Friday, 13 April 2012

ADONGO 'S LEAST WHOLE NORMAL PHYSICS

ADONGO’S LEAST WHOLE NORMAL FORAMLISM
HISTORICAL BACKGROUND
The normal curve was devised around 1720 by the mathematician Abraham De Moivre in other to solve problems connected with games of chance. Around 1870 the Belgian mathematician Adolph Quetelled had the idea of using the curve as an ideal histogram, to which histogram for data could be compared.
Around 2009, I had created a mathematical function from the normal approximation equation which could be used in modeling problems in medical science, insurance, economics, material science and biological science.
I also realized that more development is needed to solve the scientific situations that I was confronting in my time. In view of this I was able to restructure the formalism of the existing concepts of physics to a new branch of formalism called Least Whole Normal Formalism which we are to discuss next.



ADONGO’S LWN FORMALISM
Definition:
·         Radical quantity: the radical quantity is any quantity that has main influence in the quantitative product. Let us consider the quantitative equation for velocity which is given as
V = S * (1/t): the radical quantity is the time t.

·         Subjective quantity: the subjective quantity is any quantity that is determined or has main relationship with the radical quantity. Let us also consider the quantitative equation for velocity which is given as V = S * (1/t):  the subjective quantity is the distance S.

·         Non-subjective quantity: the non-subjective quantity is a chosen quantity in the quantitative product which cannot be related by the radical quantity. The quantitative equation for force which is given as 
      F = m*v*t –1:  the non-subjective quantity could be v if m is chosen as subjective quantity or it could be m if v is chosen as subjective quantity.


TWO QUANTITATIVE PRODUCT
Let us consider Q ( i , j ) = (I j * τ )*µi  where I j  is denoted as a unit non-subjective quantity and
τ the radical and µi  is the subjective quantity. The non-subjective unit quantity  I j  is always equal to one (i.e. I j = 1)


The quantitative equation Q ( i , j ) = (I j * τ )*µi    has a distribution  
 Tj  ̴  N( τ , 0)    
 Tj  ̴  n (µi , Si2 )    }    .................. ( 1)  for direct relation and



 Tj  ̴  N( τ -1 , 0)    
 Tj  ̴  n (µi , Si2 )    }    .................. ( 2)  for inverse relation.

Where j is one ( j = 1) and i  represents any quantity.
If the normal random quantity T j   is total non-subjective unit quantity and T i  is total subjective quantity, then the least whole normal function for the above distribution is
ℓ (τ) = α * τ - √ (τ) – β  (i.e. when directly related)
  (τ -1) = α * τ -1 - √ (τ -1) – β  (i.e. when inversely related)
Where the constant α  and β are denoted as quantile coefficient of  τ  or  τ -1 and quantile constant respectively are calculated as;
α = µi  / {ϕ -1(γ%)  (√Si2)}
β = Ti  /  {ϕ -1(γ%)  (√Si2)}



THE LEAST WHOLE NORMAL QUANTITY



The quantity which represents least whole radical quantity is always approximately equal to zero. The least 
 whole radical quantity is calculated as;

√ ( τ0 ) = [1+√ (1 + 4αβ)] / 2α  for direct relation and
√ ( τ0-1 ) = [1+√ (1 + 4αβ)] / 2α  for inverse relation




THE TOTAL SUBJECTIVE QUANTITY
The quantity Ti   which represents total subjective quantity is calculated as;
Ti = µi * τ0ϕ -1 (γ %) √ (Si2 * τ0 )  for direct relation and
Ti = µi * τ0-1 ϕ -1 (γ %) √ (Si2 * τ0 ) for inverse relation.

MEAN SUBJECTIVE QUANTITY
The quantity µi which represents the mean subjective quantity is calculated as;

µi2 = [ (1 / τ02)] [Ti2 + ϕ -1( γ%) S2  * τ0]  for direct relation and
µi2 = [ (1 / τ02)] [Ti2 + ϕ -1( γ%) S2  * τ0-1 ]  for inverse relation.

APPLYING THE FORMALISM
DOING WORK:
Doing works are way of transferring energies using forces. The amount of energies transferred. The amount of works done equal to sizes of the forces times the distance move.
Expected work= mean force *mean distance
i.e E (w) = µf * τ

Applying the theory of two quantitative products, we have the distribution
T1 ~ N ( τ,0)
Tf  ~ n (µf , Sf 2)    }    .................. ( 1)


Where µf  denoted as mean force and Sf 2   is the variance of the forces.
If the normal random quantity T1  which is total number of units quantity I which mean is always equal to one and Tf  which is denoted as total number of force, then it least whole normal function is calculated as;
(τ0) = α * τ0  – ( √τ0 ) – β
 (i.e when directly related)  where α and β  are calculated as;
α = µf  -1 / {ϕ-1  (γ%)  (√Si2)}
β = Tf  /  -1(γ%)  (√Si2)}

THE LEAST WHOLE DISTANCE (RADICAL QUANTITY)
The quantity Tf which represents total subjective distance is always approximately equal to zero. The least whole distance is calculated as;

τ0 = [1 + √ (1 + 4αβ) ] / 2α .........................( 0 )



TOTAL FORCES (SUBJECTIVE QUANTITY)
The quantity Tf  which represents total subjective quantity or total forces is calculated as;

Tf = µf  * τ – ϕ -1 [γ%] [√(Si2*τ) ].........................(□)


MEAN FORCE (MEAN SUBJECTIVE QUANTITY)
The quantity µf  which represent mean force is calculated as;

µf 2  = [ (1 / τ02)] [Tf 2 + ϕ -1( γ%) S 2  * τ0-1 ] .............(*)






EXAMPLE


Horses pull cars with constant horizontal forces of mean 136N and standard deviation 27N per distance. Calculate the
         i.            Total forces at distance 19500m
       ii.            Average forces at distance 19500m
(Take γ = 95% )

SOLUTION
i)                    Applying equation (□), we have

T f = µ f * τ0ϕ -1 [γ%][√(S f 2 * τ0) ]
T f  = 136 * 19500 − ϕ -1 [95%]  [√(729 ×19500)]
Tf = 2,652,000 – 1.645 × √(14,215,500)
Tf  = 2,645,797.783N



Hence, the total force is 2,645,797.783N



THREE QUANTITATIVE PRODUCT
Let us consider Q (i , j) = (Äj *τ ) * µi   where Äj  is denoted as non-subjective quantity µi  is denoted as subjective quantity and τ is the radical quantity.
If the non-subjective quantity Äj    is not equal to one, but represents any quantitative value. Then we have the distribution of the quantitative equation Q (i, j)  which is given as;
Tj ~ N (Äj* τ , σ 2 * τ )
Tj ~ n ( µi , Si2 )                  }    .................. ( 1)   for direct relation and


Tj ~ N (Äj* τ -1  , σ 2 * τ -1 )
Tj ~ n ( µi , Si2 )                       }    .................. ( 2)  for inverse relation



If the normal random quantity Tj  is total non-subjective quantities and Ti  is total subjective quantity, then the least whole normal function is given as
(τ) = α * τ  – ( √τ ) – β  (i.e when directly related)
(τ -1) = α * τ -1  – ( √τ -1 ) – β  (i.e when inversely related)

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