Methods 4 Flashcards

1
Q

Regular Singular Point

A

For a general linear second-order differential equation for w(z), of the form w”(z) + p(z)w’(z) + q(z)w(z) = 0

A point z=z0 is a regular singular point of it is not an ordinary point, but both (z-z₀)p(z) and (z-z₀)²q(z) are analytic at z₀

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2
Q

Ordinary Point

A

For a general linear second-order differential equation for w(z), of the form w”(z) + p(z)w’(z) + q(z)w(z) = 0

A point z=z₀ is an OP if both p(z) and q(z) are analytic at z₀

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3
Q

Periodic Sturm Liouville Systems

A

Periodic Boundary Conditions

y(a) = y(b) 
y'(a) = y'(b) 

Where y(x) is a periodic function defined on a

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4
Q

Regular Sturm Liouville

A

P(x) and Q(x) singular at x = +- 1

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5
Q

D’Alembert’s Ratio Test

A

Radius of convergence - property for Legendre polynomials

If regular singular points at x=+-1 - the radius of convergence if likely to be UNITY

Confirm using D’Alembert’s Ratio test
-Diverge for |z|>1 : D’Alembert’s ratio test indicates divergence

Lim|(bk+1Z^2k+2)/bkZ^2k)>1 or lim|bk/bk+1| as k tends to infinity

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6
Q

Eigwnvalue are real

A

Define the eigenvalue and eigenfunction solutions to the problem as:
Lyk = -λk yk

  1. = = -λk
  2. = = = complex conjugate of

Comparing 1 and 2: clear λk = conjugate λk

So λk are real

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7
Q

Eigenfunctions Yj(x) Yk(x) corresponding to eigenvalues λj, λk are orthogonal with respect to inner product

A

Let λj, λk be distinct eigenvalues, L is self-adjoint, λj ≠ λk

  1. w = w = -λj w
  2. w = w = w = -λk as λk are real

Subtracting 2 from 1:

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8
Q

Adjoint

A

The operator A is said to be self joint if: A’ = A

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9
Q

Legendre Equation

A

(1-x²)y” -xy’ +λy = 0 where λ = v(v+1)

  • index up
  • use naive
  • Eigenvalues: λk =k²
  • Eigenfunctions: Tk(x)

Weight function: use integrating factor
1/√(1-x²)

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10
Q

Bessel Equation

A

x²w” +xw’ +(x²-v²)w = 0

W(z) =
AJv(z) + BJ-v(x) v>0
AJ0(z) +BY0(z) v=0
AJm(z) + BYm(z) v=m

Indicial: c²-v²

Recurrence: odd terms = 0
Make a2k into bk

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