MATHEMATICS-I. CONTENTS  Ordinary Differential Equations of First Order and First Degree  Linear Differential Equations of Second and Higher Order 

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Presentation transcript:

MATHEMATICS-I

CONTENTS  Ordinary Differential Equations of First Order and First Degree  Linear Differential Equations of Second and Higher Order  Mean Value Theorems  Functions of Several Variables  Curvature, Evolutes and Envelopes  Curve Tracing  Applications of Integration  Multiple Integrals  Series and Sequences  Vector Differentiation and Vector Operators  Vector Integration  Vector Integral Theorems  Laplace transforms

TEXT BOOKS  A text book of Engineering Mathematics, Vol-I T.K.V.Iyengar, B.Krishna Gandhi and Others, S.Chand & Company  A text book of Engineering Mathematics, C.Sankaraiah, V.G.S.Book Links  A text book of Engineering Mathematics, Shahnaz A Bathul, Right Publishers  A text book of Engineering Mathematics, P.Nageshwara Rao, Y.Narasimhulu & N.Prabhakar Rao, Deepthi Publications

REFERENCES  A text book of Engineering Mathematics, B.V.Raman, Tata Mc Graw Hill  Advanced Engineering Mathematics, Irvin Kreyszig, Wiley India Pvt. Ltd.  A text Book of Engineering Mathematics, Thamson Book collection

UNIT - II LINEAR DIFFERENTIAL EQUATIONS OF SECOND AND HIGHER ORDER

UNIT HEADER Name of the Course: B. Tech Code No:07A1BS02 Year/Branch: I Year CSE,IT,ECE,EEE,ME,CIVIL,AERO Unit No: II No. of slides:18

S. No. ModuleLectureNo. PPT Slide No. 1 Introduction, Complementary function L Particular Integrals L Cauchy’s, Legendre’s linear equations, Variation of Parameters L UNIT INDEX UNIT-II

Lecture-1 INTRODUCTION  An equation of the form D n y + k 1 D n-1 y k n y = X D n y + k 1 D n-1 y k n y = X Where k 1,…..,k n are real constants and X is a continuous function of x is called an ordinary linear equation of order n with constant coefficients. Where k 1,…..,k n are real constants and X is a continuous function of x is called an ordinary linear equation of order n with constant coefficients. Its complete solution is Its complete solution is y = C.F + P.I y = C.F + P.I where C.F is a Complementary Function and where C.F is a Complementary Function and P.I is a Particular Integral. P.I is a Particular Integral.  Example:d 2 y/dx 2 +3dy/dx+4y=sinx

COMPLEMENTARY FUNCTION  If roots are real and distinct then C.F = c 1 e m1x + …+ c k e mkx C.F = c 1 e m1x + …+ c k e mkx  Example 1: Roots of an auxiliary equation are 1,2,3 then C.F = c 1 e x + c 2 e 2x + c 3 e 3x  Example 2: For a differential equation (D-1)(D+1)y=0, roots are -1 and 1. Hence (D-1)(D+1)y=0, roots are -1 and 1. Hence C.F = c 1 e -x +c 2 e x C.F = c 1 e -x +c 2 e x

Lecture-2 COMPLEMENTARY FUNCTION  If roots are real and equal then C.F = (c 1 + c 2 x +….+ c k x k )e mx C.F = (c 1 + c 2 x +….+ c k x k )e mx  Example 1: The roots of a differential equation (D-1) 3 y=0 are 1,1,1. Hence C.F.= (c 1 +c 2 x+c 3 x 2 )e x  Example 2: The roots of a differential equation (D+1) 2 y=0 are -1,-1. Hence C.F=(c 1 +c 2 x)e -x

Lecture-3 COMPLEMENTARY FUNCTION  If two roots are real and equal and rest are real and different then C.F=(c 1 +c 2 x)e m1x +c 3 e m3x +….  Example : The roots of a differential equation (D-2) 2 (D+1)y=0 are 2,2,-1. Hence C.F.=(c 1 +c 2 x)e 2x +c 3 e -X

Lecture-4 COMPLEMENTARY FUNCTION  If roots of Auxiliary equation are complex say p+iq and p-iq then C.F=e px (c 1 cosqx+c 2 sinqx)  Example: The roots of a differential equation (D 2 +1)y=0 are 0+i(1) and 0-i(1). Hence C.F=e 0x (c 1 cosx+c 2 sinx)  =(c 1 cosx+c 2 sinx)

Lecture-5 COMPLEMENTARY FUNCTION  A pair of conjugate complex roots say p+iq and p-iq are repeated twice then C.F=e px ((c 1 +c 2 x)cosqx+(c 3 +c 4 x)sinqx)  Example: The roots of a differential equation (D 2 -D+1) 2 y=0 are ½+i(1.7/2) and ½-i(1.7/2) repeated twice. Hence C.F=e 1/2x (c 1 +c 2 x)cos(1.7/2)x+ (c 3 +c 4 x)sin(1.7/2)x

Lecture-6 PARTICULAR INTEGRAL  When X = e ax put D = a in Particular Integral. If f(a) ≠ 0 then P.I. will be calculated directly. If f(a) = 0 then multiply P.I. by x and differentiate denominator. Again put D = a.Repeat the same process.  Example 1:y″+5y′+6y=e x. Here P.I=e x /12  Example 2:4D 2 y+4Dy-3y=e 2x.Here P.I=e 2x /21

Lecture-7 PARTICULAR INTEGRAL  When X = Sinax or Cosax or Sin(ax+b) or Cos(ax+b) then put D 2 = - a 2 in Particular Integral.  Example 1: D 2 y-3Dy+2y=Cos3x. Here P.I=(9Sin3x+7Cos3x)/130  Example 2: (D 2 +D+1)y=Sin2x. Here P.I= -1/13(2Cos2x+3Sin2x)

Lecture-8 PARTICULAR INTEGRAL  When X = x k or in the form of polynomial then convert f(D) into the form of binomial expansion from which we can obtain Particular Integral.  Example 1: (D 2 +D+1)y=x 3.Here P.I=x 3 -3x 2 +6  Example 2: (D 2 +D)y=x 2 +2x+4. Here P.I=x 3 /3+4x

Lecture-9 PARTICULAR INTEGRAL  When X = e ax v then put D = D+a and take out e ax to the left of f(D). Now using previous methods we can obtain Particular Integral.  Example 1:(D 4 -1)y=e x Cosx. Here P.I=-e x Cosx/5  Example 2: (D 2 -3D+2)y=xe 3x +Sin2x. Here P.I=e 3x /2(x-3/2)+1/20(3Cos2x-Sin2x)

Lecture-10 PARTICULAR INTEGRAL  When X = x.v then P.I = [{x – f " (D)/f(D)}/f(D)]v P.I = [{x – f " (D)/f(D)}/f(D)]v  Example 1: (D 2 +2D+1)y=x Cosx. Here P.I=x/2Sinx+1/2(Cosx-Sinx)  Example 2: (D 2 +3D+2)y=x e x Sinx. Here P.I=e x [x/10(Sinx-Cosx)-1/25Sinx+Cosx/10]

Lecture-11 PARTICULAR INTEGRAL  When X is any other function then Particular Integral can be obtained by resolving 1/f(D) into partial fractions.  Example 1: (D 2 +a 2 )y=Secax. Here P.I=x/a Sinax+Cosax log(Cosax)/a 2

Lecture-12 CAUCHY’S LINEAR EQUATION  Its general form is x n D n y + …. +y = X x n D n y + …. +y = X then to solve this equation put x = e z and convert into ordinary form. then to solve this equation put x = e z and convert into ordinary form.  Example 1: x 2 D 2 y+xDy+y=1  Example 2: x 3 D 3 y+3x 2 D 2 y+2xDy+6y=x 2

Lecture-13 LEGENDRE’S LINEAR EQUATION  Its general form is (ax + b) n D n y +…..+y = X (ax + b) n D n y +…..+y = X then to solve this equation put ax + b = e z and convert into ordinary form. then to solve this equation put ax + b = e z and convert into ordinary form.  Example 1: (x+1) 2 D 2 y-3(x+1)Dy+4y=x 2 +x+1  Example 2: (2x-1) 3 D 3 y+(2x-1)Dy-2y=x

Lecture-14 METHOD OF VARIATION OF PARAMETERS  Its general form is D 2 y + P Dy + Q = R D 2 y + P Dy + Q = R where P, Q, R are real valued functions of x. where P, Q, R are real valued functions of x. Let C.F = C 1 u + C 2 v Let C.F = C 1 u + C 2 v P.I = Au + Bv P.I = Au + Bv  Example 1: (D 2 +1)y=Cosecx. Here A=-x, B=log(Sinx)  Example 2: (D 2 +1)y=Cosx. Here A=Cos2x/4, B=(x+Sin2x)/2