PulsatingSphericalHarmonics.java
- /* Copyright 2002-2022 CS GROUP
- * Licensed to CS GROUP (CS) under one or more
- * contributor license agreements. See the NOTICE file distributed with
- * this work for additional information regarding copyright ownership.
- * CS 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.orekit.forces.gravity.potential;
- import org.hipparchus.util.FastMath;
- import org.hipparchus.util.MathUtils;
- import org.hipparchus.util.SinCos;
- import org.orekit.time.AbsoluteDate;
- /** Simple implementation of {@link RawSphericalHarmonicsProvider} for pulsating gravity fields.
- * @author Luc Maisonobe
- * @since 6.0
- * @deprecated as of 11.1, replaced by {@link PiecewiseSphericalHarmonics}
- */
- @Deprecated
- class PulsatingSphericalHarmonics implements RawSphericalHarmonicsProvider {
- /** Underlying part of the field. */
- private final RawSphericalHarmonicsProvider provider;
- /** Pulsation (rad/s). */
- private final double pulsation;
- /** Converter from triangular to flatten array.
- * @since 11.1
- */
- private final Flattener flattener;
- /** Cosine component of the cosine coefficients. */
- private final double[] cosC;
- /** Sine component of the cosine coefficients. */
- private final double[] sinC;
- /** Cosine component of the sine coefficients. */
- private final double[] cosS;
- /** Sine component of the sine coefficients. */
- private final double[] sinS;
- /** Simple constructor.
- * @param provider underlying part of the field
- * @param period period of the pulsation (s)
- * @param cosC cosine component of the cosine coefficients
- * @param sinC sine component of the cosine coefficients
- * @param cosS cosine component of the sine coefficients
- * @param sinS sine component of the sine coefficients
- * @deprecated as of 11.1, replaced by {@link #PulsatingSphericalHarmonics(RawSphericalHarmonicsProvider,
- * double, Flattener, double[], double[], double[], double[])}
- */
- @Deprecated
- PulsatingSphericalHarmonics(final RawSphericalHarmonicsProvider provider,
- final double period,
- final double[][] cosC, final double[][] sinC,
- final double[][] cosS, final double[][] sinS) {
- this(provider, period, buildFlattener(cosC),
- buildFlattener(cosC).flatten(cosC), buildFlattener(sinC).flatten(sinC),
- buildFlattener(cosS).flatten(cosS), buildFlattener(sinS).flatten(sinS));
- }
- /** Simple constructor.
- * @param provider underlying part of the field
- * @param period period of the pulsation (s)
- * @param flattener flattener from triangular to flatten array
- * @param cosC cosine component of the cosine coefficients
- * @param sinC sine component of the cosine coefficients
- * @param cosS cosine component of the sine coefficients
- * @param sinS sine component of the sine coefficients
- * @since 11.1
- */
- PulsatingSphericalHarmonics(final RawSphericalHarmonicsProvider provider,
- final double period, final Flattener flattener,
- final double[] cosC, final double[] sinC,
- final double[] cosS, final double[] sinS) {
- this.provider = provider;
- this.pulsation = MathUtils.TWO_PI / period;
- this.flattener = flattener;
- this.cosC = cosC.clone();
- this.sinC = sinC.clone();
- this.cosS = cosS.clone();
- this.sinS = sinS.clone();
- }
- /** Get a flattener for a triangular array.
- * @param triangular triangular array to flatten
- * @return flattener suited for triangular array dimensions
- * @since 11.1
- */
- private static Flattener buildFlattener(final double[][] triangular) {
- return new Flattener(triangular.length - 1, triangular[triangular.length - 1].length - 1);
- }
- /** {@inheritDoc} */
- public int getMaxDegree() {
- return FastMath.max(flattener.getDegree(), provider.getMaxDegree());
- }
- /** {@inheritDoc} */
- public int getMaxOrder() {
- return FastMath.max(flattener.getOrder(), provider.getMaxOrder());
- }
- /** {@inheritDoc} */
- public double getMu() {
- return provider.getMu();
- }
- /** {@inheritDoc} */
- public double getAe() {
- return provider.getAe();
- }
- /** {@inheritDoc} */
- public AbsoluteDate getReferenceDate() {
- return provider.getReferenceDate();
- }
- /** {@inheritDoc} */
- @Deprecated
- public double getOffset(final AbsoluteDate date) {
- return provider.getOffset(date);
- }
- /** {@inheritDoc} */
- public TideSystem getTideSystem() {
- return provider.getTideSystem();
- }
- @Override
- @Deprecated
- public RawSphericalHarmonics onDate(final AbsoluteDate date) {
- //raw (constant) harmonics
- final RawSphericalHarmonics raw = provider.onDate(date);
- //phase angle, will loose precision for large offsets
- final double alpha = pulsation * provider.getOffset(date);
- //pre-compute transcendental functions
- final SinCos scAlpha = FastMath.sinCos(alpha);
- return new RawSphericalHarmonics() {
- @Override
- public AbsoluteDate getDate() {
- return date;
- }
- /** {@inheritDoc} */
- public double getRawCnm(final int n, final int m) {
- // retrieve the underlying part of the coefficient
- double cnm = raw.getRawCnm(n, m);
- if (flattener.withinRange(n, m)) {
- // add pulsation
- cnm += cosC[flattener.index(n, m)] * scAlpha.cos() + sinC[flattener.index(n, m)] * scAlpha.sin();
- }
- return cnm;
- }
- /** {@inheritDoc} */
- public double getRawSnm(final int n, final int m) {
- // retrieve the constant part of the coefficient
- double snm = raw.getRawSnm(n, m);
- if (flattener.withinRange(n, m)) {
- // add pulsation
- snm += cosS[flattener.index(n, m)] * scAlpha.cos() + sinS[flattener.index(n, m)] * scAlpha.sin();
- }
- return snm;
- }
- };
- }
- }