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

Similar documents
Southern Taiwan University

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

DIFFERENTIAL EQUATION

Differential Equations

Addition of angular momentum

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

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

Addition of angular momentum

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

As the matrix of operator B is Hermitian so its eigenvalues must be real. It only remains to diagonalize the minor M 11 of matrix B.

INTEGRATION BY PARTS

[1] (20 points) Find the general solutions of y y 2y = sin(t) + e t. Solution: y(t) = y c (t) + y p (t). Complementary Solutions: y

2.3 Matrix Formulation

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

MA 262, Spring 2018, Final exam Version 01 (Green)

Engineering Mathematics I. MCQ for Phase-I

The Matrix Exponential

Section 11.6: Directional Derivatives and the Gradient Vector

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

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.


The Matrix Exponential

Problem Set 6 Solutions

y cos x = cos xdx = sin x + c y = tan x + c sec x But, y = 1 when x = 0 giving c = 1. y = tan x + sec x (A1) (C4) OR y cos x = sin x + 1 [8]

AS 5850 Finite Element Analysis

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.

Integration by Parts

Hydrogen Atom and One Electron Ions

Multiple-Choice Test Introduction to Partial Differential Equations COMPLETE SOLUTION SET

( ) Differential Equations. Unit-7. Exact Differential Equations: M d x + N d y = 0. Verify the condition

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let

1973 AP Calculus AB: Section I

VTU NOTES QUESTION PAPERS NEWS RESULTS FORUMS

Sundials and Linear Algebra

ECE602 Exam 1 April 5, You must show ALL of your work for full credit.

Basic Polyhedral theory

Introduction to Condensed Matter Physics

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

1 General boundary conditions in diffusion

Finite element discretization of Laplace and Poisson equations

Differentiation of Exponential Functions

CIE4145 : STRESS STRAIN RELATION LECTURE TOPICS

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

MATH 319, WEEK 15: The Fundamental Matrix, Non-Homogeneous Systems of Differential Equations

Function Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

Math 34A. Final Review

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

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)

2008 AP Calculus BC Multiple Choice Exam

dx equation it is called a second order differential equation.

SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott

4037 ADDITIONAL MATHEMATICS

Unit 6: Solving Exponential Equations and More

Calculus concepts derivatives

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):.

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

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

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

Self-Adjointness and Its Relationship to Quantum Mechanics. Ronald I. Frank 2016

Quasi-Classical States of the Simple Harmonic Oscillator

PHA 5127 Answers Homework 2 Fall 2001

First derivative analysis

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

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

Modeling with first order equations (Sect. 2.3).

MA1506 Tutorial 2 Solutions. Question 1. (1a) 1 ) y x. e x. 1 exp (in general, Integrating factor is. ye dx. So ) (1b) e e. e c.

Calculus II (MAC )

Introduction to the quantum theory of matter and Schrödinger s equation

2. Background Material

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS

PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS

(1) Then we could wave our hands over this and it would become:

Chapter 13 GMM for Linear Factor Models in Discount Factor form. GMM on the pricing errors gives a crosssectional

Multiple Short Term Infusion Homework # 5 PHA 5127

Differential Equations

Probability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J.

Math 120 Answers for Homework 14

TMMI37, vt2, Lecture 8; Introductory 2-dimensional elastostatics; cont.

a 1and x is any real number.

Derivation of Eigenvalue Matrix Equations

FEM FOR HEAT TRANSFER PROBLEMS دانشگاه صنعتي اصفهان- دانشكده مكانيك

Heat/Di usion Equation. 2 = 0 k constant w(x; 0) = '(x) initial condition. ( w2 2 ) t (kww x ) x + k(w x ) 2 dx. (w x ) 2 dx 0.

u 3 = u 3 (x 1, x 2, x 3 )

Thomas Whitham Sixth Form

ECE 650 1/8. Homework Set 4 - Solutions

5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values

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

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark

Elements of Statistical Thermodynamics

10. The Discrete-Time Fourier Transform (DTFT)

Homotopy perturbation technique

Classical Magnetic Dipole

Partial Derivatives: Suppose that z = f(x, y) is a function of two variables.

There is an arbitrary overall complex phase that could be added to A, but since this makes no difference we set it to zero and choose A real.

Einstein Equations for Tetrad Fields

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

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.

Strongly Connected Components

Transcription:

Eamn EDO. Givn th family of curvs y + C nd th particular orthogonal trajctory from th family of orthogonal trajctoris passing through point (0; ). Solution: In th rst plac, lt us calculat th di rntial quation associatd with this di rntial quation. y 0 C Substituting C in th family of curvs w gt C y0 ( y 0 ) y + ( y 0 ) y + y 0 y y 0 In ordr to obtain th family of orthogonal trajctoris w nd to chang y 0 by di rntial quation is y 0. Thn th nw y + y 0 y y 0 y 0 y W will solv this quation as an homognous quation rducibl to sparabl variabls. W apply th chang obtaining + y y + y 0 0 + 0 + a sparabl variabls quation 0 0 d d d d d d + d d + d d + ln ( ) + C

Sinc y y + ln jy j + C y + ln jy j C Finally, from this family w want th curv passing through (0; ), thn + ln j + 0 j C ln () C and th curv w wr looking for is y + ln jy j ln (). Solv th di rntial quation y 0 y + p + y y () Solution: Sinc th quation is homognous w ar going to apply th chang obtaining th following quation y y 0 0 + ( 0 + ) + p + ( 0 + ) + p + 0 + + p + 0 p + d d p + p d + d p + d d arg sinh () ln jj + C Undoing th chang w gt y arg sinh ln jj + C Finally, sinc y () thn arg sinh ln () + C C arg sinh Thrfor th solution is y arg sinh ln jj + arg sinh y sinh ln jj + arg sinh y sinh ln jj + arg sinh

3. Obtain th gnral solution of th quation py y 0 sin () + y 0 Solution: py y 0 sin () + y y 0 + y 3 0 sin () 4y 0 y 0 4 y y 3 sin () Dividing by y 3 w obtain y 0 4 y y 3 y 3 y 3 y 0 4 y sin () sin () Applying th chang 0 y y 0 y 3 w obtain a linar di rntial quation 0 4 () sin 0 + 4 () sin Calling P () 4 and Q () th solution is R 4 C d + C 4 ln() + C 4 + C 4 + R 4 d sin () d 4 ln() sin () d 4 sin () d sin () d Applying intgration by parts () 4 C + 4 cos () + 4 sin () cos () C 4 + 4 4 cos () + 4 3 sin () cos () 3

Undoing th chang C y 4 + 4 4 cos () + 4 3 sin () cos () y C + 4 4 cos () + 4 4 sin () 3 cos () y C + 4 cos () + 4 sin () cos () s y 4 C + 4 cos () + 4 sin () cos () 4 y p C + 4 cos () + 4 sin () cos () 4. Intgrat th following di rntial quation ( ) y 00 y 0 + y ( ) knowing that y and y ar solutions of th homognous associatd quation. Solution: Sinc y and y ar solutions of th homognous quation, w nd thm to b linarly indpndnt in ordr to obtain a Fundamntal Systm of Solutions. Th wronskian W (y ; y ; ) y y y 0 y 0 ( ) Th wronskian is di rnt from ro if 6. Thn w know that in ]; +[ (and in ] solutions ar L.I. Thrfor in ]; +[ th solutions form a Fundamntal Systm of Solutions and fy ; y g f; g y h C + C ; [) th is a solution of th homognous di rntial quation. To obtain th complt solution w will us Lagrang s mthod (th on that can b us with non-constant co cints linar di rntial quations). W ar looking for a solution of th form y p C () + C () whr C () and C () vri s th following conditions or, in our cas, Solving th systm C 0 () y + C 0 () y 0 C 0 () y 0 + C 0 () y 0 f () a n () C 0 () + C 0 () 0 C 0 () + C 0 () C 0 () C 0 () 0 0 ( ) ( ) ( ) ( ) ( ) 4

Finally, C () C () d d thrfor y p + Th gnral solution of th di rntial quation is y y h + y p C + C 5. Givn th quation indicat which is th tst function if y 00 y 0 + 0y f () f () cos (3) + sin (3) Solution: First of all w nd to solv th charactristic quation associatd with th homognous quation: r r + 0 0 Th solutions ar r 3i and r + 3i. So th solution to tst is y p A cos (3) + B sin (3) + (C cos (3) + D sin (3)) 6. Intgrat th quation + y 00 y 0 + y 0 nding rst th a particular solution of th form y a + b. thn Solution: W ar looking for a solution of th form Rplacing in th original quation y a + b y 0 a y 00 0 + 0 a + (a + b) 0 b 0 b 0 and a can tak any valu. Sinc w do not want th ro solution, lt us tak a. Thn a solution of th di rntial quation is y Knowing this particular solution w apply th following chang y y p y 0 0 + y 00 00 + 0 5

into th original quation and obtain Calling 0 p th last quation can b writtn as Solving this di rntial quation + ( 00 + 0 ) ( 0 + ) + 0 p + + 3 p 0 0 + 3 p 0 p p dp ( + 3 ) d p dp ( + 3 ) d ln jpj ( + ) d ln + ln + ln C 0 + + 3 00 0 d + + d thn Thrfor Sinc p C + 0 p C + C + d C + ln jj + D and nally is th solution of th original di rntial quation. y C 3 + ln jj + D 7. Givn th systm 0 3 4y y 0 y a) Find th solution applying th matri mthod. b) Us th limination mthod togthr with (0) 4 and y (0). Solution: a) In this cas Th ignvalus ar ja Ij A 3 4 3 4 + 0 (doubl) 6

Now lt us calculat th ignvctors for 3 4 4 A I 0 0 0 0 0 Thrfor th matri is not diagonaliabl and Y is a solution of th linar systm. W nd to obtain anothr solution L.I. with this on. To do this w ar going to tst a t + b Y t a t + b Substituting this solution in th systm a t + b D a t + b a t + a + b a t + a + b DY AY t 3 4 a t + b a t + b t t 3b 4b + 3ta 4ta t b b + ta ta Equating both sids of th quality w obtain th following systm From th rst and third quations w hav and from scond and forth quations thrfor a 3a 4a a + b 3b 4b a a a a + b b b a a a b + b 0 b a + b If w a and b 0 thn a and b. Thn th solution w wr looking for has th following shap t + Y t t Thr is only on thing to chck: Ar this solutions L.I.? Sinc W (Y ; Y ; t) t (t + ) t t t t t 6 0 th solutions ar L.I. 7

Th solution is Y C Y + C Y C t + C t + t t b) Elimination mthod: Th systm 0 3 4y y 0 y can b writtn in th form (D 3) + 4y 0 + (D + ) y 0 Applying Cramr y 0 4 0 D + D + C 3 0 0 D + Thn D + D + 0 4 0 D + y C 3 0 0 0 0 and from hr w gt ((D 3) (D + ) + 4) 0 ((D 3) (D + ) + 4) y 0 Both quations ar th sam, so w ar going to solv only for : ((D 3) (D + ) + 4) 0 D D + 0 Charactristic quation r r + 0 has only on solution r (doubl) Th solution of th quation is (t) C t + C t t Similarly th solution for y is y (t) C 3 t + C 4 t t Now w hav to nd out th rlation btwn th constants. Sinc D + D D + is of dgr, w only nd two constants. 8

Using th scond quation y 0 y of th systm and rplacing th solutions w obtain C 3 t + C 4 (t + ) t C t + C t t C 3 t C 4 t t C 3 + C 4 t + C 4 C + C t C 3 C 4 t Equating both sids C 4 C C 4 C 3 + C 4 C C 3 From th rs quation w gt C C 4 and from th scond quation C C 3 + C 4 Thrfor th solution is (t) (C 3 + C 4 ) t + C 4 t t C 3 t + C 4 (t + ) t y (t) C 3 t + C 4 t t Applying th initial condition (0) 4 C 3 + C 4 y (0) C 3 and thn C 3 C 4 Thrfor th solution of th PVI is (t) t + (t + ) t y (t) t + t t 9