PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS

Similar documents
NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

Integration by Parts

On the irreducibility of some polynomials in two variables

The Equitable Dominating Graph

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

Engineering 323 Beautiful HW #13 Page 1 of 6 Brown Problem 5-12

Content Skills Assessments Lessons. Identify, classify, and apply properties of negative and positive angles.

Derangements and Applications

u r du = ur+1 r + 1 du = ln u + C u sin u du = cos u + C cos u du = sin u + C sec u tan u du = sec u + C e u du = e u + C

CHAPTER 24 HYPERBOLIC FUNCTIONS

The Matrix Exponential

10. The Discrete-Time Fourier Transform (DTFT)

INTEGRATION BY PARTS

Differential Equations

Construction of asymmetric orthogonal arrays of strength three via a replacement method

Deift/Zhou Steepest descent, Part I

Limiting value of higher Mahler measure

International Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN

The Matrix Exponential

Two Products Manufacturer s Production Decisions with Carbon Constraint

2008 AP Calculus BC Multiple Choice Exam

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:

An Application of Hardy-Littlewood Conjecture. JinHua Fei. ChangLing Company of Electronic Technology Baoji Shannxi P.R.China

Hardy-Littlewood Conjecture and Exceptional real Zero. JinHua Fei. ChangLing Company of Electronic Technology Baoji Shannxi P.R.

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula

Basic Polyhedral theory

1973 AP Calculus AB: Section I

4037 ADDITIONAL MATHEMATICS

(Upside-Down o Direct Rotation) β - Numbers

Mathematics. Complex Number rectangular form. Quadratic equation. Quadratic equation. Complex number Functions: sinusoids. Differentiation Integration

Things I Should Know Before I Get to Calculus Class

MATHEMATICS PAPER IIB COORDINATE GEOMETRY AND CALCULUS. Note: This question paper consists of three sections A, B and C.

MSLC Math 151 WI09 Exam 2 Review Solutions

Thomas Whitham Sixth Form

For more important questions visit :

10. Limits involving infinity

Thomas Whitham Sixth Form

First derivative analysis

Rational Approximation for the one-dimensional Bratu Equation

INTEGRALS. Chapter 7. d dx. 7.1 Overview Let d dx F (x) = f (x). Then, we write f ( x)

Homotopy perturbation technique


LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM

How would you do the following integral? dx.

Differentiation of Exponential Functions

6.1 Integration by Parts and Present Value. Copyright Cengage Learning. All rights reserved.

y = 2xe x + x 2 e x at (0, 3). solution: Since y is implicitly related to x we have to use implicit differentiation: 3 6y = 0 y = 1 2 x ln(b) ln(b)

Electromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology

cycle that does not cross any edges (including its own), then it has at least

COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM

Exercise 1. Sketch the graph of the following function. (x 2

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.

nd the particular orthogonal trajectory from the family of orthogonal trajectories passing through point (0; 1).

Einstein Equations for Tetrad Fields

Section 11.6: Directional Derivatives and the Gradient Vector

Math 34A. Final Review

dx equation it is called a second order differential equation.

DISTRIBUTION OF DIFFERENCE BETWEEN INVERSES OF CONSECUTIVE INTEGERS MODULO P

Engineering Mathematics I. MCQ for Phase-I

MATHEMATICS PAPER IB COORDINATE GEOMETRY(2D &3D) AND CALCULUS. Note: This question paper consists of three sections A,B and C.

Chapter two Functions

Journal of Modern Applied Statistical Methods May, 2007, Vol. 6, No. 1, /07/$ On the Product of Maxwell and Rice Random Variables

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013

Chapter 1. Chapter 10. Chapter 2. Chapter 11. Chapter 3. Chapter 12. Chapter 4. Chapter 13. Chapter 5. Chapter 14. Chapter 6. Chapter 7.

Calculus II (MAC )

Chapter 10. The singular integral Introducing S(n) and J(n)

Where k is either given or determined from the data and c is an arbitrary constant.

On spanning trees and cycles of multicolored point sets with few intersections

Legendre Wavelets for Systems of Fredholm Integral Equations of the Second Kind

Combinatorial Networks Week 1, March 11-12

Calculus concepts derivatives

DIFFERENTIAL EQUATION

Search sequence databases 3 10/25/2016

Comparison of Some Iterative Methods of Solving Nonlinear Equations

Spectral Synthesis in the Heisenberg Group

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1

Application of Vague Soft Sets in students evaluation

Inference Methods for Stochastic Volatility Models

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.

Higher order derivatives

Calculus Revision A2 Level

EEO 401 Digital Signal Processing Prof. Mark Fowler

Complex Powers and Logs (5A) Young Won Lim 10/17/13

ABEL TYPE THEOREMS FOR THE WAVELET TRANSFORM THROUGH THE QUASIASYMPTOTIC BOUNDEDNESS

Math 102. Rumbos Spring Solutions to Assignment #8. Solution: The matrix, A, corresponding to the system in (1) is

On the number of pairs of positive integers x,y H such that x 2 +y 2 +1, x 2 +y 2 +2 are square-free

That is, we start with a general matrix: And end with a simpler matrix:

SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH.

ON RIGHT(LEFT) DUO PO-SEMIGROUPS. S. K. Lee and K. Y. Park

On the optimality of a general production lot size inventory model with variable parameters

Note If the candidate believes that e x = 0 solves to x = 0 or gives an extra solution of x = 0, then withhold the final accuracy mark.

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES

CONTINUITY AND DIFFERENTIABILITY

Mathematics 1110H Calculus I: Limits, derivatives, and Integrals Trent University, Summer 2018 Solutions to the Actual Final Examination

Square of Hamilton cycle in a random graph

1 Isoparametric Concept

A. Limits and Horizontal Asymptotes ( ) f x f x. f x. x "±# ( ).

a 1and x is any real number.

Section 6.1. Question: 2. Let H be a subgroup of a group G. Then H operates on G by left multiplication. Describe the orbits for this operation.

Transcription:

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS 1 Dharmndra Kumar Yadav, Dipak Kumar Sn ABSTRACT 1 Associat Profssor in Applid Mathmatics HMR Institut of Tchnology & Managmnt, Hamidpur, Dlhi-36(India) Associat Profssor in Mathmatics R. S. Mor Collg, Govindpur, Dhanbad-88109, Jharkhand (India) In th prsnt papr w hav provd on of th si standard forms of indfinit nonintgrabl functions (classically known as nonlmntary functions) and thir ampls givn by Yadav & Sn by applying strong Liouvill s thorm, its spcial cas, som wll-known nonlmntary functions and two proprtis du to Marchisotto & Zakri. Ky Words: Nonlmntary functions, strong Liouvill s thorm tc. 010 AMS Subjct Classification: 6A09, 6B I INTRODUCTION A natural qury ariss in calculus that what typ of functions cannot b intgratd? or which indfinit intgrals ar not lmntary? Th first ampl which lads us byond th rgion of lmntary functions is th lliptic intgrals du to John Wallis (1655). Such intgrals cannot b valuatd in trms of th lmntary functions was provd by Josph Liouvill in 1833 and th main rsults on functions with nonlmntary intgrals bgan with Strong Liouvill Thorm (1835) and Strong Liouvill Thorm (spcial cas, 1835). Marchisotto & Zakri (1994) studid nonlmntary functions and mntiond two important ampls 4 and 5 [5, pp.300-301], which ar tratd as proprtis in proving th functions lmntary and nonlmntary. By applying th abov proprtis w gt th following wll-known nonlmntary functions: d, a d,(a 0), d, d, d, sin d, cos d Proofs of Nonlmntary Functions: Yadav & Sn [6] hav givn si standard forms of indfinit nonintgrabl functions out of which form-1 is as follows: 1

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) An indfinit intgral of th form f ( ) d f '( ), whr f() is a polynomial function of dgr, or a trigonomtric (not invrs trigonomtric) function, or a hyprbolic (not invrs hyprbolic) function is always nonintgrabl i.. nonlmntary. Proof: W will prov it taking diffrnt possibl cass as follows: Cas I: Whn f() is an algbraic function (polynomial) of dgr : W hav Lt g() f ( ) f '( ) p() R() q() d g() 1 d, [Taking g() ]. From strong Liouvill thorm (spcial cas), d is lmntary if and only if thr ists a rational function R() such that g() R '() R(), whr g.c.d.(p(), q())=1. Thn w hav 1 R '() 1 R '() R() R() q()p'() p()q'() [] p()q() [q()] (1.1) p()q '() p'() q() [] p() q() Which implis q() f () as q() cannot divid p() and q (). In this cas ithr q()=k, a constant or a polynomial of dgr lss than or qual to th dgr of f (). For q()=k, from (1.1) w hav kp'() [] p()k k (1.) Comparing dgrs of in (1.) rsults out in a contradiction. Hnc q() cannot b a constant. For q() a polynomial of dgr lss than or qual to th dgr of f (), w hav sinc q() f (), lt us assum that f ()=q().h(). Thn from (1.1) q()h()q()p'() q()h()p()q'() [q()h()] p()q() [q()] h()p()q '() h()p'() 1 q()[h()] p(). (1.3) q() Which implis q() h(), sinc q() cannot divid p() and q (). Lt h()=q().ξ(). Thn from (1.3), w hav

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) 3 q() ()p'() p()q'() () [q()] [ ()] p() 1 (1.4) Comparing th dgrs of in both sids in (1.4) rsults out in a contradiction. Thrfor such R() dos not ist, i.., th givn function is nonlmntary. Cas II: Whn f() b a trigonomtric (not invrs trigonomtric) function: Lt us considr thm on by on. 1.1 For sin function, w hav sin () d d '()cos () whr φ() b any polynomial of dgr 1. On putting sinφ()=, w hav, sin () d d '()cos () [ '()] (1 ) (1.1.1) Sub-cas I: Whn φ() is linar, lt φ()=+b. Thn from (1.1.1) w hav d d [ '()] (1 ) (1 ) 1 d d (1 ) (1 ), whr p d dp,[putting1 p] (1 ) p and d 1 p dp,[putting1 p] (1 ) p. Both ar nonlmntary from ampl-4 du to Marchisotto t al [5, pp.300]. Thrfor th givn function is also nonlmntary. Sub-cas II: Whn φ() is a polynomial of dgr. Lt us considr φ()= +b+c. Thn w hav from (1.1.1), on putting sinφ()= d [ '()] (1 ) 1 d b 4c, whr k 1 4 [sin k](1 ) 4 1 d 4 1 [sin k] (1 ) (1 ) 1 F,, 1,sin d 1 3 F, y, y, y d 3

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) dy1 dy dy3 1 1 y 1,, d d y 1 d 1 y Applying strong Liouvill thorm, part (b), w find that it is lmntary if and only if thr ists an idntity of th form n d 1 U 0 c i log U i i1 4[sin k](1 ) d n du0 U' i c 1 i 4[sin k](1 ) d i1 Ui whr ach U j is a function of, y 1, y, and y 3. Considring diffrnt forms of U j lik 1 1 log[(sin k) ], log(sin k) w find that no such U j ist. Hnc th givn function is nonlmntary. Similarly w can prov it nonlmntary for highr dgr polynomials φ()., 1. For cosin function, w hav cos () d d '()sin () whr φ() b any polynomial of dgr 1. On putting cosφ()=, w hav, cos () d d d '()sin () [ '()] (1 ) [ '()] (1 ) (1..1) Sub-cas I: Whn φ() is linar, lt φ()=+b. Thn from (1..1) w hav d d [ '()] (1 ) (1 ) which is nonlmntary provd in sction 1.1 subcas-i. Sub-cas II: Whn φ() is a polynomial of dgr. Thn from (1..1) w hav d 1 d 1 [ '()] (1 ) 4 (cos k)(1 ) 1 F[,, 1,cos ]d A similar argumnt will hold as in sction 1.1 to prov it nonlmntary., 4

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) 1.3. For tangnt function, w hav on putting tanφ()=. tan () d d '()sc () d [ '()] (1 ). (1.3.1) Sub-cas I: Whn φ() is linar, lt φ()=+b. Thn from (1.3.1) w hav d d [ '()] (1 ) (1 ) 1 d d (1 i) (1 i) Now i ip d dp, putting (1 i) p (1 i) i p By strong Liouvill thorm (spcial cas), it is lmntary if and only if thr ists a rational function R() such that it satisfis th idntity 1 R '(p) ir(p) p 1 R(p) 0 and R '(p) p But R(p) cannot b ro, so such R(p) dos not ist. Hnc it is nonlmntary. Also d (1 i) p ip i i dp, putting (1 i) p Again by strong Liouvill thorm (spcial cas), it is lmntary if and only if thr ists a rational function R() which satisfis th idntity 1 R '(p) ir(p) p 1 R(p) 0 and R '(p) p But R(p) cannot b ro, so such R(p) dos not ist. Hnc it is nonlmntary. Thrfor th givn function is nonlmntary in this cas. Sub-cas II: Whn φ()= +b+c. Thn from (1.3.1) w hav d 1 d b 4c,k 1 [ '()] (1 ) 4 [tan k](1 ) 4 1 F[,,(1 ),tan ]d 1 3 F[, y, y, y ]d dy1 dy dy3 1 1 y 1,, d d d 1 y 5

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) By strong Liouvill thorm part (b), it is lmntary if and only if thr ists an idntity of th form containing U j, a function of, y 1, y, and y 3 du U i' ci 4[tan k](1 ) d U n i 1 i1 Considring diffrnt forms of U j lik log(tan -1 +k), log[ (tan -1 +k)], tc. w find that no such U j ist, i.., no such idntity ist. Hnc th givn function is nonlmntary. Similarly w can prov it nonlmntary for highr dgr polynomials φ(). i 1.4. For cotangnt function, w hav on putting cotφ()= cot () d d '()cosc () d [ '()] (1 ).. (1.4.1) Sub-cas-I: For φ()=+b, w hav from (1.4.1) d d [ '()] (1 ) (1 ) Which is nonlmntary, provd in sction 1.3, sub-cas-i. Sub-cas-II: For φ()= +b+c, w hav from (1.4.1) d 1 d b 4c,k 1 [ '()] (1 ) 4 (cot k)(1 ) 4 1 F[,,(1 ),cot ]d A similar argumnt will hold as in sction 1.3 to prov it nonlmntary. 1.5. For coscant function, w hav on putting coscφ()= cosc () d d '()cosc ()cot () d [ '()] ( 1) (1.5.1) Sub-cas I: Whn φ() is linar, lt φ()=+b. Thn from (1.5.1) w hav d d [ '()] ( 1) ( 1) d d ( 1) 6

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) Whr th first intgral d ( 1) is nonlmntary as provd in sction 1.1, sub-cas-i and th scond intgral d d is also nonlmntary from ampl-5 du to Marchisotto t al [5, pp.301]. Sub-cas II: Whn φ()= +b+c, thn from (1.5.1) w hav d [ '()] ( 1) d [ b] ( 1) d b 4c,k 1 4[cos c k] ( 1) 4 1 F[,, 1,cosc ]d 1 3 F[, y, y, y ]d dy1 dy dy3 1 1 y 1,, d d y 1 d 1 y By strong Liouvill thorm part (b), this is lmntary if and only if thr ists an idntity of th form containg U j, a function of, y 1, y, and y 3 as follows du U i' ci 4[cos c k] ( 1) d U n i 1 i1 Considring diffrnt forms of U j lik log[cosc -1 +k], log[ (cosc -1 +k)], tc., w find that no such U j ist, which satisfy th abov idntity. Hnc th givn function is nonlmntary. Similarly w can prov it for highr dgr polynomial φ(). 1.6. For scant function, w hav on putting scφ()= i sc () d d '()sc () tan () Sub-cas-I: For φ()=+b, w hav from (1.6.1) d [ '()] ( 1). (1.6.1) d d [ '()] ( 1) ( 1) 7

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) Which is nonlmntary, provd in sction 1.5, sub-cas-i. Sub-cas-II: For φ()= +b+c, w hav from (1.6.1) d 1 d b 4c,k 1 [ '()] ( 1) 4 [sc k] ( 1) 4 1 F[,, 1,sc ]d It can b provd nonlmntary by th similar procdur as has bn don in sction 1.5. Cas III: Whn f() b a hyprbolic (not invrs hyprbolic) function. Lt us considr thm on by on. 1.7. For sin hyprbolic function, w hav on putting sinhφ()= sinh () d d '()cosh () d [ '()] (1 ) (1.7.1) Sub-cas I: Whn φ() is linar, lt φ()=+b. Thn from (1.7.1) w hav d d [ '()] (1 ) (1 ) which is nonlmntary, provd in sction 1.3, sub-cas-i. Sub-cas II: Whn φ()= +b+c. Thn from (1.7.1), w hav d d [ '()] (1 ) [ b] (1 ) d b 4c, whr k 1 4(sinh k)(1 ) 4 1 F[,, 1,sinh ]d 1 3 F[, y, y, y ]d dy1 dy dy3 1 1 y 1,, d d y 1 d 1 y Applying strong Liouvill thorm part (b), it is lmntary if and only if thr ists an idntity of th form du U' n 0 i c 1 i 4(sinh k)(1 ) d i1 Ui Considring diffrnt possibl forms of U j lik log[sinh -1 +k], log[ (sinh -1 +k)], tc. w find that no such U j ist. Hnc th givn function is nonlmntary. Similarly w can prov it nonlmntary for highr dgr polynomials.. 8

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) 1.8. For cosin hyprbolic function, w hav on putting coshφ()= cosh () d d '()sinh () Sub-cas-I: For φ()=+b, w hav from (1.8.1) d [ '()] ( 1). (1.8.1) Which is nonlmntary provd in sction 1.1, sub-cas-i. Sub-cas-II: For φ()= +b+c, w hav from (1.8.1) d d [ '()] ( 1) ( 1) d 1 d b 4c,k 1 [ '()] ( 1) 4 (cosh k)( 1) 4 1 F[,, 1, cosh ]d It can now b provd nonlmntary by strong Liouvill thorm part (b). Similarly w can prov it for highr dgr polynomial φ(). 1.9. For tangnt hyprbolic function, w hav on putting tanhφ()= tanh () d d '()sch () Sub-cas-I: For φ()=+b, w hav from (1.9.1) d [ '()] (1 ) (1.9.1) d d [ '()] (1 ) (1 ) Which is nonlmntary, provd in sction 1.1, sub-cas-i. Sub-cas-II: For φ()= +b+c, w hav from (1.9.1) d 1 d b 4c,k 1 [ '()] (1 ) 4 (tanh k)(1 ) 4 F[,,(1 ),tanh 1 It can now b provd nonlmntary by strong Liouvill thorm part (b). Similarly w can prov it for highr dgr polynomial φ(). ]d 9

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) 1.10. For cotangnt hyprbolic function, w hav on putting cothφ()= Sub-cas-I: For φ()=+b, w hav from (1.10.1) cot h() d d '()cosch () d [ '()] ( 1).. (1.10.1) d [ '()] ( 1) d ( 1) Which is nonlmntary provd in sction 1.1, sub-cas-i. Sub-cas-II: For φ()= +b+c, w hav from (1.10.1) d 1 d b 4c,k 1 [ '()] ( 1) 4 (coth k)( 1) 4 1 F[,,( 1),coth ]d It can now b provd nonlmntary by strong Liouvill thorm part (b). Similarly w can prov it for highr dgr polynomial φ(). 1.11. For coscant hyprbolic function, w hav on putting coschφ()= cosch() d d '()cosch ()coth () Sub-cas-I: For φ()=+b, w hav from (1.11.1) d [ '()] ( 1) (1.11.1) d d [ '()] ( 1) ( 1) d d 1 Both ar nonlmntary provd in sction 1.5, sub-cas-i and sction 1.7, sub-cas-i rspctivly. Sub-cas-II: For φ()= +b+c, w hav from (1.11.1) d 1 d b 4c,k 1 [ '()] ( 1) 4 (cos ch k) ( 1) 4 1 F[,, 1,cosch ]d It can now b provd nonlmntary by strong Liouvill thorm part (b). Similarly w can prov it for highr dgr polynomial φ(). 1.1. For scant hyprbolic function, w hav on putting schφ()= 10

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) sch () d d '()sch () tanh () Sub-cas-I: For φ()=+b, w hav from (1.1.1) d [ '()] (1 ) (1.1.1) d d [ '()] (1 ) (1 ) d d 1 Both ar nonlmntary provd in sction 1.5, sub-cas-i and sction 1.1, sub-cas-i rspctivly. Sub-cas-II: For φ()= +b+c, w hav from (1.1.1) d 1 d 1 [ '()] (1 ) 4 (sch k) (1 ) 1 F[,, 1,sch ]d It can now b provd nonlmntary by strong Liouvill thorm part (b). Similarly w can prov it for highr dgr polynomial φ(). Lt us considr som ampls on this standard form of nonlmntary functions: a b Eampl 1: Show that th intgral d, a 0 is nonlmntary. Proof: W hav a b a b d d d Now for scond intgral, putting a = w hav b log a a a d a a 1 1 1 d d d a which is nonlmntary from ampl-5 du to Marchisotto t al [5, pp.301]. Eampl : Show that th intgral Proof: W hav sin d cos sin sin cos d cos cos d is nonlmntary. d (1 ) On putting sin=. Which is nonlmntary, provd in sction 1.1, sub-cas-i. cos Eampl 3: Show that th intgral d is nonlmntary. sin 11

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) Proof: W hav cos cos ( sin ) d sin ( sin ) d On putting cos=. Which is nonlmntary provd in sction 1.1, sub-cas-i. d (1 ) Eampl 4: Show that th intgral sc tan d is nonlmntary. Proof: W hav, on putting tan= tan 1 d 1 d d d sc (1 ) 4 (i)(1 i) 4 (i)(1 i) (A) W hav on putting 1-i = p in th first intgral of (A) ip ip ip d i dp dp dp i (i)(1 i) (1 p) p p.. (B) whr th scond and third intgrals ar nonlmntary from ampl-5 du to Marchisotto t al [5, pp.301]. Now putting 1-p=X in th first intgral of (B) w hav ip ix dp i dx (1 p) X which is also nonlmntary from ampl-5 du to Marchisotto t al [5, pp.301]. Thrfor th first intgral of (A) is nonlmntary. Similarly w can prov that th scond intgral of (A) is also nonlmntary. Thrfor th givn function is nonlmntary. sinh Eampl 5: Show that th intgral d is nonlmntary. cosh Proof: W hav on putting sinh= sinh d cosh (1 ) Which is nonlmntary provd in sction 1.3, sub-cas-i. cot Eampl 6: Show that th intgral d is nonlmntary. cosc Proof: W hav on putting =cot cot d Which is nonlmntary provd in sction 1.3, sub-cas-i. d cosc (1 ) d 1

Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) sc Eampl 7: Show that th intgral d sc.tan is nonlmntary. Proof: W hav on putting sc= sc d sc.tan ( 1) d d d ( 1) Which ar nonlmntary, provd in sction 1.5, sub-cas-i. cosc Eampl 8: Show that th intgral d is nonlmntary. cos c.cot Proof: W hav on putting cosc=, cosc d cos c.cot ( 1) Which is nonlmntary, provd in sction 1.5, sub-cas-i. d d d ( 1) sin Eampl 9: Show that th intgral d sin is nonlmntary. Proof: W hav on putting sin =, sin 1 d d sin 4 (1 ) 1 d d 4 (1 ) Whr Now sinc Whr and d is nonlmntary from ampl-5 du to Marchisotto t al [5, pp.301]. 1 d 1 d d (1 ) (1 ) (1 ) I p d dp (1 ), on putting 1-=p, which is nonlmntary p d 1 p dp on putting 1+=p, which is also nonlmntary (1 ) p from ampl-5 du to Marchisotto t al [5, pp.301]. Hnc th givn function is nonlmntary. sin Eampl 10: Show that th intgral.cos d is nonlmntary. 13

[ Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) Proof: W hav on putting sin =, sin d d 1.cos 4(1 )sin 1 F,, 1,sin d 1 3 F, y, y, y d dy1 dy dy3 1 1 y 1,, d d y 1 d 1 y Applying strong Liouvill thorm, part(b), it is lmntary if and only if thr ists an idntity of th form, containing U i a function of, y 1, y, and y 3 as n duo U' i Ci 1 i1 i d U (1 )sin Taking diffrnt possibl forms of U j w find that no such U j ist. Hnc th givn function is nonlmntary. Rfrncs [1]. Hardy G. H., Th Intgration of Functions of a Singl Variabl, nd Ed., Cambridg Univrsity Prss, London, Rprint 198, 1916 []. Ritt J. F., Intgration in Finit Trms: Liouvill s Thory of Elmntary Mthods, Columbia Univrsity Prss, Nw York, 1948 [3]. Risch R. H., Th Problm of Intgration in Finit Trms, Transactions of th Amrican Mathmatical Socity, 139, 167-189, 1969 [4]. Rosnlicht M., Intgration in Finit Trms, Th Amrican Mathmatical Monthly, 79:9, 963-97, 197 [5]. Marchisotto E. A. & Zakri G. A., An Invitation to Intgration in Finit Trms, Th Collg Mathmatics Journal, Mathmatical Association of Amrica, 5:4, 95-308, 1994 [6]. Yadav D. K. & Sn D. K., Rvisd papr on Indfinit Nonintgrabl Functions, Acta Cincia Indica, 34:3, 1383-1384, 008 14