lirik lagu james kirk bogucheski – landing vectors 2
if there is an exterior source of momentum such as the wind for an example then it’s noted with ζ, an air tunnel variable. it’s extremely difficult to measure in real time the actual force of the wind, so we divide it in 5 intensities for natural wind, 1 for a weak wind, 2 for a slightly more intense, so it goes all the way to 5, a strong wind. up to 10 if they are forces of nature such as hurricanes and tornadoes
in the quantum states, ζ is a wave propulsion which moves the tiny particles. that is noted as μζ, a microzeta, the lower wavelengths are actually the strongest ones for particle movement so from 1 to 10, 1 would be strongest and 10 would be weakest
ex: 1.2 x 10^-15 n = 16φ + 55θ + 5μζ
the same particle before also affected by the medium intensity wave propulsion
ex2:: 220 n = -33φ + 20θ + 4ζ
a medium sized object whose landing vector has a counter clockwise, upwards circ-mference trajectory affected by a hard wind
they aren’t exact equations per se, algebraically, they are references of results in a scalar reference point in the grid. this method allows more predictability and accuracy. the final point of the notation is the arriving location in the x y and z plane inside of the brackets
ex: 220 n = -33φ + 20θ + 4ζ [2, 0, 3]
if the goal was to reach the upper corner of the goal in a soccer field for an example, if the middle of the goal was [0,0,0] the upper right goal corner would be
[6, 7, 36]. in feet, z would be the depth from the penalty spot
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