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  2. Institutiones calculi differentialis - Wikipedia

    en.wikipedia.org/wiki/Institutiones_calculi...

    Institutiones calculi differentialis (Foundations of differential calculus) is a mathematical work written in 1748 by Leonhard Euler and published in 1755. It lays the groundwork for the differential calculus. It consists of a single volume containing two internal books; there are 9 chapters in book I, and 18 in book II.The first book was first ...

  3. Differential equation - Wikipedia

    en.wikipedia.org/wiki/Differential_equation

    The order of the differential equation is the highest order of derivative of the unknown function that appears in the differential equation. For example, an equation containing only first-order derivatives is a first-order differential equation, an equation containing the second-order derivative is a second-order differential equation, and so on.

  4. Viorel P. Barbu - Wikipedia

    en.wikipedia.org/wiki/Viorel_P._Barbu

    Some of his books and papers are: [5] [6] [7] G. Da Prato, V. Barbu Hamilton-Jacobi equations in Hilbert spaces, 1983. Analysis And Control Of Nonlinear Infinite Dimensional Systems ; Optimization, Optimal Control and Partial Differential Equations; Nonlinear semigroups and differential equations in Banach spaces ; Hamilton-Jacobi Equations on ...

  5. Euler's differential equation - Wikipedia

    en.wikipedia.org/wiki/Euler's_differential_equation

    Print/export Download as PDF; Printable version; In other projects ... Euler's differential equation is a first-order non-linear ordinary differential equation, ...

  6. Nikolai Piskunov - Wikipedia

    en.wikipedia.org/wiki/Nikolai_Piskunov

    He is known for the Kolmogorov–Petrovsky–Piskunov equation, [1] a key model in mathematical population dynamics, and his textbook on differential and integral calculus which was used at many technical universities and was translated into several languages.

  7. Maxwell's equations - Wikipedia

    en.wikipedia.org/wiki/Maxwell's_equations

    These all form a set of coupled partial differential equations which are often very difficult to solve: the solutions encompass all the diverse phenomena of classical electromagnetism. Some general remarks follow. As for any differential equation, boundary conditions [19] [20] [21] and initial conditions [22] are necessary for a unique solution.