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Chapter 23 ODE (Ordinary Differential Equation) . Speaker: Lung-Sheng Chien. Reference: [1] Veerle Ledoux, Study of Special Algorithms for solving Sturm-Liouville and Schrodinger Equations.

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chapter 23 ode ordinary differential equation

Chapter 23 ODE (Ordinary Differential Equation)

Speaker: Lung-Sheng Chien

Reference: [1] Veerle Ledoux, Study of Special Algorithms for solving Sturm-Liouville and Schrodinger Equations.

[2] 陳振臺, university physics, lecture 5 [3] Harris Benson, university physics, chapter 15

slide2

Hook’s Law (虎克定律) [1]

在水平方向作用於系統的力量有二(見下圖) :

我們施於物體拉扯彈簧的力

彈簧作用於物體的力

若我們施力在物體上來壓縮彈簧 (見上圖),則彈簧作用於m的力量方向同樣地與我們的施力方向相反

彈簧作用於物體 (質量m)的力試圖將物體回復到平衡位置,無論彈簧是被拉扯或被壓縮,

它的方向總是朝向平衡位置稱為回復力,因為其作用在將質量回復到平衡位置處。

虎克定律:

彈性係數和物體無關

slide3

Hook’s Law (虎克定律) [2]

如左圖所示,物體被固定於x之位置

彈簧作用於m的力與彈簧被拉扯或被壓縮的量成正比,且方向總是朝向平衡位置

我們由一個物體m繫於一個理想彈簧上開始,而此系統為在水平無摩擦的表面上。我們將此質量向右拉一個距離為,然後在物體靜止時突然 ( 瞬間地 ) 釋放,如左圖所示。

當彈簧力為唯一作用於m的力量,且朝著一個指定的方向,此時m的振盪運動就是簡諧振盪,並且其排列被稱之為簡諧振子 (simple harmonic oscillator)。

平衡點右側

牛頓第二運動定律:

平衡點左側

slide4

Hook’s Law (虎克定律) [3]

dimension analysis

We must match dimension of each term in the equation

Period (周期)

Definition:

振盪的角頻率(angular frequency),單位為 rad/s

guess

or

We need two constraints to determine unknown constant

1

Initial position:

2

Initial velocity:

where

slide5

Hook’s Law (虎克定律) [4]

Simple Harmonic Oscillation:

is shifted by phase constant

is phase (相位)

the argument

measured in radians (弧度)

Question 1: why do we guess

in equation

Question 2: where do two constant A, B (or C,D) come from?

Question 3: is the solution unique?

slide6

ODE [1]

First order linear ODE:

1

is first derivative.

First order : highest degree of differential operation

2

, then operator is linear, say

Linear : define operator

integration along curve

Observation1: when initial time is determined and initial condition

is unique

is given, then solution

However when initial condition is specified, then initial time is determined at once, hence we say

is one-parameter family, with parameter

First order linear ODE system of dimension two:

3

ODE system: more than one equation

4

system of dimension two: two equations

solution is

since system is de-couple

slide7

ODE [2]

has unique solution if two initial conditions are specified

for square matrix A

we define

implies

let

, then

Observation 2: ODE system of dimension two needs two initial conditions

, then

is unique solution of

Observation 3: if we write

we may guess that

for any square matrix A

is unique solution of

slide8

ODE [3]

Simple Harmonic Oscillation:

where

since initial velocity would also affect

Intuition: we CANNOT determine

by given initial position

It is well-known when you are in junior high school, not only free fall experiment but sliding car experiment.

Transformation between second order ODE and first order ODE system of dimension two

Define velocity

, then combine Newton’ second Law

, we have

we need two initial condition to have unique solution

From Symbolic toolbox in MATLAB, we can diagonalize matrix

MATLAB code

where

slide9

ODE [4]

Formal deduction:

with initial condition

Definition: fundamental matrix

then solution can be expressed by fundamental matrix and initial condition

From Symbolic toolbox in MATLAB,

we can compute fundamental matrix easily

slide10

ODE [5]

is composed of two fundamental solutions

fundamental matrix

is solution of

with initial condition

is solution of

with initial condition

with initial condition

is linear combination of fundamental solutions

solution of

The space of solutions of

is

The dimension of solution space is two,

slide11

ODE [6]

In order to achieve uniqueness, we need to specify two integration constant

Integral equation:

differential equation:

Existence and uniqueness (Contraction mapping principle)

Let

be continuous space equipped with norm

1

is complete under norm

2

by

define a mapping

then

Existence and uniqueness

is a contraction mapping if

slide12

ODE [7]

(ignore buoyancy 浮力)

recover force is opposite to displacement

resistive force is also opposite to displacement

Newton second’s Law:

1

what is equivalent ODE system of

2

what is fundamental matrix of this ODE system, use symbolic toolbox in MATALB

3

what is solution of

with initial condition

4

Can you use “contraction mapping principle” to prove existence and uniqueness?

slide13

ODE [7]

general solution

We have two choices to determine unknown constants A and B

1

initial condition

2

boundary condition

period

1

become discrete?

Why does angular frequency

What is physical meaning of discrete angular frequency?

2

We have still a constant B not be determined, why?

slide14

Schrodinger equation [1]

energy

is angular frequency

photon (光子):

is wave number

momentum

http://en.wikipedia.org/wiki/Matter_wave

Louis de Broglie in 1924 in his PhD thesis claims that “matter (object)” has the same relation as photon

de Broglie wavelength

de Broglie frequency of the wave

Fundamental of quantum mechanic:

matter wave (物質波) is described by wave length

and wave frequency

http://en.wikipedia.org/wiki/Schr%C3%B6dinger_equation

Erwin Schrödinger in 1926 proposed a differential equation (called Schrodinger equation) to describe atomic systems.

total energy of a particle

matter wave

and

time-dependent Schrodinger equation

slide15

Schrodinger equation [2]

Question: physical interpretation of matter wave

probability finding particle on interval

in time

total number of particles in time

Example: plane wave

particle has the same probability found in any position, not physical

time-dependent Schrodinger equation

by

remove t-dependence, replace

time-independent Schrodinger equation

(one-dimensional)

(three-dimensional)

Objective of time-independent Schrodinger equation: find a stationary solution satisfying

with proper boundary conditions

slide16

Schrodinger equation [3]

Example: Hydrogen atom (氫原子)

parameter

B.C.

http://hyperphysics.phy-astr.gsu.edu/hbase/hyde.html

discrete energy level:

http://www.touchspin.com/chem/SWFs/pt2k61012.swf

slide17

Schrodinger equation [4]

Time-independent Schrodinger equation

From dimensional analysis, we extract dimensionless quantities in this system

1

2

3

4

dimensionless form

Once characteristic length of the system is determined, for example

Then characteristic energy is

, this is near

slide18

Finite Difference Method [1]

First we consider one-dimensional problem (dimensionless form)

Finite Difference Method (有限差分法): divide interval

into N+1 uniform segments

labeled as

We approximate ODE on finite points, say we want to find a vector

satisfying

for

We don’t need to ask equation on end points, since equation only holds in interior

1

How to approximate second derivative

on grid points

2

How to achieve “solvability” though we know solution indeed exists in continuous sense

3

slide19

Finite Difference Method [2]

Definition: standard 3-point centered difference formula

we have

for some

is called local truncation error (LTE) since it is truncation from Taylor’s expansion

slide21

Finite Difference Method [4]

for

Example: n = 4

is real symmetric, then A is diagonalizable since eigenvalue of A is real

slide22

Finite Difference Method [5]

model problem: no potential ( V = 0 )

FDM

Question: can we find analytic formula for eigen-pair in this simple model problem?

solution is

solution is

FDM

for

Conjecture: we guess that eigenvector is

satisfies

(boundary condition)

Question: How about

for

slide23

Finite Difference Method [6]

model problem: no potential ( V = 0 )

eigen-function:

Finite Difference Method on model problem:

for

eigen-pair:

Question: How accurate are numerical eigen-value?

Exact wave number:

Numerical wave number:

Taylor expansion:

where

Question: eigenvalue is second order accuracy,

, is this reasonable, why?

Question: why does error of eigenvalue increase as wave number k increases?

slide24

Finite Difference Method [7]

model problem: no potential ( V = 0 )

slide25

Exercise 1: model problem (high order accuracy )

Finite Difference Method on model problem:

for

eigen-pair:

Question: how can we improve accuracy of eigenvalue of model problem?

Step 1: deduce 4-order centered finite difference scheme for second order derivative

Step 2: can you transform continuous equation to discrete equation?

for

slide26

Exercise 2: singular potential

effective potential:

finite difference with uniform mesh platform: MATLAB

bound state

There are only six bound state (energy E < 0 )

Definition: bound state means

Exercise: plot first 10 eigen-function and interpret why only first lowest six eigenvalue corresponds to “bound state”