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<tr BGCOLOR="#EEEEFF"> <tr> <tr> <tr> <tr> <tr> <tr> </table> </p> <p> <table border="1" align="center"> <tr BGCOLOR="#CCCCFF"> <tr BGCOLOR="#EEEEFF"> <tr> <tr> <tr> <tr> <tr> <tr> </table> </p> </subsection> <subsection name="15.5 Derivatives" href="derivatives"> <p> If in addition to state y(t) the user needs to compute the sensitivity of the final state with respect to the initial state (dy/dy<sub>0) or the sensitivity of the final state with respect to some parameters of the ODE (dy/dp<sub>k), he needs to register the variational equations as a set of secondary equations appended to the main state before the integration starts. Then the integration will propagate the compound state composed of both the main state and its partial derivatives. At the end of the integration, the Jacobian matrices are extracted from the integrated secondary state. The <a href="../apidocs/org/apache/commons/math3/ode/JacobianMatrices.html">JacobianMatrices</a> class can do most of this as long as the local derivatives are provided to it. It will set up the variational equations, register them as secondary equations into the ODE, and it will set up the initial values and retrieve the intermediate and final values as Jacobian matrices. </p> <p> If for example the original state dimension is 6 and there are 3 parameters, the compound state will be a 60 elements array. The first 6 elements will be the original state, the next 36 elements will represent the 6x6 Jacobian matrix of the final state with respect to the initial state, and the remaining 18 elements will represent the 6x3 Jacobian matrix of the final state with respect to the 3 parameters. The <a href="../apidocs/org/apache/commons/math3/ode/JacobianMatrices.html">JacobianMatrices</a> class does the mapping between the 60 elements compound state and the Jacobian matrices and sets up the correcsponding secondary equations. </p> <p> As the variational equations are considered to be secondary equations here, variable step integrators ignore them for step size control: they rely only on the main state. This feature is a design choice. The rationale is to get exactly the same steps, regardless of the Jacobians being computed or not, hence ensuring reproducible results in both cases. </p> <p> What remains of user responsibility is to provide the local Jacobians df(t, y, p)/dy and df(t, y, p)/dp<sub>k corresponding the the main ODE y'=f(t, y, p). The main ODE is as usual provided by the user as a class implementing the <a href="../apidocs/org/apache/commons/math3/ode/FirstOrderDifferentialEquations.html">FirstOrderDifferentialEquations interface or a sub-interface. </p> <p> If the ODE is simple enough that the user can implement df(t, y, p)/dy directly, then instead of providing an implementation of the <a href="../apidocs/org/apache/commons/math3/ode/FirstOrderDifferentialEquations.html">FirstOrderDifferentialEquations</a> interface only, the user should rather provide an implementation of the <a href="../apidocs/org/apache/commons/math3/ode/MainStateJacobianProvider.html">MainStateJacobianProvider</a> interface, which extends the previous interface by adding a method to compute df(t, y, p)/dy. The user class is used as a constructor parameter of the <a href="../apidocs/org/apache/commons/math3/ode/JacobianMatrices.html">JacobianMatrices class. If the ODE is too complex or the user simply does not bother implementing df(t, y, p)/dy directly, then the ODE can still be implemented using the simple <a href="../apidocs/org/apache/commons/math3/ode/FirstOrderDifferentialEquations.html">FirstOrderDifferentialEquations</a> interface and given as such to another constructor of the <a href="../apidocs/org/apache/commons/math3/ode/JacobianMatrices.html">JacobianMatrices</a> class, but in this case an array hy must also be provided that will contain the step size to use form each component of the main state vector y, and the Jacobian f(t, y, p)/dy will be computed internally using finite differences. This will of course trigger more evaluations of the ODE at each step and will suffer from finite differences errors, but it is much simpler to implement from a user point of view. </p> <p> The parameters are identified by a name (a simple user defined string), which are also specified at <a href="../apidocs/org/apache/commons/math3/ode/JacobianMatrices.html">JacobianMatrices</a> class construction. If the ODE is simple enough that the user can implement df(t, y, p)/dp<sub>k directly for some of the parameters pk, then he can provide one or more classes implementing the <a href="../apidocs/org/apache/commons/math3/ode/ParameterJacobianProvider.html">ParameterJacobianProvider</a> interface by calling the JacobianMatrices.addParameterJacobianProvide method. The parameters are handled one at a time, but all the calls to ParameterJacobianProvider.computeParameterJacobian will be grouped in one sequence after the call to MainStateJacobianProvider.computeMainStateJacobian This feature can be used when all the derivatives share a lot of costly computation. In this case, the user is advised to compute all the needed derivatives at once during the call to computeMainStateJacobian, including the partial derivatives with respect to the parameters and to store the derivatives temporary. Then when the next calls to computeParameterJacobian will be triggerred, it will be sufficient to return the already computed derivatives. With this architecture, many computation can be saved. This of course implies that the classes implementing both interfaces know each other (they can even be the same class if desired, but it is not required). If the ODE is too complex or the user simply does not bother implementing df(t, y, p)/dp<sub>k directly for some k, then the JacobianMatrices.setParameterStep method should be called so finite differences are used to compute the derivatives for this parameter. It is possible to have some parameters for which derivatives are provided by a direct implementation while other parameters are computed using finite differences during the same integration. </p> <p> The following example corresponds to a simple case where all derivatives can be computed analytically. The state is a 2D point travelling along a circle. There are three parameters : the two coordinates of the center and the angular velocity. </p> <source> public class CircleODE implements MainStateJacobianProvider, ParameterJacobianProvider { public static final String CENTER_X = "cx"; public static final String CENTER_Y = "cy"; public static final String OMEGA = "omega"; private double[] c; private double omega; private double[][] savedDfDp; public CircleODE(double[] c, double omega) { this.c = c; this.omega = omega; this.savedDfDp = new double; } public int getDimension() { return 2; } public void computeDerivatives(double t, double[] y, double[] yDot) { // the state is a 2D point, the ODE therefore corresponds to the velocity yDot = omega * (c - y); yDot = omega * (y - c); } public Collection<String> getParametersNames() { return Arrays.asList(CENTER_X, CENTER_Y, OMEGA); } public boolean isSupported(String name) { return CENTER_X.equals(name) || CENTER_Y.equals(name) || OMEGA.equals(name); } public void computeMainStateJacobian(double t, double[] y, double[] yDot, double[][] dFdY) { // compute the Jacobian of the main state dFdY = 0; dFdY = -omega; dFdY = omega; dFdY = 0; // precompute the derivatives with respect to the parameters, // they will be provided back when computeParameterJacobian are called later on savedDfDp = 0; savedDfDp = omega; savedDfDp = c - y; savedDfDp = -omega; savedDfDp = 0; savedDfDp = y - c; } public void computeParameterJacobian(double t, double[] y, double[] yDot, String paramName, double[] dFdP) { // we simply return the derivatives precomputed earlier if (CENTER_X.equals(paramName)) { dFdP = savedDfDp; dFdP = savedDfDp; } else if (CENTER_Y.equals(paramName)) { dFdP = savedDfDp; dFdP = savedDfDp; } else { dFdP = savedDfDp; dFdP = savedDfDp; } } } </source> <p> This ODE is integrated as follows: </p> <source> CircleODE circle = new CircleODE(new double[] {1.0, 1.0 }, 0.1); // here, we could select only a subset of the parameters, or use another order JacobianMatrices jm = new JacobianMatrices(circle, CircleODE.CENTER_X, CircleODE.CENTER_Y, CircleODE.OMEGA); jm.addParameterJacobianProvider(circle); ExpandableStatefulODE efode = new ExpandableStatefulODE(circle); efode.setTime(0); double[] y = { 1.0, 0.0 }; efode.setPrimaryState(y); // create the variational equations and append them to the main equations, as secondary equations jm.registerVariationalEquations(efode); // integrate the compound state, with both main and additional equations DormandPrince853Integrator integrator = new DormandPrince853Integrator(1.0e-6, 1.0e3, 1.0e-10, 1.0e-12); integrator.setMaxEvaluations(5000); integrator.integrate(efode, 20.0); // retrieve the Jacobian of the final state with respect to initial state double[][] dYdY0 = new double; jm.getCurrentMainSetJacobian(dYdY0); // retrieve the Jacobians of the final state with resepct to the various parameters double[] dYdCx = new double; double[] dYdCy = new double; double[] dYdOm = new double; jm.getCurrentParameterJacobian(CircleODE.CENTER_X, dYdCx); jm.getCurrentParameterJacobian(CircleODE.CENTER_Y, dYdCy); jm.getCurrentParameterJacobian(CircleODE.OMEGA, dYdOm); </source> </subsection> </section> </body> </document>

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# Java example source code file (ode.xml)

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## The ode.xml Java example source code

```<?xml version="1.0"?>

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<?xml-stylesheet type="text/xsl" href="./xdoc.xsl"?>
<document url="ode.html">

<properties>
<title>The Commons Math User Guide - Ordinary Differential Equations Integration
</properties>

<body>
<section name="15 Ordinary Differential Equations Integration">
<subsection name="15.1 Overview" href="overview">
<p>
The ode package provides classes to solve Ordinary Differential Equations problems.
</p>
<p>
This package solves Initial Value Problems of the form y'=f(t,y) with t<sub>0
and y(t<sub>0)=y0 known. The provided integrators compute an estimate
of y(t) from t=t<sub>0 to t=t1.
</p>
<p>
All integrators provide dense output. This means that besides computing the state vector
at discrete times, they also provide a cheap mean to get both the state and its derivative
between the time steps. They do so through classes extending the
<a href="../apidocs/org/apache/commons/math3/ode/sampling/StepInterpolator.html">StepInterpolator
abstract class, which are made available to the user at the end of each step.
</p>
<p>
All integrators handle multiple discrete events detection based on switching
functions. This means that the integrator can be driven by user specified discrete events
(occurring when the sign of user-supplied <i>switching function changes). The steps are
shortened as needed to ensure the events occur at step boundaries (even if the integrator
is a fixed-step integrator). When the events are triggered, integration can
be stopped (this is called a G-stop facility), the state vector can be changed, or integration
can simply go on. The latter case is useful to handle discontinuities in the differential
equations gracefully and get accurate dense output even close to the discontinuity.
</p>
<p>
All integrators support setting a maximal number of evaluations of differential
equations function. If this number is exceeded, an exception will be thrown during
integration. This can be used to prevent infinite loops if for example error control or
discrete events create a really large number of extremely small steps. By default, the
maximal number of evaluation is set to <code>Integer.MAX_VALUE (i.e. 231-1
or 2147483647). It is recommended to set this maximal number to a value suited to the ODE
problem, integration range, and step size or error control settings.
</p>
<p>
All integrators support expanding the main ODE with one or more secondary ODE to manage
additional state that will be integrated together with the main state. This can be used
for example to integrate variational equations and compute not only the main state but also
its partial derivatives with respect to either the initial state or some parameters, these
derivatives being handled be secondary ODE (see below for an example).
</p>
<p>
Two parallel APIs are available. The first is devoted to solve ode for which the integration free
variable t and the state y(t) are primitive double and primitive double array respectively. Starting
with version 3.6, a second API is devoted to solve ode for which the integration free
variable t and the state y(t) are <code>RealFieldElement and `RealFieldElement`
array respectively. This allow for example users to integrate ode where the computation values
are for example <code>DerivativeStructure elements, hence automatically computing
partial derivatives with respect to some equations parameters without a need to set up the
variational equations. Another example is to use <code>Dfp elements in order to solve
ode with extended precision. As of 3.6, the API are slightly different, mainly in the way they
handle arrays. Both API will become more similar in 4.0 and future versions as the older
primitive double API will be modified to match the newer field API. This cannot be done in
3.6 for compatibility reasons.
</p>
<p>
The user should describe his problem in his own classes which should implement the
<a href="../apidocs/org/apache/commons/math3/ode/FirstOrderDifferentialEquations.html">FirstOrderDifferentialEquations
interface (or  <a href="../apidocs/org/apache/commons/math3/ode/FirstOrderFieldDifferentialEquations.html">FirstOrderFieldDifferentialEquations
interface). Then he should pass it to the integrator he prefers among all the classes that implement
the <a href="../apidocs/org/apache/commons/math3/ode/FirstOrderIntegrator.html">FirstOrderIntegrator
interface (or the <a href="../apidocs/org/apache/commons/math3/ode/FirstOrderFieldIntegrator.html">FirstOrderFieldIntegrator
interface). The following example shows how to implement the simple two-dimensional problem using double primitives:
<ul>
<li>y'0(t) = ω × (c1 - y1(t))
<li>y'1(t) = ω × (y0(t) - c0)
</ul>
with some initial state y(t<sub>0) = (y0(t0), y1(t0)).
In fact, the exact solution of this problem is that y(t) moves along a circle
centered at c = (c<sub>0, c1) with constant angular rate ω.
</p>
<source>
private static class CircleODE implements FirstOrderDifferentialEquations {

private double[] c;
private double omega;

public CircleODE(double[] c, double omega) {
this.c     = c;
this.omega = omega;
}

public int getDimension() {
return 2;
}

public void computeDerivatives(double t, double[] y, double[] yDot) {
yDot = omega * (c - y);
yDot = omega * (y - c);
}

}
</source>
<p>
Computing the state y(16.0) starting from y(0.0) = (0.0, 1.0) and integrating the ODE
is done as follows (using Dormand-Prince 8(5,3) integrator as an example):
</p>
<source>
FirstOrderIntegrator dp853 = new DormandPrince853Integrator(1.0e-8, 100.0, 1.0e-10, 1.0e-10);
FirstOrderDifferentialEquations ode = new CircleODE(new double[] { 1.0, 1.0 }, 0.1);
double[] y = new double[] { 0.0, 1.0 }; // initial state
dp853.integrate(ode, 0.0, y, 16.0, y); // now y contains final state at time t=16.0
</source>
</subsection>
<subsection name="15.2 Continuous Output" href="continuous">
<p>
The solution of the integration problem is provided by two means. The first one is aimed towards
simple use: the state vector at the end of the integration process is copied in the y array of the
<code>FirstOrderIntegrator.integrate method, as shown by previous example. The second one
should be used when more in-depth information is needed throughout the integration process. The user
can register an object implementing the
<a href="../apidocs/org/apache/commons/math3/ode/sampling/StepHandler.html">StepHandler interface or a
<a href="../apidocs/org/apache/commons/math3/ode/sampling/StepNormalizer.html">StepNormalizer object wrapping
a user-specified object implementing the
<a href="../apidocs/org/apache/commons/math3/ode/sampling/FixedStepHandler.html">FixedStepHandler interface
into the integrator before calling the <code>FirstOrderIntegrator.integrate method. The user object
will be called appropriately during the integration process, allowing the user to process intermediate
results. The default step handler does nothing. Considering again the previous example, we want to print the
trajectory of the point to check it really is a circle arc. We simply add the following before the call
to integrator.integrate:
</p>
<source>
StepHandler stepHandler = new StepHandler() {
public void init(double t0, double[] y0, double t) {
}

public void handleStep(StepInterpolator interpolator, boolean isLast) {
double   t = interpolator.getCurrentTime();
double[] y = interpolator.getInterpolatedState();
System.out.println(t + " " + y + " " + y);
}
};
integrator.addStepHandler(stepHandler);
</source>
<p>
<a href="../apidocs/org/apache/commons/math3/ode/ContinuousOutputModel.html">ContinuousOutputModel
is a special-purpose step handler that is able to store all steps and to provide transparent access to
any intermediate result once the integration is over. An important feature of this class is that it
implements the <code>Serializable interface. This means that a complete continuous model of the
integrated function throughout the integration range can be serialized and reused later (if stored into
a persistent medium like a file system or a database) or elsewhere (if sent to another application).
Only the result of the integration is stored, there is no reference to the integrated problem by itself.
</p>
<p>
Other default implementations of the <a href="../apidocs/org/apache/commons/math3/ode/sampling/StepHandler.html">StepHandler
interface are available for general needs
(<a href="../apidocs/org/apache/commons/math3/ode/sampling/DummyStepHandler.html">DummyStepHandler,
<a href="../apidocs/org/apache/commons/math3/ode/sampling/StepNormalizer.html">StepNormalizer) and custom
implementations can be developed for specific needs. As an example, if an application is to be
completely driven by the integration process, then most of the application code will be run inside a
step handler specific to this application.
</p>
<p>
Some integrators (the simple ones) use fixed steps that are set at creation time. The more efficient
integrators use variable steps that are handled internally in order to control the integration error
of the main state with respect to a specified accuracy (these integrators extend the
<a href="../apidocs/org/apache/commons/math3/ode/AdaptiveStepsizeIntegrator.html">AdaptiveStepsizeIntegrator
abstract class). The secondary equations are explicitly ignored for step size control, in order to get reproducible
results regardless of the secondary equations being integrated or not. The step handler which is called after each
successful step shows up the variable stepsize. The <a href="../apidocs/org/apache/commons/math3/ode/sampling/StepNormalizer.html">StepNormalizer
class can be used to convert the variable stepsize into a fixed stepsize that can be handled by classes
implementing the <a href="../apidocs/org/apache/commons/math3/ode/sampling/FixedStepHandler.html">FixedStepHandler
interface. Adaptive stepsize integrators can automatically compute the initial stepsize by themselves,
however the user can specify it if he prefers to retain full control over the integration or if the
automatic guess is wrong.
</p>
</subsection>
<subsection name="15.3 Discrete Events Handling" href="events">
<p>
ODE problems are continuous ones. However, sometimes discrete events must be
taken into account. The most frequent case is the stop condition of the integrator
is not defined by the time t but by a target condition on state y (say y = 1.0
for example).
</p>
<p>
Discrete events detection is based on switching functions. The user provides
a simple <a href="../apidocs/org/apache/commons/math3/ode/events/EventHandler.html">g(t, y)
function depending on the current time and state. The integrator will monitor
the value of the function throughout integration range and will trigger the
event when its sign changes. The magnitude of the value is almost irrelevant.
For the sake of root finding, it should however be continuous (but not necessarily smooth)
at least in the roots vicinity. The steps are shortened as needed to ensure the events occur
at step boundaries (even if the integrator is a fixed-step integrator).
</p>
<p>
When an event is triggered, the event time, current state and an indicator
whether the switching function was increasing or decreasing at event time
are provided to the user. Several different options are available to him:
</p>
<ul>
<li>integration can be stopped (this is called a G-stop facility),
<li>the state vector or the derivatives can be changed,
<li>or integration can simply go on.
</ul>

<p>
The first case, G-stop, is the most common one. A typical use case is when an
ODE must be solved up to some target state is reached, with a known value of
the state but an unknown occurrence time. As an example, if we want to monitor
a chemical reaction up to some predefined concentration for the first substance,
we can use the following switching function setting:
</p>
<source>
public double g(double t, double[] y) {
return y - targetConcentration;
}

public int eventOccurred(double t, double[] y, boolean increasing) {
return STOP;
}
</source>

<p>
The second case, change state vector or derivatives is encountered when dealing
with discontinuous dynamical models. A typical case would be the motion of a
spacecraft when thrusters are fired for orbital maneuvers. The acceleration is
smooth as long as no maneuvers are performed, depending only on gravity, drag,
third body attraction, radiation pressure. Firing a thruster introduces a
discontinuity that must be handled appropriately by the integrator. In such a case,
we would use a switching function setting similar to this:
</p>
<source>
public double g(double t, double[] y) {
return (t - tManeuverStart) * (t - tManeuverStop);
}

public int eventOccurred(double t, double[] y, boolean increasing) {
return RESET_DERIVATIVES;
}
</source>

<p>
The third case is useful mainly for monitoring purposes, a simple example is:
</p>
<source>
public double g(double t, double[] y) {
return y - y;
}

public int eventOccurred(double t, double[] y, boolean increasing) {
logger.log("y0(t) and y1(t) curves cross at t = " + t);
return CONTINUE;
}
</source>
</subsection>
<subsection name="15.4 Available Integrators" href="integrators">
<p>
The tables below show the various integrators available for non-stiff problems. Note that the
implementations of Adams-Bashforth and Adams-Moulton are adaptive stepsize, not fixed stepsize
as is usual for these multi-step integrators. This is due to the fact the implementation relies
on the Nordsieck vector representation of the state.
</p>
<p>
<table border="1" align="center">
<tr BGCOLOR="#CCCCFF">```
Fixed Step Integrators
NameOrder
Euler1
Midpoint2
Classical Runge-Kutta4
Gill4
3/84
Luther6
Adaptive Stepsize Integrators
NameIntegration OrderError Estimation Order
Higham and Hall54
Dormand-Prince 5(4)54
Dormand-Prince 8(5,3)85 and 3
Gragg-Bulirsch-Stoervariable (up to 18 by default)variable
Adams-Bashforthvariablevariable
Adams-Moultonvariablevariable

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