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DEPARTMENT OF MATHEMATI CS [ YEAR OF ESTABLISHMENT – 1997 ] DEPARTMENT OF MATHEMATICS, CVRCE.

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Presentation on theme: "DEPARTMENT OF MATHEMATI CS [ YEAR OF ESTABLISHMENT – 1997 ] DEPARTMENT OF MATHEMATICS, CVRCE."— Presentation transcript:

1 DEPARTMENT OF MATHEMATI CS [ YEAR OF ESTABLISHMENT – 1997 ] DEPARTMENT OF MATHEMATICS, CVRCE

2 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]

3 MATHEMATICS - II DEPARTMENT OF MATHEMATICS, CVRCE FOURIER INTEGRAL [chapter – 10.8] LECTURE :16

4 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

5 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

6 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

7 FROM FOURIER SERIES TO FOURIER INTEGRAL From (1), (2), (3), and (4), we get

8 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

9 FROM FOURIER SERIES TO FOURIER INTEGRAL Set is absolutely integrable.

10 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).

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12 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.

13 EXAMPLE-1: Find the Fourier integral representation of the function The Fourier integral of the given function f(x) is Solution:

14 PROBLEMS ON FOURIER INTEGRAL

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17 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.

18 DIRICHLET’S DISCONTINUOUS FACTOR The above integral is called Dirichlet’s discontinuous factor.

19 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)

20 FOURIER COSINE INTEGRAL

21 The Fourier integral of an even function is also known as Fourier cosine integral.

22 FOURIER SINE INTEGRAL

23 The Fourier integral of an odd function is also known as Fourier sine integral.

24 PROBLEMS INVOLVING FOURIER COSINE AND SINE INTEGRAL The Fourier cosine integral of the given function f(x) is Solution:

25 PROBLEMS INVOLVING FOURIER COSINE AND SINE INTEGRAL

26 The Fourier sine integral of the given function f(x) is

27 Hence the Fourier sine integral of the given function is PROBLEMS INVOLVING FOURIER COSINE AND SINE INTEGRAL

28 LAPLACE INTEGRALS From Example – 2 by Fourier cosine integral representation, we find that (A)

29 LAPLACE INTEGRALS From Example – 2 by Fourier sine integral representation, we find that The integrals (A) and (B) are called as Laplace integrals. (B)

30 SOME MORE PROBLEMS Solution:

31 SOME MORE PROBLEMS

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36 Solution: SOME MORE PROBLEMS

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39 Solution:

40 SOME MORE PROBLEMS

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42 The Fourier cosine integral of the function f(x) is given by SOME MORE PROBLEMS Solution:

43 SOME MORE PROBLEMS

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45 The Fourier cosine integral of f(x) is given by SOME MORE PROBLEMS Solution:

46 Hence from (1) we obtain the required Fourier cosine integral as SOME MORE PROBLEMS

47 The Fourier cosine integral of the given function f(x) is SOME MORE PROBLEMS

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49 Hence the Fourier cosine integral of the given function is

50 The Fourier sine integral of the given function f(x) is SOME MORE PROBLEMS

51 Hence the Fourier sine integral of the given function is

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