| Home | Libraries | People | FAQ | More

### Overview

odeint is a library for solving initial value problems (IVP) of ordinary differential equations. Mathematically, these problems are formulated as follows:

x'(t) = f(x,t), x(0) = x0.

x and f can be vectors and the solution is some function x(t) fulfilling both equations above. In the following we will refer to x'(t) also `dxdt` which is also our notation for the derivative in the source code.

Ordinary differential equations occur nearly everywhere in natural sciences. For example, the whole Newtonian mechanics are described by second order differential equations. Be sure, you will find them in every discipline. They also occur if partial differential equations (PDEs) are discretized. Then, a system of coupled ordinary differential occurs, sometimes also referred as lattices ODEs.

Numerical approximations for the solution x(t) are calculated iteratively. The easiest algorithm is the Euler scheme, where starting at x(0) one finds x(dt) = x(0) + dt f(x(0),0). Now one can use x(dt) and obtain x(2dt) in a similar way and so on. The Euler method is of order 1, that means the error at each step is ~ dt2. This is, of course, not very satisfying, which is why the Euler method is rarely used for real life problems and serves just as illustrative example.

The main focus of odeint is to provide numerical methods implemented in a way where the algorithm is completely independent on the data structure used to represent the state x. In doing so, odeint is applicable for a broad variety of situations and it can be used with many other libraries. Besides the usual case where the state is defined as a `std::vector` or a `boost::array`, we provide native support for the following libraries:

- Boost.uBLAS
- Thrust, making odeint naturally running on CUDA devices
- gsl_vector for compatibility with the many numerical function in the GSL
- Boost.Range
- Boost.Fusion (the state type can be a fusion vector)
- Boost.Units
- Intel Math Kernel Library for maximum performance
- VexCL for OpenCL
- Boost.Graph (still experimentally)

In odeint, the following algorithms are implemented:

Table 1.1. Stepper Algorithms

Algorithm | Class | Concept | System Concept | Order | Error Estimation | Dense Output | Internal state | Remarks
--- | --- | --- | --- | --- | --- | --- | --- | ---
Explicit Euler | `euler` | Dense Output Stepper | System | 1 | No | Yes | No | Very simple, only for demonstrating purpose
Modified Midpoint | `modified_midpoint` | Stepper | System | configurable (2) | No | No | No | Used in Bulirsch-Stoer implementation
Runge-Kutta 4 | `runge_kutta4` | Stepper | System | 4 | No | No | No | The classical Runge-Kutta scheme, good general scheme without error control
Cash-Karp | `runge_kutta_cash_karp54` | Error Stepper | System | 5 | Yes (4) | No | No | Good general scheme with error estimation, to be used in controlled_error_stepper
Dormand-Prince 5 | `runge_kutta_dopri5` | Error Stepper | System | 5 | Yes (4) | Yes | Yes | Standard method with error control and dense output, to be used in controlled_error_stepper and in dense_output_controlled_explicit_fsal.
Fehlberg 78 | `runge_kutta_fehlberg78` | Error Stepper | System | 8 | Yes (7) | No | No | Good high order method with error estimation, to be used in controlled_error_stepper.
Adams Bashforth | `adams_bashforth` | Stepper | System | configurable | No | No | Yes | Multistep method
Adams Bashforth Moulton | `adams_bashforth_moulton` | Stepper | System | configurable | No | No | Yes | Combined multistep method
Controlled Runge-Kutta | `controlled_runge_kutta` | Controlled Stepper | System | depends | Yes | No | depends | Error control for Error Stepper. Requires an Error Stepper from above. Order depends on the given ErrorStepper
Dense Output Runge-Kutta | `dense_output_runge_kutta` | Dense Output Stepper | System | depends | No | Yes | Yes | Dense output for Stepper and Error Stepper from above if they provide dense output functionality (like `euler` and `runge_kutta_dopri5`). Order depends on the given stepper.
Bulirsch-Stoer | `bulirsch_stoer` | Controlled Stepper | System | variable | Yes | No | No | Stepper with step size and order control. Very good if high precision is required.
Bulirsch-Stoer Dense Output | `bulirsch_stoer_dense_out` | Dense Output Stepper | System | variable | Yes | Yes | No | Stepper with step size and order control as well as dense output. Very good if high precision and dense output is required.
Implicit Euler | `implicit_euler` | Stepper | Implicit System | 1 | No | No | No | Basic implicit routine. Requires the Jacobian. Works only with Boost.uBLAS vectors as state types.
Rosenbrock 4 | `rosenbrock4` | Error Stepper | Implicit System | 4 | Yes | Yes | No | Good for stiff systems. Works only with Boost.uBLAS vectors as state types.
Controlled Rosenbrock 4 | `rosenbrock4_controller` | Controlled Stepper | Implicit System | 4 | Yes | Yes | No | Rosenbrock 4 with error control. Works only with Boost.uBLAS vectors as state types.
Dense Output Rosenbrock 4 | `rosenbrock4_dense_output` | Dense Output Stepper | Implicit System | 4 | Yes | Yes | No | Controlled Rosenbrock 4 with dense output. Works only with Boost.uBLAS vectors as state types.
Symplectic Euler | `symplectic_euler` | Stepper | Symplectic System Simple Symplectic System | 1 | No | No | No | Basic symplectic solver for separable Hamiltonian system
Symplectic RKN McLachlan | `symplectic_rkn_sb3a_mclachlan` | Stepper | Symplectic System Simple Symplectic System | 4 | No | No | No | Symplectic solver for separable Hamiltonian system with 6 stages and order 4.
Symplectic RKN McLachlan | `symplectic_rkn_sb3a_m4_mclachlan` | Stepper | Symplectic System Simple Symplectic System | 4 | No | No | No | Symplectic solver with 5 stages and order 4, can be used with arbitrary precision types.
Velocity Verlet | `velocity_verlet` | Stepper | Second Order System | 1 | No | No | Yes | Velocity verlet method suitable for molecular dynamics simulation.