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  2. Quartic function - Wikipedia

    en.wikipedia.org/wiki/Quartic_function

    be the general quartic equation we want to solve. Dividing by a 4, provides the equivalent equation x 4 + bx 3 + cx 2 + dx + e = 0, with b = ⁠ a 3 / a 4 ⁠, c = ⁠ a 2 / a 4 ⁠, d = ⁠ a 1 / a 4 ⁠, and e = ⁠ a 0 / a 4 ⁠. Substituting y − ⁠ b / 4 ⁠ for x gives, after regrouping the terms, the equation y 4 + py 2 + qy + r = 0, where

  3. Quartic equation - Wikipedia

    en.wikipedia.org/wiki/Quartic_equation

    This is a cubic equation in y. Solve for y using any method for solving such equations (e.g. conversion to a reduced cubic and application of Cardano's formula). Any of the three possible roots will do.

  4. Dormand–Prince method - Wikipedia

    en.wikipedia.org/wiki/Dormand–Prince_method

    In numerical analysis, the Dormand–Prince (RKDP) method or DOPRI method, is an embedded method for solving ordinary differential equations (ODE). [1] The method is a member of the Runge–Kutta family of ODE solvers. More specifically, it uses six function evaluations to calculate fourth- and fifth-order accurate solutions.

  5. Trachtenberg system - Wikipedia

    en.wikipedia.org/wiki/Trachtenberg_system

    The fourth digit of the answer is and carry to the next digit. Continue with the same method to obtain the remaining digits. 2 Finger method. Trachtenberg called this the 2 Finger Method. The calculations for finding the fourth digit from the example above are illustrated at right.

  6. List of Runge–Kutta methods - Wikipedia

    en.wikipedia.org/wiki/List_of_Runge–Kutta_methods

    All are implicit methods, have order 2s − 2 and they all have c 1 = 0 and c s = 1. Unlike any explicit method, it's possible for these methods to have the order greater than the number of stages. Lobatto lived before the classic fourth-order method was popularized by Runge and Kutta.

  7. Biharmonic equation - Wikipedia

    en.wikipedia.org/wiki/Biharmonic_equation

    In mathematics, the biharmonic equation is a fourth-order partial differential equation which arises in areas of continuum mechanics, including linear elasticity theory and the solution of Stokes flows. Specifically, it is used in the modeling of thin structures that react elastically to external forces.