Edwards-Penney, sections 5.4, 10.1, 10.2, 10.3 The textbook topics, definitions and theorems

Edwards-Penney 5.1, 5.2, 5.3, 5.4 (15.6 K, txt, 23 Dec 2012)

Edwards-Penney 10.1, 10.2, 10.3, 10.4, 10.5 (20.5 K, txt, 03 Mar 2013)

PROBLEM SESSIONChapter 4 exercises. 4.7 Independence. Classify as indep/dep. Cite these results. THEOREM. Any set of distinct Euler solution atoms is independent. THEOREM. Wronskian determinant nonzero => functions in Wronskian row 1 are independent. THEOREM. Subsets of independent sets are independent. THEOREM. S1 is a finite list of k vectors. S2 is a finite list of k vectors (the same number). span(S1) = span(S2) If S2 is independent, then S1 is also independent. 4.7-13: sin x, cos x 4.7-14: exp(x), x exp(x) 4.7-15: 1+x,1-x, 1-x^2 [This is S1. Verify S2 = 1,x,x^2 works in the theorem.] 4.7-16: 1+x, x+x^2, 1-x^2 4.7-17: cos 2x, sin^2 x, cos^2 x 4.7-18: 2 cos x + 3 sin x, 4 cos x + 5 sin x [This is S1. What is S2?]

Second order and higher order differential Equations.Application. LRC circuit equation. LQ'' + RQ' + (1/C)Q = 0 LI'' + RI' + I/C = 0. The RLC circuit diagram and the physical parameters. Forcing terms in electrical systems. Battery. Generator. LRC-circuit DE derivation. Voltage drop laws of Faraday, Ohm, Coulomb. Kirchoff's laws. Electrical-mechanical analogy.: Electrical circuits (124.8 K, pdf, 04 Mar 2012)SlidesDetailed look at the second order caseREF. Theorems 1,2,3 in section 5.3 of Edwards-Penney. Quadratic equations again. Constant-coefficient second order homogeneous differential equations. Characteristic equation and its factors determine the atoms. The three possible cases 1. Two real roots 2. Two equal real roots 3. A complex conjugate pair of roots The three possible kinds of solutions 1. y=c1 exp(r1 x) + c2 exp(r2 x) If one root is zero, then the exponential equals 1. 2. y=c1 exp(r1 x) + c2 x exp(r1 x) 3. y= c1 exp(ax) cos(bx) + c2 exp(ax) sin(bx) If in root a+ib, the real part a=0, then this is a pure harmonic oscillation [because exp(ax)=1] y= c1 cos(bx) + c2 sin(bx) Sample equations: y''=0, y''+2y'+y=0, y''-4y'+4y=0, y'' + 3y' + 2y=0, x'' + x = 0, x'' + 2x' + 5x = 0, x'' + 8x' + 16x=0, 0.03I'' + 0.005 I = 0, Q'' + 100Q=0, REVIEW OF SECTIONS 5.1, 5.2, 5.3 PROBLEM TYPES. Example: Linear DE given by roots of the characteristic equation. Example: Linear DE given by factors of the characteristic polynomial. Example: Construct a linear DE of order 2 from a list of two atoms that are known to be solutions. Example: Construct a linear DE from characteristic equation roots. Example: Construct a linear DE from its general solution. COMPLEX ROOTS of the CHARACTERISTIC EQUATION Solving a DE when the characteristic equation has complex roots. Equations with both real roots and complex roots. (D^4 + D^2)y = 0, (D+1)^2(D^2+4)^2 y = 0 An equation with 4 complex roots. How to find the 4 atoms. (D^2+4)(D^2+16)y=0 SHORTCUT. One pair of complex conjugate roots identifies two Euler solution atoms. Only one of the two complex roots is required to construct the two atoms.Drill Partial Fractionstop=x-1, bot=(x+1)(x^2+4) top/bot = A/(x+1)+(Bx+C)/(x^2+4); find A,B,C. Sampling in partial fractions. Method of atoms in partial fractions. Heaviside's coverup method. Maple example with 6 constants top:=x-1; bottom:=(x+1)^2*(x^2+1)^2; convert(top/bottom,parfrac,x);

Slides on Section 5.4Damped oscillations overdamped, critically damped, underdamped, pseudo-period [Chapter 5] phase-amplitude form of the solution [chapter 5] Cafe door. Pet door. Undamped oscillations. Harmonic oscillator.: phase-amplitude, cafe door, pet door, damping classification (148.4 K, pdf, 03 Mar 2013)SlidesPartly solved 5.4-20See the FAQ at the web site for answers and details.: FAQ for section 5.4 (4.7 K, txt, 05 Dec 2012) The problem breaks into two distinct initial value problems: (1) 2x'' + 16x' + 40x=0, x(0)=5, x'(0)=4 Characteristic equation 2(r^2+8r+20)=0. Roots r=-4+2i,r=-4-2i. Solution Atoms=e^{-4t}cos 2t, e^{-4t}sin 2t. UNDERDAMPED. (2) 2x'' + 0x' + 40x=0, x(0)=5, x'(0)=4 Characteristic equation 2(r^2+0+20)=0. Roots r=sqrt(20)i,r=-sqrt(20)i. The Euler solution atoms are cos( sqrt(20)t), sin( sqrt(20)t). UNDAMPED HARMONIC OSCILLATION. Each system has general solution a linear combination of Euler solution atoms. Evaluate the constants in the linear combination, in each of the two cases, using the initial conditions x(0)=5, x'(0)=4. There are two linear algebra problems to solve. Answers: (1) Coefficients 5, 2 for 2x'' + 16x' + 40x=0 Amplitude = sqrt(5^2 + 12^2) = 13 (2) Coefficients 5, 2/sqrt(5) for 2x'' + 0x' + 40x=0 Amplitude = sqrt(5^2 + 4/5) = sqrt(129/5) Plots can be made from these answers directly. Write each solution in phase-amplitude form, a trig problem. See section 5.4 for specific instructions. The book's answers: (1) tan(alpha) = 5/12 (2) tan(alpha) = 5 sqrt(5)/2TextPartly solved 5.4-34.See the FAQ at the web site for answers and details.: FAQ for section 5.4 (4.7 K, txt, 05 Dec 2012) The DE is 3.125 x'' + cx' + kx=0. The characteristic equation is 3.125r^2 + cr + kr=0 which factors into 3.125(r-a-ib)(r-a+ib)=0 having complex roots a+ib, a-ib. Problems 32, 33 find the numbers a, b from the given information. This is an inverse problem, one in which experimental data is used to discover the differential equation model. The book uses its own notation for the symbols a,b: a ==> -p and b ==> omega1. Because the two roots a+ib, a-ib determine the quadratic equation, then c and k are known in terms of symbols a,b. References: Sections 5.4, 5.6. Forced oscillations.Text: Unforced vibrations 2008 (667.9 K, pdf, 03 Mar 2012)Slides: phase-amplitude, cafe door, pet door, damping classification (148.4 K, pdf, 03 Mar 2013)Slides: Forced undamped vibrations (214.2 K, pdf, 03 Mar 2012)Slides: Forced damped vibrations (280.7 K, pdf, 04 Mar 2012)Slides: Forced vibrations and resonance (240.3 K, pdf, 04 Mar 2012)Slides: Undetermined coefficients, pure resonance, practical resonance (152.8 K, pdf, 03 Mar 2013)Slides: Electrical circuits (124.8 K, pdf, 04 Mar 2012)Slides

More exam 2 review, problems 4,5Lecture: Basic Laplace theory.Reading: Chapter 10. Read 5.5, 5.6, ch6, ch7, ch8, ch9 later. Direct Laplace transform == Laplace integral. Def: Direct Laplace transform == Laplace integral == int(f(t)exp(-st),t=0..infinity) == L(f(t)).Introduction and History of Laplace's methodPhotos of Newton and Laplace: portraits of the Two Greats.: Laplace and Newton calculus. Photos of Newton and Laplace. (200.2 K, pdf, 04 Mar 2012) The method of quadrature for higher order equations and systems. Calculus for chapter one quadrature versus the Laplace calculus. The Laplace integrator dx=exp(-st)dt. The abbreviation L(f(t)) for the Laplace integral of f(t). Lerch's cancelation law and the fundamental theorem of calculus.SlidesIntro to Laplace Theory: Intro to Laplace theory. Calculus assumed. (163.0 K, pdf, 19 Mar 2012) A Brief Laplace Table 1, t, t^2, t^n, exp(at), cos(bt), sin(bt) Some Laplace rules: Linearity, Lerch Laplace's L-notation and the forward tableSlidesLaplace theory references: Laplace and Newton calculus. Photos. (200.2 K, pdf, 04 Mar 2012)Slides: Intro to Laplace theory. Calculus assumed. (163.0 K, pdf, 19 Mar 2012)Slides: Laplace theory 2008 (351.3 K, pdf, 09 Apr 2013)Manuscript: Laplace rules (160.3 K, pdf, 04 Mar 2012)Slides: Laplace table proofs (169.6 K, pdf, 04 Mar 2012)Slides: Laplace examples (149.1 K, pdf, 04 Mar 2012)Slides: Piecewise functions and Laplace theory (108.5 K, pdf, 03 Mar 2013)Slides: Maple Lab 7. Laplace applications (156.0 K, pdf, 04 Dec 2012)MAPLE: Laplace resolvent method (88.1 K, pdf, 04 Mar 2012)Slides: Cable hoist example (73.2 K, pdf, 21 Aug 2008)Slides: Sliding plates example (105.8 K, pdf, 21 Aug 2008)Slides: Heaviside's method 2008 (186.8 K, pdf, 20 Oct 2009)Manuscript: DE systems, examples, theory (785.8 K, pdf, 16 Nov 2008)Manuscript: Laplace theory 2008 (351.3 K, pdf, 09 Apr 2013)Manuscript: Ch10 Laplace solutions 10.1 to 10.4 (1068.7 K, pdf, 28 Nov 2010)Transparencies: Laplace theory problem notes S2013 (17.2 K, txt, 03 Dec 2012)Text: Final exam study guide (8.2 K, txt, 05 Dec 2012)Text: Laplace second order systems (288.1 K, pdf, 04 Mar 2012)Slides

A brief Laplace table. Forward table. Backward table. Extensions of the Table. Laplace rules. Linearity. The s-differentiation theorem (d/ds)L(f(t))=L((-t)f(t)). Shift theorem. Parts theorem. Finding Laplace integrals using Laplace calculus. Solving differential equations by Laplace's method.Basic Theorems of Laplace TheoryFunctions of exponential order Existence theorem for Laplace integrals Euler solution atoms have a Laplace integral Lerch's theorem Linearity. The s-differentiation theorem (d/ds)L(f(t))=L((-t)f(t)). Shift theorem L(exp(at)f(t)) = L(f(t))|s->(s-a) Parts theorem L(y')=sL(y)-y(0)

Exam 2 review and Problem session on ch5 problems.Exam 2 review for problems 1,2,3,4,5.

History of the Laplace Transform REF: Deakin (1981), Development of the Laplace transform 1737 to 1937 EULER LAPLACE 1784 End of WWII 1945 Fourier Transform Mellin Transform and Gamma function Laplace transform: one-sided and 2-sided transform Applications: DE, PDE, difference equations, functional equations Diffusion equation for spatial diffusion problems Solving y' = -1, y(0)=2 [done on Wednesday] DEF. Gamma function DEF. Unit step u(t-a)=1 for t>=a, else zero DEF. Ramp t->(t-a)u(t-a) Backward table problems: examples Forward table problems: examples Computing Laplace integrals L(f(t)) with rules Solving an equation L(y(t))=expression in s for y(t) Complex roots and quadratic factors Partial fraction methods Trig identities and their use in Laplace calculations Hyperbolic functions and Laplace calculations Why the forward and backward tables don't have cosh, sinh entries