SATHYABAMA UNIVERSITY
|
|
- Darren Bridges
- 6 years ago
- Views:
Transcription
1 DEPARTMENT OF MATHEMATICS ENGINEERING MATHEMATICS IV (SMTX ) SATHYABAMA UNIVERSITY DEPARTMENT OF MATHEMATICS Engineering Mathematics-IV (SMTX) Question Bank UNIT I. What is the value of b n when the function f()= epanded as a Fourier series in (-π, π)?. State Dirichlet conditions for a function to be epanded as a Fourier series.. If f() = sin in -π π, find a n 4. Write the comple form of Fourier series of f() in <<l. 5. Find the Fourier cosine series for the function f()=k, <<π 6. State parseval s identity on Fourier series 7. If f() = c e in n is the comple form of the Fourier series corresponding to f() in (,π ), Write the formula for C n. 8. Write the formulas for finding the Euler s constants in the Fourier series epansion of f() in (-π, π). 9. Find the root mean square value of the function f() = in the interval (,).. Define Harmonic analysis.. Obtain the Fourier Series for f ( ) = + in (-π, π). Deduce that π =. 6. Epand the function f( ) = sin as a Fourier series in the interval π.. Epress f() = in half range cosine series in the range < < and deduce the value of to Obtain the Fourier series of f ( ) = cos in -π π 5. (a) Find the comple form of Fourier series for f() = e -a in the interval.
2 DEPARTMENT OF MATHEMATICS ENGINEERING MATHEMATICS IV (SMTX ) (b) Epand f() =, < < as a half range sine series. 6. Find the Fourier series epansion of the periodic function f() of period, defined by +, < f()= Deduce, that π = (n ) 8 7. Obtain Fourier series for f()= ( i ) + 5 π +... = 7 8 l,, ( ii) + < l l l + 5. Hence deduce that +... = 8. Compute the first two harmonics of the Fourier series of f() given by the following table. π π π 4π 5π π f() π 8 9. Find the Fourier series of f() = in π π and deduce = π / 6 n. Obtain the first two harmonics in the Fourier series epansion in (,6) for the function y = f() defined by the table given below. X 4 5 Y UNIT II. Form the partial differential equation from z = (-a) + (y-b) + by eliminating a and b.. Find the partial differential equation by eliminating arbitrary constants a & b. from z = (+a)(y+b). Write the complete integral for the partial differential equation z = p +qy +pq. 4. Find the complete solution of z = p + qy + p q 5. Form the p.d.e by eliminating the arbitrary function from z = f( + y ). 6. Find the particular integral of ( D - 6DD +9D )z = cos (+y). 7. Solve ( D 4 D 4 )z =. 8. Find the particular integral of (D DD )z = sincosy. 9. Find the complete integral of p + q = pq. D DD + D z =. Solve ( ).
3 DEPARTMENT OF MATHEMATICS ENGINEERING MATHEMATICS IV (SMTX ). Find the singular integral of the PDE z = p + qy + p - q.. Form the partial differential equation by eliminating the arbitrary functions f and g in z = f( + y) + g(-y). Solve( D + DD D )z = e + y + sin(+y). 4. Solve : ( -yz)p + (y - z) q = z y. 5. Solve : (y +z )p + y( z + )q = z(y ). 6. Solve (D 6DD + 5D )z = e sinhy. 7. Solve (mz ny) p + (n lz) q = ly m. 8. Solve (D + 4DD 5D )z = + y + π. 9. Solve z + z y 6 z y = y cos.. Find the general solution of (z y ) p + y ( z )q = z(y ) UNIT III. The steady state temperature distribution is considered in a square plate with sides =, y =, = a and y = a. The edge y = is kept at a constant temperature T and the other three edges are insulated. The same state is continued subsequently. Epress the problem mathematically.. State any two laws which are assumed to derive one dimensional heat equation. State two-dimensional Laplace equation. u u 4. How many boundary conditions are required to solve completely = α t 5. What is meant by Steady state condition in heat flow? 6. An insulated rod of length cm has its end A and B maintained at o C and o C respectively and the rod is in steady state condition. Find the temperature at any point in terms of its distance from one end.
4 DEPARTMENT OF MATHEMATICS ENGINEERING MATHEMATICS IV (SMTX ) 7. A bar cm long with insulated sides has its ends kept at 4 C and C until steady state conditions prevail. Find the initial temperature distribution in the bar. 8. A tightly stretched string with fied end points = and = l is initially in a position given by y(, ) = f(). If the string is released from rest, write down the most general solution of the vibrating motion of the string. 9. A bar cm long with insulated sides has its ends kept at C and 6 C until steady state conditions prevail. Write the initial and boundary conditions of one dimensional heat equation.. Write down various solutions of the one dimensional wave equation.. A taut string of length L is fastened at both ends. The midpoint of the string is taken to a height of b and then released from rest in this position. Find the displacement of the string at any time t.. A tightly stretched string with fied end points = and = l is initially in a position given by y (, ) = V o sin (π/l). If it is released from rest from this position. Find the displacement y at any distance from one end at any time t.. A string AB of length l tightly stretched between A and B is initially at rest in the equilibrium position. If each point of the string is suddenly given a velocity λ( l ) find the transverse displacement of the string at subsequent time t. 4. If a string of length l is initially at rest in equilibrium position and each point of it is given y the velocity sin π = V, < < l. determine the transverse t (,) l displacement y(,t). 5. The end A and B of a bar of length l maintained at o C and o C respectively until steady state conditions prevail. If the temperature at B is reduced suddenly to o C and kept so. Find the temperature u(, t) at a distance from A and at time t. 6. The two long edges y = and y = l of a long rectangular plate are insulated. If the temperature in the short edge at infinity is kept at o C, while that in the short edge = is kept at ky(l y), find the steady-state temperature distribution in the plate. 7. A rod of length cms has its ends A and B kept at C and 8 C respectively until steady state conditions prevail. The temperature at each end is then suddenly reduced to C and kept so. Find the resulting temperature function u(,t). 8. A square plate bounded by the lines =, y=,y= are kept at constant temperature c whereas the net edge = is kept at c. Find the distribution over the plate. 4
5 DEPARTMENT OF MATHEMATICS ENGINEERING MATHEMATICS IV (SMTX ) 9. A rod of length cms has its ends A and B kept at C and 8 C respectively until steady state conditions prevail. The temperature at end A is then suddenly increased to 6 C and at end B decreased to 6 C. Find the subsequent temperature function u(,t).. Find the Steady state temperature at any point of a square plate whose two adjacent edges are kept at C and and the other two edges are kept at the constant temperature C UNIT IV. State Parseval s identity for Fourier transforms. Find finite fourier sine transform of f() = K in (,). If F(s) is the Fourier transform of f(), write the Fourier transform of f()sin a in terms of F.T 4. If F(s) = F(f()) then show that F(f ()) = -is F(s). 5. Find the Fourier sine transform of e -a. 6. State the shifting property on Fourier transforms. 7. Find the Fourier transform of f() if, < a f() =, > a > s F f ( a) = F a a d 9. Prove that Fs[ f ( )] = Fc[ f ( )] ds. State Convolution Theorem. 8. Prove that { } ) Find the Fourier transform of hence deduce that, ( ) =, f and > sin t sin t ( i ) d ( ii) d t t 4 ) Find the Fourier transform of a, f ( ) =, a > a and Hence deduce that i t t t sin cos t t t dt ii dt t t sin cos ( ) ( ) 5
6 DEPARTMENT OF MATHEMATICS ENGINEERING MATHEMATICS IV (SMTX ) ) Find the Fourier sine transform of e -a and hence evaluate 4) Find the Fourier cosine transform of transform of a e. a e sin s d + and hence evaluate the fourier sine 5) Using Parseval s identity on Fourier transform evaluate d & ( + ) a ( + a ) d 6) Find the Fourier transform of e a, a>. For what value of a the given function is self reciprocal s and hence show that F e = e 7) Find F c and + a F s a + 8) State and prove Parseval s identity on Fourier transform. 9) State the prove convolution theorem on Fourier transform. ) Evaluate d ( + a )( + b ) using Fourier cosine transforms. If F (z) = ( z )( z z )( 4 z ) 4 UNIT V, find f (). a n for n. Find the Z-transform of (n) = n! otherwise. Define Z-Transforms. 4. Find Z[a n n]. 5. Find the Z- transform of na n u(n). 6. Find Z[e at+b ]. 6
7 DEPARTMENT OF MATHEMATICS ENGINEERING MATHEMATICS IV (SMTX ) 7. Find Z[a n- ]. 8. Prove that Z[f(n+)] = z[f(z) f()] df( z) 9. Prove that z[ nf ( n)] = z dz. Define Convolution of two sequences. n. Solve the equation u u + 9u = given u = n n+ n u =. Using convolution theorem find z Z ( z 4)( z ) z z. Find the inverse Z-transform of ( z ) ( z 4) 4. State and prove convolution theorem on Z-transforms. 9z 5. Find Z by using residue method. (z ) ( z ) 6. Find Z[a n r n cosnθ ] and Z[a n r n sinnθ ] z 7. Prove that z = z log ( n+ ) z 8. Find z z z+ when < z < ( z ) ( z ) 9. Using Z-transform solve the equation yn + + 4yn+ 5yn = 4n 8, given y()= and y() = -5. z. Find the inverse Z-transform of z z+ 7
8 DEPARTMENT OF MATHEMATICS ENGINEERING MATHEMATICS IV (SMTX ) 8
VALLIAMMAI ENGINEERING COLLEGE SRM Nagar, Kattankulathur DEPARTMENT OF MATHEMATICS QUESTION BANK
SUBJECT VALLIAMMAI ENGINEERING COLLEGE SRM Nagar, Kattankulathur 63 3. DEPARTMENT OF MATHEMATICS QUESTION BANK : MA6351- TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS SEM / YEAR : III Sem / II year (COMMON
More informationName of the Student: Fourier Series in the interval (0,2l)
Engineering Mathematics 15 SUBJECT NAME : Transforms and Partial Diff. Eqn. SUBJECT CODE : MA11 MATERIAL NAME : University Questions REGULATION : R8 WEBSITE : www.hariganesh.com UPDATED ON : May-June 15
More informationBranch: Name of the Student: Unit I (Fourier Series) Fourier Series in the interval (0,2 l) Engineering Mathematics Material SUBJECT NAME
13 SUBJECT NAME SUBJECT CODE MATERIAL NAME MATERIAL CODE UPDATED ON : Transforms and Partial Differential Equation : MA11 : University Questions :SKMA13 : May June 13 Name of the Student: Branch: Unit
More informationMA6351-TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS. Question Bank. Department of Mathematics FATIMA MICHAEL COLLEGE OF ENGINEERING & TECHNOLOGY
MA6351-TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS Question Bank Department of Mathematics FATIMA MICHAEL COLLEGE OF ENGINEERING & TECHNOLOGY MADURAI 625 020, Tamilnadu, India 1. Define PDE and Order
More informationCODE: GR17A1003 GR 17 SET - 1
SET - 1 I B. Tech II Semester Regular Examinations, May 18 Transform Calculus and Fourier Series (Common to all branches) Time: 3 hours Max Marks: 7 PART A Answer ALL questions. All questions carry equal
More informationB.E./B.TECH. DEGREE EXAMINATION, CHENNAI-APRIL/MAY TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS(COMMON TO ALL BRANCHES)
B.E./B.TECH. DEGREE EXAMINATION, CHENNAI-APRIL/MAY 2010. TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS(COMMON TO ALL BRANCHES) 1. Write the conditions for a function to satisfy for the existence of a Fourier
More information[Engineering Mathematics]
[MATHS IV] [Engineering Mathematics] [Partial Differential Equations] [Partial Differentiation and formation of Partial Differential Equations has already been covered in Maths II syllabus. Present chapter
More informationPartial Differential Equations
++++++++++ Partial Differential Equations Previous year Questions from 017 to 199 Ramanasri Institute 017 W E B S I T E : M A T H E M A T I C S O P T I O N A L. C O M C O N T A C T : 8 7 5 0 7 0 6 6 /
More information3150 Review Problems for Final Exam. (1) Find the Fourier series of the 2π-periodic function whose values are given on [0, 2π) by cos(x) 0 x π f(x) =
350 Review Problems for Final Eam () Find the Fourier series of the 2π-periodic function whose values are given on [0, 2π) by cos() 0 π f() = 0 π < < 2π (2) Let F and G be arbitrary differentiable functions
More informationFOURIER TRANSFORMS. At, is sometimes taken as 0.5 or it may not have any specific value. Shifting at
Chapter 2 FOURIER TRANSFORMS 2.1 Introduction The Fourier series expresses any periodic function into a sum of sinusoids. The Fourier transform is the extension of this idea to non-periodic functions by
More informationBabu Banarasi Das Northern India Institute of Technology, Lucknow
Babu Banarasi Das Northern India Institute of Technology, Lucknow B.Tech Second Semester Academic Session: 2012-13 Question Bank Maths II (EAS -203) Unit I: Ordinary Differential Equation 1-If dy/dx +
More informationMathematical Modeling using Partial Differential Equations (PDE s)
Mathematical Modeling using Partial Differential Equations (PDE s) 145. Physical Models: heat conduction, vibration. 146. Mathematical Models: why build them. The solution to the mathematical model will
More informationPartial Differential Equations
++++++++++ Partial Differential Equations Previous ear Questions from 016 to 199 Ramanasri 017 S H O P NO- 4, 1 S T F L O O R, N E A R R A P I D F L O U R M I L L S, O L D R A J E N D E R N A G A R, N
More informationFOURIER SERIES, TRANSFORMS, AND BOUNDARY VALUE PROBLEMS
fc FOURIER SERIES, TRANSFORMS, AND BOUNDARY VALUE PROBLEMS Second Edition J. RAY HANNA Professor Emeritus University of Wyoming Laramie, Wyoming JOHN H. ROWLAND Department of Mathematics and Department
More informationBoundary-value Problems in Rectangular Coordinates
Boundary-value Problems in Rectangular Coordinates 2009 Outline Separation of Variables: Heat Equation on a Slab Separation of Variables: Vibrating String Separation of Variables: Laplace Equation Review
More information: Transforms and Partial Differential Equations
Trasforms ad Partial Differetial Equatios 018 SUBJECT NAME : Trasforms ad Partial Differetial Equatios SUBJECT CODE : MA 6351 MATERIAL NAME : Part A questios REGULATION : R013 WEBSITE : wwwharigaeshcom
More informationMATH 131P: PRACTICE FINAL SOLUTIONS DECEMBER 12, 2012
MATH 3P: PRACTICE FINAL SOLUTIONS DECEMBER, This is a closed ook, closed notes, no calculators/computers exam. There are 6 prolems. Write your solutions to Prolems -3 in lue ook #, and your solutions to
More information25.2. Applications of PDEs. Introduction. Prerequisites. Learning Outcomes
Applications of PDEs 25.2 Introduction In this Section we discuss briefly some of the most important PDEs that arise in various branches of science and engineering. We shall see that some equations can
More informationPractice Problems For Test 3
Practice Problems For Test 3 Power Series Preliminary Material. Find the interval of convergence of the following. Be sure to determine the convergence at the endpoints. (a) ( ) k (x ) k (x 3) k= k (b)
More informationPractice Problems For Test 3
Practice Problems For Test 3 Power Series Preliminary Material. Find the interval of convergence of the following. Be sure to determine the convergence at the endpoints. (a) ( ) k (x ) k (x 3) k= k (b)
More informationGATE EE Topic wise Questions SIGNALS & SYSTEMS
www.gatehelp.com GATE EE Topic wise Questions YEAR 010 ONE MARK Question. 1 For the system /( s + 1), the approximate time taken for a step response to reach 98% of the final value is (A) 1 s (B) s (C)
More informationM445: Heat equation with sources
M5: Heat equation with sources David Gurarie I. On Fourier and Newton s cooling laws The Newton s law claims the temperature rate to be proportional to the di erence: d dt T = (T T ) () The Fourier law
More informationPARTIAL DIFFERENTIAL EQUATIONS and BOUNDARY VALUE PROBLEMS
PARTIAL DIFFERENTIAL EQUATIONS and BOUNDARY VALUE PROBLEMS NAKHLE H. ASMAR University of Missouri PRENTICE HALL, Upper Saddle River, New Jersey 07458 Contents Preface vii A Preview of Applications and
More informationLecture 11: Fourier Cosine Series
Introductory lecture notes on Partial Differential Equations - c Anthony Peirce Not to be copied, used, or revised without eplicit written permission from the copyright owner ecture : Fourier Cosine Series
More informationMath 251 December 14, 2005 Final Exam. 1 18pt 2 16pt 3 12pt 4 14pt 5 12pt 6 14pt 7 14pt 8 16pt 9 20pt 10 14pt Total 150pt
Math 251 December 14, 2005 Final Exam Name Section There are 10 questions on this exam. Many of them have multiple parts. The point value of each question is indicated either at the beginning of each question
More informationReview of Fourier Transform
Review of Fourier Transform Fourier series works for periodic signals only. What s about aperiodic signals? This is very large & important class of signals Aperiodic signal can be considered as periodic
More informationClassification of partial differential equations and their solution characteristics
9 TH INDO GERMAN WINTER ACADEMY 2010 Classification of partial differential equations and their solution characteristics By Ankita Bhutani IIT Roorkee Tutors: Prof. V. Buwa Prof. S. V. R. Rao Prof. U.
More information1. Partial differential equations. Chapter 12: Partial Differential Equations. Examples. 2. The one-dimensional wave equation
1. Partial differential equations Definitions Examples A partial differential equation PDE is an equation giving a relation between a function of two or more variables u and its partial derivatives. The
More informationMcGill University April 20, Advanced Calculus for Engineers
McGill University April 0, 016 Faculty of Science Final examination Advanced Calculus for Engineers Math 64 April 0, 016 Time: PM-5PM Examiner: Prof. R. Choksi Associate Examiner: Prof. A. Hundemer Student
More informationx y x 2 2 x y x x y x U x y x y
Lecture 7 Appendi B: Some sample problems from Boas Here are some solutions to the sample problems assigned for hapter 4 4: 8 Solution: We want to learn about the analyticity properties of the function
More informationFourier Analysis Fourier Series C H A P T E R 1 1
C H A P T E R Fourier Analysis 474 This chapter on Fourier analysis covers three broad areas: Fourier series in Secs...4, more general orthonormal series called Sturm iouville epansions in Secs..5 and.6
More informationName of the Student:
SUBJECT NAME : Trasforms ad Partial Diff Eq SUBJECT CODE : MA MATERIAL NAME : Problem Material MATERIAL CODE : JM8AM6 REGULATION : R8 UPDATED ON : April-May 4 (Sca the above QR code for the direct dowload
More informationHomework 7 Solutions
Homework 7 Solutions # (Section.4: The following functions are defined on an interval of length. Sketch the even and odd etensions of each function over the interval [, ]. (a f( =, f ( Even etension of
More informationDynamics of structures
Dynamics of structures 2.Vibrations: single degree of freedom system Arnaud Deraemaeker (aderaema@ulb.ac.be) 1 One degree of freedom systems in real life 2 1 Reduction of a system to a one dof system Example
More informationCHAPTER 4. Introduction to the. Heat Conduction Model
A SERIES OF CLASS NOTES FOR 005-006 TO INTRODUCE LINEAR AND NONLINEAR PROBLEMS TO ENGINEERS, SCIENTISTS, AND APPLIED MATHEMATICIANS DE CLASS NOTES 4 A COLLECTION OF HANDOUTS ON PARTIAL DIFFERENTIAL EQUATIONS
More informationLecture6. Partial Differential Equations
EP219 ecture notes - prepared by- Assoc. Prof. Dr. Eser OĞAR 2012-Spring ecture6. Partial Differential Equations 6.1 Review of Differential Equation We have studied the theoretical aspects of the solution
More informationQUESTION BANK SIGNALS AND SYSTEMS (4 th SEM ECE)
QUESTION BANK SIGNALS AND SYSTEMS (4 th SEM ECE) 1. For the signal shown in Fig. 1, find x(2t + 3). i. Fig. 1 2. What is the classification of the systems? 3. What are the Dirichlet s conditions of Fourier
More informationMATH 251 Final Examination August 14, 2015 FORM A. Name: Student Number: Section:
MATH 251 Final Examination August 14, 2015 FORM A Name: Student Number: Section: This exam has 11 questions for a total of 150 points. Show all your work! In order to obtain full credit for partial credit
More informationChapter 10: Partial Differential Equations
1.1: Introduction Chapter 1: Partial Differential Equations Definition: A differential equations whose dependent variable varies with respect to more than one independent variable is called a partial differential
More informationUsing the TI-92+ : examples
Using the TI-9+ : eamples Michel Beaudin École de technologie supérieure 1100, rue Notre-Dame Ouest Montréal (Québec) Canada, H3C 1K3 mbeaudin@seg.etsmtl.ca 1- Introduction We incorporated the use of the
More informationF = m a. t 2. stress = k(x) strain
The Wave Equation Consider a bar made of an elastic material. The bar hangs down vertically from an attachment point = and can vibrate vertically but not horizontally. Since chapter 5 is the chapter on
More informationMath Assignment 14
Math 2280 - Assignment 14 Dylan Zwick Spring 2014 Section 9.5-1, 3, 5, 7, 9 Section 9.6-1, 3, 5, 7, 14 Section 9.7-1, 2, 3, 4 1 Section 9.5 - Heat Conduction and Separation of Variables 9.5.1 - Solve the
More informationMATH 251 Final Examination December 19, 2012 FORM A. Name: Student Number: Section:
MATH 251 Final Examination December 19, 2012 FORM A Name: Student Number: Section: This exam has 17 questions for a total of 150 points. In order to obtain full credit for partial credit problems, all
More informationDEPARTMENT OF MATHEMATICS FACULTY OF ENGINERING AND TECHNOLOGY SRM UNIVERSITY MA0211- MATHEMATICS III SEMESTER III ACADEMIC YEAR:
DEPARTMENT OF MATHEMATICS FACULTY OF ENGINERING AND TECHNOLOGY SRM UNIVERSITY MA0211- MATHEMATICS III SEMESTER III ACADEMIC YEAR: 2011 2012 LECTURE SCHEME / PLAN The objective is to equip the students
More information12.7 Heat Equation: Modeling Very Long Bars.
568 CHAP. Partial Differential Equations (PDEs).7 Heat Equation: Modeling Very Long Bars. Solution by Fourier Integrals and Transforms Our discussion of the heat equation () u t c u x in the last section
More informationVibrating Strings and Heat Flow
Vibrating Strings and Heat Flow Consider an infinite vibrating string Assume that the -ais is the equilibrium position of the string and that the tension in the string at rest in equilibrium is τ Let u(,
More informationMath 251 December 14, 2005 Answer Key to Final Exam. 1 18pt 2 16pt 3 12pt 4 14pt 5 12pt 6 14pt 7 14pt 8 16pt 9 20pt 10 14pt Total 150pt
Name Section Math 51 December 14, 5 Answer Key to Final Exam There are 1 questions on this exam. Many of them have multiple parts. The point value of each question is indicated either at the beginning
More informationHomework for Math , Fall 2016
Homework for Math 5440 1, Fall 2016 A. Treibergs, Instructor November 22, 2016 Our text is by Walter A. Strauss, Introduction to Partial Differential Equations 2nd ed., Wiley, 2007. Please read the relevant
More informationB.Tech. Theory Examination (Semester IV) Engineering Mathematics III
Solved Question Paper 5-6 B.Tech. Theory Eamination (Semester IV) 5-6 Engineering Mathematics III Time : hours] [Maimum Marks : Section-A. Attempt all questions of this section. Each question carry equal
More informationChapter 12 Partial Differential Equations
Chapter 12 Partial Differential Equations Advanced Engineering Mathematics Wei-Ta Chu National Chung Cheng University wtchu@cs.ccu.edu.tw 1 2 12.1 Basic Concepts of PDEs Partial Differential Equation A
More informationSolutions to Assignment 7
MTHE 237 Fall 215 Solutions to Assignment 7 Problem 1 Show that the Laplace transform of cos(αt) satisfies L{cosαt = s s 2 +α 2 L(cos αt) e st cos(αt)dt A s α e st sin(αt)dt e stsin(αt) α { e stsin(αt)
More informationPDE and Boundary-Value Problems Winter Term 2014/2015
PDE and Boundary-Value Problems Winter Term 2014/2015 Lecture 12 Saarland University 15. Dezember 2014 c Daria Apushkinskaya (UdS) PDE and BVP lecture 12 15. Dezember 2014 1 / 24 Purpose of Lesson To introduce
More informationSAMPLE FINAL EXAM SOLUTIONS
LAST (family) NAME: FIRST (given) NAME: ID # : MATHEMATICS 3FF3 McMaster University Final Examination Day Class Duration of Examination: 3 hours Dr. J.-P. Gabardo THIS EXAMINATION PAPER INCLUDES 22 PAGES
More informationENGI 9420 Lecture Notes 8 - PDEs Page 8.01
ENGI 940 Lecture Notes 8 - PDEs Page 8.01 8. Partial Differential Equations Partial differential equations (PDEs) are equations involving functions of more than one variable and their partial derivatives
More information(I understand that cheating is a serious offense)
TITLE PAGE NAME: (Print in ink) STUDENT NUMBER: SEAT NUMBER: SIGNATURE: (in ink) (I understand that cheating is a serious offense) INSTRUCTIONS TO STUDENTS: This is a 3 hour exam. Please show your work
More informationf (t) K(t, u) d t. f (t) K 1 (t, u) d u. Integral Transform Inverse Fourier Transform
Integral Transforms Massoud Malek An integral transform maps an equation from its original domain into another domain, where it might be manipulated and solved much more easily than in the original domain.
More informationCHEE 319 Tutorial 3 Solutions. 1. Using partial fraction expansions, find the causal function f whose Laplace transform. F (s) F (s) = C 1 s + C 2
CHEE 39 Tutorial 3 Solutions. Using partial fraction expansions, find the causal function f whose Laplace transform is given by: F (s) 0 f(t)e st dt (.) F (s) = s(s+) ; Solution: Note that the polynomial
More informationThe method to find a basis of Euler-Cauchy equation by transforms
Global Journal of Pure and Applied Mathematics. ISSN 0973-1768 Volume 12, Number 5 (2016), pp. 4159 4165 Research India Publications http://www.ripublication.com/gjpam.htm The method to find a basis of
More informationLaplace Transforms and use in Automatic Control
Laplace Transforms and use in Automatic Control P.S. Gandhi Mechanical Engineering IIT Bombay Acknowledgements: P.Santosh Krishna, SYSCON Recap Fourier series Fourier transform: aperiodic Convolution integral
More informationMath 2930 Worksheet Final Exam Review
Math 293 Worksheet Final Exam Review Week 14 November 3th, 217 Question 1. (* Solve the initial value problem y y = 2xe x, y( = 1 Question 2. (* Consider the differential equation: y = y y 3. (a Find the
More informationFigure 5.16 Compound pendulum: (a) At rest in equilibrium, (b) General position with coordinate θ, Freebody
Lecture 27. THE COMPOUND PENDULUM Figure 5.16 Compound pendulum: (a) At rest in equilibrium, (b) General position with coordinate θ, Freebody diagram The term compound is used to distinguish the present
More informationCHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION. Professor Dae Ryook Yang
CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dept. of Chemical and Biological Engineering 5-1 Road Map of the Lecture V Laplace Transform and Transfer
More information3.2 Complex Sinusoids and Frequency Response of LTI Systems
3. Introduction. A signal can be represented as a weighted superposition of complex sinusoids. x(t) or x[n]. LTI system: LTI System Output = A weighted superposition of the system response to each complex
More informationLECTURE 12 Sections Introduction to the Fourier series of periodic signals
Signals and Systems I Wednesday, February 11, 29 LECURE 12 Sections 3.1-3.3 Introduction to the Fourier series of periodic signals Chapter 3: Fourier Series of periodic signals 3. Introduction 3.1 Historical
More informationProperties of Fourier Cosine and Sine Transforms
International Journal of Sciences: Basic and Applied Research (IJSBAR) ISSN 237-4531 (Print & Online) http://gssrr.org/index.php?journal=journalofbasicandapplied ---------------------------------------------------------------------------------------------------------------------------
More informationTyn Myint-U Lokenath Debnath. Linear Partial Differential Equations for Scientists and Engineers. Fourth Edition. Birkhauser Boston Basel Berlin
Tyn Myint-U Lokenath Debnath Linear Partial Differential Equations for Scientists and Engineers Fourth Edition Birkhauser Boston Basel Berlin Preface to the Fourth Edition Preface to the Third Edition
More informationClassification of Phase Portraits at Equilibria for u (t) = f( u(t))
Classification of Phase Portraits at Equilibria for u t = f ut Transfer of Local Linearized Phase Portrait Transfer of Local Linearized Stability How to Classify Linear Equilibria Justification of the
More informationTRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS TWO MARKS Q & A APPLICATIONS OF PARTIAL DIFFERENTIAL Z-TRANSFORMS AND DIFFERENCE EQUATIONS
TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS TWO MARKS Q & A UNIT-I UNIT-II UNIT-III UNIT-IV FOURIER SERIES FOURIER TRANSFORM PARTIAL DIFFERENTIAL EQUATIONS APPLICATIONS OF PARTIAL DIFFERENTIAL EQUATIONS
More informationSeismic Waves Propagation in Complex Media
H4.SMR/1586-1 "7th Workshop on Three-Dimensional Modelling of Seismic Waves Generation and their Propagation" 5 October - 5 November 004 Seismic Waves Propagation in Comple Media Fabio ROMANELLI Dept.
More informationPartial Differential Equations
Partial Differential Equations Xu Chen Assistant Professor United Technologies Engineering Build, Rm. 382 Department of Mechanical Engineering University of Connecticut xchen@engr.uconn.edu Contents 1
More informationSteady and unsteady diffusion
Chapter 5 Steady and unsteady diffusion In this chapter, we solve the diffusion and forced convection equations, in which it is necessary to evaluate the temperature or concentration fields when the velocity
More informationMathematical Methods and its Applications (Solution of assignment-12) Solution 1 From the definition of Fourier transforms, we have.
For 2 weeks course only Mathematical Methods and its Applications (Solution of assignment-2 Solution From the definition of Fourier transforms, we have F e at2 e at2 e it dt e at2 +(it/a dt ( setting (
More informationTopic 3: Fourier Series (FS)
ELEC264: Signals And Systems Topic 3: Fourier Series (FS) o o o o Introduction to frequency analysis of signals CT FS Fourier series of CT periodic signals Signal Symmetry and CT Fourier Series Properties
More informationMATH 251 Final Examination August 10, 2011 FORM A. Name: Student Number: Section:
MATH 251 Final Examination August 10, 2011 FORM A Name: Student Number: Section: This exam has 10 questions for a total of 150 points. In order to obtain full credit for partial credit problems, all work
More informationFOURIER SERIES. Chapter Introduction
Chapter 1 FOURIER SERIES 1.1 Introduction Fourier series introduced by a French physicist Joseph Fourier (1768-1830), is a mathematical tool that converts some specific periodic signals into everlasting
More informationRepresenting a Signal
The Fourier Series Representing a Signal The convolution method for finding the response of a system to an excitation takes advantage of the linearity and timeinvariance of the system and represents the
More informationFourier Series and Transforms. Revision Lecture
E. (5-6) : / 3 Periodic signals can be written as a sum of sine and cosine waves: u(t) u(t) = a + n= (a ncosπnft+b n sinπnft) T = + T/3 T/ T +.65sin(πFt) -.6sin(πFt) +.6sin(πFt) + -.3cos(πFt) + T/ Fundamental
More informationTHE METHOD OF SEPARATION OF VARIABLES
THE METHOD OF SEPARATION OF VARIABES To solve the BVPs that we have encountered so far, we will use separation of variables on the homogeneous part of the BVP. This separation of variables leads to problems
More informationThe Variants of Energy Integral Induced by the Vibrating String
Applied Mathematical Sciences, Vol. 9, 15, no. 34, 1655-1661 HIKARI td, www.m-hikari.com http://d.doi.org/1.1988/ams.15.5168 The Variants of Energy Integral Induced by the Vibrating String Hwajoon Kim
More informationPartial Differential Equations
Partial Differential Equations Partial differential equations (PDEs) are equations involving functions of more than one variable and their partial derivatives with respect to those variables. Most (but
More informationMathematics Qualifying Exam Study Material
Mathematics Qualifying Exam Study Material The candidate is expected to have a thorough understanding of engineering mathematics topics. These topics are listed below for clarification. Not all instructors
More informationspring mass equilibrium position +v max
Lecture 20 Oscillations (Chapter 11) Review of Simple Harmonic Motion Parameters Graphical Representation of SHM Review of mass-spring pendulum periods Let s review Simple Harmonic Motion. Recall we used
More informationModule 4 : Laplace and Z Transform Problem Set 4
Module 4 : Laplace and Z Transform Problem Set 4 Problem 1 The input x(t) and output y(t) of a causal LTI system are related to the block diagram representation shown in the figure. (a) Determine a differential
More informationCHAPTER 1 Introduction to Differential Equations 1 CHAPTER 2 First-Order Equations 29
Contents PREFACE xiii CHAPTER 1 Introduction to Differential Equations 1 1.1 Introduction to Differential Equations: Vocabulary... 2 Exercises 1.1 10 1.2 A Graphical Approach to Solutions: Slope Fields
More informationSubject: Mathematics III Subject Code: Branch: B. Tech. all branches Semester: (3rd SEM) i) Dr. G. Pradhan (Coordinator) ii) Ms.
Subject: Mathematics III Subject Code: BSCM1205 Branch: B. Tech. all branches Semester: (3 rd SEM) Lecture notes prepared by: i) Dr. G. Pradhan (Coordinator) Asst. Prof. in Mathematics College of Engineering
More informationLecture Notes on Partial Dierential Equations (PDE)/ MaSc 221+MaSc 225
Lecture Notes on Partial Dierential Equations (PDE)/ MaSc 221+MaSc 225 Dr. Asmaa Al Themairi Assistant Professor a a Department of Mathematical sciences, University of Princess Nourah bint Abdulrahman,
More informationMATH 251 Final Examination December 16, 2014 FORM A. Name: Student Number: Section:
MATH 2 Final Examination December 6, 204 FORM A Name: Student Number: Section: This exam has 7 questions for a total of 0 points. In order to obtain full credit for partial credit problems, all work must
More informationSolving the Heat Equation (Sect. 10.5).
Solving the Heat Equation Sect. 1.5. Review: The Stationary Heat Equation. The Heat Equation. The Initial-Boundary Value Problem. The separation of variables method. An example of separation of variables.
More informationPHYS 301 HOMEWORK #13-- SOLUTIONS
PHYS 31 HOMEWORK #13-- SOLUTIONS 1. The wave equation is : 2 u x = 1 2 u 2 v 2 t 2 Since we have that u = f (x - vt) and u = f (x + vt), we substitute these expressions into the wave equation.starting
More information3 rd class Mech. Eng. Dept. hamdiahmed.weebly.com Fourier Series
Definition 1 Fourier Series A function f is said to be piecewise continuous on [a, b] if there exists finitely many points a = x 1 < x 2
More information4 The Harmonics of Vibrating Strings
4 The Harmonics of Vibrating Strings 4. Harmonics and Vibrations What I am going to tell you about is what we teach our physics students in the third or fourth year of graduate school... It is my task
More informationSolve Wave Equation from Scratch [2013 HSSP]
1 Solve Wave Equation from Scratch [2013 HSSP] Yuqi Zhu MIT Department of Physics, 77 Massachusetts Ave., Cambridge, MA 02139 (Dated: August 18, 2013) I. COURSE INFO Topics Date 07/07 Comple number, Cauchy-Riemann
More informationChapter 11 Vibrations and Waves
Chapter 11 Vibrations and Waves If an object vibrates or oscillates back and forth over the same path, each cycle taking the same amount of time, the motion is called periodic. The mass and spring system
More informationThe most up-to-date version of this collection of homework exercises can always be found at bob/math467/mmm.pdf.
Millersville University Department of Mathematics MATH 467 Partial Differential Equations January 23, 2012 The most up-to-date version of this collection of homework exercises can always be found at http://banach.millersville.edu/
More informationFinal: Solutions Math 118A, Fall 2013
Final: Solutions Math 118A, Fall 2013 1. [20 pts] For each of the following PDEs for u(x, y), give their order and say if they are nonlinear or linear. If they are linear, say if they are homogeneous or
More informationChapter 13. F =!kx. Vibrations and Waves. ! = 2" f = 2" T. Hooke s Law Reviewed. Sinusoidal Oscillation Graphing x vs. t. Phases.
Chapter 13 Vibrations and Waves Hooke s Law Reviewed F =!k When is positive, F is negative ; When at equilibrium (=0, F = 0 ; When is negative, F is positive ; 1 2 Sinusoidal Oscillation Graphing vs. t
More informationMidterm 2: Sample solutions Math 118A, Fall 2013
Midterm 2: Sample solutions Math 118A, Fall 213 1. Find all separated solutions u(r,t = F(rG(t of the radially symmetric heat equation u t = k ( r u. r r r Solve for G(t explicitly. Write down an ODE for
More informationMA 201, Mathematics III, July-November 2018, Laplace Transform (Contd.)
MA 201, Mathematics III, July-November 2018, Laplace Transform (Contd.) Lecture 19 Lecture 19 MA 201, PDE (2018) 1 / 24 Application of Laplace transform in solving ODEs ODEs with constant coefficients
More informationCOPYRIGHTED MATERIAL. Index
Index A Admissible function, 163 Amplification factor, 36 Amplitude, 1, 22 Amplitude-modulated carrier, 630 Amplitude ratio, 36 Antinodes, 612 Approximate analytical methods, 647 Assumed modes method,
More informationSpotlight on Laplace s Equation
16 Spotlight on Laplace s Equation Reference: Sections 1.1,1.2, and 1.5. Laplace s equation is the undriven, linear, second-order PDE 2 u = (1) We defined diffusivity on page 587. where 2 is the Laplacian
More information