Student Example

  • December 2019
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Graphic Organizer Leonhard Euler and Jean d’Alembert: Argue over solutions 1 𝐹(π‘₯, 𝑑) = [𝑓(π‘₯ + 𝑑) + 𝑓(π‘₯ βˆ’ 𝑑)] 2

D’Alembert and Euler: f must be continuous or discontinuious

Daniel Bernouslli, Euler, d’Alemvert, Joseph Lagrange: Solutions must have a specific form but is rejected. πœ‹π‘₯ 2πœ‹π‘₯ 𝑓(π‘₯) = π‘Ž1 ( ) + π‘Ž2 ( )+β‹― 𝐿 𝐿

Joseph Fourier: A bounded function has the form ∞ 1 𝑓(π‘₯) = π‘Ž0 + βˆ‘ π‘Žπ‘› cos π‘›πœ‹π‘₯ /π‘Ž + 𝑏𝑛 sin π‘›πœ‹π‘₯ /π‘Ž 2 𝑛=1

Joseph Fourier: A function is continuous the same way it is today

Fourier: Arbitrary functions behave well ∞ 1 𝑏 𝑓(π‘₯) = ∫ 𝑓(π‘Ž)π‘‘π‘Ž ∫ cos(𝑝π‘₯ βˆ’ π‘π‘Ž) 𝑑𝑝 2πœ‹ π‘Ž βˆ’βˆž

Fourier: A general function is smooth

Fourier, Lagrange, Henri Lebesgue: Coefficents attempted to be validated by Fourier. Lagrange improved this. Henri gave a proper definition.

Integrals change from area to antiderivative.

Augustin Cauchy: Provided world modern definition of continuity and defined definite integral.

Cauchy: Defines Cauchy sum as definite integral.

Cauchy: Functions are equations.

Discontinuous functions have the form 𝑛

𝑓(π‘₯) = βˆ‘ π‘‹πΌπ‘Ÿ (π‘₯)π‘”π‘Ÿ (π‘₯)π‘Ÿ π‘Ÿ=1

Peter Gustav Lejeune-Dirichlet: Gave first proof of convergence.

Lejeune-Dirichlet: Believed proof would work for discontinuities

Rudolf Lipschitz: Tried to improve Dirichlet’s proof.

Dirichlet and George Cantor: Proof extends to sets created by Cantor

Dirichlet: Introduced function 1 π‘₯ 𝑖𝑠 π‘Ÿπ‘Žπ‘‘π‘–π‘œπ‘›π‘Žπ‘™ 𝑓(π‘₯) = { 0 π‘₯ 𝑖𝑠 π‘–π‘Ÿπ‘Ÿπ‘Žπ‘‘π‘–π‘œπ‘›π‘Žπ‘™

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