1 /* Copyright 2002-2025 CS GROUP
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.propagation.integration;
18
19 import org.hipparchus.CalculusFieldElement;
20 import org.orekit.propagation.FieldAdditionalDataProvider;
21 import org.orekit.propagation.FieldSpacecraftState;
22 import org.orekit.time.FieldAbsoluteDate;
23
24 /** Provider for additional derivatives.
25 *
26 * <p>
27 * In some cases users may need to integrate some problem-specific equations along with
28 * classical spacecraft equations of motions. One example is optimal control in low
29 * thrust where adjoint parameters linked to the minimized Hamiltonian must be integrated.
30 * Another example is formation flying or rendez-vous which use the Clohessy-Whiltshire
31 * equations for the relative motion.
32 * </p>
33 * <p>
34 * This interface allows users to add such equations to a {@link
35 * org.orekit.propagation.numerical.FieldNumericalPropagator numerical propagator} or a {@link
36 * org.orekit.propagation.semianalytical.dsst.FieldDSSTPropagator DSST propagator}. Users provide the
37 * equations as an implementation of this interface and register it to the propagator thanks to
38 * its {@link FieldAbstractIntegratedPropagator#addAdditionalDerivativesProvider(FieldAdditionalDerivativesProvider)}
39 * method. Several such objects can be registered with each numerical propagator, but it is
40 * recommended to gather in the same object the sets of parameters which equations can interact
41 * on each others states.
42 * </p>
43 * <p>
44 * This interface is the numerical (read not already integrated) counterpart of
45 * the {@link FieldAdditionalDataProvider} interface.
46 * It allows to append various additional state parameters to any {@link
47 * org.orekit.propagation.numerical.FieldNumericalPropagator numerical propagator} or {@link
48 * org.orekit.propagation.semianalytical.dsst.FieldDSSTPropagator DSST propagator}.
49 * </p>
50 * @see org.orekit.propagation.integration.FieldAbstractIntegratedPropagator
51 * @author Luc Maisonobe
52 * @since 11.1
53 * @param <T> type of the field elements
54 */
55 public interface FieldAdditionalDerivativesProvider<T extends CalculusFieldElement<T>> {
56
57 /** Get the name of the additional derivatives (which will become state once integrated).
58 * @return name of the additional state (names containing "orekit"
59 * with any case are reserved for the library internal use)
60 */
61 String getName();
62
63 /** Get the dimension of the generated derivative.
64 * @return dimension of the generated
65 */
66 int getDimension();
67
68 /** Initialize the generator at the start of propagation.
69 * @param initialState initial state information at the start of propagation
70 * @param target date of propagation
71 */
72 default void init(final FieldSpacecraftState<T> initialState, final FieldAbsoluteDate<T> target) {
73 // nothing by default
74 }
75
76 /** Check if this provider should yield so another provider has an opportunity to add missing parts.
77 * <p>
78 * Decision to yield is often based on an additional state being {@link FieldSpacecraftState#hasAdditionalData(String)
79 * already available} in the provided {@code state} (but it could theoretically also depend on
80 * an additional state derivative being {@link FieldSpacecraftState#hasAdditionalStateDerivative(String)
81 * already available}, or any other criterion). If for example a provider needs the state transition
82 * matrix, it could implement this method as:
83 * </p>
84 * <pre>{@code
85 * public boolean yields(final FieldSpacecraftState<T> state) {
86 * return !state.getAdditionalStates().containsKey("STM");
87 * }
88 * }</pre>
89 * <p>
90 * The default implementation returns {@code false}, meaning that derivative data can be
91 * {@link #combinedDerivatives(FieldSpacecraftState) computed} immediately.
92 * </p>
93 * @param state state to handle
94 * @return true if this provider should yield so another provider has an opportunity to add missing parts
95 * as the state is incrementally built up
96 */
97 default boolean yields(FieldSpacecraftState<T> state) {
98 return false;
99 }
100
101 /** Compute the derivatives related to the additional state (and optionally main state increments).
102 * @param s current state information: date, kinematics, attitude, and
103 * additional states this equations depend on (according to the
104 * {@link #yields(FieldSpacecraftState) yields} method)
105 * @return computed combined derivatives, which may include some incremental
106 * coupling effect to add to main state derivatives
107 * @since 11.2
108 */
109 FieldCombinedDerivatives<T> combinedDerivatives(FieldSpacecraftState<T> s);
110
111 }