Presentation on theme: "DEPARTMENT OF MATHEMATI CS [ YEAR OF ESTABLISHMENT – 1997 ] DEPARTMENT OF MATHEMATICS, CVRCE."— Presentation transcript:
DEPARTMENT OF MATHEMATI CS [ YEAR OF ESTABLISHMENT – 1997 ] DEPARTMENT OF MATHEMATICS, CVRCE
MATHEMATICS - II ● LAPLACE TRANSFORMS ● FOURIER SERIES ● FOURIER TRANSFORMS ● VECTOR DIFFERENTIAL CALCULUS ● VECTOR INTEGRAL CALCULUS ● LINE, DOUBLE, SURFACE, VOLUME INTEGRALS ● BETA AND GAMMA FUNCTIONS FOR BTECH SECOND SEMESTER COURSE [COMMON TO ALL BRANCHES OF ENGINEERING] DEPARTMENT OF MATHEMATICS, CVRCE TEXT BOOK: ADVANCED ENGINEERING MATHEMATICS BY ERWIN KREYSZIG [8 th EDITION]
MATHEMATICS - II DEPARTMENT OF MATHEMATICS, CVRCE FOURIER INTEGRAL [chapter – 10.8] LECTURE :16
DEPARTMENT OF MATHEMATICS, CVRCE LAYOUT OF LECTURE EXISTENCE OF FOURIER INTEGRAL INTRODUCTI ON & MOTIVATION FROM FOURIER SERIES TO FOURIER INTEGRAL APPLICATIONS FOURIER SINE AND COSINE INTEGRALS SOME PROBLEMS
INTRODUCTION & MOTIVATION FOURIER SERIES ARE POWERFUL TOOLS IN TREATING VARIOUS PROBLLEMS INVOLVING PERIODIC FUNCTIONS. HOWEVER, FOURIER SERIES ARE NOT APPLICABLE TO MANY PRACTICAL PROBLEMS SUCH AS A SINGLE PULSE OF AN ELECTRICAL SIGNAL OR MECHANICAL FORCE VIBRATION WHICH INVOLVE NONPERIODIC FUNCTIONS. THIS SHOWS THAT METHOD OF FOURIER SERIES NEEDS TO BE EXTENDED. HERE WE START WITH THE FOURIER SERIES OF AN ARBITRARY PERIODIC FUNCTION f L OF PERIOD 2L AND THEN LET L SO AS TO DEVELOP FOURIER INTEGRAL OF A NON-PERIODIC FUNCTION. Jean Baptiste Joseph Fourier (Mar21st 1768 –May16th 1830) French Mathematician & Physicist
FROM FOURIER SERIES TO FOURIER INTEGRAL Let f L (x) be an arbitrary periodic function whose period is 2L which can be represented by its Fourier series as follows: DEPARTMENT OF MATHEMATICS, CVRCE
FROM FOURIER SERIES TO FOURIER INTEGRAL From (1), (2), (3), and (4), we get
FROM FOURIER SERIES TO FOURIER INTEGRAL The representation (6) is valid for any fixed L, arbitrary large but finite. We now let L and assume that the resultant non-periodic function is absolutely integrable on x-axis, i.e. the resulting non- periodic function
FROM FOURIER SERIES TO FOURIER INTEGRAL Set is absolutely integrable.
Applying (8) and (9) in (7), we get FROM FOURIER SERIES TO FOURIER INTEGRAL Representation (10) with A(w) and B(w) given by (8) and (9), respectively, is called a Fourier integral of f(x).
Theorem If a function f(x) is piecewise continuous in every finite interval and has a right-hand derivative and left-hand derivative at every point and if the integral exists, then f(x) can be represented by a Fourier integral. At a point where f(x) is discontinuous the value of the Fourier integral equals the average of the left and right hand limits of f(x) at that point.
EXAMPLE-1: Find the Fourier integral representation of the function The Fourier integral of the given function f(x) is Solution:
DIRICHLET’S DISCONTINUOUS FACTOR From Example – 1 by Fourier integral representation, we find that At x= 1, the function f(x) is discontinuous. Hence the value of the Fourier integral at 1 is ½ [f(1-0)+f(1+0)] = ½[0+1]=1/2.
DIRICHLET’S DISCONTINUOUS FACTOR The above integral is called Dirichlet’s discontinuous factor.
Sine integral Dirichlet’s discontinuous factor is given by. Putting x= 0 in the above expression we get. The integral (1) is the limit of the integral as u The integral is called the sine integral and it is denoted by Si(u)