Rate of Convergence of the Sine Imprecise Functions
Автор: Kangujam Priyokumar Singh, Sahalad Borgoyary
Журнал: International Journal of Intelligent Systems and Applications(IJISA) @ijisa
Статья в выпуске: 10 vol.8, 2016 года.
Бесплатный доступ
We convert polynomial function of degree nth into imprecise form to obtain an important point called conversion point. For some particular region, we collect the finite number of data points to obtain the most economical function called imprecise function. Conversion point of the functions is shown with the help of MUPAD graph. Further we study the area of the imprecise function occurred by the multiplication of sine function to know how much variation of the imprecise functions are obtained for the respective intervals. For different imprecise polynomial we study level of the rate of convergence.
Rate of Convergence, Imprecise Function, Conversion Point, Imprecise Number, Diversion Point, Imprecise Polynomials
Короткий адрес: https://sciup.org/15010864
IDR: 15010864
Текст научной статьи Rate of Convergence of the Sine Imprecise Functions
Published Online October 2016 in MECS
Imprecise function which is obtained by the multiplication of some other functions is called multiplication factor. Thus any continuous function is multiplied by sine or cosine function to obtain imprecise polynomials. For a certain region we will collect finite number of data collection of points. And with the help of these points we will identify most valuable function or the controllable function called imprecise function for these points.
Area bounded by the imprecise function help us to know how the variation of the effect of impreciseness of an object is occurred for the different intervals. For this reason we define formula of the area of an imprecise number in the general summation form. Thus the area formulae of the different angles of sine functions are also play an important role in this article.
The remaining sections of the article are divided into the following ways:
Section II is contain about the preliminary definition of imprecise function, section III is contain definition of new function called imprecise function, Section IV is contain conversion point obtain by the help of multiplication of the sine and cosine function, Section V is contain rate of convergence of different imprecise function so that we can study variation of the effect of imprecise for the respective intervals. Finally section VI is the conclusion and the summary of this article.
-
II. P reliminaries
Before starting this article it is necessary to recall the definition of imprecise number, partial presence, membership value etc. over the real line which are discussed in the article [9],[10],[12] [13], [15] and [16].
-
A. Imprecise Number:
Imprecise number is a closed interval N=[α,β,γ] which is divided into closed sub-intervals with the partial presence of element β in both the intervals.
-
B. Partial presence:
Partial presence of an element in an imprecise real number [a, p, у] is described by the present level indicator function p(x) which is counted from the reference function r(x) such that present level indicator for any x, a < x < у , is (p(x) — r(x)) , where 0 < r(x) < p (x) < 1
-
C. Membership value:
If an imprecise number N = [а,Р,у] is associated with a presence level indicator function ^(x) such that,
(цi (x), when a < < P P p2 (x), when X X x < у
0, h
With a constant reference function 0 in the entire real line. Where ( ) is continuous and non-decreasing in the interval [ , ] , and ( ) is a continuous and nonincreasing in the interval [ , ] with цi (a) = ц 2 (У) = 0, then ( ( ) — ( )) is called membership value of the indicator function ( )
-
D. Normal Imprecise Number:
A normal imprecise number N = [a, p, у] is associated with a presence level indicator function ( ) such that,
(цi (x), hhen a < x < P ц2 (x), when P < x < у
0, h
With a constant reference function 0 in the entire real line. Where ц(x1) is continuous and non-decreasing in the interval [ , ] and ( ) is a continuous and nonincreasing in the interval [ , ] with ц i (a) = ц ((у) = 0
ц i (Р) = ц (СР ) = 1
Here, the imprecise number is characterized by {х, ц ^ (х), 0 : х е R } , R being the real line.
For any real line, 0 < цi (x) < ц( (x) < 1 normal and subnormal imprecise number will be characterized in common, {x^ 1(х),ц2(%): x е R }, where цi(x) is called membership function measured from the reference function ( ) and ( ( ) — ( )) is called the membership value of the indicator function.
Here, the number is normal imprecise number when membership value of indicator function цм (x) is equal to 1 otherwise subnormal if not equal to 1. Moreover if the membership value of цм (x) is equal to 1 then the set is universal set and the null or empty set if the value of pN (x) is equal to 0.
-
III. I mprecise F unctions
Imprecise number is an interval definable number where the interval is an area bounded by some section of a function formed by the impreciseness of objects. So, the function which contains such type of imprecise intervals within in it is known imprecise function. At present this phenomenon is occurring available in the field of science and technology. For example possible of impreciseness of electromagnetic wave frequency in between the server and the receiver is an imprecise function. Where, the finite numbers of imprecise numbers are occurred in between the locations. So, the bigger function to connect these two locations is an imprecise function. From this point of view it can be introduced some conditions for the imprecise functions as follows:
-
(i) Function must be continuous in some region
-
(ii) Function should be oscillation in nature
-
(iii) Function must have finite number of maximum and minimum values within the interval.
-
(iv) Function should be semi-periodic/periodic in nature.
Generally, formation of effect of the impreciseness in the form of sine and cosine functions for a certain region is interval definable number. Thus, effect of any function which is defined for any intervals can be converted into imprecise function with the help of multiplication factors of sine and cosine functions.
-
A. Conversion point-
- It is a point from where non- imprecise function starts to convert into imprecise function. If we can identify this point, then we will get easily their applications. As for example loudness of sound causes brain and heart diseases because of non-imprecise function of character produces from a sound device. So, it may be possible to control by converting them into human ear audible level by the help of volume regulatory. Further in present most of the times ultraviolet ray reaches in the ground is non-imprecise function form due to lake of the friction of Ozone layer caused by the environmental pollutions. This phenomenon is creating problems in the life of living being causing skin disease etc. Thus if we can invent a new device having Ozone layer character, then it will save us from these type of problems. This may be possible due to the multiplication factor which can convert any function into imprecise function form.
Normally these phenomena are already applied in many of the experiment like volume regulator or the regulators used in the different fields for their practical purposes.
-
IV. C onversion of P olynomials into I mprecise F unctions
There are many polynomials, which are raised to infinite direction without coming back to the ground level. So it is called uncontrolled function. But this type of function can also be transformed into oscillation form to meet the ground level repeatedly from a certain point. This point is known as conversion point. This phenomenon is occurred by the multiplication of a function which can convert into imprecise function form. This multipliable function is called multiplication factors.
Thus the imprecise function obtained by the multiplication of sine function is known as sine imprecise function and the imprecise function obtained by the multiplication of cosine is called cosine imprecise function.
For this purpose, let us consider
Pl (Х1 , У1 ), Р2 (Х2 , У2), Рз (хз , Уз)……………․․ ……………․Рп (%п+1, Уп+1), be the nth collection of points, which are above and below the given polynomial of degree n,
-
У = + с±х + с2х2 + с3х3 ……․․+ спх (1)
To convert it into imprecise form, let us multiply this polynomial by a sine function.
Thus,
У =(Со + сгх + с2х2 + с3х3 + ………․․+ спх ) sin( 1х ); leZ (2)
will be a sine imprecise polynomial of degree n.
To obtain standard imprecise polynomial averagely passing closed to these points, we follow the rules of matrix multiplication as follows:
As, the point Pl , р2 ,………………․ Рп are satisfied the given polynomial. By the law of roots, we will get nth set of simultaneous linear equations having arbitrary constants С0, Ci ,С 2 ,………………․․
․․……,cn as follows:
У1 =(со + С1Х1 + c2Xi2 + Сзх13 ………………………+ Си ^-1 )sin( 1хт )
У2 =(со + С1Х2 + С2Х2 + Сзх23 ………………………+ Си ^2 )sin( 1х2 )
Уз =(со + С1хз + с2х32 + Сзхз3 ………………………+ Си Х3 )sin( 1х3 )
Уп=(со + Ci%n + С2ХП2 + Сзхп3 ………………………+спхп ) sin(^)
Which can be written in the matrix form as гУ.]
⎢⎡⎥
⎣⎦
[ ( 1хА ) хг sin( lxt ) sin ( lx2 ) х2 sin( lx2 )
sin ( lxn ) Xn sin( lxn )
x-^sin ( lxt ) x2nsin ( lx2 )
xnnsin ( lxn )
]
ГСО] ⎢⎡ 2 ⎥⎤
⎣
≅ = ( say )
Where,
A = ⎢ 1
2 3 4 /у П
1 Ai Ai Ai …………․ Ai I x2 X22 x23 x24 ………… ^2” ⎥
…………

To obtained the solutions of arbitrary constants, we write,
AT (AX)=ATB(6)
Where AT is the transpose matrix of A.
Values of ATA = ( aH )
( )×( ti+ 1.)
and ATB = (bt)(n+1)×1
such that aij =∑k=l[xk’"2{sin(lxk )}2 ]
and bi =∑ k=l [ Укхк sin( lxk )],1 ≤ i ≤( n +1) (10)
n= order of the polynomial, m=no of collection of points, Xt and 7t ordinates and the abscissa of the given points.
Solution of the arbitrary constants
Cq , Cl , c2,………………………,cn can be obtained with the help of Gauss-elimination method of general form
Rt → Ri - × at, ;
a ( i-l )( i-l )
(2≤ i ≤n+1),(1≤ j ≤n)
Steps of transformation will be done as follows:
(2≤ i ≤n+1wℎen j =1)
(3 ≤ i ≤и+1wℎen j =2)
(и+1≤ i ≤и+1wℎen j = ) (11)
These operations help us to get upper triangular matrix. By backward substitution we will get the solution of the mentioned arbitrary constants.
Thus any polynomial can be obtained into controllable form by multiplication of sine and cosine function.
For the different value of I we will get different value of the constants. Because of different value of the constants we will have different imprecise functions. This characteristic of function is very important in the field of applications.
A. Sine imprecise Polynomial of degree one-
Example-1 ( Sine imprecise function of polynomial of degree one with angle, X):
Let У= + c4x be a polynomial of degree one. So, in particular
У =(Со + с4х ) sin( X ), for I = 1 (12)
is a sine imprecise polynomial of degree one.
Let us consider (1,3.2), (2,4),(3,-2.5), (4,
-
4.5) ,(5,6),(6,-7.5),(7,5.5) be the points in the data collection which are above and below the x-axis.
So, %! =1,Х2 =2,х3 =3,х4 = 4, х5 =5,х6 =6,X?=7
У1 = 3․2, Уг =4,Уз = -2․5,
У4 = -4․5, Уз =6,Уб = -7․5, У? = 5․5
By the law of roots the given imprecise function satisfies the given collection of points to have linear simultaneous equation to form a matrix as follows:
From (4), (5), (6) …………․․․ (10), we have
АХ =
=>( АТА ) X =
Where, АТА = ( ан ) , (п+1)×(п+1)
ЛЧ = ( ац )( п+1)× 1 ,х=* +
Such that Оц =∑ ™=1хк 7 {sin( Хк )}2
and Ь[ =∑ ™=1УкХк sin( Хк ), 1 ≤ i ≤( п +1)
Here, m=no. of points=7, n= degree of the polynomial=1
АТА = ( ац ) 2 х 2 and АТВ = ( bi )2 ×1
Where Clij =∑ k=lxk 7 {sin( Хк )}2
and bi =∑ к=1Укхк sin( хк ), 1 ≤ i ≤2
=∑ {sin( )} 2 ац =∑хк {sin(хк )} к=1
= ( Х1 )+ sin2 ( х2 )+ sin2 ( х3 )+ sin2 ( х4 )
+ sin2 ( ^5)+ sin2 ( х6 )+ sin2 ( х7 )
= 0․04250,
= =∑ {sin( )} ,
= =∑ {sin( )} к=1
= ( хг )+ x2sin2 ( Х2 )+ x3sin2 ( х3 )+ x4sin2 ( х4 )
+ x5sin2 ( х5 )+ x6sin2 ( х6 )
+ x7sin2 ( х7 )
= 0․23883
«22 =∑ Хк2 {sin( Хк )}2
к=1
= ( Х1 )+ x22sin2 ( х2 )+ x32sin2 ( хз )
+ x42sin2 (х4)+ x52sin2 ( ^5 ) + x62sin2 ( х6 )+ x72sin2 ( х7 )
= 1․141868, bi =∑УкХк sin(хк )
к=1
= sin( Х1 )+ УгХ2 sin( х2 )+ УзХз sin( Хз )
+ у4х4 sin( Хд, )+ У5Х5 sin(%5 )
+ У6х6 sin( Хб )+ у7х7 sin( х? )
= 1․345599
=∑ „п(, )
°2 =∑ Укхк sin( )
к=1
= sin( Х1 )+ У2х2 sin( х2 )+ УзХз2 sin( Хз )
+ у4х42 sin(%4)+У5^52 sin(%5 )
+ Уб^б2 sin( Хь )+ у7х72 sin( х7 ) = 12․10867
0․04 0․23 Со 1․34
Thus *0․23 1․41+ *С1+ = *12․․10+
From the formula (11), we have
^ → Ri - × ац ; (2 ≤ i ≤ 2), (1 ≤ j ≤1)
Cl ( i-i )( t-г )
0․04 0․23 со+=*1․28+
0 0․087 ci + = *4․39+
=> 0․04с0 + 0․23С1 = 1․28, 0․087С1 = 4․39
So, ci = ․ 39 = 50․45,
1 о․087
с0 =004(1․28-0․23ci )
0․04
= (1․28 - 0․23 × 50․45) = -258․08
0․04
So, У = (-258․08 + 50․45 х ) sin( х ) (13)

Fig.1. Graph of y = -258․08 + 50․45x and y = (-258․08 + 50․45x)sin(x)
Here, 258 ․ 08 = 5․115 QTld к < 5․115 < 2 It , for which , ․ ․ ․ ,
X= 2и are the nearest two values such that sin(X)=0
So, the graph starts to oscillate from the point, X = ․ ≃ 5․699( approx․ ) along the positive x- axis and X = ․ ≃ 4․128(approx)․ along the negative x-axis which is shown in the Fig1.
So,
5․115 + 2 n 5․115 + 2 n 5․115 + 2 П \
. , (-258․08 + 50․45 ( )) sin( )/
Such that ац =∑ k'=lxk 7 {sin(2 Xk )}2 and = ∑ к=1Укхк sin(2 xk ), 1 ≤ i ≤( П +1)
Here, m=no. polynomial=1
of points=7 and n= degree of the
ATA = ( aij )
V ×2
and ATB = ( ац )
V ×1
Where CLij =∑ k=lxk 7 {sin(2 xk )}2 and = ∑ к=1Укхк sin(2 xk ), 1 ≤ i≤2
dll =∑ xk° {sin(2 xk )}2
k=l
= (2%1)+ sin2 (2 X2 )+ sin2 (2 X3 )+ sin2 (2 x4 )
+ sin2 (2 xs )+ sin2 (2 x6 )+ sin2 (2 xi )
= 0․16828,
«12 = =∑ Xk {sin(2 xk )}2
k=l
= (2 X1 )+ x2sin2 (2 X2 )+ x3sin2 (2 x3 )
+ x4sin2 (2 x4 )+ x5sin2 (2 x5 ) + x6sin2 (2 x6 )+ x7sin2 (2 x7 )
= 0․94102, is called conversion point along the positive x-axis.
Example-2 (Sine imprecise function of polynomial of degree one with angle, 2 X):
Let У= + сгх be a polynomial of degree one. So, in particular
У =(Co + сгх ) sin(2 X ), for I = 2 (14)
is an imprecise polynomial of degree one.
Let us consider the same example taken for the equation (12)
Here, (1,3.2), (2,4),(3,-2.5),(4,-4.5),(5,6),(6,-
-
7.5) ,(7,5.5)are the points in the data collection which are above and below the x-axis.
a-22 =∑ xk2 {sin(2 xk )}2
k=l
= (2%1)+ x22sin2 (2 X2 )+ x32sin2 (2 X3 )
+ x42sin2 (2 x4 )+ x52sin2 (2 xs ) + x62sin2 (2x&)+ x72sin2 (2 xi )
= 5․60673, bl =∑Укхк sin(4)
k=l
= sin(2 X1 )+ У2Х2 sin(2 X2 )+Уз^з sin(2 X3 )
+ У4Х4 sin(2X4)+У5^5 sin(2Xg )
+ Уб^б sin(2%5)+ У?Х7 sin(2X? )
= 2․49223
So, X1 = 1, x2 = 2, x3 = 3, x4 = 4, x5 = 5, x6 = 6, x7 =7
У1 = 3․2, y2 = 4, Уз = -2․5,
У4 = -4․5, Уб = 6, Уб = -7․5, У? = 5․5
By the law of roots the given imprecise function satisfies the given collection of points to have linear simultaneous equation to form a matrix as follows:
From (4),(5),(6)………….(10),we have
AX =
=> ( ATA ) X =
Where, ДТД = ( ач )( n+1)×(n+1)
ATB = (bt)(n+1)×1,X=*Cl + b2 =∑Укхк2 sin(4)
k=l
= sin(2 X1 )+ У2Х22 sin(2 X2 )+ Узхз2 sin(2 X3 )
+ У4Х42 sin(2X4)+ У5Х52 sin(2Xg )
+ Уб^б2 sin(2Xg)+У7Х72 sin(2X?)
= 23․96444
0․16 0․94 co 2․49
Thus *0․94 5․60+ *Cl+ = *23․․96+
From the formula (11),we have-
Rt → Rt -
Rj
× atj ; a ( t-i )( t-i )
(2 ≤ i ≤ 2), (1 ≤ j ≤ 1)
0․16 0․94 co+=*2․49+ 0 0․07 Cl + = *9․33+
So, as above we get
У4 = -4․5, Ув =6,Уб = -7․5, У? =5․5
=> 0․16с0 + 0․94С1 = 2․49, 0․07С1 = 9․33
9․33
С =90․․3037=133․28,
Со = (2․49 - 0․94С1 )
0․16
= (2․49 - 0․94 × 133․28) = -746․64
0․16
So, У = (-746․64 + 133․28 х ) sin(2 х ) (15)

Fig.2. Graph of = (-746․64 + 133․28x) and y= (-746․64 + 133․28x)sin(2x)
Here, ․ ≃ 5․60 and —<5․60<2и for which X= 2л are the nearest two values such that sin(2X)=0
So, the graph starts to oscillate from the point, X = ․ 60+27Г ≃ 5․9423( approx ․) along the positive x-axis and х = × - ․ 60+Зтг ≃ 5․156( approx ․) along the negative x-axis which is shown in the Fig 2.
So,
-746․64 +
․ 60+2лЛ 1
5 ․ 60+27ГА ×sin(2× ․ )
133․28 ( )
By the law of roots the given imprecise function satisfies the given collection of points to have linear simultaneous equation to form a matrix as follows:
From (4),(5),(6)………….(10),we have
АХ =
=>( АТА ) X =
Where, лгл = ( ац )( п+1)×(п+1)
АТВ = ( bt ) ( п+1 )× 1, X =*С1 +
Such that aij =∑ ™=1Хк 7 {sin(3 Хк )}2 and = ∑ к=1Укхк sin(3 хк ), 1 ≤ i≤(п+1)
Here, m=no. of points=7 and n= degree of the polynomial=1
АТА = ( ац )2×2 and АТВ = ( ац )2× .
Where aij =∑ к=1хк 7 {sin(3 хк )}2 and = ∑к=1Ук4sin(3 хк ),1 ≤ i ≤2
∑
хк° {sin(3 хк )}2
к=1
= (3%1)+sin2 (3х2)+sin2 (3 хз )+ sin2 (3 х4 )
+ sin2 (3 х5 )+ sin2 (3 х6 )+ sin2 (3 х7 )
= 0․27677,
∑ Хк {sin(3 хк )}2 к=1
а12 =
= (3Х1)+ x22sin2 (3 Х2 )
+ x32sin2 (3 хз )+ x42sin2 (3 х4 )
+ x52sin2 (3 xs )+ x62sin2 (3 х& ) + x72sin2 (3 xi )
= 2․077794, is called conversion point along the positive x-axis.
Example-3 (Sine imprecise function of polynomial of degree one with angle, 3 X):
Let У= + с^х be a polynomial of degree one. So, in particular
У =(Со + с^х ) sin(3 X ), for I =3 (16)
∑ хк2 {sin(3 Хк )}2
к=1
x^sin2 (3Х1)+ x22sin2 (3 Х2 )+ x32sin2 (3 хз )
+ x42sin2 (3 х4 )+ x52sin2 (3 ^5 ) + x62sin2 (3 х6 )+ x72sin2 (3 %7 )
= 12․36365, is an imprecise polynomial of degree one.
Let us consider the same example for the equation (12)
Here, (1,3.2),(2,4),(3,-2.5),(4,-4.5),(5,6),(6,-7.5),(7,5.5) are the points in the data collection which are above and below the x-axis.
So, хг =1, х2 =2, х3 =3, х4 =4, х5 =5, х6 =6, х7 =7
У1 = 3․2, У2 =4,Уз = -2․5,
∑ УкХк sin(3 хк )
к=1
= sin(3 Х1 )+У 2X2 sin(3 Х2. )+ У 3X3 sin(3 Хз )
+ у4%4 sin(3%4)+ У5Х5 sin(3 XS )
+ У&х6 sin(3 Х6 )+ у7х7 sin(3 X? )
= 3․744006
=∑ sin(3xk)
=∑ sin(3 )
k=l
= sin(%1)+Уз^ sin(3^2)+Уз^з2 sin(3X3 )
+ У4Х42 sin(3X4)+У5^52 sin(3Xg )
+ Уб^б2 sin(3Xg)+У7%72 sin(3X? )
= 35․319439
0․27 2․07 co1 _
Thus *2․07 12․36+*Cl+=
3․74
*35․31+
From the formula (11),we have-
Ri → Ri -
Rj
×
a ( t-i )( t-i )
^ij ;
(2≤ i ≤2),(1≤ j ≤1)
0․27
*0
2․07 co+=*3․74+
3․51 Cl+ = *6․63+
-
So, as above we get
=> 0․27 Co + 2․07Cl=3․74,-3․51Cl = 6․63
6․63
Cl = ․ =-1․888,
-3․51
co =027(3․74-2․07ci ) 0․27
= (3․74 - 2․07 × (-1․88))
0․27
= 28․26
So, У =(28․26-1․88 x ) sin(3 x ) (17)

Fig. 3. Graph of y = (28․26 - 1․88x) and y = (28․26 - 1․88x)sin(3x)
Here, ․ ≃ 15․03( approx ․) QTld —<15․03<
1 ․88 x ✓ 3
5 я , for which X = 5я are the nearest two
з values such that sin(3X)=0
So, the graph starts to oscillate from the point, X= ․ 03+5тг ≃ 15․370(approx․) along the positive x- axis, and x= × - ․ 03 + 1471 ≃ 14․837(approx․) along the
negative x-axis which is shown in the Fig 3. So,
( ․ 03 + 5тг no 1 oor15 ․ 03+57ГXX . 15 ․ 03+57Гх \
․ , (28․26 - 1․88( ․ ))sin(3 × ․ ))m is called conversion point along the positive x-axis.
B. Sine imprecise function of polynomial of degree two:
Let у= + сгх + c±x2 be a polynomial of degree two. So, in particular
У =( Cq + сгх + C1X2 ) sin( X ), for I =1 (18)
is an imprecise polynomial of degree two.
Let us consider (1,0.5), (2,2.5),(3,2),(4,4),
(5,3.5),(6,6),(7,7) be the points in the data collection.
So, %1=1, ^2 =2, ^3 =3, X4=4, ^5 =5, ^6 =6,X?=7
У1 = 0․5, У2 = 2․5, Уз =2,
У4 =4,У5 = 3․5, Уб=6,У? =5․5
From (4),(5),(6)………….(10),we have
AX =
=>( ATA ) X =
Where ATA = (a7/)
( 71+1)×( )
and ATB = ( bn )(n+1)×1
Such that aij =∑ ™=lxk 7 {sin(Xk)}2 and =
∑ к1=1Укхк sin( xk ), 1 ≤ i≤( П +1)
Here, m=no. of points=7 and n= degree of the polynomial=2
ATA = ( Clij )3×3 and ATB = ( dtj )3×4
Where at] =∑ k=lxk 7 {sin( xk )}2 and bi =∑ к=1Укхк sin( xk ),1 ≤ i ≤3
∑ xk° {sin( xk )}2
k=l
= 0․0148521,
a13
=
∑ xk {sin( ^ )}2 k=l
= 0․341889,
∑[ xk2 {sin( xk )}2]
k=l
=∑ xk {sin( xk )}2
k=l
= 1․418684
= 0․341889,
And
Thus
Я22 =∑ Xk2 {sin( Xk )}2 = 1․1418684, k=l
a32 =∑Xk3 {sin(xk)}2 = 8․799282, k=l a33 =∑Xk4 {sin(Xk)}2 = 56․055255 k=l
bl
=∑ Xkyk sin( Xk ) = 11․593562,
k=l
^2 =∑хк2Укsin(Xk) = 68․812246, k=l
Ь3 =∑ хк3Ук sin( Xk ) = 424․896557
k=l the simultaneous equation is converted
into
461․55c2 = 5143․86
So, co = -78․13, C1 = 0․63, c2 = 11․14 and = (-78․13 + 0․63 x + 11․14 x2 )sin( X ) (19)

Fig.4. 2D graph of y = (-78․13 + 0․63x + 11․14x )sin(x)
Thus the solution is
0․63 ± √0․63 +4×78․13×11․14
= 2×78․13
= 0․38( approx ),-0․37( approx ) and - я <-0․37<0 and 0< X < H
following simple matrix form:
0․015
[ 0․34
1․14
0․34
1․14
8․80
1․14 1 [C° 11․59
8․80][Cl]=[68․81] 56․06J Lei 424․90
From the formula (11),we have-
Ri → Ri - × O-ij ; ci (i-l)(i-l)
0․015
(2≤ i ≤3); j =1
0․34
-6․56
-17․04
11․59
1․14
-17․04
-30․58
][ « ]
-193․89
-455․94
R[ → Ri - × O-ij ;
Cl ( i-l )( i-l )
(2≤ i ≤3); j =2
0․015 0․34 1․14 |
co" |
11․59 |
|
[ 0 -6․59 -17․04] |
[Cl |
= |
-193․8] |
0 0 461․55 |
A. |
5143․86 |
=> 0․015c0 + 0․34Cl + 1․14c2 = 11․59
=> -6․59Cl - 17․04c2 = -193․98
So, the graph starts to oscillate from the point, X= ․ ≃1․76(approx) along the positive x-axis, and X = ․ ≃ -1․75( approx) along the negative x-axis which is shown in the Fig 4.
So,
( °- ․ 38+.,(-78․13+0․63( “ ․ 38+.)+
11․14(“ ․ 38+. ) )sin(“ ․ 38+. ))
is called conversion point along the positive x-axis.
Further from the same point, imprecise function will come back to the original function of polynomial when we remove the multiplication factors. So sometime it is called diversion point of the imprecise function with respect to the multiplication factor sine.
Thus from the above calculations, we have observed that if the angle of the trigonometry function is increased then conversion point come closer to the origin of the coordinate axis system. It means that considered experiment starts to oscillate within the short period of time to have short wave length and larger energy in the system.
For example if the wings of a Generator moves more angle then speed is increased and the energy output will be larger and larger due to short wave length and the closer conversion point.
V. R ate E ffect of I mpreciseness for the I mprecise F unctions
It is the ratio of the volume occupied by the objects
and the volume of the place where the object is used. This value gives us information for any places whether the design experiment is properly done or not. If it is not properly designed then we will modify it again and again. Normally one is the value of the rate effect of impreciseness for which an experiment well designed or not is counted. To study how per the behavior of the object is effecting to the medium, it is very much necessary to know area occupied by any particular object.
-
A. Area bounded by sine imprecise functions of polynomial of degree one:
To obtain area by the help of integration all the interval cannot be allowed to take as a limit for the imprecise function. For example- lit
J (с 0 + c ( x) sin(x) xx — 0, о
J (c0 + c( x) sin(2x) dx — 0 о etc. For this reason to obtain area of an imprecise function imprecise number will be taken as a limit of the integration. After defining area obtained by the imprecise number we will obtain area of the imprecise function for any interval in the summation form.
-
(i) Sine imprecise function of angle multiplication one:
Thus for an imprecise function, will be measured in our system separately for the respective function so that we can have better information how their character change for long interval in an imprecise function. Here the limit of the integrations are taken in between maximum and minimum point, as in between this two points the above mentioned membership function and the reference functions are counted. For this example let us define the area bounded by an imprecise function of degree one obtained by sine multiplication of function as follows:
7 ( — J ( c 0 + c ( x) sin(x) dx = C 0 + C (
^2
— J(c 0 + qx) sin(x) dx
= C o + С((л — 1)
^з
/4
ЗТГ
= J (c 0 + c ( x) sin(x) dx
-
— С ( (я + 1)
2тг
= J (co + c(x) sin(x) dx 37Г
T
= — C 0 — С ( (2я — 1)
for I = 1,y = (c 0 + c ( x)sin(x) ,
we have section of intervals, [o,p к ] , [я,у,2я] , [2я,у,3я] , [3я,у,4я]
,
having indicator functions for as follows:
Un to = <
0(х); 0 < x < —
Ф to; — < x < пя
such that 0(0) = <р(яя) = 0 /КП\ /КП\ an d 0 (—) = ф (—)
Here, the function has maximum level at the point
П7Г
.
So, we can call, *0,ря] , [я,у,2я] , *2я,у,3я] ,
[3я, ^, 4я] are an
imprecise number. Since the indicator function has membership function and the reference function for an imprecise number. The area of the imprecise function
J (C 0 + qx) sin(x) dx
2tt
= C 0 + C ( (2 я + 1)
Зтг
J ( + ) sin( )
= C 0 + C ( (3 я — 1)
/ 7 = J ( C0
Зтг
+ ) sin( )
— — C 0 — C ( (3я + 1)
J ( + ) sin( )
7тг
— — C 0 — C ( (4я — 1) so on.
Here, negative signs are shown area bounded by the imprecise function lower part of the x-axis.
Area of the membership imprecise function = 7 ( + |/ 3 | + 7 5 + |/ 7 | — ^0 + C ( Z £=1 [( k — 1)я + 1] ; n=8
Area of the reference imprecise function is
^2 +|/4|+ к +| ^8 |=2С° + С1 ∑к=1[ кл - 1],; n=8
Area of this imprecise function for this interval is к+к+|к|+|к|+к+|к|+|к|
=∫(с0 + сгх ) sin( X ) dx
о
=(2×4×1)с0 + С1 ∑[(2 к -1) л ]
к=1
Thus the area of this imprecise function in the interval [0, Л ] is
such that ∅(0) = Ф(у)=0 /ПЛ\ /ПЛх and∅(4)=Ф(4)
Here, function has maximum level at the point = .
So we can call,
*0 n Л 1
,;,2 + , * 2, , + , *2 , ,3 + , *3 , ,4 +
are all an imprecise numbers. Now,
к =∫( =.
+ сгх ) sin(2 X ) dx = +
пл к=∫(со + с.х)sin( 1) «X
=(2 ․1) + ∑ [(2 -1) ] (21)
This value is known as the membership value of the
sine imprecise polynomial of degree one for the angle X .
к =∫(co + C1x )sin(2 x) dx
= +—+ Cl ( Л -1)
=+2+ 4
Thus --------------------------: ;И ∈ N is called
Total area bonded by the experiment
rate per imprecise number of the respective intervals.
So, Total area bonded by the experiment *
rate of convergence of the imprecise function.
If
∑ In________________
.Total area bouded by the experiment
; П ∈ N
≤1,
the
3л
T к=∫(Co + c^x) sin(X) dx
2"
_ c0 сг ( Л +1)
=-2- 4
system is completely controllable. Otherwise we have to modify this function to into the controllable form.
Variance of this function in the respective interval is a2 = * {∑ In } +
Lno ․ of observation!
Standard deviation,
к = ∫(Co + CTX ) sin(2 X ) dx
3л co ci (2л-1)
=-2- 4
∑
In ;И ∈ N )2
Tota area bouded by the experiment /
Here the variance is the variation of area in the function for the different intervals.
(ii) Sine imprecise function of angle multiplication two:
For an imprecise function, for I=2,У=(Cq + C^X)sin(2X),
we have section of intervals,
*0 Г 9 7л Л -rrl
, ; ,2 + , * 2, , + , *2 , ,3 + , *3 , ,4 + ……………
….……, having indicator functions for as follows:
kN ( X )=
{
∅ ( X ); 0≤ X ≤
, . пл
(
X
); ≤
X
≤
15=∫(co +C1x)sin(2 x)
dx
_ co сг
(2
Л
+1)
=2+ 4
3л к=∫(Со + стх) sin(2X) dx т со . ci (3л-1) =2+ 4 7л
Ь
=∫(Со +
стх
) sin(2
X
)
dx
Зл
_ Со С!
(3
л
+1)
=-2- 4 In
Is
=∫(Со +
сгх
) sin(2
х
)
dx
7тт
_ co ci
(
4тг-1
= - - )
so on.
2 4 V Here, negative signs are shown area bounded by the imprecise function lower part of the x-axis.
Area of the membership imprecise function is =/1
+
| ^3
|+/5
+| ^7 |
и
П
Ci
= c0 + ∑[(
k
-1)я+1];n=8
Area of the reference imprecise function is
+|
и
|+
Ie
+|
Is
|
И CiVr,
= co + ∑[
ku
-1];
n
=8
k=l Area of this imprecise function in this interval is k+ /2+|/3|+|/4|+Is+|/7|+|4| 2л
=∫(Co +
c^x
) sin(2
X
)
dx
(2×2×2)
×
=2 + ∑[(2
k
-1)
U
]
∫(Co +
сгх
) sin(2
X
)
dx
2 ×4
(2×4×2)
co Cl - V rr? , !
= 2 +2 ∑[(2 -1) ] k=l
Thus the area of the imprecise the function in the interval
[0, Я]
is
П7Г k=∫(Co + c^x) sin(2X) dx 2n
= (2и×2)+ 5 ∑[(2
k
-1)
и
]
k=l
This value is known as the membership value of the sine imprecise polynomial of degree one for the angle
2
X
.
Thus --------------------------:
;
n
∈
N
is called
Total area bonded by the experiment rate per imprecise number of the respective intervals.
So,
Total area bonded by the experiment *
rate of convergence of the imprecise function.
,
∑
In
Total area bonded by the experiment ; ∈ - ≤ 1, the system is completely controllable. Otherwise we have to modify this function to into the controllable form.
Variance of this function in the respective interval is
a2
= *
{∑
In
}
+
Lno․
of observations
Standard deviation, ∑
*0, 7,7 +
,
*J, ,3+
, ……………, having
Un
(
х
)=
∅
(
X
); 0≤
X
, . ИЯ
ИЯ < — ≤6 ИЯ
Ф
(
х
); ≤
х
≤
/4=∫(Со +
сгх
) sin(3
X
)
dx
(2 -1) =-3- 9 (2×4×3)Co 3 з×4
+ i ∑[(2
к
-1)
я
]
к=1 Thus the area of the imprecise function in the interval [0, Я]is ls=∫(co + c.x)sin(3 x) dx 2л
_ CO C1
(2
я
+1)
=3+ 9 пл к=∫(со + с.х)sin(3 1) dx Зп = (2 п×3)+ I ∑[(2к-1)я];пℰR к=1
I6
= ∫(Co +
c^x
) sin(3
X
)
dx
"о"
_ co сг
(3
к
-1)
=3+ 9
7л
6
I7
=∫(Co +
сгх
) sin(3
X
)
dx
_ c0
c^
(3
я
+1)
=-3- 9
4=∫(Co +
CTX
) sin(3
X
)
dx
7л
_ co ci
(
47Г-1
)
= - - )
so on.
3 9 7 Here, negative signs are shown area bounded by the imprecise function lower part of the x-axis.
Area of the membership imprecise function is =/1
+
| ^3 |+
Is
= +
I
∑
k=l
[(
k
-1)
я
+1];n=6
Area of the reference imprecise function is , И с,
^2 +| ^4 |+
k
= 1 co + 2 ∑[
кя
-1];n=6
k=l
Area of this imprecise function in the this interval is
/1 + ^2 +| ^3 |+|/4|+/5 +
=
∫(Co +
сгх
) sin(3
X
)
dx
(2×1×3)
×
=3 +I ∑[(2
к
-1)
я
]
к=1
∫(Co +
стх
) sin(3
X
)
dx
о
This value is known as the membership value of the sine imprecise polynomial of degree one for the angle
3
X
.
Thus
;
Т1
∈
N
is called
Total area bonded by the experiment rate per imprecise number of the respective intervals. So, Total area bonded by the experiment ; ∈ is called rate of convergence of the imprecise function.
,
∑ d .
; 71 6 J , system is completely controllable. Otherwise we have to modify this function to into the controllable form. Variance of this function in the respective interval is a2 = * {∑ In } +
Lno․
of observation]
Standard deviation, ∑
In
;И
∈
N
)
Tota area bonded by the experiment / Here the variance is the variation of area in the function for the different intervals. Thus (21), (23) and (25) lead us to introduce a general formula for finding the area of sine imprecise function of degree one as follows: пл
∫(Co +
cYx
) sin(
lx
)
dx
In = (2n×I)+ ∑[(2к-1)я]; I∈Z k=l
Here for any imprecise number total no. of membership and the reference function is always
2
nl forn
∈
R and I
∈
Z
VI.
C
onclusion
Obtaining a general formula of imprecise function in various situations was the main objective of this article. So the general formula of sine imprecise function is defined with the help of finite numbers of data collection of points in the beginning. This formula is tested in the particular problems. Finally area of the sine imprecise function is obtained by the help of integration and summation. Here the limits of the integration is taken from the imprecise number of different interval within the imprecise function and proposed a new formula of area in the last part of the article.
A
cknowledgment
The authors first would like to thank the CIT, Kokrajhar for providing available facilities to bring out this article. Secondly would like thank the Bodoland University for their encouragement to bring out this article. Finally would like to thank all the reviewers for their careful reading of this article and for their helpful comments which are helped to improve this work.
Список литературы Rate of Convergence of the Sine Imprecise Functions
- J. L. Krahula and J. F. Polhemus, Use of Fourier Series in the Finite Element Method, AIAA Journal, Vol. 6, No. 4 (1968), 726-728.
- E.O. Attinger, A. Anné and D.A. McDonald, Use of Fourier Series for the Analysis of Biological Systems, The Biophysical Society. Published by Elsevier Inc., Vol. 6, No.3 (1966), 291–304.
- H. Akima, A New Method of Interpolation and Smooth Curve Fitting Based on Local Procedures, Journal of the ACM, Vol. 17, No. 4 (1970), 589-602.
- C. Zhu and F. W. Paul, A Fourier Series Neural Network and Its Application to System Identification, J. Dyn. Sys., Meas., Control Vol.117, No.3 (1995), 253-261.
- C. H. Cheng, A new Approach to Ranking Fuzzy Numbers by Distance Method, Fuzzy Sets and Systems, Vol. 95 (1998), 307-317.
- E.J. Ekpenyong, C.O. Omekara, Application of Fourier Series Analysis To Temperature Data, Global Journal of Mathematical Sciences Vol. 7, No.1( 2008), 5-14.
- F. Toutounian and A. Ataei, A New Method for Computing Moore-Penrose Inverse Matrices, Journal of Computational and Applied Mathematics, Vol. 228, No. 1 (2009), 412-417.
- M. Kahm, grofitt: Fitting Biological Growth Curves with R, Journal of Statistical Software, Vol. 33, No.7 (2010).
- H.K. Baruah, Theory of Fuzzy Sets: Beliefs and Realities, I.J. Energy Information and Communications. Vol.2, No.2 (2011), 1-22.
- H.K. Baruah, Construction of Membership Function of a Fuzzy Number, ICIC Express Letters, Vol. 5, No.2 (2011), 545-549.
- M. Abbasian, H. S. Yazdi, ans A. V. Mazloom, Kernel Machine Based Fourier Series, I. J. of Advanced Science and Technology Vol. 33 (2011).
- H.K .Baruah, An introduction to the theory of imprecise Sets: The Mathematics of Partial Presence, J. Math. Computer Science, Vol. 2, No.2 (2012), 110-124.
- T. J. Neog and D. K. Sut, An Introduction to the Theory of Imprecise Soft Sets, I.J. Intelligent Systems and Applications, Vol.11 (2012), 75-83.
- S. Narayanamoorthy, S. Saranya, and S. Maheswari, A Method for Solving Fuzzy Transportation Problem (FTP) using Fuzzy Russell's Method, I.J. Intelligent Systems and Applications, Vol. 2 (2013), 71-75.
- S. Borgoyary, A Few Applications of Imprecise Numbers, I.J. Intelligent Systems and Applications, Vol. 7, No.8 (2015), 9-17.
- S. Borgoyary, An Introduction of Two and Three Dimensional Imprecise Numbers, I.J. Information Engineering and Electronic Business, Vol.7, No.5 (2015), 27-38.