Separation of Variables Eigenvalues of the Laplace Operator Bernd - - PowerPoint PPT Presentation

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Separation of Variables Eigenvalues of the Laplace Operator Bernd - - PowerPoint PPT Presentation

What is Separation of Variables? Eigenvalue Problems for the Laplace Operator Separation of Variables Eigenvalues of the Laplace Operator Bernd Schr oder logo1 Bernd Schr oder Louisiana Tech University, College of Engineering and


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SLIDE 1

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

Separation of Variables – Eigenvalues of the Laplace Operator

Bernd Schr¨

  • der

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 2

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

Separation of Variables

  • 1. Solution technique for partial differential equations.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 3

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

Separation of Variables

  • 1. Solution technique for partial differential equations.
  • 2. If the unknown function u depends on variables x,y,z,t, we

assume there is a solution of the form u = f(x,y,z)T(t).

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 4

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

Separation of Variables

  • 1. Solution technique for partial differential equations.
  • 2. If the unknown function u depends on variables x,y,z,t, we

assume there is a solution of the form u = f(x,y,z)T(t).

  • 3. The special form of this solution function allows us to

replace the original partial differential equation with several ordinary differential equations.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 5

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

Separation of Variables

  • 1. Solution technique for partial differential equations.
  • 2. If the unknown function u depends on variables x,y,z,t, we

assume there is a solution of the form u = f(x,y,z)T(t).

  • 3. The special form of this solution function allows us to

replace the original partial differential equation with several ordinary differential equations.

  • 4. Key step: If a(t) = b(x,y,z), then a and b must be constant.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 6

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

Separation of Variables

  • 1. Solution technique for partial differential equations.
  • 2. If the unknown function u depends on variables x,y,z,t, we

assume there is a solution of the form u = f(x,y,z)T(t).

  • 3. The special form of this solution function allows us to

replace the original partial differential equation with several ordinary differential equations.

  • 4. Key step: If a(t) = b(x,y,z), then a and b must be constant.
  • 5. Solutions of the ordinary differential equations we obtain

must typically be processed some more to give useful results for the partial differential equations.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 7

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

Separation of Variables

  • 1. Solution technique for partial differential equations.
  • 2. If the unknown function u depends on variables x,y,z,t, we

assume there is a solution of the form u = f(x,y,z)T(t).

  • 3. The special form of this solution function allows us to

replace the original partial differential equation with several ordinary differential equations.

  • 4. Key step: If a(t) = b(x,y,z), then a and b must be constant.
  • 5. Solutions of the ordinary differential equations we obtain

must typically be processed some more to give useful results for the partial differential equations.

  • 6. Some very powerful and deep theorems can be used to

formally justify the approach for many equations involving the Laplace operator.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 8

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

How Deep?

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 9

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

How Deep?

plus about 200 pages of really awesome functional analysis.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 10

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Wave Equation ∆u = k∂ 2u ∂t2

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 11

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Wave Equation ∆u = k∂ 2u ∂t2

∆u = k∂ 2u ∂t2

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 12

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Wave Equation ∆u = k∂ 2u ∂t2

∆u = k∂ 2u ∂t2 u(x,y,z,t) = f(x,y,z)T(t)

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 13

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Wave Equation ∆u = k∂ 2u ∂t2

∆u = k∂ 2u ∂t2 u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ 2 ∂t2

  • kf(x,y,z)T(t)
  • Bernd Schr¨
  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 14

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Wave Equation ∆u = k∂ 2u ∂t2

∆u = k∂ 2u ∂t2 u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ 2 ∂t2

  • kf(x,y,z)T(t)
  • T∆f

= kf T′′

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 15

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Wave Equation ∆u = k∂ 2u ∂t2

∆u = k∂ 2u ∂t2 u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ 2 ∂t2

  • kf(x,y,z)T(t)
  • T∆f

= kf T′′ T∆f Tf = k f T′′ Tf

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 16

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Wave Equation ∆u = k∂ 2u ∂t2

∆u = k∂ 2u ∂t2 u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ 2 ∂t2

  • kf(x,y,z)T(t)
  • T∆f

= kf T′′ T∆f Tf = k f T′′ Tf ∆f f = kT′′ T

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

slide-17
SLIDE 17

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Wave Equation ∆u = k∂ 2u ∂t2

∆u = k∂ 2u ∂t2 u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ 2 ∂t2

  • kf(x,y,z)T(t)
  • T∆f

= kf T′′ T∆f Tf = k f T′′ Tf ∆f f = kT′′ T = λ

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

slide-18
SLIDE 18

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Wave Equation ∆u = k∂ 2u ∂t2

∆u = k∂ 2u ∂t2 u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ 2 ∂t2

  • kf(x,y,z)T(t)
  • T∆f

= kf T′′ T∆f Tf = k f T′′ Tf ∆f f = kT′′ T = λ ∆f = λf

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 19

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Wave Equation ∆u = k∂ 2u ∂t2

∆u = k∂ 2u ∂t2 u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ 2 ∂t2

  • kf(x,y,z)T(t)
  • T∆f

= kf T′′ T∆f Tf = k f T′′ Tf ∆f f = kT′′ T = λ ∆f = λf T′′ − λ k T = 0

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 20

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Heat Equation ∆u = k∂u ∂t

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

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SLIDE 21

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Heat Equation ∆u = k∂u ∂t

∆u = k∂u ∂t

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

slide-22
SLIDE 22

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Heat Equation ∆u = k∂u ∂t

∆u = k∂u ∂t u(x,y,z,t) = f(x,y,z)T(t)

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

slide-23
SLIDE 23

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Heat Equation ∆u = k∂u ∂t

∆u = k∂u ∂t u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ ∂t

  • kf(x,y,z)T(t)
  • Bernd Schr¨
  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

slide-24
SLIDE 24

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Heat Equation ∆u = k∂u ∂t

∆u = k∂u ∂t u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ ∂t

  • kf(x,y,z)T(t)
  • T∆f

= kf T′

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

slide-25
SLIDE 25

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Heat Equation ∆u = k∂u ∂t

∆u = k∂u ∂t u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ ∂t

  • kf(x,y,z)T(t)
  • T∆f

= kf T′ T∆f Tf = k f T′ Tf

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

slide-26
SLIDE 26

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Heat Equation ∆u = k∂u ∂t

∆u = k∂u ∂t u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ ∂t

  • kf(x,y,z)T(t)
  • T∆f

= kf T′ T∆f Tf = k f T′ Tf ∆f f = kT′ T

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

slide-27
SLIDE 27

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Heat Equation ∆u = k∂u ∂t

∆u = k∂u ∂t u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ ∂t

  • kf(x,y,z)T(t)
  • T∆f

= kf T′ T∆f Tf = k f T′ Tf ∆f f = kT′ T = λ

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

slide-28
SLIDE 28

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Heat Equation ∆u = k∂u ∂t

∆u = k∂u ∂t u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ ∂t

  • kf(x,y,z)T(t)
  • T∆f

= kf T′ T∆f Tf = k f T′ Tf ∆f f = kT′ T = λ ∆f = λf

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator

slide-29
SLIDE 29

logo1 What is Separation of Variables? Eigenvalue Problems for the Laplace Operator

The Heat Equation ∆u = k∂u ∂t

∆u = k∂u ∂t u(x,y,z,t) = f(x,y,z)T(t) ∆

  • f(x,y,z)T(t)
  • =

∂ ∂t

  • kf(x,y,z)T(t)
  • T∆f

= kf T′ T∆f Tf = k f T′ Tf ∆f f = kT′ T = λ ∆f = λf T′ = λ k T

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Separation of Variables – Eigenvalues of the Laplace Operator