SlideShare a Scribd company logo
Number Systems
Background: Number Systems is a post to explore number systems in general and for use in the
physical and computational sciences.
Post 8.1
Natural Events in Fibonacci Number Space
Medical Sciences
Posts 1 – 8 have established:
1 𝐷 = (1 +
𝛾∞
𝑓
𝑇𝐷
)
−1
(1 +
𝛾 𝐷
𝑓
𝑇𝐷
)
+1
For natural events, this definition should correlate to the Bernoulli base of natural logarithms:
∫
1
𝑥
𝑑𝑥
𝑒
1
= 1 where lim
𝑛→∞
(1 +
1
𝑛
)
𝑛
= 𝑒
A mathematical description of nature should not be accurate unless the number system complies
with both natural conditions of the number one shown above.
Natural examples:
1
𝑐3
2 =
1
35
2 𝑥 10−16
meter-2 sec+2
h = 6.6260700 E-34 = 6.6260700 x (1∞ − 𝑅 𝐸
𝑓{3}
) x 10-34
meter+2 kg+1 sec-1
𝒘𝒉𝒆𝒓𝒆 𝒂 𝒈 = 𝒈
when g = gEarthSurface <g units: acceleration+1 second+2>
It has been shown
𝐸
𝐸 𝐵
= 𝑚𝑉𝐵
To be rigorous, energy can be defined as a ratio:
𝐸
𝐸 𝐵
= 𝑚𝑉𝐵
Kilogram+1 Meter+3
Define
𝐸 𝑅 = 𝑚3 𝑉3
𝑬 = 𝒎𝑽
Then the dimensionless chemistry of hydrocarbon molecules should be a direct function of mass
and physical size.
𝐶𝐻3
This molecule has unique spatial symmetry:
Post 8.1.1 is intended to clarify the significance of CH3 in Fibonacci energy space.

More Related Content

What's hot

Sets and disjoint sets union123
Sets and disjoint sets union123Sets and disjoint sets union123
Sets and disjoint sets union123
Ankita Goyal
 
DIAPOSITIVA
DIAPOSITIVADIAPOSITIVA
DIAPOSITIVA
Armando
 
Extrapolation
ExtrapolationExtrapolation
Extrapolation
carlos
 
Extrapolation
ExtrapolationExtrapolation
Extrapolation
jonathan
 

What's hot (16)

ELECTROMAGNETICS: Laplace’s and poisson’s equation
ELECTROMAGNETICS: Laplace’s and poisson’s equationELECTROMAGNETICS: Laplace’s and poisson’s equation
ELECTROMAGNETICS: Laplace’s and poisson’s equation
 
Algorithms for Global Positioning
Algorithms for Global PositioningAlgorithms for Global Positioning
Algorithms for Global Positioning
 
Guhui
GuhuiGuhui
Guhui
 
Basics of quantum mechanics
Basics of quantum mechanicsBasics of quantum mechanics
Basics of quantum mechanics
 
Scientific notation
Scientific notationScientific notation
Scientific notation
 
Kgeppt spvm 0_try1
Kgeppt spvm 0_try1Kgeppt spvm 0_try1
Kgeppt spvm 0_try1
 
Computational Physics - modelling the two-dimensional gravitational problem b...
Computational Physics - modelling the two-dimensional gravitational problem b...Computational Physics - modelling the two-dimensional gravitational problem b...
Computational Physics - modelling the two-dimensional gravitational problem b...
 
Sets and disjoint sets union123
Sets and disjoint sets union123Sets and disjoint sets union123
Sets and disjoint sets union123
 
PRML 9.1-9.2: K-means Clustering & Mixtures of Gaussians
PRML 9.1-9.2: K-means Clustering & Mixtures of GaussiansPRML 9.1-9.2: K-means Clustering & Mixtures of Gaussians
PRML 9.1-9.2: K-means Clustering & Mixtures of Gaussians
 
8.5 Bingo
8.5 Bingo8.5 Bingo
8.5 Bingo
 
FINAL POSTER
FINAL POSTERFINAL POSTER
FINAL POSTER
 
Advance heat transfer 2
Advance heat transfer 2Advance heat transfer 2
Advance heat transfer 2
 
DIAPOSITIVA
DIAPOSITIVADIAPOSITIVA
DIAPOSITIVA
 
Extrapolation
ExtrapolationExtrapolation
Extrapolation
 
Extrapolation
ExtrapolationExtrapolation
Extrapolation
 
Extrapolation
ExtrapolationExtrapolation
Extrapolation
 

Similar to Post_Number Systems_8.1

Post_Number Systems_8.3
Post_Number Systems_8.3Post_Number Systems_8.3
Post_Number Systems_8.3
Marc King
 
Post_Number Systems_8.3-3
Post_Number Systems_8.3-3Post_Number Systems_8.3-3
Post_Number Systems_8.3-3
Marc King
 
Post_Number Systems_7
Post_Number Systems_7Post_Number Systems_7
Post_Number Systems_7
Marc King
 
Post_Number Systems_8.1.3
Post_Number Systems_8.1.3Post_Number Systems_8.1.3
Post_Number Systems_8.1.3
Marc King
 
Post_Number Systems_6
Post_Number Systems_6Post_Number Systems_6
Post_Number Systems_6
Marc King
 
Post_Number Systems_8.1.4
Post_Number Systems_8.1.4Post_Number Systems_8.1.4
Post_Number Systems_8.1.4
Marc King
 
Post_Number Systems_5
Post_Number Systems_5Post_Number Systems_5
Post_Number Systems_5
Marc King
 
Post_Number Systems_4
Post_Number Systems_4Post_Number Systems_4
Post_Number Systems_4
Marc King
 
Post_Number Systems_8
Post_Number Systems_8Post_Number Systems_8
Post_Number Systems_8
Marc King
 
Post_Number Systems_3
Post_Number Systems_3Post_Number Systems_3
Post_Number Systems_3
Marc King
 
Post_Number Systems_8.1.6
Post_Number Systems_8.1.6Post_Number Systems_8.1.6
Post_Number Systems_8.1.6
Marc King
 
Post_Number Systems_8.1.11
Post_Number Systems_8.1.11Post_Number Systems_8.1.11
Post_Number Systems_8.1.11
Marc King
 
Post_Number Systems_2
Post_Number Systems_2Post_Number Systems_2
Post_Number Systems_2
Marc King
 
damping_constant_spring
damping_constant_springdamping_constant_spring
damping_constant_spring
N'Vida Yotcho
 

Similar to Post_Number Systems_8.1 (20)

Post_Number Systems_8.3
Post_Number Systems_8.3Post_Number Systems_8.3
Post_Number Systems_8.3
 
Post_Number Systems_8.3-3
Post_Number Systems_8.3-3Post_Number Systems_8.3-3
Post_Number Systems_8.3-3
 
Post_Number Systems_7
Post_Number Systems_7Post_Number Systems_7
Post_Number Systems_7
 
Post_Number Systems_8.1.3
Post_Number Systems_8.1.3Post_Number Systems_8.1.3
Post_Number Systems_8.1.3
 
Post_Number Systems_6
Post_Number Systems_6Post_Number Systems_6
Post_Number Systems_6
 
Post_Number Systems_8.1.4
Post_Number Systems_8.1.4Post_Number Systems_8.1.4
Post_Number Systems_8.1.4
 
Post_Number Systems_5
Post_Number Systems_5Post_Number Systems_5
Post_Number Systems_5
 
Post_Number Systems_4
Post_Number Systems_4Post_Number Systems_4
Post_Number Systems_4
 
Post_Number Systems_8
Post_Number Systems_8Post_Number Systems_8
Post_Number Systems_8
 
Post_Number Systems_3
Post_Number Systems_3Post_Number Systems_3
Post_Number Systems_3
 
Post_Number Systems_8.1.6
Post_Number Systems_8.1.6Post_Number Systems_8.1.6
Post_Number Systems_8.1.6
 
Post_Number Systems_8.1.11
Post_Number Systems_8.1.11Post_Number Systems_8.1.11
Post_Number Systems_8.1.11
 
Post_Number Systems_2
Post_Number Systems_2Post_Number Systems_2
Post_Number Systems_2
 
damping_constant_spring
damping_constant_springdamping_constant_spring
damping_constant_spring
 
05_AJMS_332_21.pdf
05_AJMS_332_21.pdf05_AJMS_332_21.pdf
05_AJMS_332_21.pdf
 
ADAPTIVE STABILIZATION AND SYNCHRONIZATION OF LÜ-LIKE ATTRACTOR
ADAPTIVE STABILIZATION AND SYNCHRONIZATION OF LÜ-LIKE ATTRACTORADAPTIVE STABILIZATION AND SYNCHRONIZATION OF LÜ-LIKE ATTRACTOR
ADAPTIVE STABILIZATION AND SYNCHRONIZATION OF LÜ-LIKE ATTRACTOR
 
Trialdraftsppformat dimen test1
Trialdraftsppformat dimen   test1Trialdraftsppformat dimen   test1
Trialdraftsppformat dimen test1
 
Presentation esa udrescu
Presentation esa udrescuPresentation esa udrescu
Presentation esa udrescu
 
2 classical field theories
2 classical field theories2 classical field theories
2 classical field theories
 
ANTI-SYNCHRONIZATION OF HYPERCHAOTIC PANG AND HYPERCHAOTIC WANG-CHEN SYSTEMS ...
ANTI-SYNCHRONIZATION OF HYPERCHAOTIC PANG AND HYPERCHAOTIC WANG-CHEN SYSTEMS ...ANTI-SYNCHRONIZATION OF HYPERCHAOTIC PANG AND HYPERCHAOTIC WANG-CHEN SYSTEMS ...
ANTI-SYNCHRONIZATION OF HYPERCHAOTIC PANG AND HYPERCHAOTIC WANG-CHEN SYSTEMS ...
 

More from Marc King

Post_Number Systems_8.3.1
Post_Number Systems_8.3.1Post_Number Systems_8.3.1
Post_Number Systems_8.3.1
Marc King
 
Post_Number Systems_8.1.12reduced
Post_Number Systems_8.1.12reducedPost_Number Systems_8.1.12reduced
Post_Number Systems_8.1.12reduced
Marc King
 
Satellite Infrared
Satellite InfraredSatellite Infrared
Satellite Infrared
Marc King
 
Post_Number Systems_8.1.12
Post_Number Systems_8.1.12Post_Number Systems_8.1.12
Post_Number Systems_8.1.12
Marc King
 
Post_Number Systems_8.1.7
Post_Number Systems_8.1.7Post_Number Systems_8.1.7
Post_Number Systems_8.1.7
Marc King
 
Post_Number Systems_8.1.5
Post_Number Systems_8.1.5Post_Number Systems_8.1.5
Post_Number Systems_8.1.5
Marc King
 
Post_Number Systems_1
Post_Number Systems_1Post_Number Systems_1
Post_Number Systems_1
Marc King
 
Speed of Light
Speed of LightSpeed of Light
Speed of Light
Marc King
 
Stereoisomer
StereoisomerStereoisomer
Stereoisomer
Marc King
 
Fibonacci_Hubble
Fibonacci_HubbleFibonacci_Hubble
Fibonacci_Hubble
Marc King
 
Time_Exercise
Time_ExerciseTime_Exercise
Time_Exercise
Marc King
 

More from Marc King (13)

Post_Number Systems_8.3.1
Post_Number Systems_8.3.1Post_Number Systems_8.3.1
Post_Number Systems_8.3.1
 
Post_Number Systems_8.1.12reduced
Post_Number Systems_8.1.12reducedPost_Number Systems_8.1.12reduced
Post_Number Systems_8.1.12reduced
 
Satellite Infrared
Satellite InfraredSatellite Infrared
Satellite Infrared
 
Post_Number Systems_8.1.12
Post_Number Systems_8.1.12Post_Number Systems_8.1.12
Post_Number Systems_8.1.12
 
Post_Number Systems_8.1.7
Post_Number Systems_8.1.7Post_Number Systems_8.1.7
Post_Number Systems_8.1.7
 
Post_Number Systems_8.1.5
Post_Number Systems_8.1.5Post_Number Systems_8.1.5
Post_Number Systems_8.1.5
 
Post_Number Systems_1
Post_Number Systems_1Post_Number Systems_1
Post_Number Systems_1
 
Speed of Light
Speed of LightSpeed of Light
Speed of Light
 
Chirp_Mass
Chirp_MassChirp_Mass
Chirp_Mass
 
Stonehenge
StonehengeStonehenge
Stonehenge
 
Stereoisomer
StereoisomerStereoisomer
Stereoisomer
 
Fibonacci_Hubble
Fibonacci_HubbleFibonacci_Hubble
Fibonacci_Hubble
 
Time_Exercise
Time_ExerciseTime_Exercise
Time_Exercise
 

Post_Number Systems_8.1

  • 1. Number Systems Background: Number Systems is a post to explore number systems in general and for use in the physical and computational sciences. Post 8.1 Natural Events in Fibonacci Number Space Medical Sciences Posts 1 – 8 have established: 1 𝐷 = (1 + 𝛾∞ 𝑓 𝑇𝐷 ) −1 (1 + 𝛾 𝐷 𝑓 𝑇𝐷 ) +1 For natural events, this definition should correlate to the Bernoulli base of natural logarithms: ∫ 1 𝑥 𝑑𝑥 𝑒 1 = 1 where lim 𝑛→∞ (1 + 1 𝑛 ) 𝑛 = 𝑒 A mathematical description of nature should not be accurate unless the number system complies with both natural conditions of the number one shown above. Natural examples: 1 𝑐3 2 = 1 35 2 𝑥 10−16 meter-2 sec+2 h = 6.6260700 E-34 = 6.6260700 x (1∞ − 𝑅 𝐸 𝑓{3} ) x 10-34 meter+2 kg+1 sec-1 𝒘𝒉𝒆𝒓𝒆 𝒂 𝒈 = 𝒈 when g = gEarthSurface <g units: acceleration+1 second+2> It has been shown 𝐸 𝐸 𝐵 = 𝑚𝑉𝐵 To be rigorous, energy can be defined as a ratio: 𝐸 𝐸 𝐵 = 𝑚𝑉𝐵 Kilogram+1 Meter+3
  • 2. Define 𝐸 𝑅 = 𝑚3 𝑉3 𝑬 = 𝒎𝑽 Then the dimensionless chemistry of hydrocarbon molecules should be a direct function of mass and physical size. 𝐶𝐻3 This molecule has unique spatial symmetry: Post 8.1.1 is intended to clarify the significance of CH3 in Fibonacci energy space.