changed Nordsieck transformer to an Adams-specific Nordsieck transformer
the transformer associated with BDF integrator will be quite different git-svn-id: https://svn.apache.org/repos/asf/commons/proper/math/trunk@789158 13f79535-47bb-0310-9956-ffa450edef68
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@ -15,7 +15,7 @@
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* limitations under the License.
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*/
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package org.apache.commons.math.ode;
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package org.apache.commons.math.ode.nonstiff;
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import java.util.Arrays;
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import java.util.HashMap;
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@ -32,13 +32,12 @@ import org.apache.commons.math.linear.FieldMatrix;
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import org.apache.commons.math.linear.MatrixUtils;
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import org.apache.commons.math.linear.MatrixVisitorException;
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import org.apache.commons.math.linear.RealMatrix;
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import org.apache.commons.math.ode.nonstiff.AdamsBashforthIntegrator;
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import org.apache.commons.math.ode.nonstiff.AdamsMoultonIntegrator;
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/** Transformer for Nordsieck vectors.
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* <p>This class i used by {@link MultistepIntegrator multistep integrators}
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* to convert between classical representation with several previous first
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* derivatives and Nordsieck representation with higher order scaled derivatives.</p>
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/** Transformer to Nordsieck vectors for Adams integrators.
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* <p>This class i used by {@link AdamsBashforthIntegrator Adams-Bashforth} and
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* {@link AdamsMoultonIntegrator Adams-Moulton} integrators to convert between
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* classical representation with several previous first derivatives and Nordsieck
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* representation with higher order scaled derivatives.</p>
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*
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* <p>We define scaled derivatives s<sub>i</sub>(n) at step n as:
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* <pre>
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@ -89,18 +88,9 @@ import org.apache.commons.math.ode.nonstiff.AdamsMoultonIntegrator;
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* </pre></p>
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*
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* <p>Changing -i into +i in the formula above can be used to compute a similar transform between
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* classical representation and Nordsieck vector at step start. The resulting Q matrix is simply
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* classical representation and Nordsieck vector at step start. The resulting matrix is simply
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* the absolute value of matrix P.</p>
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*
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* <p>Using the Nordsieck vector has several advantages:
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* <ul>
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* <li>it greatly simplifies step interpolation as the interpolator mainly applies
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* Taylor series formulas,</li>
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* <li>it simplifies step changes that occur when discrete events that truncate
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* the step are triggered,</li>
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* <li>it allows to extend the methods in order to support adaptive stepsize (not implemented yet).</li>
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* </ul></p>
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*
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*
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* <p>For {@link AdamsBashforthIntegrator Adams-Bashforth} method, the Nordsieck vector
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* at step n+1 is computed from the Nordsieck vector at step n as follows:
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* <ul>
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@ -126,16 +116,6 @@ import org.apache.commons.math.ode.nonstiff.AdamsMoultonIntegrator;
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* <li>S<sub>1</sub>(n+1) = h f(t<sub>n+1</sub>, Y<sub>n+1</sub>)</li>
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* <li>R<sub>n+1</sub> = (s<sub>1</sub>(n) - s<sub>1</sub>(n+1)) P<sup>-1</sup> u + P<sup>-1</sup> A P r<sub>n</sub></li>
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* </ul>
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* where A is a rows shifting matrix (the lower left part is an identity matrix):
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* <pre>
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* [ 0 0 ... 0 0 | 0 ]
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* [ ---------------+---]
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* [ 1 0 ... 0 0 | 0 ]
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* A = [ 0 1 ... 0 0 | 0 ]
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* [ ... | 0 ]
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* [ 0 0 ... 1 0 | 0 ]
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* [ 0 0 ... 0 1 | 0 ]
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* </pre>
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* From this predicted vector, the corrected vector is computed as follows:
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* <ul>
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* <li>y<sub>n+1</sub> = y<sub>n</sub> + S<sub>1</sub>(n+1) + [ -1 +1 -1 +1 ... ±1 ] r<sub>n+1</sub></li>
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@ -153,32 +133,33 @@ import org.apache.commons.math.ode.nonstiff.AdamsMoultonIntegrator;
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* @version $Revision$ $Date$
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* @since 2.0
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*/
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public class NordsieckTransformer {
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public class AdamsNordsieckTransformer {
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/** Cache for already computed coefficients. */
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private static final Map<Integer, NordsieckTransformer> cache =
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new HashMap<Integer, NordsieckTransformer>();
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private static final Map<Integer, AdamsNordsieckTransformer> cache =
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new HashMap<Integer, AdamsNordsieckTransformer>();
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/** Initialization matrix for the higher order derivatives wrt y'', y''' ... */
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private final RealMatrix initialization;
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private final Array2DRowRealMatrix initialization;
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/** Update matrix for the higher order derivatives h<sup>2</sup>/2y'', h<sup>3</sup>/6 y''' ... */
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private final RealMatrix update;
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private final Array2DRowRealMatrix update;
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/** Update coefficients of the higher order derivatives wrt y'. */
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private final double[] c1;
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/** Simple constructor.
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* @param nSteps number of steps of the multistep method
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* (including the one being computed)
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* (excluding the one being computed)
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*/
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private NordsieckTransformer(final int nSteps) {
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private AdamsNordsieckTransformer(final int nSteps) {
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// compute exact coefficients
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FieldMatrix<BigFraction> bigP = buildP(nSteps);
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FieldDecompositionSolver<BigFraction> pSolver =
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new FieldLUDecompositionImpl<BigFraction>(bigP).getSolver();
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BigFraction[] u = new BigFraction[nSteps - 1];
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BigFraction[] u = new BigFraction[nSteps];
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Arrays.fill(u, BigFraction.ONE);
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BigFraction[] bigC1 = pSolver.solve(u);
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@ -190,12 +171,12 @@ public class NordsieckTransformer {
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// shift rows
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shiftedP[i] = shiftedP[i - 1];
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}
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shiftedP[0] = new BigFraction[nSteps - 1];
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shiftedP[0] = new BigFraction[nSteps];
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Arrays.fill(shiftedP[0], BigFraction.ZERO);
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FieldMatrix<BigFraction> bigMSupdate =
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pSolver.solve(new Array2DRowFieldMatrix<BigFraction>(shiftedP, false));
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// initialization coefficients, computed from a Q matrix = abs(P)
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// initialization coefficients, computed from a R matrix = abs(P)
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bigP.walkInOptimizedOrder(new DefaultFieldMatrixChangingVisitor<BigFraction>(BigFraction.ZERO) {
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/** {@inheritDoc} */
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@Override
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@ -203,14 +184,14 @@ public class NordsieckTransformer {
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return ((column & 0x1) == 0x1) ? value : value.negate();
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}
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});
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FieldMatrix<BigFraction> bigQInverse =
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FieldMatrix<BigFraction> bigRInverse =
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new FieldLUDecompositionImpl<BigFraction>(bigP).getSolver().getInverse();
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// convert coefficients to double
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initialization = MatrixUtils.bigFractionMatrixToRealMatrix(bigQInverse);
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initialization = MatrixUtils.bigFractionMatrixToRealMatrix(bigRInverse);
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update = MatrixUtils.bigFractionMatrixToRealMatrix(bigMSupdate);
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c1 = new double[nSteps - 1];
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for (int i = 0; i < nSteps - 1; ++i) {
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c1 = new double[nSteps];
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for (int i = 0; i < nSteps; ++i) {
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c1[i] = bigC1[i].doubleValue();
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}
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@ -218,37 +199,45 @@ public class NordsieckTransformer {
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/** Get the Nordsieck transformer for a given number of steps.
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* @param nSteps number of steps of the multistep method
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* (including the one being computed)
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* (excluding the one being computed)
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* @return Nordsieck transformer for the specified number of steps
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*/
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public static NordsieckTransformer getInstance(final int nSteps) {
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public static AdamsNordsieckTransformer getInstance(final int nSteps) {
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synchronized(cache) {
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NordsieckTransformer t = cache.get(nSteps);
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AdamsNordsieckTransformer t = cache.get(nSteps);
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if (t == null) {
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t = new NordsieckTransformer(nSteps);
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t = new AdamsNordsieckTransformer(nSteps);
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cache.put(nSteps, t);
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}
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return t;
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}
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}
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/** Build the P matrix transforming multistep to Nordsieck.
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* <p>
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* Multistep representation uses y(k), s<sub>1</sub>(k), s<sub>1</sub>(k-1) ... s<sub>1</sub>(k-(n-1)).
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* Nordsieck representation uses y(k), s<sub>1</sub>(k), s<sub>2</sub>(k) ... s<sub>n</sub>(k).
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* The two representations share their two first components y(k) and
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* s<sub>1</sub>(k). The P matrix is used to transform the remaining ones:
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/** Get the number of steps of the method
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* (excluding the one being computed).
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* @return number of steps of the method
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* (excluding the one being computed)
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*/
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public int getNSteps() {
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return c1.length;
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}
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/** Build the P matrix.
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* <p>The P matrix general terms are shifted j (-i)<sup>j-1</sup> terms:
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* <pre>
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* [ s<sub>1</sub>(k-1) ... s<sub>1</sub>(k-(n-1)]<sup>T</sup> = s<sub>1</sub>(k) [1 ... 1]<sup>T</sup> + P [s<sub>2</sub>(k) ... s<sub>n</sub>(k)]<sup>T</sup>
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* </pre>
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* </p>
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* [ -2 3 -4 5 ... ]
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* [ -4 12 -32 80 ... ]
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* P = [ -6 27 -108 405 ... ]
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* [ -8 48 -256 1280 ... ]
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* [ ... ]
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* </pre></p>
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* @param nSteps number of steps of the multistep method
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* (including the one being computed)
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* (excluding the one being computed)
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* @return P matrix
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*/
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private FieldMatrix<BigFraction> buildP(final int nSteps) {
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final BigFraction[][] pData = new BigFraction[nSteps - 1][nSteps - 1];
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final BigFraction[][] pData = new BigFraction[nSteps][nSteps];
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for (int i = 0; i < pData.length; ++i) {
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// build the P matrix elements from Taylor series formulas
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* will be modified
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* @return high order derivatives at step start
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*/
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public RealMatrix initializeHighOrderDerivatives(final double[] first,
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public Array2DRowRealMatrix initializeHighOrderDerivatives(final double[] first,
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final double[][] multistep) {
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for (int i = 0; i < multistep.length; ++i) {
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final double[] msI = multistep[i];
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return initialization.multiply(new Array2DRowRealMatrix(multistep, false));
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}
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/** Update the high order scaled derivatives (phase 1).
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/** Update the high order scaled derivatives for Adams integrators (phase 1).
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* <p>The complete update of high order derivatives has a form similar to:
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* <pre>
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* r<sub>n+1</sub> = (s<sub>1</sub>(n) - s<sub>1</sub>(n+1)) P<sup>-1</sup> u + P<sup>-1</sup> A P r<sub>n</sub>
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* @return updated high order derivatives
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* @see #updateHighOrderDerivativesPhase2(double[], double[], RealMatrix)
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*/
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public RealMatrix updateHighOrderDerivativesPhase1(final RealMatrix highOrder) {
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public Array2DRowRealMatrix updateHighOrderDerivativesPhase1(final Array2DRowRealMatrix highOrder) {
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return update.multiply(highOrder);
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}
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/** Update the high order scaled derivatives (phase 2).
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/** Update the high order scaled derivatives Adams integrators (phase 2).
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* <p>The complete update of high order derivatives has a form similar to:
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* <pre>
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* r<sub>n+1</sub> = (s<sub>1</sub>(n) - s<sub>1</sub>(n+1)) P<sup>-1</sup> u + P<sup>-1</sup> A P r<sub>n</sub>
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