All Downloads are FREE. Search and download functionalities are using the official Maven repository.

org.apache.commons.math3.ode.nonstiff.RungeKuttaFieldIntegrator Maven / Gradle / Ivy

The newest version!
/*
 * Licensed to the Apache Software Foundation (ASF) under one or more
 * contributor license agreements.  See the NOTICE file distributed with
 * this work for additional information regarding copyright ownership.
 * The ASF licenses this file to You under the Apache License, Version 2.0
 * (the "License"); you may not use this file except in compliance with
 * the License.  You may obtain a copy of the License at
 *
 *      http://www.apache.org/licenses/LICENSE-2.0
 *
 * Unless required by applicable law or agreed to in writing, software
 * distributed under the License is distributed on an "AS IS" BASIS,
 * WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.
 * See the License for the specific language governing permissions and
 * limitations under the License.
 */

package org.apache.commons.math3.ode.nonstiff;


import org.apache.commons.math3.Field;
import org.apache.commons.math3.RealFieldElement;
import org.apache.commons.math3.exception.DimensionMismatchException;
import org.apache.commons.math3.exception.MaxCountExceededException;
import org.apache.commons.math3.exception.NoBracketingException;
import org.apache.commons.math3.exception.NumberIsTooSmallException;
import org.apache.commons.math3.ode.AbstractFieldIntegrator;
import org.apache.commons.math3.ode.FieldEquationsMapper;
import org.apache.commons.math3.ode.FieldExpandableODE;
import org.apache.commons.math3.ode.FirstOrderFieldDifferentialEquations;
import org.apache.commons.math3.ode.FieldODEState;
import org.apache.commons.math3.ode.FieldODEStateAndDerivative;
import org.apache.commons.math3.util.MathArrays;

/**
 * This class implements the common part of all fixed step Runge-Kutta
 * integrators for Ordinary Differential Equations.
 *
 * 

These methods are explicit Runge-Kutta methods, their Butcher * arrays are as follows : *

 *    0  |
 *   c2  | a21
 *   c3  | a31  a32
 *   ... |        ...
 *   cs  | as1  as2  ...  ass-1
 *       |--------------------------
 *       |  b1   b2  ...   bs-1  bs
 * 
*

* * @see EulerFieldIntegrator * @see ClassicalRungeKuttaFieldIntegrator * @see GillFieldIntegrator * @see MidpointFieldIntegrator * @param the type of the field elements * @since 3.6 */ public abstract class RungeKuttaFieldIntegrator> extends AbstractFieldIntegrator implements FieldButcherArrayProvider { /** Time steps from Butcher array (without the first zero). */ private final T[] c; /** Internal weights from Butcher array (without the first empty row). */ private final T[][] a; /** External weights for the high order method from Butcher array. */ private final T[] b; /** Integration step. */ private final T step; /** Simple constructor. * Build a Runge-Kutta integrator with the given * step. The default step handler does nothing. * @param field field to which the time and state vector elements belong * @param name name of the method * @param step integration step */ protected RungeKuttaFieldIntegrator(final Field field, final String name, final T step) { super(field, name); this.c = getC(); this.a = getA(); this.b = getB(); this.step = step.abs(); } /** Create a fraction. * @param p numerator * @param q denominator * @return p/q computed in the instance field */ protected T fraction(final int p, final int q) { return getField().getZero().add(p).divide(q); } /** Create an interpolator. * @param forward integration direction indicator * @param yDotK slopes at the intermediate points * @param globalPreviousState start of the global step * @param globalCurrentState end of the global step * @param mapper equations mapper for the all equations * @return external weights for the high order method from Butcher array */ protected abstract RungeKuttaFieldStepInterpolator createInterpolator(boolean forward, T[][] yDotK, final FieldODEStateAndDerivative globalPreviousState, final FieldODEStateAndDerivative globalCurrentState, FieldEquationsMapper mapper); /** {@inheritDoc} */ public FieldODEStateAndDerivative integrate(final FieldExpandableODE equations, final FieldODEState initialState, final T finalTime) throws NumberIsTooSmallException, DimensionMismatchException, MaxCountExceededException, NoBracketingException { sanityChecks(initialState, finalTime); final T t0 = initialState.getTime(); final T[] y0 = equations.getMapper().mapState(initialState); setStepStart(initIntegration(equations, t0, y0, finalTime)); final boolean forward = finalTime.subtract(initialState.getTime()).getReal() > 0; // create some internal working arrays final int stages = c.length + 1; T[] y = y0; final T[][] yDotK = MathArrays.buildArray(getField(), stages, -1); final T[] yTmp = MathArrays.buildArray(getField(), y0.length); // set up integration control objects if (forward) { if (getStepStart().getTime().add(step).subtract(finalTime).getReal() >= 0) { setStepSize(finalTime.subtract(getStepStart().getTime())); } else { setStepSize(step); } } else { if (getStepStart().getTime().subtract(step).subtract(finalTime).getReal() <= 0) { setStepSize(finalTime.subtract(getStepStart().getTime())); } else { setStepSize(step.negate()); } } // main integration loop setIsLastStep(false); do { // first stage y = equations.getMapper().mapState(getStepStart()); yDotK[0] = equations.getMapper().mapDerivative(getStepStart()); // next stages for (int k = 1; k < stages; ++k) { for (int j = 0; j < y0.length; ++j) { T sum = yDotK[0][j].multiply(a[k-1][0]); for (int l = 1; l < k; ++l) { sum = sum.add(yDotK[l][j].multiply(a[k-1][l])); } yTmp[j] = y[j].add(getStepSize().multiply(sum)); } yDotK[k] = computeDerivatives(getStepStart().getTime().add(getStepSize().multiply(c[k-1])), yTmp); } // estimate the state at the end of the step for (int j = 0; j < y0.length; ++j) { T sum = yDotK[0][j].multiply(b[0]); for (int l = 1; l < stages; ++l) { sum = sum.add(yDotK[l][j].multiply(b[l])); } yTmp[j] = y[j].add(getStepSize().multiply(sum)); } final T stepEnd = getStepStart().getTime().add(getStepSize()); final T[] yDotTmp = computeDerivatives(stepEnd, yTmp); final FieldODEStateAndDerivative stateTmp = new FieldODEStateAndDerivative(stepEnd, yTmp, yDotTmp); // discrete events handling System.arraycopy(yTmp, 0, y, 0, y0.length); setStepStart(acceptStep(createInterpolator(forward, yDotK, getStepStart(), stateTmp, equations.getMapper()), finalTime)); if (!isLastStep()) { // stepsize control for next step final T nextT = getStepStart().getTime().add(getStepSize()); final boolean nextIsLast = forward ? (nextT.subtract(finalTime).getReal() >= 0) : (nextT.subtract(finalTime).getReal() <= 0); if (nextIsLast) { setStepSize(finalTime.subtract(getStepStart().getTime())); } } } while (!isLastStep()); final FieldODEStateAndDerivative finalState = getStepStart(); setStepStart(null); setStepSize(null); return finalState; } /** Fast computation of a single step of ODE integration. *

This method is intended for the limited use case of * very fast computation of only one step without using any of the * rich features of general integrators that may take some time * to set up (i.e. no step handlers, no events handlers, no additional * states, no interpolators, no error control, no evaluations count, * no sanity checks ...). It handles the strict minimum of computation, * so it can be embedded in outer loops.

*

* This method is not used at all by the {@link #integrate(FieldExpandableODE, * FieldODEState, RealFieldElement)} method. It also completely ignores the step set at * construction time, and uses only a single step to go from {@code t0} to {@code t}. *

*

* As this method does not use any of the state-dependent features of the integrator, * it should be reasonably thread-safe if and only if the provided differential * equations are themselves thread-safe. *

* @param equations differential equations to integrate * @param t0 initial time * @param y0 initial value of the state vector at t0 * @param t target time for the integration * (can be set to a value smaller than {@code t0} for backward integration) * @return state vector at {@code t} */ public T[] singleStep(final FirstOrderFieldDifferentialEquations equations, final T t0, final T[] y0, final T t) { // create some internal working arrays final T[] y = y0.clone(); final int stages = c.length + 1; final T[][] yDotK = MathArrays.buildArray(getField(), stages, -1); final T[] yTmp = y0.clone(); // first stage final T h = t.subtract(t0); yDotK[0] = equations.computeDerivatives(t0, y); // next stages for (int k = 1; k < stages; ++k) { for (int j = 0; j < y0.length; ++j) { T sum = yDotK[0][j].multiply(a[k-1][0]); for (int l = 1; l < k; ++l) { sum = sum.add(yDotK[l][j].multiply(a[k-1][l])); } yTmp[j] = y[j].add(h.multiply(sum)); } yDotK[k] = equations.computeDerivatives(t0.add(h.multiply(c[k-1])), yTmp); } // estimate the state at the end of the step for (int j = 0; j < y0.length; ++j) { T sum = yDotK[0][j].multiply(b[0]); for (int l = 1; l < stages; ++l) { sum = sum.add(yDotK[l][j].multiply(b[l])); } y[j] = y[j].add(h.multiply(sum)); } return y; } }




© 2015 - 2024 Weber Informatics LLC | Privacy Policy