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The following table gives an overview over all examples.
Table 1.4. Examples Overview
| File | Brief Description | 
|---|---|
| This examples shows how member functions can be used as system functions in odeint. | |
| 
                  This examples shows how member functions can be used as system
                  functions in odeint with  | |
| Shows the usage of the Bulirsch-Stoer method. | |
| The chaotic system examples integrates the Lorenz system and calculates the Lyapunov exponents. | |
| Example calculating the elliptic functions using Bulirsch-Stoer and Runge-Kutta-Dopri5 Steppers with dense output. | |
| The Fermi-Pasta-Ulam (FPU) example shows how odeint can be used to integrate lattice systems. | |
| Shows skeletal code on how to implement own factory functions. | |
| The harmonic oscillator examples gives a brief introduction to odeint and shows the usage of the classical Runge-Kutta-solvers. | |
| This examples shows how Boost.Units can be used with odeint. | |
| The Heun example shows how an custom Runge-Kutta stepper can be created with odeint generic Runge-Kutta method. | |
| 
                  Example of a phase lattice integration using  | |
| Alternative way of integrating lorenz by using a self defined point3d data type as state type. | |
| Simple example showing how to get odeint to work with a self-defined vector type. | |
| The phase oscillator ensemble example shows how globally coupled oscillators can be analyzed and how statistical measures can be computed during integration. | |
| Shows the strength of odeint's memory management by simulating a Hamiltonian system on an expanding lattice. | |
| Integrating a simple, one-dimensional ODE showing the usage of integrate- and generate-functions. | |
| The solar system example shows the usage of the symplectic solvers. | |
| Trivial example showing the usability of the several stepper classes. | |
| The stiff system example shows the usage of the stiff solvers using the Jacobian of the system function. | |
| Implementation of a custom stepper - the stochastic euler - for solving stochastic differential equations. | |
| The Stuart-Landau example shows how odeint can be used with complex state types. | |
| The 2D phase oscillator example shows how a two-dimensional lattice works with odeint and how matrix types can be used as state types in odeint. | |
| This stiff system example again shows the usage of the stiff solvers by integrating the van der Pol oscillator. | |
| This examples integrates the Lorenz system by means of an arbitrary precision type. | |
| The MTL-Gauss-packet example shows how the MTL can be easily used with odeint. | |
| This examples shows the usage of the MTL implicit Euler method with a sparse matrix type. | |
| The Thrust phase oscillator ensemble example shows how globally coupled oscillators can be analyzed with Thrust and CUDA, employing the power of modern graphic devices. | |
| The Thrust phase oscillator chain example shows how chains of nearest neighbor coupled oscillators can be integrated with Thrust and odeint. | |
| The Lorenz parameters examples show how ensembles of ordinary differential equations can be solved by means of Thrust to study the dependence of an ODE on some parameters. | |
| Another examples for the usage of Thrust. | |
| This example shows how the ublas vector types can be used with odeint. | |
| This example shows how the VexCL - a framework for OpenCL computation - can be used with odeint. | |
| OpenMP Lorenz attractor parameter study with continuous data. | |
| OpenMP Lorenz attractor parameter study with split data. | |
| 
                  OpenMP Lorenz attractor parameter study with nested  | |
| OpenMP nearest neighbour coupled phase chain with continuous state. | |
| OpenMP nearest neighbour coupled phase chain with split state. | |
| MPI nearest neighbour coupled phase chain. | |
| 
                  This examples shows how a  | |
| This examples shows how gcc libquadmath can be used with odeint. It provides a high precision floating point type which is adapted to odeint in this example. | |
| A very basic molecular dynamics simulation with the Velocity-Verlet method. |