August 25th, update information (2).
- kyonissho
- Aug 25
- 1 min read
Article:
No.3188. Planck Constant in Trigonometric Functions.
Update:
from
cos^-1(ħ) = π/2 | ħ = reduced Planck constant Dirac's constant
cos(ħ) = 1 | cos^-1(ħ) : cos(ħ) = 90° : 0°
sin^-1(ħ) = 1.054571726x10^(-34) | Dirac's constant itself,
sin(ħ) = 1.054571726x10^(-34) | sin^-1(ħ) : sin(ħ) = 1 : 1
tan^-1(ħ) = 1.054571726x10^(-34) | tan^1(ħ), tan(ħ), sin^-1(ħ)
tan(ħ) = 1.054571726x10^(-34) | and sin(ħ) = the constant.
Very impressive, powerful and practicable constant.
to
Misjudgement:
(cos^-1(ħ) = π/2 | ħ = reduced Planck constant Dirac's constant
cos(ħ) = 1 | cos^-1(ħ) : cos(ħ) = 90° : 0°
sin^-1(ħ) = 1.054571726x10^(-34) | Dirac's constant itself,
sin(ħ) = 1.054571726x10^(-34) | sin^-1(ħ) : sin(ħ) = 1 : 1
tan^-1(ħ) = 1.054571726x10^(-34) | tan^1(ħ), tan(ħ), sin^-1(ħ)
tan(ħ) = 1.054571726x10^(-34) | and sin(ħ) = the constant.
Very impressive, powerful and practicable constant.)
Correct judgement:
Above calculation was derived because of ħ ≒ 0 by my calculator. Although a enough small number, but it is great proportion constant, may make coordinates far from trigonometric function's center.
Another assumption:
R^1 of linearly independent existence isn't everywhere according to ħ, because there is -gravity.
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