1   /* Copyright 2022-2025 Romain Serra
2    * Licensed to CS GROUP (CS) under one or more
3    * contributor license agreements.  See the NOTICE file distributed with
4    * this work for additional information regarding copyright ownership.
5    * CS licenses this file to You under the Apache License, Version 2.0
6    * (the "License"); you may not use this file except in compliance with
7    * the License.  You may obtain a copy of the License at
8    *
9    *   http://www.apache.org/licenses/LICENSE-2.0
10   *
11   * Unless required by applicable law or agreed to in writing, software
12   * distributed under the License is distributed on an "AS IS" BASIS,
13   * WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.
14   * See the License for the specific language governing permissions and
15   * limitations under the License.
16   */
17  package org.orekit.frames;
18  
19  import org.hipparchus.CalculusFieldElement;
20  import org.hipparchus.Field;
21  import org.hipparchus.geometry.euclidean.threed.FieldRotation;
22  import org.hipparchus.geometry.euclidean.threed.FieldVector3D;
23  import org.hipparchus.util.MathArrays;
24  import org.orekit.time.AbsoluteDate;
25  import org.orekit.time.FieldAbsoluteDate;
26  import org.orekit.utils.FieldPVCoordinates;
27  import org.orekit.utils.PVCoordinates;
28  import org.orekit.utils.TimeStampedFieldPVCoordinates;
29  import org.orekit.utils.TimeStampedPVCoordinates;
30  
31  import java.util.Arrays;
32  
33  /**
34   * A transform that only includes translation and rotation as well as their respective rates.
35   * It is kinematic in the sense that it cannot transform an acceleration vector.
36   *
37   * @author Romain Serra
38   * @see FieldStaticTransform
39   * @see FieldTransform
40   * @see KinematicTransform
41   * @since 12.1
42   */
43  public interface FieldKinematicTransform<T extends CalculusFieldElement<T>> extends FieldStaticTransform<T> {
44  
45      /**
46       * Get the identity kinematic transform.
47       *
48       * @param <T> type of the elements
49       * @param field field used by default
50       * @return identity transform.
51       */
52      static <T extends CalculusFieldElement<T>> FieldKinematicTransform<T> getIdentity(final Field<T> field) {
53          return FieldTransform.getIdentity(field);
54      }
55  
56      /** Compute a composite velocity.
57       * @param first first applied transform
58       * @param second second applied transform
59       * @param <T> the type of the field elements
60       * @return velocity part of the composite transform
61       */
62      static <T extends CalculusFieldElement<T>> FieldVector3D<T> compositeVelocity(final FieldKinematicTransform<T> first,
63                                                                                    final FieldKinematicTransform<T> second) {
64  
65          final FieldVector3D<T> v1 = first.getVelocity();
66          final FieldRotation<T> r1 = first.getRotation();
67          final FieldVector3D<T> o1 = first.getRotationRate();
68          final FieldVector3D<T> p2 = second.getTranslation();
69          final FieldVector3D<T> v2 = second.getVelocity();
70  
71          final FieldVector3D<T> crossP = FieldVector3D.crossProduct(o1, p2);
72  
73          return v1.add(r1.applyInverseTo(v2.add(crossP)));
74      }
75  
76      /** Compute a composite rotation rate.
77       * @param <T> type of the elements
78       * @param first first applied transform
79       * @param second second applied transform
80       * @return rotation rate part of the composite transform
81       */
82      static <T extends CalculusFieldElement<T>> FieldVector3D<T> compositeRotationRate(final FieldKinematicTransform<T> first,
83                                                                                        final FieldKinematicTransform<T> second) {
84  
85          final FieldVector3D<T> o1 = first.getRotationRate();
86          final FieldRotation<T> r2 = second.getRotation();
87          final FieldVector3D<T> o2 = second.getRotationRate();
88  
89          return o2.add(r2.applyTo(o1));
90      }
91  
92      /** Transform {@link PVCoordinates}, without the acceleration vector.
93       * @param pv the position-velocity couple to transform.
94       * @return transformed position-velocity
95       */
96      default FieldPVCoordinates<T> transformOnlyPV(final FieldPVCoordinates<T> pv) {
97          final FieldVector3D<T> transformedP = transformPosition(pv.getPosition());
98          final FieldVector3D<T> crossP       = FieldVector3D.crossProduct(getRotationRate(), transformedP);
99          final FieldVector3D<T> transformedV = getRotation().applyTo(pv.getVelocity().add(getVelocity())).subtract(crossP);
100         return new FieldPVCoordinates<>(transformedP, transformedV);
101     }
102 
103     /** Transform {@link TimeStampedPVCoordinates}, without the acceleration vector.
104      * <p>
105      * In order to allow the user more flexibility, this method does <em>not</em> check for
106      * consistency between the transform {@link #getDate() date} and the time-stamped
107      * position-velocity {@link TimeStampedPVCoordinates#getDate() date}. The returned
108      * value will always have the same {@link TimeStampedPVCoordinates#getDate() date} as
109      * the input argument, regardless of the instance {@link #getDate() date}.
110      * </p>
111      * @param pv the position-velocity couple to transform.
112      * @return transformed position-velocity
113      */
114     default TimeStampedFieldPVCoordinates<T> transformOnlyPV(final TimeStampedFieldPVCoordinates<T> pv) {
115         final FieldVector3D<T> transformedP = transformPosition(pv.getPosition());
116         final FieldVector3D<T> crossP       = FieldVector3D.crossProduct(getRotationRate(), transformedP);
117         final FieldVector3D<T> transformedV = getRotation().applyTo(pv.getVelocity().add(getVelocity())).subtract(crossP);
118         return new TimeStampedFieldPVCoordinates<>(pv.getDate(), transformedP, transformedV,
119                 FieldVector3D.getZero(pv.getDate().getField()));
120     }
121 
122     /** Compute the Jacobian of the {@link #transformOnlyPV(FieldPVCoordinates)} (FieldPVCoordinates)}
123      * method of the transform.
124      * <p>
125      * Element {@code jacobian[i][j]} is the derivative of Cartesian coordinate i
126      * of the transformed {@link FieldPVCoordinates} with respect to Cartesian coordinate j
127      * of the input {@link FieldPVCoordinates} in method {@link #transformOnlyPV(FieldPVCoordinates)}.
128      * </p>
129      * <p>
130      * This definition implies that if we define position-velocity coordinates
131      * <pre>
132      * PV₁ = transform.transformPVCoordinates(PV₀), then
133      * </pre>
134      * <p> their differentials dPV₁ and dPV₀ will obey the following relation
135      * where J is the matrix computed by this method:
136      * <pre>
137      * dPV₁ = J &times; dPV₀
138      * </pre>
139      *
140      * @return Jacobian matrix
141      */
142     default T[][] getPVJacobian() {
143         final Field<T> field = getFieldDate().getField();
144         final T zero = field.getZero();
145         final T[][] jacobian = MathArrays.buildArray(field, 6, 6);
146 
147         // elementary matrix for rotation
148         final T[][] mData = getRotation().getMatrix();
149 
150         // dP1/dP0
151         System.arraycopy(mData[0], 0, jacobian[0], 0, 3);
152         System.arraycopy(mData[1], 0, jacobian[1], 0, 3);
153         System.arraycopy(mData[2], 0, jacobian[2], 0, 3);
154 
155         // dP1/dV0
156         Arrays.fill(jacobian[0], 3, 6, zero);
157         Arrays.fill(jacobian[1], 3, 6, zero);
158         Arrays.fill(jacobian[2], 3, 6, zero);
159 
160         // dV1/dP0
161         final FieldVector3D<T> o = getRotationRate();
162         final T ox = o.getX();
163         final T oy = o.getY();
164         final T oz = o.getZ();
165         for (int i = 0; i < 3; ++i) {
166             jacobian[3][i] = oz.multiply(mData[1][i]).subtract(oy.multiply(mData[2][i]));
167             jacobian[4][i] = ox.multiply(mData[2][i]).subtract(oz.multiply(mData[0][i]));
168             jacobian[5][i] = oy.multiply(mData[0][i]).subtract(ox.multiply(mData[1][i]));
169         }
170 
171         // dV1/dV0
172         System.arraycopy(mData[0], 0, jacobian[3], 3, 3);
173         System.arraycopy(mData[1], 0, jacobian[4], 3, 3);
174         System.arraycopy(mData[2], 0, jacobian[5], 3, 3);
175 
176         return jacobian;
177     }
178 
179     /** Get the first time derivative of the translation.
180      * @return first time derivative of the translation
181      * @see #getTranslation()
182      */
183     FieldVector3D<T> getVelocity();
184 
185     /** Get the first time derivative of the rotation.
186      * <p>The norm represents the angular rate.</p>
187      * @return First time derivative of the rotation
188      * @see #getRotation()
189      */
190     FieldVector3D<T> getRotationRate();
191 
192     /**
193      * Get the inverse transform of the instance.
194      *
195      * @return inverse transform of the instance
196      */
197     FieldKinematicTransform<T> getInverse();
198 
199     /**
200      * Build a transform by combining two existing ones.
201      * <p>
202      * Note that the dates of the two existing transformed are <em>ignored</em>,
203      * and the combined transform date is set to the date supplied in this
204      * constructor without any attempt to shift the raw transforms. This is a
205      * design choice allowing user full control of the combination.
206      * </p>
207      *
208      * @param <T> type of the elements
209      * @param date   date of the transform
210      * @param first  first transform applied
211      * @param second second transform applied
212      * @return the newly created kinematic transform that has the same effect as
213      * applying {@code first}, then {@code second}.
214      * @see #of(FieldAbsoluteDate, FieldPVCoordinates, FieldRotation, FieldVector3D)
215      */
216     static <T extends CalculusFieldElement<T>> FieldKinematicTransform<T> compose(final FieldAbsoluteDate<T> date,
217                                                                                   final FieldKinematicTransform<T> first,
218                                                                                   final FieldKinematicTransform<T> second) {
219         final FieldVector3D<T> composedTranslation = FieldStaticTransform.compositeTranslation(first, second);
220         final FieldVector3D<T> composedTranslationRate = FieldKinematicTransform.compositeVelocity(first, second);
221         return of(date, new FieldPVCoordinates<>(composedTranslation, composedTranslationRate),
222                 FieldStaticTransform.compositeRotation(first, second),
223                 FieldKinematicTransform.compositeRotationRate(first, second));
224     }
225 
226     /**
227      * Create a new kinematic transform from a rotation and zero, constant translation.
228      *
229      * @param <T> type of the elements
230      * @param date     of translation.
231      * @param rotation to apply after the translation. That is after translating
232      *                 applying this rotation produces positions expressed in
233      *                 the new frame.
234      * @param rotationRate rate of rotation
235      * @return the newly created kinematic transform.
236      * @see #of(FieldAbsoluteDate, FieldPVCoordinates, FieldRotation, FieldVector3D)
237      */
238     static <T extends CalculusFieldElement<T>> FieldKinematicTransform<T> of(final FieldAbsoluteDate<T> date,
239                                                                              final FieldRotation<T> rotation,
240                                                                              final FieldVector3D<T> rotationRate) {
241         return of(date, FieldPVCoordinates.getZero(date.getField()), rotation, rotationRate);
242     }
243 
244     /**
245      * Create a new kinematic transform from a translation and its rate.
246      *
247      * @param <T> type of the elements
248      * @param date        of translation.
249      * @param pvCoordinates translation (with rate) to apply, expressed in the old frame. That is, the
250      *                    opposite of the coordinates of the new origin in the
251      *                    old frame.
252      * @return the newly created kinematic transform.
253      * @see #of(FieldAbsoluteDate, FieldPVCoordinates, FieldRotation, FieldVector3D)
254      */
255     static <T extends CalculusFieldElement<T>> FieldKinematicTransform<T> of(final FieldAbsoluteDate<T> date,
256                                                                              final FieldPVCoordinates<T> pvCoordinates) {
257         final Field<T> field = date.getField();
258         return of(date, pvCoordinates, FieldRotation.getIdentity(field), FieldVector3D.getZero(field));
259     }
260 
261     /**
262      * Create a new kinematic transform from a non-Field version.
263      *
264      * @param <T> type of the elements
265      * @param field field.
266      * @param kinematicTransform non-Field kinematic transform
267      * @return the newly created kinematic transform.
268      * @see #of(FieldAbsoluteDate, FieldPVCoordinates, FieldRotation, FieldVector3D)
269      */
270     static <T extends CalculusFieldElement<T>> FieldKinematicTransform<T> of(final Field<T> field,
271                                                                              final KinematicTransform kinematicTransform) {
272         final FieldAbsoluteDate<T> date = new FieldAbsoluteDate<>(field, kinematicTransform.getDate());
273         final FieldPVCoordinates<T> pvCoordinates = new FieldPVCoordinates<>(field,
274             new PVCoordinates(kinematicTransform.getTranslation(), kinematicTransform.getVelocity()));
275         final FieldRotation<T> rotation = new FieldRotation<>(field, kinematicTransform.getRotation());
276         final FieldVector3D<T> rotationRate = new FieldVector3D<>(field, kinematicTransform.getRotationRate());
277         return of(date, pvCoordinates, rotation, rotationRate);
278     }
279 
280     /**
281      * Create a new kinematic transform from a translation and rotation.
282      *
283      * @param <T> type of the elements
284      * @param date        of translation.
285      * @param pvCoordinates translation (with rate) to apply, expressed in the old frame. That is, the
286      *                    opposite of the coordinates of the new origin in the
287      *                    old frame.
288      * @param rotation    to apply after the translation. That is after
289      *                    translating applying this rotation produces positions
290      *                    expressed in the new frame.
291      * @param rotationRate rate of rotation
292      * @return the newly created kinematic transform.
293      * @see #compose(FieldAbsoluteDate, FieldKinematicTransform, FieldKinematicTransform)
294      * @see #of(FieldAbsoluteDate, FieldPVCoordinates, FieldRotation, FieldVector3D)
295      * @see #of(FieldAbsoluteDate, FieldPVCoordinates, FieldRotation, FieldVector3D)
296      */
297     static <T extends CalculusFieldElement<T>> FieldKinematicTransform<T> of(final FieldAbsoluteDate<T> date,
298                                                                           final FieldPVCoordinates<T> pvCoordinates,
299                                                                           final FieldRotation<T> rotation,
300                                                                           final FieldVector3D<T> rotationRate) {
301         return new FieldKinematicTransform<T>() {
302 
303             @Override
304             public FieldKinematicTransform<T> getInverse() {
305                 final FieldRotation<T> r = getRotation();
306                 final FieldVector3D<T> rp = r.applyTo(getTranslation());
307                 final FieldVector3D<T> pInv = rp.negate();
308                 final FieldVector3D<T> crossP      = FieldVector3D.crossProduct(getRotationRate(), rp);
309                 final FieldVector3D<T> vInv        = crossP.subtract(getRotation().applyTo(getVelocity()));
310                 final FieldRotation<T> rInv = r.revert();
311                 return FieldKinematicTransform.of(date, new FieldPVCoordinates<>(pInv, vInv),
312                         rInv, rInv.applyTo(getRotationRate()).negate());
313             }
314 
315             @Override
316             public AbsoluteDate getDate() {
317                 return date.toAbsoluteDate();
318             }
319 
320             @Override
321             public FieldAbsoluteDate<T> getFieldDate() {
322                 return date;
323             }
324 
325             @Override
326             public FieldVector3D<T> getTranslation() {
327                 return pvCoordinates.getPosition();
328             }
329 
330             @Override
331             public FieldRotation<T> getRotation() {
332                 return rotation;
333             }
334 
335             @Override
336             public FieldVector3D<T> getVelocity() {
337                 return pvCoordinates.getVelocity();
338             }
339 
340             @Override
341             public FieldVector3D<T> getRotationRate() {
342                 return rotationRate;
343             }
344         };
345     }
346 
347 }