/2, as the diatonic,
we arrive at a collection of irregular scales with two step sizes:
this creates four "modes" with the following intervals
first mode: sLLLsLL "phrygian"
second mode: LLLsLLL "lydian"
third mode: LLsLLLs "ionian"
fourth mode: LsLLLsL "dorian"
[ 0 0> 1/1 B [ 2 -1> 4/3 E [ 5 -3> 32/27 A [ 8 -5> 256/243 D [10 -6> 1024/729 G [13 -8> 8192/6561 C [16 -10> 65536/59049 F [-1 1> 3/2 B' +---------------------+ |F |16 | |15 | |14 | C |13 | |12 | |11 | G |10 | |9 | D |8 | |7 | |6 | A |5 | |4 | |3 | E |2 | |1 | B|0 +---------------------+ |A 9 8 7 6 5 4 3 2 1 0|
(one possible solution)
[ 0 0 0> 1/1 C [-1 1 0> 3/2 G [ 1 -2 1> 10/9 D [ 0 -1 1> 5/3 A [-2 0 1> 5/4 E [-3 1 1> 15/8 B [-1 -2 5> 4/3 F [ 1 0 0> 2/1 C'