Graphic Organizer Leonhard Euler and Jean dβAlembert: Argue over solutions 1 πΉ(π₯, π‘) = [π(π₯ + π‘) + π(π₯ β π‘)] 2
DβAlembert and Euler: f must be continuous or discontinuious
Daniel Bernouslli, Euler, dβAlemvert, Joseph Lagrange: Solutions must have a specific form but is rejected. ππ₯ 2ππ₯ π(π₯) = π1 ( ) + π2 ( )+β― πΏ πΏ
Joseph Fourier: A bounded function has the form β 1 π(π₯) = π0 + β ππ cos πππ₯ /π + ππ sin πππ₯ /π 2 π=1
Joseph Fourier: A function is continuous the same way it is today
Fourier: Arbitrary functions behave well β 1 π π(π₯) = β« π(π)ππ β« cos(ππ₯ β ππ) ππ 2π π ββ
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 π
π(π₯) = β ππΌπ (π₯)ππ (π₯)π π=1
Peter Gustav Lejeune-Dirichlet: Gave first proof of convergence.
Lejeune-Dirichlet: Believed proof would work for discontinuities
Rudolf Lipschitz: Tried to improve Dirichletβs proof.
Dirichlet and George Cantor: Proof extends to sets created by Cantor
Dirichlet: Introduced function 1 π₯ ππ πππ‘πππππ π(π₯) = { 0 π₯ ππ πππππ‘πππππ