User:Egm6321.f09/Lecture plan

"What's the application?" lesson 2

= All versions =

Fall 2011, Fall 2010, Fall 2009

= Recorded lectures, TA user page =

Recorded lectures in E-Learning at UF (password required): Click Continue, type username and password, click at EGM 6321, click Course Content; at "Lecture Videos" link, click at drop down menu, then select "Preview" to go to the web page with lecture video links.

TA user page: Summary of HW statements, for students to interact with TA.

= Lecture transparencies, report table =

These

Lecture Transparencies were written in real time during the lectures (i.e., not prepared ahead of the lectures). Additional presentations (video, wiki, static html) made in class may not be recorded on these transparencies.

djvu: (install the viewers evince or DjView4) [[media:egm6321.f09.mtg1.djvu|Mtg 1]], [[media:egm6321.f09.mtg2.djvu|Mtg 2]], [[media:egm6321.f09.mtg3.djvu|Mtg 3]], [[media:egm6321.f09.mtg4.djvu|Mtg 4]], [[media:egm6321.f09.mtg5.djvu|Mtg 5]], [[media:egm6321.f09.mtg6.djvu|Mtg 6]], [[media:egm6321.f09.mtg7.djvu|Mtg 7]], [[media:egm6321.f09.mtg8.djvu|Mtg 8]], [[media:egm6321.f09.mtg9.djvu|Mtg 9]], [[media:egm6321.f09.mtg10.djvu|Mtg 10]], [[media:egm6321.f09.mtg11.djvu|Mtg 11]], [[media:egm6321.f09.mtg12.djvu|Mtg 12]], [[media:egm6321.f09.mtg13.djvu|Mtg 13]], [[media:egm6321.f09.mtg14.djvu|Mtg 14]], [[media:egm6321.f09.mtg15.djvu|Mtg 15]], [[media:egm6321.f09.mtg16.djvu|Mtg 16]], [[media:egm6321.f09.mtg17.djvu|Mtg 17]], [[media:egm6321.f09.mtg18.djvu|Mtg 18]], [[media:egm6321.f09.mtg19.djvu|Mtg 19]], [[media:egm6321.f09.mtg20.djvu|Mtg 20]], [[media:egm6321.f09.mtg21.djvu|Mtg 21]], [[media:egm6321.f09.mtg22.djvu|Mtg 22]], [[media:egm6321.f09.mtg23.djvu|Mtg 23]], [[media:egm6321.f09.mtg24.djvu|Mtg 24]], [[media:egm6321.f09.mtg25.djvu|Mtg 25]], Mtgs 26+27 Exam 1, [[media:egm6321.f09.mtg28.djvu|Mtg 28]], [[media:egm6321.f09.mtg29.djvu|Mtg 29]], [[media:egm6321.f09.mtg30.djvu|Mtg 30]], [[media:egm6321.f09.mtg31.djvu|Mtg 31]], [[media:egm6321.f09.mtg32.djvu|Mtg 32]], [[media:egm6321.f09.mtg33.djvu|Mtg 33]], [[media:egm6321.f09.mtg34.djvu|Mtg 34]], [[media:egm6321.f09.mtg35.djvu|Mtg 35]], [[media:egm6321.f09.mtg36.djvu|Mtg 36]], [[media:egm6321.f09.mtg37.djvu|Mtg 37]], [[media:egm6321.f09.mtg38.djvu|Mtg 38]], [[media:egm6321.f09.mtg39.djvu|Mtg 39]], [[media:egm6321.f09.mtg40.djvu|Mtg 40]], [[media:egm6321.f09.mtg41.djvu|Mtg 41]], Mtgs 42+43 Exam 2, [[media:egm6321.f09.mtg44.djvu|Mtg 44]],

Report table

Mourning the Death of Handwriting, By Claire Suddath. Time Magazine, Monday, Aug. 03, 2009.

Op-Art: The Write Stuff, by Inga Dubay and Barbara Getty, NY Times, 8 Sep 2009.

= References =

Books
$$\displaystyle \clubsuit$$ A.C. King, J. Billingham, S.R. Otto, Differential equations: Linear, nonlinear, ordinary, partial, Cambridge University Press, 2003. ISBN-10: 0521016878 ISBN-13: 978-0521016872. UF library 0511078315 (electronic bk.) Google books Amazon.com

$$\displaystyle \clubsuit$$ D. Zwillinger, Handbook of Differential Equations, Third Edition, Academic Press, 1998. ISBN-10: 0127843965. ISBN-13: 978-0127843964. UF library QA371.Z88 1989, 2 copies, one for in-library use. Google books Amazon.com

$$\displaystyle \clubsuit$$ O.D. Kellogg, Foundations of potential theory, Dover publications, 1954. UF library QA825 .K4x 1953 Google books Amazon.com

$$\displaystyle \clubsuit$$ P.M. Morse, H. Feshbach, Methods of theoretical physics, Parts I & II, McGraw-Hill, 1953. UF library QC20 .M6 google books amazon.com

$$\displaystyle \clubsuit$$ M. Abramowitz & I. Stegun, Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables, New York: Dover Publications, 1972. Read online, Download Wikipedia

$$\displaystyle \clubsuit$$ N.N. Lebedev, Special Functions & Their Applications, Dover Publications, 1972. ISBN 0486606244 (pbk). UF library QA351.L3613 1972 Google books Amazon.com

$$\displaystyle \clubsuit$$ K. Oldham, J. Myland, J. Spanier, An atlas of functions, 2nd edition, Springer, 2008. 1st edition, UF library QA331.S685 1987 google books amazon.com

$$\displaystyle \clubsuit$$ A.F. Nikiforov, S.K. Suslov, V.B. Uvarov, Classical Orthogonal Polynomials of a Discrete Variable, Springer, 1991. UF library QC20.7.O75N5513 1991 Google Amazon

Web references
$$\displaystyle \spadesuit$$ Related MIT OpenCourseWare courses

$$\displaystyle \spadesuit$$ Wolfram|Alpha is ... "learning resource available to your students at no cost that works as a computational knowledge engine. Wolfram|Alpha is not a search engine like Google or Yahoo!, because unlike a traditional search engine, Wolfram|Alpha has the capability to instantly compute the answer to previously unasked questions instead of scouring the web and returning links to pages that already exist. The results are displayed in an easy-to-read, understandable format that can be used as a primary source for educational and academic purposes."

$$\displaystyle \spadesuit$$ EqWorld, The World of Mathematical Equations. It is a good idea to verify the sources, as the site is not responsible for accuracy and correctness; see Rights and obligations of contributors and website administration.
 * 2nd-order linear ODEs
 * 2nd-order non-linear ODEs
 * ODE education

$$\displaystyle \spadesuit$$ ODE (Wikipedia): Be careful; always verify the sources.

Papers
$$\displaystyle \clubsuit$$ Vu-Quoc, L., and Olsson, M., Formulation of a basic building-block model for interaction of high-speed vehicles on flexible structures, ASME Journal of Applied Mechanics, Vol.56, No.2, pp.451-458, 1989. (pdf)

$$\displaystyle \clubsuit$$ Vu-Quoc, L., and Olsson, M., A computational procedure for interaction of high-speed vehicles on flexible structures without assuming known vehicle nominal motion, Computer Methods in Applied Mechanics and Engineering, Vol.76, pp.207-244, 1989. (pdf)

$$\displaystyle \clubsuit$$ Vu-Quoc, L., and Tran, V.X., Singularity analysis and fracture energy release rate for composites: Piecewise homogeneous-anisotropic materials, Computer Methods in Applied Mechanics and Engineering, John H. Argyris Memorial Issue, Vol.195, No.37-40, pp.5162-5197, 15 July 2006. (pdf)

= Motivation =

High-speed maglev trains
$$\displaystyle \clubsuit$$ German Transrapid (Maglev), electromagnetic (attraction) maglevs. German Transrapid Emsland 500 km/hr (video, 7:37 min) (500 / 1.6 = 312.5 mi / hr). The Transrapid story (video, history of development, electromagnetic systems vs electrodynamic systems): Part 1 (8:28 min) Part 2 (8:07 min).

Shanghai maglev train (video, 5:35 min).

Equations of motion for high-speed vehicles interacting with flexible guideways; see Vu-Quoc & Olsson (1989 a b ): Actually, system of coupled nonlinear 2nd-order ordinary differential equations and partial differential equations.

$$\displaystyle \clubsuit$$ Japanese Maglev, electrodynamic (repulsion) maglevs, with retractable wheels. Japanese maglev at 581 km/hr (video, 4:43 min) (581 / 1.6 = 363 mi / hr).

$$\displaystyle \clubsuit$$ French TGV speed record 574.8 km / hr = 357.2 mi / hr (non maglev, wheel-on-rail trains)

Debate on high-speed rail (Sep 2009)
Siemens Fills Russia’s Need for High-Speed Train, by A.E. Kramer, NY Times, September 24, 2009.

Stimulus Puts High-Speed Rail On The Fast Track, NPR, Morning Edition, 24 Feb 2009; audio 4:10 min.

States Make Pitches For High-Speed-Rail Money, NPR, All Things Considered, 21 Aug 09, audio 7:42 min.

California Edges Ahead In High-Speed-Train 'Race', NPR, All Things Considered, 3 Sep 09.

High-Speed Rail Skeptic Outlines Position, NPR, All Things Considered, 3 Sep 09.

More with Google search for "NPR high speed rail"

Equations of motion
Coupled nonlinear 2nd-order ODE and PDEs with varying coefficients, which depend on the unknown functions to be solved for. Particularization to linear 2nd-order ODEs with varying coefficients.

= Linear 2nd-order ODEs with varying coefficients (L2-ODE-VC) =

Even though this section is about linear 2nd-order ODEs with varying coefficients, many of the methods listed in this section apply to nonlinear ODEs in general, with linear ODEs as particular cases. We present the general nonlinear case first, then particularize to the linear case.

Helmholtz equation (PDE)
Helmholtz equation (Wikipedia)

Vibrating membranes
Wolfram: Acoustics demos Vibrations of a rectangular membrane

Vibration of circular membrane, animation, Wolfram demo Bessel function Jn Bessel function J2, WolframAlpha

Chladni figures Chladni patterns (youtube) Chladni patterns on a vibrating plate excited by an acoustic speaker

Acoustics of drums, by T.D. Rossling, Physics Today, Vol.45, No.3, pp.40-47, Mar 1992.

Ansatz (wikipedia): A guessed expression for the solution, as in trial solution.

Helmholtz equation (Wikipedia)

Irrotational, compressible, non-viscous fluids
Morse & Feshbach (1953), p.307

Sound field animations, D.A. Russell, Kettering University.

One-dimensional wave equation
Morse & Feshbach (1953), p.125

Three-dimensional wave equation
Morse & Feshbach (1953), p.509, p.523

Ellipsoidal coordinates
Elliptic coordinates (Wikipedia) Ellipsoidal coordinates (Wikipedia) Hyperboloid (Wikipedia)

Morse & Feshbach (1953), p.512

Separated equations: L2-ODC-VC (1)
Morse & Feshbach (1953), p.523

Reduction of order method 0: Missing dependent variable
Zwillinger (1998), Sec 55

Integrating-factor method (1)
Zwillinger (1998), Sec 79

General L1-ODE-VC (2)
See General L1-ODE-VC (1).

Reduction of order method 1: Exact nonlinear ODEs
Zwillinger (1998), Sec 63: Applicable to nonlinear ODEs, in particular linear 2nd-order ODEs.

Nonlinear 1st-order ODEs (2)
See Nonlinear 1st-order ODEs (N1-ODEs) (1) and Integrating-factor method: Nonlinear 1st-order ODEs

Legendre L2-ODE-VC (1)
King et al. (2003), p.31

Nonlinear nth-order ODEs
Zwillinger (1998), Sec 63, p.289

General Nn-ODEs
$$F(x, y^{(0)}, y^{(1)}, \ldots, y^{(n)}) = 0$$

Application: N3-ODE
involving $$f_i := \partial F / \partial y^{(i)} $$.

Superposition of solution for L2-ODE-VC
Here, we treat the cases in which at least a solution (homogeneous or particular) can be guessed by inspection; the other solution can then be generated from the guessed solution.

For the cases in which the solutions cannot be guessed by inspection, see Solution by power series: Frobenius method.

Euler equations: Special homogeneous Ln-ODE-VC
Zwillinger (1998), Sec 61

Method of trial solution (undetermined coefficients)
This method is also known as the method of undertermined coefficients; the terminology "trial solution" is more descriptive since the method involves guessing the solution mathematical expression, called the trial solution, which have unknown coefficients to be determined by substituting the trial solutions into the differential equation.

King et al. (2003), Appendix 5

Zwillinger (1998), Sec 94

Wikipedia

Reduction of order method 2: Undetermined factor (1)
King et al. (2003), p.5

Zwillinger (1998), Sec 85

Non-homogeneous L2-ODE-VC
Zwillinger (1998), Sec 94

Non-homogeneous L2-ODE-CC
Boyce & DiPrima

Variation of parameters
King et al. (2003), p.7 Zwillinger (1998), Sec 95

Solution by power series: Frobenius method (1)
Zwillinger (1998), Sec 90

Singular points
18.305 Advanced Analytic Methods in Science and Engineering Fall 2004, Lecture 6 (pdf)

Regular singular points
18.305 Advanced Analytic Methods in Science and Engineering Fall 2004, Lecture 7 (pdf)

Irregular singular points
18.305 Advanced Analytic Methods in Science and Engineering Fall 2004, Lecture 8 (pdf)

= Legendre functions =

Kellogg (1953), p.125 King et al. (2003), p.31

Coefficients of series solution
Lecture transparency p.33-1, Eq.(2) and Eq.(5):



\displaystyle \langle f, P_m \rangle =  \int\limits_{\theta = -\pi/2}^{\theta = \pi/2} f (\theta) P_m (\sin \theta) d (\sin \theta) =  \int\limits_{\mu = -1}^{\mu = 1} f (\mu) P_m (\mu) d (\mu) $$

Integration involving transcendental functions: Abramovitz & Stegun, p.77

Bessel differential equation (1)
King et al. (2003), p.80

Application: Gauss-Legendre quadrature
Gauss quadrature (wikipedia) Legendre polynomials (wikipedia) Abramovitz & Stegun, p.887 Abramovitz & Stegun, Table 25.4, p.916

"What's the application?" lesson 2
3 Americans Share Nobel for Medicine, By Nicholas Wade, NY Times, Published: October 5, 2009.

Legendre polynomials
Legendre polynomials (wikipedia)

Axisymmetric case
Using the astronomy convention for spherical coordinates, the general solution for the Laplace equation before applying any boundary conditions is:

$$\psi (r,\theta) = \sum_{n} \left(A_n r^n + B_n r^{-(n+1)} \right ) \left[ C_n P_n (\mu) + D_n Q_n (\mu) \right ] \, \quad \mu := \sin \theta$$

Laplace equation in spherical coordinates
Fluid flow experiment around a cylinder (video) (not a sphere, but the streamlines are similar to those of a flow around a sphere)

Moving cylinder in a fluid (video)

Bypassing 2nd homogeneous solution
King et al. (2003), p.44

Rodrigues's formula
Olinde Rodrigues (1795-1851)

= Unified general theory of classical orthogonal functions =

Nikiforov et al. (1991), Chap 1.

Orthogonality
= Boundary value problems =

= Asymptotic methods =

= Other nonlinear ODEs =

Van der Pol equation
Scholarpedia

= Simulations =

An asteroid breakup 160 Myr ago as the probable source of the K/T impactor, William F. Bottke, David Vokrouhlický & David Nesvorný, Nature 449, 48-53 (6 September 2007).

Asteroids: Spun in the sun, William F. Bottke, Nature 446, 382-383 (22 March 2007).

Asteroids: How to make a flying saucer, William F. Bottke, Nature 454, 173-174 (10 July 2008).

Asteroid, NASA. Pictures of asteroids Ida, Eros, and Chicxulub (Yucatan) impact, extinction of dinausaurs.

Large asteroid impacting the Earth, simulation

Hubble Space Telescope Captures Rare Jupiter Collision, 07.24.09

Near Earth Objects Program, JPL.

Solar system collision: Set Target Earth (land only), Projectile Rock, Projectile diameter 10 km, Projectile velocity 60 km / sec; click Kaboom; see photo of Chicxulub impact.