move python/src/a/*.pxi to python/src/a.pyx
[liba.git] / include / a / trajbell.h
blob228de89d8374aa79b95a836a18dbc54d8a7caced
1 /*!
2 @file trajbell.h
3 @brief bell-shaped velocity trajectory
4 @details Trajectory Planning for Automatic Machines and Robots
5 */
7 #ifndef LIBA_TRAJBELL_H
8 #define LIBA_TRAJBELL_H
10 #include "a.h"
12 /*!
13 @ingroup A
14 @addtogroup A_TRAJBELL bell-shaped velocity trajectory
18 typedef struct a_trajbell a_trajbell;
20 #if defined(__cplusplus)
21 extern "C" {
22 #endif /* __cplusplus */
24 /*!
25 @brief generate for bell-shaped velocity trajectory
26 @details If \f$p_0>p_1\f$, then \f{aligned}{p_0=-p_0\\p_1=-p_1\\v_0=-v_0\\v_1=-v_1\f}
27 1. If \f$(v_m-v_0)j_m<a_m^2\f$, the maximum acceleration is not reached,
28 then \f{aligned}{T_{aj}&=\sqrt{\frac{v_m-v_0}{j_m}}\\T_a&=2T_{aj}\\a_m&=+j_mT_{aj}\f}
29 else \f{aligned}{T_{aj}&=\frac{a_m}{j_m}\\T_a&=T_{aj}+\frac{v_m-v_0}{a_m}\\a_m&=+a_m\f}
30 2. If \f$(v_m-v_1)j_m<a_m^2\f$, the maximum deceleration is not reached,
31 then \f{aligned}{T_{dj}&=\sqrt{\frac{v_m-v_1}{j_m}}\\T_d&=2T_{dj}\\d_m&=-j_mT_{dj}\f}
32 else \f{aligned}{T_{dj}&=\frac{a_m}{j_m}\\T_d&=T_{dj}+\frac{v_m-v_1}{a_m}\\d_m&=-a_m\f}
33 3. Calculate the constant velocity phase \f[T_v=\frac{p_1-p_0}{v_m}
34 -\frac{T_a}{2}\left(1+\frac{v_0}{v_m}\right)-\frac{T_d}{2}\left(1+\frac{v_1}{v_m}\right)\f]
35 If \f$T_v>0\f$, then there is a constant velocity phase and the phase calculation ends.
36 4. If \f$T_v<=0\f$, then \f$T_v=0\f$, \f{aligned}{T_{aj}&=T_{dj}=T_{j}=\frac{a_m}{j_m}\\
37 T_a&=\cfrac{\frac{a_m^2}{j_m}+\sqrt\Delta-2v_0}{2a_m}\\T_d&=\cfrac{\frac{a_m^2}{j_m}+\sqrt\Delta-2v_1}{2a_m}\\
38 \Delta&=\frac{a_m^4}{j_m^2}+2(v_0^2+v_1^2)+a_m\left(4(p_1-p_0)-2\frac{a_m}{j_m}(v_0+v_1)\right)\f}<br>
39 a. If \f$T_a<0\f$, there is only deceleration phase, then \f$T_a=0\f$,\f$T_{aj}=0\f$,
40 \f{aligned}{T_d&=2\cfrac{p_1-p_0}{v_1+v_0}\\
41 T_{dj}&=\frac{j_m(p_1-p_0)-\sqrt{j_m(j_m(p_1-p_0)^2+(v_1-v_0)(v_1+v_0)^2)}}{j_m(v_1+v_0 )}\f}
42 b. If \f$T_d<0\f$, there is only acceleration phase, then \f$T_d=0\f$,\f$T_{dj}=0\f$,
43 \f{aligned}{T_a&=2\cfrac{p_1-p_0}{v_1+v_0}\\
44 T_{aj}&=\frac{j_m(p_1-p_0)-\sqrt{j_m(j_m(p_1-p_0)^2+(v_0-v_1)(v_1+v_0)^2)}}{j_m(v_1+v_0 )}\f}
45 c. If \f$T_a\ge2T_j\f$, \f$T_d\ge2T_j\f$, then
46 \f{aligned}{a_m&=+j_mT_{aj}\\d_m&=-j_mT_{dj}\\v_m&=v_0+(T_a-T_{aj})a_m=v_1-(T_d-T_{dj})d_m\f}
47 d. If none of the above conditions are met, let \f$a_m=\alpha a_m, 0<\alpha<1\f$, and then repeat step 4.
48 5. Finally, use formulas to calculate position, velocity and acceleration.
49 @param[in,out] ctx points to an instance of bell-shaped velocity trajectory
50 @param[in] jm defines the maximum jerk during system operation
51 @param[in] am defines the maximum acceleration during system operation
52 @param[in] vm defines the maximum velocity during system operation
53 @param[in] p0 defines the initial position
54 @param[in] p1 defines the final position
55 @param[in] v0 defines the initial velocity
56 @param[in] v1 defines the final velocity
57 @return total duration
59 A_EXTERN a_float a_trajbell_gen(a_trajbell *ctx, a_float jm, a_float am, a_float vm,
60 a_float p0, a_float p1, a_float v0, a_float v1);
62 /*!
63 @brief calculate position for bell-shaped velocity trajectory
64 \f[
65 p(t)=\begin{cases}
66 p_0+v_0t+j_m\cfrac{t^3}{6},&t\in[0,T_{aj}]\\
67 p_0+v_0t+\cfrac{a_m}{6}(3t^3-3tT_{aj}+T_{aj}^2),&t\in[T_{aj},T_a-T_{aj}]\\
68 p_0+(v_m+v_0)\cfrac{T_a}{2}-v_m(T_a-t)+j_m\cfrac{(T_a-t)^3}{6},&t\in[T_a-T_{aj},T_a]\\
69 p_0+(v_m+v_0)\cfrac{T_a}{2}+v_m(t-T_a),&t\in[T_a,T_a+T_v]\\
70 p_1-(v_m+v_1)\cfrac{T_d}{2}+v_m(t-T+T_d)-j_m\cfrac{(t-T+T_d)^3}{6},&t\in[T-T_d,T-T_d+T_{dj}]\\
71 p_1-(v_m+v_1)\cfrac{T_d}{2}+v_m(t-T+T_d)\\
72 \quad+\cfrac{d_m}{6}\left(3(t-T+T_d)^2-3(t-T+T_d)T_{dj}+T_{dj}^2\right),&t\in[T-T_d+T_{dj},T-T_{dj}]\\
73 p_1-v_1(T-t)-j_m\cfrac{(T-t)^3}{6},&t\in[T-T_{dj},T]
74 \end{cases}
75 \f]
76 @param[in] ctx points to an instance of bell-shaped velocity trajectory
77 @param[in] dt difference between current time and initial time
78 @return position output
80 A_EXTERN a_float a_trajbell_pos(a_trajbell const *ctx, a_float dt);
82 /*!
83 @brief calculate velocity for bell-shaped velocity trajectory
84 \f[
85 \dot{p}(t)=\begin{cases}
86 v_0+j_m\frac{t^2}{2},&t\in[0,T_{aj}]\\
87 v_0+a_m(t-\cfrac{T_{aj}}{2}),&t\in[T_{aj},T_a-T_{aj}]\\
88 v_m-j_m\cfrac{(T_a-t)^2}{2},&t\in[T_a-T_{aj},T_a]\\
89 v_m,&t\in[T_a,T_a+T_v]\\
90 v_m-j_m\cfrac{(t-T+T_d)^2}{2},&t\in[T-T_d,T-T_d+T_{dj}]\\
91 v_m+d_m(t-T+T_d-\cfrac{T_{dj}}{2}),&t\in[T-T_d+T_{dj},T-T_{dj}]\\
92 v_1+j_m\cfrac{(T-t)^2}{2},&t\in[T-T_{dj},T]
93 \end{cases}
94 \f]
95 @param[in] ctx points to an instance of bell-shaped velocity trajectory
96 @param[in] dt difference between current time and initial time
97 @return velocity output
99 A_EXTERN a_float a_trajbell_vel(a_trajbell const *ctx, a_float dt);
102 @brief calculate acceleration for bell-shaped velocity trajectory
104 \ddot{p}(t)=\begin{cases}
105 j_mt,&t\in[0,T_{aj}]\\
106 j_mT_{aj}=a_m,&t\in[T_{aj},T_a-T_{aj}]\\
107 j_m(T_a-t),&t\in[T_a-T_{aj},T_a]\\
108 0,&t\in[T_a,T_a+T_v]\\
109 -j_m(t-T+T_d),&t\in[T-T_d,T-T_d+T_{dj}]\\
110 -j_mT_{dj}=d_m,&t\in[T-T_d+T_{dj},T-T_{dj}]\\
111 -j_m(T-t),&t\in[T-T_{dj},T]
112 \end{cases}
114 @param[in] ctx points to an instance of bell-shaped velocity trajectory
115 @param[in] dt difference between current time and initial time
116 @return acceleration output
118 A_EXTERN a_float a_trajbell_acc(a_trajbell const *ctx, a_float dt);
121 @brief calculate jerk for bell-shaped velocity trajectory
123 p^{(3)}(t)=\begin{cases}
124 j_m,&t\in[0,T_{aj}]\\
125 0,&t\in[T_{aj},T_a-T_{aj}]\\
126 -j_m,&t\in[T_a-T_{aj},T_a]\\
127 0,&t\in[T_a,T_a+T_v]\\
128 -j_m,&t\in[T-T_d,T-T_d+T_{dj}]\\
129 0,&t\in[T-T_d+T_{dj},T-T_{dj}]\\
130 j_m,&t\in[T-T_{dj},T]
131 \end{cases}
133 @param[in] ctx points to an instance of bell-shaped velocity trajectory
134 @param[in] dt difference between current time and initial time
135 @return jerk output
137 A_EXTERN a_float a_trajbell_jer(a_trajbell const *ctx, a_float dt);
139 #if defined(__cplusplus)
140 } /* extern "C" */
141 namespace a
143 typedef struct a_trajbell trajbell;
144 } /* namespace a */
145 #endif /* __cplusplus */
148 @brief instance structure for bell-shaped velocity trajectory
150 struct a_trajbell
152 a_float t; //!< total duration
153 a_float tv; //!< constant velocity phase
154 a_float ta; //!< acceleration phase
155 a_float td; //!< deceleration phase
156 a_float taj; //!< time-interval in which the jerk is constant (j max or j min ) during the acceleration phase
157 a_float tdj; //!< time-interval in which the jerk is constant (j max or j min ) during the deceleration phase
158 a_float p0; //!< initial position
159 a_float p1; //!< final position
160 a_float v0; //!< initial velocity
161 a_float v1; //!< final velocity
162 a_float vm; //!< maximum velocity
163 a_float jm; //!< maximum jerk
164 a_float am; //!< maximum acceleration
165 a_float dm; //!< maximum deceleration
166 #if defined(__cplusplus)
167 A_INLINE a_float gen(a_float _jm, a_float _am, a_float _vm, a_float _p0, a_float _p1,
168 a_float _v0 = 0, a_float _v1 = 0)
170 return a_trajbell_gen(this, _jm, _am, _vm, _p0, _p1, _v0, _v1);
172 A_INLINE a_float pos(a_float dt) const
174 return a_trajbell_pos(this, dt);
176 A_INLINE a_float vel(a_float dt) const
178 return a_trajbell_vel(this, dt);
180 A_INLINE a_float acc(a_float dt) const
182 return a_trajbell_acc(this, dt);
184 A_INLINE a_float jer(a_float dt) const
186 return a_trajbell_jer(this, dt);
188 #endif /* __cplusplus */
191 /*! @} A_TRAJBELL */
193 #endif /* a/trajbell.h */