The integration of Equation 2 is as follows: 1 Q max − Q t = k 2 t + c.
The integration of Equation 1 is as follows: − ln Q max − Q t = k 1 t + c, Open image in new window (2).
The integration in Equation 1 is performed over the whole surface of the deformed tubule.
For the integration in Equation (11), we construct a Metropolis–Hasting algorithm presented in Algorithm 1. Algorithm 1 A Metropolis–Hastings algorithm for posterior sampling of parameters θ, k and f.
With the aid of Gauss-Chebyshev integration technique, the integral equations are further reduced to a system of algebraic equations.
The residuals υ it are assumed to be normally distributed, and white noise is the one-period lagged error correction term derived from the co-integration equation.
Translation by the author: "...Lie's group theory for the integration of equations is not the true generalization of the method applied by Galois for algebraic equations".
We also obtain the solution using the integration of equations of motions performing a Fourth Order Runge-Kutta Method.
Molecular dynamics (MD) simulations allow the exploration of the phase space of biopolymers through the integration of equations of motion of their constituent atoms.
Therefore, the mutation is not convenient for solving the integration of Equations 19 and 20.
