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)
ℓ (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 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 * τ0 – ϕ -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;
ℓ (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
/ {ϕ -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 * τ0 − ϕ -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
ℓ (τ) = α * τ
– ( √τ ) – β (i.e when directly related)
ℓ (τ -1) = α * τ -1 – ( √τ
-1 ) – β (i.e when
inversely related)
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