dy dy 2 dy d Y 2 dx dx Substituting these into the given differential equation d 2 Y dy 2Y = 2x + 3 ( ) ( 1 + 2b)= 3

Size: px
Start display at page:

Download "dy dy 2 dy d Y 2 dx dx Substituting these into the given differential equation d 2 Y dy 2Y = 2x + 3 ( ) ( 1 + 2b)= 3"

Transcription

1 Solutions 14() 1 Coplete solutions to Eerise 14() 1. (a) Sine f()= 18 is a onstant so Y = C, differentiating this zero. Substituting for Y into Y = 18 C = 18, hene C = 9 The partiular integral Y = 9. (This partiular integral an be seen learly without going through all the ehanis above. Only the last ter on the left hand side y plays a part. Sine you need 18, Y = 9). (b) Sine f()= + 3 is a linear funtion so Y = a + b d Y = a, = Substituting these into the given differential equation d Y Y = + 3 a a+ b = + 3 a a + b = + 3 Equating oeffiients of : a = hene a = 1 onstants: ( a + b)= 3 ( 1 + b)= 3 b = hene b = 1 Substituting a = 1 and b = 1 into Y = a + b Y = 1 () Sine f()= 13sin( 3) our trial funtion is (see (14.16)) Y = aos( 3) + bsin ( 3) = 3asin( 3) + 3bos( 3) by (6.13) by(6.1) = 9aos 3 9bsin 3 by (6.1) by (6.13) Substituting into Y = 13sin ( 3) 9aos 3 9bsin 3 3asin 3 + 3bos 3 aos 3 + bsin 3 = 13sin 3 (6.1) sin ( ) = os( ) (6.13) [ os( ) ] = sin( )

2 ( 9a 3b a) os( 3) + ( 3a 9b b) sin ( 3) = 13sin ( 3) ( 11a 3b) os( 3) + ( 3a 11b) sin ( 3) = 13sin ( 3) Solutions 14() Equating oeffiients of os( 3): 11a 3b = sin( 3): 3a 11b = 13 Solving these siultaneous equations a = 3 and b = 11. Putting a = 3 and b = 11 into our trial funtion Y = a os( 3)+ bsin( 3) the partiular integral Y = 3os( 3) 11sin( 3) (d) Sine f()= os() our trial funtion is given by Y = aos + bsin ( ) = asin + b os sin = aos b Substituting into Y = os ( ) aos( ) bsin ( ) asin ( ) + bos( ) aos( ) + bsin ( ) = os( a b a os + b+ a b sin = os Equating oeffiients of os : 3a b= 1 ( 3a b) os( ) + ( a 3b) sin( ) = os( ) sin : a 3b=, a= 3b Solving these siultaneous equations a = 3, b = 1. Substituting these into () Y = os( ) sin ( ) = 3os( ) + sin ( ) (e) Straightforward, y = e 3 4. The first two, (a) and (b), are unopliated. (a) y = Ae + Be + 3 (b) y = Ae 3 + Be + 7 () First we find the opleentary funtion y, (right hand side is equal to zero). The harateristi equation is + + 1= ( + 1) =, = 1 ( equal roots) By (14.5) y = ( A+ B)e. Sine f( )= 36e 5 so by (14.17), Y = Ce 5 Differentiating ) (14.5) Equal roots,, y = ( A + B)e (14.7) If f( )= Ae then y = Ce

3 Solutions 14() 3 Substituting into = 5Ce Y e 5 5 = 5Ce = Ce + 5Ce + Ce = 36e 5 36Ce 5 = 36e 5 whih C = 1 Substituting C = 1 into Y = Ce 5 the partiular integral Y = e 5 Adding the opleentary funtion, y, and the partiular integral the general solution y = A+ B e + e 5 (d) Sae proedure as part (a). The harateristi equation is + 3 4= ( 4)( 1) + = = 4, = 1 1 Sine we have distint roots so 4 y = Ae + Be Partiular integral Y: Sine f()= 34sin () we try the funtion Y = aos + bsin = asin + b os sin = aos b Substituting into + 3 4Y = 34sin ( ) aos( ) bsin ( ) + 3 asin ( ) + bos( ) 4 aos( ) + bsin ( ) = 34sin ( a+ 3b 4a os + b 3a 4b sin = 34sin ( 3b 5a) os( ) + ( 5b 3a) sin( ) = 34sin( ) Equating oeffiients of os : 3b 5a= sin : 5b 3a= 34 Solving these siultaneous equations a = 3, b = 5. Substituting for a and b into our trial funtion, Y = a os( )+ bsin( ), Y = 3os + 5sin and the general solution, y = y + Y, is 5sin 4 y = Ae + Be + 3os + )

4 Solutions 14() 4 3. By adding to both sides, the given differential equation beoes + = g Dividing through by + = g (*) Copleentary funtion : + = The harateristi equation r + = r + = By (14.8) = Aos( ωt) + Bsin ( ωt) where ω = Partiular integral X: Sine + = g and g is a onstant so X=C, X = X =. Substituting these into (*) C = g whih C = g Hene X = g. The general solution is = + X so we have 4. We have g = Aos( ωt) + Bsin ( ωt) + where ω = d 1 =.5+ 4 dt 3 3 ( ) d 3 = (.5 + 4) dividing by dt d 4 =.5 (*) dt Charateristi equation is r 4 =, solving r1 = and r =. By (14.4) = Ae t + Be t Sine f()=.5 our trial funtion is a onstant, X = C. Substituting into (*) 4C =.5 C =.15 The general solution is found by adding together the opleentary funtion, = Ae t + Be t, and the partiular integral, X =.15: t t = Ae + Be.15 r 1 r (14.4) If r1 and r then y = Ae + Be r + = y = Aos + Bsin ) (14.8) (

5 Solutions 14() 5 5. By adding to both sides, the differential equation beoes + = F αt sin Copleentary funtion : + =, + = Thus the harateristi equation is By (14.8) A ( t) B ( t) Partiular integral X: By (14.16) r + = = os ω + sin ω where ω = ( α ) sin ( α ) X = aos t + b t Differentiating X = α asin ( αt) + bos( αt) X = α aos( αt) bsin ( αt) = α aos( αt) + bsin ( αt) Substituting into F X + X = sin ( αt) F α aos( αt) + bsin ( αt) + aos( t) bsin ( t) sin α + α = αt F α aos( αt) + α bsin ( αt) = sin ( αt) Equating oeffiients of os( αt): α a =, a = beause α sin( αt): α b = F F F b = α = α / / F Substituting a = and b = into X = aos( αt)+ bsin αt α F X = sin ( αt ) α The general solution, = + X, is F = Aos( ωt) + Bsin ( ωt) + sin ( α t) where ω = α If f ( ) Asin then Y aos bsin ) (14.16) = = + (

6 Solutions 14() 6 6. Very siilar to solution Rearranging the equation to + + = g + L (*) Two parts, first find the opleentary funtion; + + = Dividing by + + = The harateristi equation is r + r + = Using the quadrati equation forula, (1.16), ± r = = ± 1 = ± 4 1 = ± 4 1 = ± ( 4 ) 1 1 r = ± j 4 = ± j 4 beause < 4 Using (14.6) with α = and β = 1 4 t ( β ) ( β ) = e Aos t + Bsin t where represents the opleentary funtion. We need to find the partiular integral; Sine the right hand side of (*) is a onstant, g + L, so by (14. 11) X = C, X = and X = Substituting into X Ý + X Ý + X = g + L C = g + L g C = + L (1.16) b± b 4a r = a (14.6) α If = α ± jβ then = e t Aos( βt) + Bsin ( βt) (14.11) If f ( ) = onstant then Y =C

7 Solutions 14() 7 g Hene the partiular integral is X = + L. The general solution, = + X, is t g = e Aos( βt) + Bsin ( βt) + + L 1 where β = Dividing the given differential equation by CL we have di 1 di i I + + = (*) dt RC dt LC LC Putting R = 1 3, C = 9 and L = = = RC = = 3 9 LC 5 Substituting these and I = 5 3 into (*) di 5 di ( 1 ) + ( ) i = ( )( 5 ) dt dt Copleentary funtion i : The harateristi equation is ( 1 ) + ( ) = Putting a = 1, b = 1 5 and = 9 into (1.16) By (14.4) ( 1 ) ( 1 ) ( 4 ) ± = 4 4 = ( 5 ) ± (.36 ) =.764 and = ( ) t ( ) t i = Ae + Be Partiular integral I : Sine the right hand side of (**) is 9 trial funtion. 5 3 Substituting into ( (**), a onstant, so our I = K ( K is onstant) di 5 di I = 5 ) dt dt K = 5 K = 5 I = (1.16) (14.4) b b 4a ± = a t If and then y = Ae + Be 1 1 t

8 Solutions 14() 8 We now i = i + I 4 4 (. ) t (. ) t i = Ae + Be By looing at EXAMPLE 7 of this hapter, we now the opleentary funtion y = Ae + Be. (Sae harateristi equation). The trial funtion is Y = Ce beause Ce is already part of the opleentary funtion. Y = Ce ( ) Differentiating by using the produt rule (6.31) = Ce Ce = Ce ( Ce Ce ) = Ce + Ce Substituting into Y = 5e Ce + Ce Ce + Ce Ce = 5e C + C C + C C e = 5e 3C = 5 C = 5 / Hene Y = e putting C = into ( ) 3 3 The general solution is given by y= y + Y, so we have y = Ae + Be e 3.(a) Charateristi equation is = 5 ( )( ) = = 3, = 1 1 Sine we have two distint roots so y = Ae 3 + Be Hene the trial funtion is Y = Ce 3 (b) Charateristi equation is + 9= + 3 = By (14.8), y = Aos( 3)+ Bsin( 3). The trial funtion ould be aos( 3) + bsin ( 3 ) Sine a os( 3) is already part of the opleentary funtion, so we try Y = aos( 3) + bsin ( 3) (6.31) ( uv) = u v + v u (14.8) + = then y = Aos( )+ Bsin( )

9 Solutions 14() The differential equation an be rearranged to d y P P π + y = sin (*) EI EI L Copleentary funtion y ; As before P y = Aos( )+ Bsin( ) where = EI Partiular integral Y ; Sine the right hand side of (*) is P π sin EI L (14.16) our trial funtion is π π Y = Cos + Dsin (**) L L π π π = Csin Dos L + L L π π π = Cos Dsin L + L L Substituting into d Y + P EI Y = P π sin EI L π π π P π π Cos Dsin Cos Dsin L + L L + EI + L L P π = sin EI L Equating oeffiients of os π L ; P π C = EI L C = Equating oeffiients of sin π L ; P π P D EI L = EI PL π EI P D = ( EI ) L EI so by Multiply through by EI D ( PL π EI ) Substituting C = and D = L PL = P D = EIπ PL PL EIπ into (**) PL (14.16) If f()= Asin( ) then Y = a os( ) + bsin( )

10 Solutions 14() PL sin π Y = EIπ PL L The general solution, y, is given by PL π y = Aos( ) + Bsin ( ) + sin EIπ PL L

Differential Equations 8/24/2010

Differential Equations 8/24/2010 Differential Equations A Differential i Equation (DE) is an equation ontaining one or more derivatives of an unknown dependant d variable with respet to (wrt) one or more independent variables. Solution

More information

Strauss PDEs 2e: Section Exercise 3 Page 1 of 13. u tt c 2 u xx = cos x. ( 2 t c 2 2 x)u = cos x. v = ( t c x )u

Strauss PDEs 2e: Section Exercise 3 Page 1 of 13. u tt c 2 u xx = cos x. ( 2 t c 2 2 x)u = cos x. v = ( t c x )u Strauss PDEs e: Setion 3.4 - Exerise 3 Page 1 of 13 Exerise 3 Solve u tt = u xx + os x, u(x, ) = sin x, u t (x, ) = 1 + x. Solution Solution by Operator Fatorization Bring u xx to the other side. Write

More information

HOW TO FACTOR. Next you reason that if it factors, then the factorization will look something like,

HOW TO FACTOR. Next you reason that if it factors, then the factorization will look something like, HOW TO FACTOR ax bx I now want to talk a bit about how to fator ax bx where all the oeffiients a, b, and are integers. The method that most people are taught these days in high shool (assuming you go to

More information

MAC Calculus II Summer All you need to know on partial fractions and more

MAC Calculus II Summer All you need to know on partial fractions and more MC -75-Calulus II Summer 00 ll you need to know on partial frations and more What are partial frations? following forms:.... where, α are onstants. Partial frations are frations of one of the + α, ( +

More information

Rectangular Waveguide

Rectangular Waveguide 0/30/07 EE 4347 Applied Eletromagnetis Topi 5 Retangular Waveguide Leture 5 These notes ma ontain oprighted material obtained under air use rules. Distribution o these materials is stritl prohibited Slide

More information

Some facts you should know that would be convenient when evaluating a limit:

Some facts you should know that would be convenient when evaluating a limit: Some fats you should know that would be onvenient when evaluating a it: When evaluating a it of fration of two funtions, f(x) x a g(x) If f and g are both ontinuous inside an open interval that ontains

More information

CHAPTER P Preparation for Calculus

CHAPTER P Preparation for Calculus PART I CHAPTER P Preparation for Calulus Setion P. Graphs and Models...................... Setion P. Linear Models and Rates of Change............. 7 Setion P. Funtions and Their Graphs.................

More information

Chapter 2: Solution of First order ODE

Chapter 2: Solution of First order ODE 0 Chapter : Solution of irst order ODE Se. Separable Equations The differential equation of the form that is is alled separable if f = h g; In order to solve it perform the following steps: Rewrite the

More information

CHEE 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 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 information

ME 391 Mechanical Engineering Analysis

ME 391 Mechanical Engineering Analysis Solve the following differential equations. ME 9 Mechanical Engineering Analysis Eam # Practice Problems Solutions. e u 5sin() with u(=)= We may rearrange this equation to e u 5sin() and note that it is

More information

ON THE LEAST PRIMITIVE ROOT EXPRESSIBLE AS A SUM OF TWO SQUARES

ON THE LEAST PRIMITIVE ROOT EXPRESSIBLE AS A SUM OF TWO SQUARES #A55 INTEGERS 3 (203) ON THE LEAST PRIMITIVE ROOT EPRESSIBLE AS A SUM OF TWO SQUARES Christopher Ambrose Mathematishes Institut, Georg-August Universität Göttingen, Göttingen, Deutshland ambrose@uni-math.gwdg.de

More information

Strauss PDEs 2e: Section Exercise 1 Page 1 of 6

Strauss PDEs 2e: Section Exercise 1 Page 1 of 6 Strauss PDEs e: Setion.1 - Exerise 1 Page 1 of 6 Exerise 1 Solve u tt = u xx, u(x, 0) = e x, u t (x, 0) = sin x. Solution Solution by Operator Fatorization By fatoring the wave equation and making a substitution,

More information

Tutorial 4 (week 4) Solutions

Tutorial 4 (week 4) Solutions THE UNIVERSITY OF SYDNEY PURE MATHEMATICS Summer Shool Math26 28 Tutorial week s You are given the following data points: x 2 y 2 Construt a Lagrange basis {p p p 2 p 3 } of P 3 using the x values from

More information

x(t) y(t) c c F(t) F(t) EN40: Dynamics and Vibrations Homework 6: Forced Vibrations Due Friday April 5, 2018

x(t) y(t) c c F(t) F(t) EN40: Dynamics and Vibrations Homework 6: Forced Vibrations Due Friday April 5, 2018 EN40: Dynais and Vibrations Hoewor 6: Fored Vibrations Due Friday April 5, 2018 Shool of Engineering Brown University 1. The vibration isolation syste shown in the figure has =20g, = 19.8 N / = 1.259 Ns

More information

and ζ in 1.1)? 1.2 What is the value of the magnification factor M for system A, (with force frequency ω = ωn

and ζ in 1.1)? 1.2 What is the value of the magnification factor M for system A, (with force frequency ω = ωn EN40: Dynais and Vibrations Hoework 6: Fored Vibrations, Rigid Body Kineatis Due Friday April 7, 017 Shool of Engineering Brown University 1. Syste A in the figure is ritially daped. The aplitude of the

More information

We consider the nonrelativistic regime so no pair production or annihilation.the hamiltonian for interaction of fields and sources is 1 (p

We consider the nonrelativistic regime so no pair production or annihilation.the hamiltonian for interaction of fields and sources is 1 (p .. RADIATIVE TRANSITIONS Marh 3, 5 Leture XXIV Quantization of the E-M field. Radiative transitions We onsider the nonrelativisti regime so no pair prodution or annihilation.the hamiltonian for interation

More information

Scholarship Calculus (93202) 2013 page 1 of 8. ( 6) ± 20 = 3± 5, so x = ln( 3± 5) 2. 1(a) Expression for dy = 0 [1st mark], [2nd mark], width is

Scholarship Calculus (93202) 2013 page 1 of 8. ( 6) ± 20 = 3± 5, so x = ln( 3± 5) 2. 1(a) Expression for dy = 0 [1st mark], [2nd mark], width is Sholarship Calulus 93) 3 page of 8 Assessent Shedule 3 Sholarship Calulus 93) Evidene Stateent Question One a) e x e x Solving dy dx ln x x x ln ϕ e x e x e x e x ϕ, we find e x x e y The drop is widest

More information

Math 54. Selected Solutions for Week 10

Math 54. Selected Solutions for Week 10 Math 54. Selected Solutions for Week 10 Section 4.1 (Page 399) 9. Find a synchronous solution of the form A cos Ωt+B sin Ωt to the given forced oscillator equation using the method of Example 4 to solve

More information

To derive the other Pythagorean Identities, divide the entire equation by + = θ = sin. sinθ cosθ tanθ = 1

To derive the other Pythagorean Identities, divide the entire equation by + = θ = sin. sinθ cosθ tanθ = 1 Syllabus Objetives: 3.3 The student will simplify trigonometri expressions and prove trigonometri identities (fundamental identities). 3.4 The student will solve trigonometri equations with and without

More information

Quantum Mechanics: Wheeler: Physics 6210

Quantum Mechanics: Wheeler: Physics 6210 Quantum Mehanis: Wheeler: Physis 60 Problems some modified from Sakurai, hapter. W. S..: The Pauli matries, σ i, are a triple of matries, σ, σ i = σ, σ, σ 3 given by σ = σ = σ 3 = i i Let stand for the

More information

( k) Integrating by using (8.2) and taking the constant of integration to be 0: ( ) C = m. v dv = v = 0.1 t = +

( k) Integrating by using (8.2) and taking the constant of integration to be 0: ( ) C = m. v dv = v = 0.1 t = + Solutions 13 1 Complete solutions to Miscellaneous Exercise 13 Throughout these solutions I hae assumed the argument, x, in ln () x to be positie. 1. Rearranging gies d( pv) dm C = pv m Integrating by

More information

1 sin 2 r = 1 n 2 sin 2 i

1 sin 2 r = 1 n 2 sin 2 i Physis 505 Fall 005 Homework Assignment #11 Solutions Textbook problems: Ch. 7: 7.3, 7.5, 7.8, 7.16 7.3 Two plane semi-infinite slabs of the same uniform, isotropi, nonpermeable, lossless dieletri with

More information

Edexcel Further Pure 2

Edexcel Further Pure 2 Edecel Further Pure Second order differential equations Section : Non-homogeneous second order differential equations Notes and Eamples These notes contain subsections on Finding particular integrals Finding

More information

Section 3.4. Second Order Nonhomogeneous. The corresponding homogeneous equation. is called the reduced equation of (N).

Section 3.4. Second Order Nonhomogeneous. The corresponding homogeneous equation. is called the reduced equation of (N). Section 3.4. Second Order Nonhomogeneous Equations y + p(x)y + q(x)y = f(x) (N) The corresponding homogeneous equation y + p(x)y + q(x)y = 0 (H) is called the reduced equation of (N). 1 General Results

More information

Lecture 24: Spinodal Decomposition: Part 3: kinetics of the

Lecture 24: Spinodal Decomposition: Part 3: kinetics of the Leture 4: Spinodal Deoposition: Part 3: kinetis of the oposition flutuation Today s topis Diffusion kinetis of spinodal deoposition in ters of the onentration (oposition) flutuation as a funtion of tie:

More information

FW Phys 130 G:\130 lecture\130 tests\formulas final03.docx page 1 of 7

FW Phys 130 G:\130 lecture\130 tests\formulas final03.docx page 1 of 7 FW Phys 13 G:\13 leture\13 tests\forulas final3.dox page 1 of 7 dr dr r x y z ur ru (1.1) dt dt All onseratie fores derie fro a potential funtion U(x,y,z) (1.) U U U F gradu U,, x y z 1 MG 1 dr MG E K

More information

REFERENCE: CROFT & DAVISON CHAPTER 20 BLOCKS 1-3

REFERENCE: CROFT & DAVISON CHAPTER 20 BLOCKS 1-3 IV ORDINARY DIFFERENTIAL EQUATIONS REFERENCE: CROFT & DAVISON CHAPTER 0 BLOCKS 1-3 INTRODUCTION AND TERMINOLOGY INTRODUCTION A differential equation (d.e.) e) is an equation involving an unknown function

More information

Chapter 3 : Linear Differential Eqn. Chapter 3 : Linear Differential Eqn.

Chapter 3 : Linear Differential Eqn. Chapter 3 : Linear Differential Eqn. 1.0 Introduction Linear differential equations is all about to find the total solution y(t), where : y(t) = homogeneous solution [ y h (t) ] + particular solution y p (t) General form of differential equation

More information

Journal of Theoretics Vol.4-4

Journal of Theoretics Vol.4-4 Journal of Theoretis ol.4-4 Cherenko s Partiles as Magnetons Dipl. Ing. Andrija Radoić Nike Strugara 3a, 3 Beograd, Yugoslaia Eail: andrijar@eunet.yu Abstrat: The artile will show that the forula for Cherenko

More information

MA304 Differential Geometry

MA304 Differential Geometry MA304 Differential Geoetry Hoework 4 solutions Spring 018 6% of the final ark 1. The paraeterised curve αt = t cosh t for t R is called the catenary. Find the curvature of αt. Solution. Fro hoework question

More information

ELG 3150 Introduction to Control Systems. TA: Fouad Khalil, P.Eng., Ph.D. Student

ELG 3150 Introduction to Control Systems. TA: Fouad Khalil, P.Eng., Ph.D. Student ELG 350 Introduction to Control Systems TA: Fouad Khalil, P.Eng., Ph.D. Student fkhalil@site.uottawa.ca My agenda for this tutorial session I will introduce the Laplace Transforms as a useful tool for

More information

Ordinary differential equations

Ordinary differential equations Class 7 Today s topics The nonhomogeneous equation Resonance u + pu + qu = g(t). The nonhomogeneous second order linear equation This is the nonhomogeneous second order linear equation u + pu + qu = g(t).

More information

Damped Harmonic Motion

Damped Harmonic Motion Daped Haronic Motion PY154 Special Topics in Physics PY154 1 Driven Daped Haronic Motion What if we apply a haronic force?: F h Be it The total force is then: dx F Fh kx b dt d x dt Assue a solution of

More information

Derivation of Non-Einsteinian Relativistic Equations from Momentum Conservation Law

Derivation of Non-Einsteinian Relativistic Equations from Momentum Conservation Law Asian Journal of Applied Siene and Engineering, Volue, No 1/13 ISSN 35-915X(p); 37-9584(e) Derivation of Non-Einsteinian Relativisti Equations fro Moentu Conservation Law M.O.G. Talukder Varendra University,

More information

Methods of evaluating tests

Methods of evaluating tests Methods of evaluating tests Let X,, 1 Xn be i.i.d. Bernoulli( p ). Then 5 j= 1 j ( 5, ) T = X Binomial p. We test 1 H : p vs. 1 1 H : p>. We saw that a LRT is 1 if t k* φ ( x ) =. otherwise (t is the observed

More information

2/5/13. y H. Assume propagation in the positive z-direction: β β x

2/5/13. y H. Assume propagation in the positive z-direction: β β x /5/3 Retangular Waveguides Mawell s Equatins: = t jω assumed E = jωµ H E E = jωµ H E E = jωµ H E E = jωµ H H = jωε E H H = jωε E H H = jωε E H H = jωε E /5/3 Assume prpagatin in the psitive -diretin: e

More information

n n=1 (air) n 1 sin 2 r =

n n=1 (air) n 1 sin 2 r = Physis 55 Fall 7 Homework Assignment #11 Solutions Textbook problems: Ch. 7: 7.3, 7.4, 7.6, 7.8 7.3 Two plane semi-infinite slabs of the same uniform, isotropi, nonpermeable, lossless dieletri with index

More information

Mathematics II. Tutorial 5 Basic mathematical modelling. Groups: B03 & B08. Ngo Quoc Anh Department of Mathematics National University of Singapore

Mathematics II. Tutorial 5 Basic mathematical modelling. Groups: B03 & B08. Ngo Quoc Anh Department of Mathematics National University of Singapore Mathematis II Tutorial 5 Basi mathematial modelling Groups: B03 & B08 February 29, 2012 Mathematis II Ngo Quo Anh Ngo Quo Anh Department of Mathematis National University of Singapore 1/13 : The ost of

More information

Ordinary Differential Equations

Ordinary Differential Equations Ordinary Differential Equations (MA102 Mathematics II) Shyamashree Upadhyay IIT Guwahati Shyamashree Upadhyay ( IIT Guwahati ) Ordinary Differential Equations 1 / 15 Method of Undetermined Coefficients

More information

Moment of inertia: (1.3) Kinetic energy of rotation: Angular momentum of a solid object rotating around a fixed axis: Wave particle relationships: ω =

Moment of inertia: (1.3) Kinetic energy of rotation: Angular momentum of a solid object rotating around a fixed axis: Wave particle relationships: ω = FW Phys 13 E:\Exel files\h 18 Reiew of FormulasM3.do page 1 of 6 Rotational formulas: (1.1) The angular momentum L of a point mass m, moing with eloity is gien by the etor produt between its radius etor

More information

6.4 Dividing Polynomials: Long Division and Synthetic Division

6.4 Dividing Polynomials: Long Division and Synthetic Division 6 CHAPTER 6 Rational Epressions 6. Whih of the following are equivalent to? y a., b. # y. y, y 6. Whih of the following are equivalent to 5? a a. 5, b. a 5, 5. # a a 6. In your own words, eplain one method

More information

Extra Credit Solutions Math 181, Fall 2018 Instructor: Dr. Doreen De Leon

Extra Credit Solutions Math 181, Fall 2018 Instructor: Dr. Doreen De Leon Extra Credit Solutions Math 181, Fall 018 Instrutor: Dr. Doreen De Leon 1. In eah problem below, the given sstem is an almost linear sstem at eah of its equilibrium points. For eah, (i Find the (real equilibrium

More information

Wave Propagation through Random Media

Wave Propagation through Random Media Chapter 3. Wave Propagation through Random Media 3. Charateristis of Wave Behavior Sound propagation through random media is the entral part of this investigation. This hapter presents a frame of referene

More information

y 2 Well it is a cos graph with amplitude of 3 and only half a waveform between 0 and 2π because the cos argument is x /2: y =3cos π 2

y 2 Well it is a cos graph with amplitude of 3 and only half a waveform between 0 and 2π because the cos argument is x /2: y =3cos π 2 Complete Solutions Eamination Questions Complete Solutions to Eamination Questions 4. (a) How do we sketch the graph of y 3? Well it is a graph with amplitude of 3 and only half a waveform between 0 and

More information

REVISION SHEET FP2 (Edx) CALCULUS. x x 0.5. x x 1.5. π π. Standard Calculus of Inverse Trig and Hyperbolic Trig Functions = + = + arcsin x = +

REVISION SHEET FP2 (Edx) CALCULUS. x x 0.5. x x 1.5. π π. Standard Calculus of Inverse Trig and Hyperbolic Trig Functions = + = + arcsin x = + the Further Mathematis netwk www.fmnetwk.g.uk V 07 REVISION SHEET FP (Ed) CLCULUS The main ideas are: Calulus using inverse trig funtions & hperboli trig funtions and their inverses. Malaurin series Differentiating

More information

Chapter Review of of Random Processes

Chapter Review of of Random Processes Chapter.. Review of of Random Proesses Random Variables and Error Funtions Conepts of Random Proesses 3 Wide-sense Stationary Proesses and Transmission over LTI 4 White Gaussian Noise Proesses @G.Gong

More information

2. Failure to submit this paper in its entirety at the end of the examination may result in disqualification.

2. Failure to submit this paper in its entirety at the end of the examination may result in disqualification. Memorial University of Newfoundland St. John s, Newfoundland and Labrador Chemistry 101 Intersession 007 Midterm Exam May 8 th, 007 Time: 0 Minutes Name: MUN #: Dr. Peter Warburton READ THE FOLLOWING CAREFULLY!

More information

This is the law of sines. For any triangle, the following is true.

This is the law of sines. For any triangle, the following is true. Unit 15: Law of Sines Basic Skills eview This is the law of sines. For any triangle, the following is true. Using this formula, you can find values for unknown angles and sides when given some of the values

More information

Get Solution of These Packages & Learn by Video Tutorials on SHORT REVISION

Get Solution of These Packages & Learn by Video Tutorials on  SHORT REVISION SHORT REVISION The symol a a is alled the determinant of order two Its value is given y : D = a a a The symol a is alled the determinant of order three Its value an e found as : D = a a + a a a D = a +

More information

Chapter 15 Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium 5/27/2014

Chapter 15 Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium 5/27/2014 Amount of reatant/produt 5/7/01 quilibrium in Chemial Reations Lets look bak at our hypothetial reation from the kinetis hapter. A + B C Chapter 15 quilibrium [A] Why doesn t the onentration of A ever

More information

Congruences and Modular Arithmetic

Congruences and Modular Arithmetic Congruenes and Modular Aritheti 6-17-2016 a is ongruent to b od n eans that n a b. Notation: a = b (od n). Congruene od n is an equivalene relation. Hene, ongruenes have any of the sae properties as ordinary

More information

A Characterization of Wavelet Convergence in Sobolev Spaces

A Characterization of Wavelet Convergence in Sobolev Spaces A Charaterization of Wavelet Convergene in Sobolev Spaes Mark A. Kon 1 oston University Louise Arakelian Raphael Howard University Dediated to Prof. Robert Carroll on the oasion of his 70th birthday. Abstrat

More information

ME357 Problem Set The wheel is a thin homogeneous disk that rolls without slip. sin. The wall moves with a specified motion x t. sin..

ME357 Problem Set The wheel is a thin homogeneous disk that rolls without slip. sin. The wall moves with a specified motion x t. sin.. ME357 Proble Set 3 Derive the equation(s) of otion for the systes shown using Newton s Method. For ultiple degree of freedo systes put you answer in atri for. Unless otherwise speified the degrees of freedo

More information

RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s) AND L(s, χ)

RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s) AND L(s, χ) RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s AND L(s, χ FELIX RUBIN SEMINAR ON MODULAR FORMS, WINTER TERM 6 Abstrat. In this hapter, we will see a proof of the analyti ontinuation of the Riemann

More information

Lesson 23: The Defining Equation of a Line

Lesson 23: The Defining Equation of a Line Student Outomes Students know that two equations in the form of ax + y = and a x + y = graph as the same line when a = = and at least one of a or is nonzero. a Students know that the graph of a linear

More information

Tests of fit for symmetric variance gamma distributions

Tests of fit for symmetric variance gamma distributions Tests of fit for symmetri variane gamma distributions Fragiadakis Kostas UADPhilEon, National and Kapodistrian University of Athens, 4 Euripidou Street, 05 59 Athens, Greee. Keywords: Variane Gamma Distribution,

More information

Module 4 Lesson 2 Exercises Answer Key squared square root

Module 4 Lesson 2 Exercises Answer Key squared square root Module Lesson Eerises Answer Key 1. The volume is 1 L so onentrations an be done by inspetion. Just substitute values and solve for K [ CO][ HO] K CO H (0.8)(0.8) (0.55) (0.55) K 0.659. [CH ][HS] K [H

More information

SPLINE ESTIMATION OF SINGLE-INDEX MODELS

SPLINE ESTIMATION OF SINGLE-INDEX MODELS SPLINE ESIMAION OF SINGLE-INDEX MODELS Li Wang and Lijian Yang University of Georgia and Mihigan State University Supplementary Material his note ontains proofs for the main results he following two propositions

More information

Section 3.4. Second Order Nonhomogeneous. The corresponding homogeneous equation. is called the reduced equation of (N).

Section 3.4. Second Order Nonhomogeneous. The corresponding homogeneous equation. is called the reduced equation of (N). Section 3.4. Second Order Nonhomogeneous Equations y + p(x)y + q(x)y = f(x) (N) The corresponding homogeneous equation y + p(x)y + q(x)y = 0 (H) is called the reduced equation of (N). 1 General Results

More information

Simple FIR Digital Filters. Simple FIR Digital Filters. Simple Digital Filters. Simple FIR Digital Filters. Simple FIR Digital Filters

Simple FIR Digital Filters. Simple FIR Digital Filters. Simple Digital Filters. Simple FIR Digital Filters. Simple FIR Digital Filters Simple Digital Filters Later in the ourse we shall review various methods of designing frequeny-seletive filters satisfying presribed speifiations We now desribe several low-order FIR and IIR digital filters

More information

Chapter 15 Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium 2/3/2014

Chapter 15 Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium 2/3/2014 Amount of reatant/produt //01 quilibrium in Chemial Reations Lets look bak at our hypothetial reation from the kinetis hapter. A + B C Chapter 15 quilibrium [A] Why doesn t the onentration of A ever go

More information

The simulation analysis of the bridge rectifier continuous operation in AC circuit

The simulation analysis of the bridge rectifier continuous operation in AC circuit Computer Appliations in Eletrial Engineering Vol. 4 6 DOI 8/j.8-448.6. The simulation analysis of the bridge retifier ontinuous operation in AC iruit Mirosław Wiślik, Paweł Strząbała Kiele University of

More information

TENSOR FORM OF SPECIAL RELATIVITY

TENSOR FORM OF SPECIAL RELATIVITY TENSOR FORM OF SPECIAL RELATIVITY We begin by realling that the fundamental priniple of Speial Relativity is that all physial laws must look the same to all inertial observers. This is easiest done by

More information

LONGITUDINAL NATURAL FREQUENCIES OF RODS AND RESPONSE TO INITIAL CONDITIONS Revision B

LONGITUDINAL NATURAL FREQUENCIES OF RODS AND RESPONSE TO INITIAL CONDITIONS Revision B By Tom Irvine Email: tomirvine@aol.om ONGITUDINA NATURA FREQUENCIES OF RODS AND RESPONSE TO INITIA CONDITIONS Revision B Marh 4, 009 Consider a thin rod. E, A, m E is the modulus of elastiity. A is the

More information

Theory. Coupled Rooms

Theory. Coupled Rooms Theory of Coupled Rooms For: nternal only Report No.: R/50/TCR Prepared by:. N. taey B.., MO Otober 00 .00 Objet.. The objet of this doument is present the theory alulations to estimate the reverberant

More information

MA2331 Tutorial Sheet 5, Solutions December 2014 (Due 12 December 2014 in class) F = xyi+ 1 2 x2 j+k = φ (1)

MA2331 Tutorial Sheet 5, Solutions December 2014 (Due 12 December 2014 in class) F = xyi+ 1 2 x2 j+k = φ (1) MA2331 Tutorial Sheet 5, Solutions. 1 4 Deember 214 (Due 12 Deember 214 in lass) Questions 1. ompute the line integrals: (a) (dx xy + 1 2 dy x2 + dz) where is the line segment joining the origin and the

More information

Analytical Study of Stability of Systems of ODEs

Analytical Study of Stability of Systems of ODEs D. Keffer, ChE 55,Universit of Tennessee, Ma, 999 Analtial Stud of Stabilit of Sstems of ODEs David Keffer Department of Chemial Engineering Universit of Tennessee, Knoxville date begun: September 999

More information

Intermediate Math Circles November 18, 2009 Solving Linear Diophantine Equations

Intermediate Math Circles November 18, 2009 Solving Linear Diophantine Equations 1 University of Waterloo Faulty of Mathematis Centre for Eduation in Mathematis and Computing Intermediate Math Cirles November 18, 2009 Solving Linear Diophantine Equations Diophantine equations are equations

More information

Math 225B: Differential Geometry, Homework 6

Math 225B: Differential Geometry, Homework 6 ath 225B: Differential Geometry, Homework 6 Ian Coley February 13, 214 Problem 8.7. Let ω be a 1-form on a manifol. Suppose that ω = for every lose urve in. Show that ω is exat. We laim that this onition

More information

Overview. Review Multidimensional PDEs. Review Diffusion Solutions. Review Separation of Variables. More diffusion solutions February 2, 2009

Overview. Review Multidimensional PDEs. Review Diffusion Solutions. Review Separation of Variables. More diffusion solutions February 2, 2009 More diffusion solutions February, 9 More Diffusion Equation Solutions arry Caretto Mechanical Engineering 5B Seinar in Engineering Analysis February, 9 Overview Review last class Separation of variables

More information

Advanced Computational Fluid Dynamics AA215A Lecture 4

Advanced Computational Fluid Dynamics AA215A Lecture 4 Advaned Computational Fluid Dynamis AA5A Leture 4 Antony Jameson Winter Quarter,, Stanford, CA Abstrat Leture 4 overs analysis of the equations of gas dynamis Contents Analysis of the equations of gas

More information

Math 211. Substitute Lecture. November 20, 2000

Math 211. Substitute Lecture. November 20, 2000 1 Math 211 Substitute Lecture November 20, 2000 2 Solutions to y + py + qy =0. Look for exponential solutions y(t) =e λt. Characteristic equation: λ 2 + pλ + q =0. Characteristic polynomial: λ 2 + pλ +

More information

Convergence of the Logarithmic Means of Two-Dimensional Trigonometric Fourier Series

Convergence of the Logarithmic Means of Two-Dimensional Trigonometric Fourier Series Bulletin of TICMI Vol. 0, No., 06, 48 56 Convergene of the Logarithmi Means of Two-Dimensional Trigonometri Fourier Series Davit Ishhnelidze Batumi Shota Rustaveli State University Reeived April 8, 06;

More information

Electric Circuit Theory

Electric Circuit Theory Electric Circuit Theory Nam Ki Min nkmin@korea.ac.kr 010-9419-2320 Chapter 8 Natural and Step Responses of RLC Circuits Nam Ki Min nkmin@korea.ac.kr 010-9419-2320 8.1 Introduction to the Natural Response

More information

19.3 SPECTROSCOPY OF ALDEHYDES AND KETONES

19.3 SPECTROSCOPY OF ALDEHYDES AND KETONES 19.3 PETRPY F ALDEHYDE AND KETNE 895 d 33 d+ bond dipole of the bond EPM of aetone Beause of their polarities, aldehydes and ketones have higher boiling points than alkenes or alkanes with similar moleular

More information

Waveguides. Parallel plate waveguide Rectangular Waveguides Circular Waveguide Dielectric Waveguide

Waveguides. Parallel plate waveguide Rectangular Waveguides Circular Waveguide Dielectric Waveguide Waveguides Parallel plate waveguide Retangular Waveguides Cirular Waveguide Dieletri Waveguide 1 Waveguides In the previous hapters, a pair of ond utors was used to guide eletromagne ti wave propagation.

More information

Subject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % (

Subject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % ( 16.50 Leture 0 Subjet: Introdution to Component Mathing and Off-Design Operation At this point it is well to reflet on whih of the many parameters we have introdued (like M, τ, τ t, ϑ t, f, et.) are free

More information

Selection of 'optimal' poles for SISO pole placement design: SRL LQR design example Prediction and current estimators

Selection of 'optimal' poles for SISO pole placement design: SRL LQR design example Prediction and current estimators L5: Leture 5 Symmetri Root Lous LQR Design State Estimation Seletion of 'otimal' oles for SISO ole laement design: SRL LQR design examle Predition and urrent estimators L5:2 Otimal ole laement for SISO

More information

C R. Consider from point of view of energy! Consider the RC and LC series circuits shown:

C R. Consider from point of view of energy! Consider the RC and LC series circuits shown: ircuits onsider the R and series circuits shown: ++++ ---- R ++++ ---- Suppose that the circuits are formed at t with the capacitor charged to value. There is a qualitative difference in the time development

More information

ELECTROMAGNETIC WAVES

ELECTROMAGNETIC WAVES ELECTROMAGNETIC WAVES Now we will study eletromagneti waves in vauum or inside a medium, a dieletri. (A metalli system an also be represented as a dieletri but is more ompliated due to damping or attenuation

More information

Worked Solutions to Problems

Worked Solutions to Problems rd International Cheistry Olypiad Preparatory Probles Wored Solutions to Probles. Water A. Phase diagra a. he three phases of water oeist in equilibriu at a unique teperature and pressure (alled the triple

More information

Math : Solutions to Assignment 10

Math : Solutions to Assignment 10 Math -3: Solutions to Assignment. There are two tanks. The first tank initially has gallons of pure water. The second tank initially has 8 gallons of a water/salt solution with oz of salt. Both tanks drain

More information

(Newton s 2 nd Law for linear motion)

(Newton s 2 nd Law for linear motion) PHYSICS 3 Final Exaination ( Deeber Tie liit 3 hours Answer all 6 questions You and an assistant are holding the (opposite ends of a long plank when oops! the butterfingered assistant drops his end If

More information

Complete Shrimp Game Solution

Complete Shrimp Game Solution Complete Shrimp Game Solution Florian Ederer Feruary 7, 207 The inverse demand urve is given y P (Q a ; Q ; Q ) = 00 0:5 (Q a + Q + Q ) The pro t funtion for rm i = fa; ; g is i (Q a ; Q ; Q ) = Q i [P

More information

6 Second Order Linear Differential Equations

6 Second Order Linear Differential Equations 6 Second Order Linear Differential Equations A differential equation for an unknown function y = f(x) that depends on a variable x is any equation that ties together functions of x with y and its derivatives.

More information

To work algebraically with exponential functions, we need to use the laws of exponents. You should

To work algebraically with exponential functions, we need to use the laws of exponents. You should Prealulus: Exponential and Logisti Funtions Conepts: Exponential Funtions, the base e, logisti funtions, properties. Laws of Exponents memorize these laws. To work algebraially with exponential funtions,

More information

Journal of Inequalities in Pure and Applied Mathematics

Journal of Inequalities in Pure and Applied Mathematics Journal of Inequalities in Pure and Applied Mathematis A NEW ARRANGEMENT INEQUALITY MOHAMMAD JAVAHERI University of Oregon Department of Mathematis Fenton Hall, Eugene, OR 97403. EMail: javaheri@uoregon.edu

More information

Math53: Ordinary Differential Equations Autumn 2004

Math53: Ordinary Differential Equations Autumn 2004 Math53: Ordinary Differential Equations Autumn 2004 Unit 2 Summary Second- and Higher-Order Ordinary Differential Equations Extremely Important: Euler s formula Very Important: finding solutions to linear

More information

Periodic functions: simple harmonic oscillator

Periodic functions: simple harmonic oscillator Periodic functions: simple harmonic oscillator Recall the simple harmonic oscillator (e.g. mass-spring system) d 2 y dt 2 + ω2 0y = 0 Solution can be written in various ways: y(t) = Ae iω 0t y(t) = A cos

More information

µ Differential Equations MAΘ National Convention 2017 For all questions, answer choice E) NOTA means that none of the above answers is correct.

µ Differential Equations MAΘ National Convention 2017 For all questions, answer choice E) NOTA means that none of the above answers is correct. µ Differential Equations MAΘ National Convention 07 For all questions, answer choice E) NOTA means that none of the above answers is correct.. C) Since f (, ) = +, (0) = and h =. Use Euler s method, we

More information

max min z i i=1 x j k s.t. j=1 x j j:i T j

max min z i i=1 x j k s.t. j=1 x j j:i T j AM 221: Advaned Optimization Spring 2016 Prof. Yaron Singer Leture 22 April 18th 1 Overview In this leture, we will study the pipage rounding tehnique whih is a deterministi rounding proedure that an be

More information

Section 3.4. Second Order Nonhomogeneous. The corresponding homogeneous equation

Section 3.4. Second Order Nonhomogeneous. The corresponding homogeneous equation Section 3.4. Second Order Nonhomogeneous Equations y + p(x)y + q(x)y = f(x) (N) The corresponding homogeneous equation y + p(x)y + q(x)y = 0 (H) is called the reduced equation of (N). 1 General Results

More information

ENGI Second Order Linear ODEs Page Second Order Linear Ordinary Differential Equations

ENGI Second Order Linear ODEs Page Second Order Linear Ordinary Differential Equations ENGI 344 - Second Order Linear ODEs age -01. Second Order Linear Ordinary Differential Equations The general second order linear ordinary differential equation is of the form d y dy x Q x y Rx dx dx Of

More information

Earlier Lecture. This gas tube is called as Pulse Tube and this phenomenon is called as Pulse Tube action.

Earlier Lecture. This gas tube is called as Pulse Tube and this phenomenon is called as Pulse Tube action. 31 1 Earlier Leture In te earlier leture, we ave seen a Pulse Tube (PT) ryoooler in wi te meanial displaer is removed and an osillating gas flow in te tin walled tube produes ooling. Tis gas tube is alled

More information

HIGHER SECONDARY FIRST YEAR MATHEMATICS

HIGHER SECONDARY FIRST YEAR MATHEMATICS HIGHER SECONDARY FIRST YEAR MATHEMATICS ANALYTICAL GEOMETRY Creative Questions Time :.5 Hrs Marks : 45 Part - I Choose the orret answer 0 = 0. The angle between the straight lines 4y y 0 is a) 0 30 b)

More information

The Hanging Chain. John McCuan. January 19, 2006

The Hanging Chain. John McCuan. January 19, 2006 The Hanging Chain John MCuan January 19, 2006 1 Introdution We onsider a hain of length L attahed to two points (a, u a and (b, u b in the plane. It is assumed that the hain hangs in the plane under a

More information

The Effectiveness of the Linear Hull Effect

The Effectiveness of the Linear Hull Effect The Effetiveness of the Linear Hull Effet S. Murphy Tehnial Report RHUL MA 009 9 6 Otober 009 Department of Mathematis Royal Holloway, University of London Egham, Surrey TW0 0EX, England http://www.rhul.a.uk/mathematis/tehreports

More information

( ) ( ) Volumetric Properties of Pure Fluids, part 4. The generic cubic equation of state:

( ) ( ) Volumetric Properties of Pure Fluids, part 4. The generic cubic equation of state: CE304, Spring 2004 Leture 6 Volumetri roperties of ure Fluids, part 4 The generi ubi equation of state: There are many possible equations of state (and many have been proposed) that have the same general

More information

Review for Ma 221 Final Exam

Review for Ma 221 Final Exam Review for Ma 22 Final Exam The Ma 22 Final Exam from December 995.a) Solve the initial value problem 2xcosy 3x2 y dx x 3 x 2 sin y y dy 0 y 0 2 The equation is first order, for which we have techniques

More information

Symmetric Root Locus. LQR Design

Symmetric Root Locus. LQR Design Leture 5 Symmetri Root Lous LQR Design State Estimation Seletion of 'otimal' oles for SISO ole laement design: SRL LQR design examle Predition and urrent estimators L5:1 L5:2 Otimal ole laement for SISO

More information