Numerical values used in the simulations for the robotic arm [8].

## Abstract

Motion planning is a significant stage in the control of autonomous systems. As an alternative method, guidance approach is proposed for the motion planning of those systems. In guided munitions, guidance laws determine the success of the guidance systems designed to steer systems such as missiles and guided bombs towards predefined targets. The guidance laws designated according to determinative agents such as the firing position of the munition, target type, and operational requirements try to provide the munition with arriving at the target point even under the disturbing effects. In this study, the applicability of the guidance laws to autonomous systems is investigated in a manner similar to the approach for the guided munitions. For this purpose, the motion planning of the selected robotic arm, tracked land vehicle, and quadrotor is tried to be performed in order to move them to predefined target points. Having designed the control systems compatible to the selected guidance laws for the considered systems, the corresponding guidance scheme is constructed. Eventually, after conducting the relevant computer simulations, it is observed that the desired target chase can be made in a successive manner for all cases.

### Keywords

- motion planning
- guidance
- guidance law
- linear homing
- autonomous system

## 1. Introduction

Motion planning constitutes one of the primary stages in the control of autonomous systems. The autonomous systems can perform their planned tasks under several environmental conditions as per the designated motion planning algorithms in accordance certain performance criteria. The mentioned criteria may include minimum energy or minimum time consumption and shortest path length. For the motion planning purpose, several different algorithms are proposed by relevant researchers. These methods have certain advantages and disadvantages over the others [1, 2, 3, 4].

As an alternative approach, guidance schemes can be used in motion planning. Those schemes involve an upper-level guidance algorithm and a lower-level control system. In fact, guidance and control loops can be introduced as officer and soldier, respectively. In other words, as the guidance algorithm behaves as the “master,” the control system takes the “slave” role in this scene [5].

The guidance schemes are widely implemented to munitions. Guidance and control systems are designed in a compatible manner with munition dynamics so that the munitions including missiles and guided bombs can carry payloads towards specified target points as planned. The guidance part of the mentioned guidance and control system constitutes the kinematic relationships established as per the relative position between the munition and intended target point, while the control system is the closed-loop control system constructed based on the dynamic model of the munition under consideration in order to realize the guidance commands generated by the guidance part. In this extent, the guidance approach enrolls as a motion planning scheme for the munition [5].

The type of the command yielded by the guidance system depends on the selected guidance law. Namely, as the output of the proportional navigation guidance law which constitutes the most widely used guidance law in guided munitions is the lateral component of the linear acceleration vector of the munition or change of the lateral angular component of the linear velocity vector in time as per the application, the command of the body pursuit guidance law becomes the components of the angle between the body longitudinal axis of the munition and the lateral axis of the Earth-fixed frame [5, 6].

Guidance laws designated to move the guided munitions towards specified target points make their motion planning in a sense. Regarding this property, there seems no serious obstacle on their implementation on autonomous systems other than guided munition. In this study, the orientation of the sample autonomous mechatronic systems involving a robotic arm, tracked land vehicle, and quadrotor to predefined target points using the linear homing guidance (LHG) law and the relevant computer simulations is carried out. Here, these systems are chosen as very common systems encountered in the physical world. In the considered cases, the LHG law is an angle-based approach, and it takes the flight path angle components of the systems into consideration. Also, the selection of the mentioned mechatronic systems allows evaluating the convenience of the proposed approach in the planar and spatial engagement situations. Moreover, single- and two-stage control systems are utilized in accordance with the LHG law.

Guidance-based motion planning schemes are developed for certain robotic arm configurations [7]. In this scene, the indicated strategy allows the operators to run the moving belt of the robotic arm-belt assembly line within a mounting line in a more continuous and faster manner than the usual methods. Moreover, it may become to suppress or at least minimize the drawbacks of the conventional approaches by regarding the guidance-based motion planning method. Namely, although many conventional methods require the belt assembly to halt at intermediate placing instants, the guidance-based approach makes possible to place the objects under consideration onto the belt while it remains running during operation [8].

Different from wheeled vehicles, tracked land vehicles are directed as per a sliding motion which depends on the rotation of the vehicle about an instantaneous rotation center. In other words, they can be oriented to left or right by rotating about their instantaneous rotation center in the convenient sense. Regarding the motion of these vehicles on soil surfaces especially, the motion planning becomes harder. As a remedy to this inconvenience, the guidance-based path planning approach is proposed in the present study [8].

As the third application, the motion planning of a quadrotor which is intended to carry a payload from a stationary initial point to a prescribed moving land platform at a moderate distance for either military or civil purpose is investigated. Here, the payload can be munition, food, or first aid material. Since the moving platform specified as the target is assumed to be far away from the initial point, it is desired for the quadrotor to catch it within the shortest time duration possible and consume the energy at a minimum level [8, 9].

In the computer simulations in which the planar motion of the robotic arm and tracked land vehicle and the spatial motion of the quadrotor are taken into consideration, it is assumed that the targets are moving along specified trajectories. Here, regarding the motion characteristics of the autonomous systems dealt with, the robotic arm operates on the horizontal plane, and the vertical displacement of the tracked land vehicle is in a negligible level compared to its longitudinal and lateral motion on the ground plane. Thus, the motion profiles are described on a plane for both the systems. Unlike them, the quadrotor flies in the sky towards all three directions. This fact leads to handle its dynamic behavior in a three-dimensional space. Having completed the computer simulations, it is observed that all three systems can be carried to the intended target points by LHG law [8].

As a motion planning strategy, guidance approach can be applied to service robots which are utilized to accomplish certain motion profiles apart from the industrial systems. In this way, it is intended to perform hazardous, tedious, and time-consuming tasks in a more efficient and accurate manner in daily use. The mentioned category for service robots, actually, involves not only articulated robot manipulators but also moving and flying autonomous structures as well.

## 2. Description of the systems

### 2.1 Description of the robotic arm

The schematic views of the robotic arm and mounting line, i.e., trajectory, containing the slot on which the component grasped by the gripper of the arm is placed is given in Figure 1.

The system whose schematic view is presented in Figure 1 consists of a two-degree-of-freedom robotic arm and moving mounting line. Here, the object to be put on the slot on the mounting line by the gripper of the robotic arm is taken in spherical geometry, and thus its orientation is ignored. This way, the degree of freedom of the carried object is reduced to two. In other words, it becomes possible to define the instantaneous planar location of the object by regarding the lateral and vertical position components of a point, i.e., point P, on the object. So, a robotic arm is required with minimum degree of freedom of two in order for the object with two degrees of freedom to be carried upon a specified point on the plane without any control deficiency. The definitions made in Figure 1 are listed as follows [8]:

x and y: lateral and vertical axes of the Earth-fixed frame symbolized by *F0.*

*F0.*

O and A: joints of the robotic arm.

a_{1} and a_{2}: lengths of the first and second links of the arm.

θ_{1} and θ_{2}: first and second joint angles of the robotic arm.

P: point defined on the gripper of the robotic arm.

x_{P} and y_{P}: lateral and vertical position components of point P.

S: midpoint of the slot on the mounting platform.

S_{i}: form changing points of the mounting line (i = 1, 2, 3, and 4).

v_{S}: speed of the slot on the mounting line.

x_{S} and y_{S}: lateral and vertical position components of point S.

ρ: turn radius of the mounting line.

ψ: rotation angle on the circular tip parts of the mounting line.

L: total length of the mounting line.

d: perpendicular distance between the connection point of the robotic arm to the ground and the point of the mounting line closest to that connection point.

^{2}).

Regarding these definitions, the mathematical model of the robotic arm can be expressed in a compact matrix form as follows [8]:

where, as

In the shorthand definitions above, m_{1}, m_{2}, Ic_{1}, and Ic_{2} denote the masses of the first and second links of the manipulator and the moments of inertia of these links with respect to their mass centers indicated by C_{1} and C_{2}, respectively. Also, b_{1} and b_{2} represent the viscous friction coefficients at the first and second joints as well as the definitions of

### 2.2 Description of the tracked land vehicle

As the second system examined, the schematic description of the tracked land vehicle is shown in Figure 2. The explanations of the quantities labeled in Figure 2 are given as follows [8]:

O, G, and C: origin of *F0 *, mass canter of the tracked vehicle, and instantaneous rotation center of the vehicle.

*F0.*

*Fb.*

x and y: position components of point G on *F0.*

ψ: orientation angle of the vehicle on the vertical plane.

x_{C} and y_{C}: position components point C in *Fb.*

a, b, c, d, and v: dimensional parameters of the vehicle.

m: mass of the tracked land vehicle.

ρ_{xL} and ρ_{xR}: lateral friction force density acting on the left and right tracks.

For the tracked land vehicle, as u_{x}, u_{y}, and u_{z} denote the inputs and b_{x}, b_{y}, and b_{ψ} indicate the gravity and frictional force components, governing differential equations can be written in the following manner [8]:

where

Regarding these definitions, T_{L} and T_{R} stand for the actuation torques exerted by the power transmission gears on the left and right tracks; r_{S} and I_{z} represent the radius of its actuation gear and moment of inertia of the vehicle about the rotation axis indicated by the unit vector _{x} and μ_{y} stand for the static friction coefficients between the tracks of the vehicle and surface on the lateral planes. Here, the symbols

### 2.3 Description of the quadrotor

The schematic view of the quadrotor, the third system under consideration, and engagement geometry between the quadrotor and moving land platform are presented in Figures 3 and 4, respectively [8].

As indicated in Figure 3, the front and rear rotors expressed as numbers 1 and 3, respectively, have rotations in positive sense around the axis represented by unit vector *Fb *, whose origin is attached at point C and whose axes are shown by unit vectors

In Figure 3, L and Ω_{j} (j = 1, 2, 3, and 4) stand for the distance between the center of rotation of each motor and point C and angular speed of the electromechanical actuator, i.e., electrical servomotor, used to move the propeller j, respectively. In addition to those parameters, the symbols in Figure 3 can be listed as follows [8]:

T: target point on the moving platform for the quadrotor.

T_{i}: points at which the shape of the trajectory of the moving platform changes (i = 0, 1, and 2).

v_{T}: linear speed of point T on the moving platform.

ρ: radius of curvature of the trajectory of the moving platform.

ψ: rotation angle of the rounded tip portions of the trajectory of the moving platform.

H: total length of the trajectory of the moving platform.

D: perpendicular distance between the origin of *F0 *, i.e., point O, and the midline of the section of the trajectory of the moving platform closest to this point.

Considering the related kinematic and dynamic parameters of the quadrotor system, the dynamic model of the quadrotor can be set as follows using the relevant kinematic and dynamic parameters with angular position parameters of ϕ, θ, and ψ and translational position parameters of x, y, and z [8]:

where

In the definitions above, J_{x}, J_{y}, and J_{z} show the moment of inertia components of the quadrotor around the axes defined by unit vectors _{v} represents the moment of inertia of each rotor about its axis of rotation, d indicates the drag factor, and K_{ϕ}, K_{θ}, K_{ψ}, K_{x}, K_{y}, and K_{z} stand for the aerodynamic moment and force components acting on the system in the roll, pitch, and yaw planes and along the longitudinal, lateral, and vertical planes, respectively. Furthermore, b indicates thrust factor of the motors [8].

## 3. Control systems

Since the guidance commands generated by the LHG law which is considered to make the motion planning of the autonomous systems so as to bring them to the specified point on the target trajectories are in terms of the linear velocity components of the mass centers of those systems, the main control variables of the systems are selected to be velocity components [8]. Also, for the sake of maintaining the stability of the systems, the gain matrices of the relevant control systems are continuously updated throughout the planned motion using the state information of target acquired by certain means like a camera.

### 3.1 Robotic arm control system

Because the guidance signals produced by the LHG law are in terms of the angle between the velocity vector of point P and lateral axis, the control variable of the robotic arm control system is chosen to be the joint speeds, i.e.,

Here, as

The relevant control rule can be written according to the computed torque method with the addition of the integral action to nullify the steady-state errors by regarding the error definition in Eq. (11) as follows [10]:

Here, as “T” represents the matrix transpose, _{1} and T_{2}. Also,

The differential equation corresponding to the error dynamics of the control system for the robotic arm are obtained using Eqs. (11) and (12) in the following fashion:

As ω_{ci} and ζ_{ci} denote the desired bandwidth and damping ratio of link i (i = 1 and 2), the error dynamics can be written for a second-order ideal system with two degrees of freedom as follows [10]:

where

Consequently,

### 3.2 Tracked land vehicle control system

During the control of the tracked land vehicle for the angular variables, the angular position requirement for ψ should also be satisfied. For this purpose, a two-stage cascaded control scheme is constructed for the tracked land vehicle. In this algorithm, the outer loop is responsible of making linear velocity control in accordance with the guidance commands, while the inner loop makes the angular position control such that the orientation angle requirement arising during the linear velocity control is realized [8].

Here, the expressions which will be considered for the design of the linear velocity control system which is termed as “the primary control system” can be arranged in the forthcoming state space form from Eqs. (2) and (3) as

The control rule of the primary control system can be established using the computed torque control method according to the PI control action like the robotic arm control system so as to nullify the steady-state errors [8]:

In the above equation,

Substituting Eq. (18) into Eq. (17) yields the next equation for the error dynamics of the primary control system [8]:

As ω_{pi} and ζ_{pi} denote the desired bandwidth and damping ratio of link i (i = 1 and 2) for the primary control system, the error dynamics can be written for a second-order ideal system with two degrees of freedom as follows [8]:

where

Equating Eq. (19) to Eq. (20), the gain matrices are found for the primary control system as follows [8]:

The control rule for the angular control system called “the secondary control system” can be set using the computed torque method according to the PD (proportional plus derivative) control action in the following fashion [8]:

In the above expression, b_{ψ}, ψ_{d}, K_{sp}, K_{sd}, and e_{s} represent the inertia gain for the vehicle, desired input variable for the secondary control system, gain of the proportional control action, gain of the derivative control action, and error, respectively. Also,

Plugging Eq. (23) into Eq. (4), the error dynamics of the secondary control system is determined as follows [8]:

As ω_{s} and ζ_{s} indicate the desired bandwidth and damping ratio for variable ψ for the secondary control system, the error dynamics can be written for a second-order ideal system with single degree of freedom as given below:

Matching Eqs. (24) and (25) results in the forthcoming gains for the secondary control system [8]:

### 3.3 Quadrotor control system

The same two-stage control system is designed for the quadrotor as that for the tracked land vehicle. For the primary control system, these expressions can be rearranged in the state space form by assigning the columns of the state variables and inputs of the system to be

where

The control law of the primary control system including an integral action can be designed as per the computed torque method with PI action in the following manner [8]:

In the expression above,

Substituting Eq. (29) into Eq. (28), the error dynamics of the primary control system is obtained as follows [8]:

As ω_{pi} and ζ_{pi} represent the desired bandwidth and damping ratio of the i^{th} state variable (i = 1, 2, and 3) of the primary control system, respectively, the error dynamics of a second-order ideal system with three degrees of freedom can be described using the forthcoming expression [8]:

where

Matching Eqs. (30) and (31), the gain matrices appear for the primary control system as follows:

As the corresponding columns of the state variables and inputs of the system are shown to be

where

In a similar manner, the control law can be written according to the computed torque method with PD action for the secondary control system as follows [8]:

Here,

In the proposed entire control scheme, the desired values of ϕ and θ are calculated using u_{x}, u_{y}, and u_{z} inputs along with the parameter u_{F} by regarding the definitions within Eqs. (5)–(10). In other words, the reference inputs, or commands, to ϕ and θ are generated by the outer loop. On the other hand, the remaining angular position variable ψ is adjusted to be a constant value. That means its reference value is set as a fixed quantity. In this sense, the desired value of ψ is then specified to be zero as the decision on keeping the quadrotor with no angular motion in the yaw plane [11, 12].

Inserting Eq. (35) into Eq. (34), the error dynamics of the secondary control system is obtained as

As ω_{si} and ζ_{si} denote the desired bandwidth and damping ratio of the i^{th} state variable (i = 1, 2, and 3) of the secondary control system, the error dynamics of a second-order ideal system with three degrees of freedom can be described using the following equation [8]:

where

Equating Eqs. (47) and (48) to each other yields the gain matrices of the secondary control system as shown below [8]:

## 4. Engagement geometry

Since the motion of the moving land platform for the quadrotor, i.e., trajectory of the target point, is dealt with in the three-dimensional space, the lateral projection of the engagement geometry drawn for the quadrotor can be used for the engagements of the robotic arm and tracked land vehicle with their targets as well.

The engagement geometry between the quadrotor and the moving land platform is described in the horizontal and vertical planes separately. Thus, the vertical engagement between point C, the mass center of the quadrotor, and point T on the moving platform can be depicted as seen in Figure 5. The lateral engagement geometry between points C and T can be similarly constructed using the same expressions [8].

In Figure 5, v_{C}, γ_{q}, r_{T/C}, γ_{t}, and λ_{p} show the resultant speed of point C, orientation angle of v_{C} from the horizontal plane, relative position of point T with respect to point C, orientation angle of v_{T} from the horizontal axis, and orientation angle of r_{T/C} from the horizontal axis. Here, the next equations are held for v_{C}, γ_{t}, and λ_{p} [8]:

Similarly, the orientation angle of r_{T/C} from the horizontal plane, i.e., λ_{y}, can be obtained as follows [8]:

The final offset between points C and T at the end of the engagement, i.e., d_{miss}, is calculated using the next formula as t_{F} indicates the termination time [8]:

Here, as x_{C}, y_{C}, and z_{C} stand for the position components of point C and x_{T}, y_{T}, and z_{T} stand for the position components of point T on *F0 *,

## 5. Guidance law

In order for the considered point on the relevant system (point P for the robotic arm, point C for the tracked land vehicle, and point C for the quadrotor) to catch the desired point on the moving platform (point S for the robotic arm and point T for the tracked land vehicle and quadrotor), the guidance commands can be derived according to the LHG law for which the mechatronic system-target engagement geometry is depicted in Figure 6 [13].

In Figure 6, M, T, and P stand for the mechatronic system, the target, and the predicted intercept point, respectively. Also,

Regarding the LHG geometry expressed above verbally, the relevant guidance commands can be derived in terms of the orientation angles of v_{C} from the lateral and vertical axes (

where

In Eqs. (45) and (46), the components of the linear velocity vector of point T whose amplitude is v_{T}, i.e., v_{Tx}, v_{Ty}, and v_{Tz}, are defined in the following equations [6, 8]:

Furthermore, the remaining time till the end of the engagement, i.e., Δt, is formulated below:

In the above equation,

In this work, it is assumed that the speed and orientation parameters of the moving target are obtained by processing the data acquired by the camera on the system under control. Since the control inputs of the designed control system are linear velocity components, the guidance commands given in Eqs. (45) and (46) should be expressed in terms of the linear velocity parameters for realization. This transformation can be done by writing the velocity vector of point C with amplitude v_{C} in terms of its components on *F0 *as follows [6, 8]:

## 6. Computer simulations

The system trajectories acquired from the computer simulations performed in accordance with the numerical values given in Tables 1–3 for the robotic arm, tracked land vehicle, and quadrotor are submitted in Figures 7–10 along with the corresponding target motions. Having constructed the engagement geometry between the mechatronic system under consideration and target, the LHG law is applied for these situations. In the simulations, disturbance effects due to the nonlinear friction characteristic and noise on the sensors on the joints are assumed to randomly change within the intervals of ±10 N·m and ±1 × 10^{−3} rad for the robotic arm. Also, it is regarded that the angular and linear dynamics of the quadrotor are subjected to random disturbing moment and force with maximum amplitudes of 50 N·m and 100 N, respectively. The simulations of the tracked land vehicle are made on nominal operating conditions [8].

Parameter | Numerical value |
---|---|

a_{1} and a_{2} | 1.25 m |

d_{1} and d_{2} | 0.625 m |

m_{1} and m_{2} | 10 kg |

I_{c1} and I_{c2} | 1.302 kg·m^{2} |

b_{1} and b_{2} | 0.001 N·m·s/rad |

ω_{c1} and ω_{c2} | 10 Hz |

ζ_{c1} and ζ_{c2} | 0.707 |

L | 2 m |

ρ | 0.5 m |

d | 1.5 m |

Parameter | Numerical value |
---|---|

a | 2.5 m |

b | 4 m |

v | 1.25 m |

m | 25,000 kg |

I_{z} | 60,000 kg·m^{2} |

r_{s} | 0.3 m |

μ_{x} and μ_{y} | 0.4 |

ω_{p1} and ω_{p2} | 10 Hz |

f_{s} | 30 Hz |

ζ_{p1}, ζ_{p2}, and ζ_{s} | 0.707 |

Parameter | Numerical value |
---|---|

L | 0.25 m |

b | 5 × 10^{−5} N·s^{2} |

d | 1 × 10^{−6} N·m·s^{2} |

m | 2 kg |

I_{x} and I_{y} | 0.2 kg·m^{2} |

I_{z} | 0.3 kg·m^{2} |

J_{v} | 1 × 10^{−3} kg·m^{2} |

K_{x}, K_{y}, and K_{z} | 0.01 N·s/m |

K_{ϕ}, K_{θ}, and K_{ψ} | 0.012 N·s/m |

ω_{pi} | 5 Hz |

ω_{si} | 15 Hz |

ζ_{pi} and ζ_{si} | 0.707 |

H | 50 m |

ρ | 15 m |

D | 50 m |

Solver step | 1 ms |

## 7. Conclusion

As a result of the performed computer simulations, it is shown that the considered autonomous mechatronic systems, i.e., the robotic arm, tracked land vehicle, and quadrotor, can catch the specified target points by regarding the LHG law. Although only one engagement case is presented for each of the systems above, the same result is attained for different situations, too. In this scene, one of the most important considerations is the capacity of the actuators of the autonomous systems. Namely, if the maximum force or torque, hence maximum current, level of the actuators (electric motors) does not satisfy the requirements arising due to the planned motion profile, then the relevant system cannot track the target as planned. In general, it can be concluded that the motion planning of mechatronic systems including the service robots can be made against predefined target points by choosing a convenient guidance law.