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[ Original Paper ] | |
Journal of Advanced Marine Engineering and Technology - Vol. 47, No. 6, pp. 360-366 | |
Abbreviation: JAMET | |
ISSN: 2234-7925 (Print) 2765-4796 (Online) | |
Print publication date 31 Dec 2023 | |
Received 10 Nov 2023 Revised 20 Nov 2023 Accepted 30 Nov 2023 | |
DOI: https://doi.org/10.5916/jamet.2023.47.6.360 | |
Object transportation using multiple mobile robots: Coupling and decoupling configuration of an object and robots | |
Jin-Kyu Choi^{†}
; Hao Tian^{1} ; Yun-Su Ha^{2}
| |
1M. S. Candidate, Graduate School, Korea Maritime & Ocean University, Tel: 051-410-4342 (kmoutianhao@gmail.com) | |
2Professor, Division of Artificial Intelligence Engineering, Korea Maritime & Ocean Universit, Tel: 051-410-4347 (hys@kmou.ac.kr) | |
Correspondence to : ^{†}Professor, Ocean Science & Technology School, Korea Maritime & Ocean University, 727, Taejong-ro, Yeongdo-gu, Busan 49112, South Korea, E-mail: jk-choi@kmou.ac.kr, Tel: 051-410-4342 | |
Copyright © The Korean Society of Marine Engineering This is an Open Access article distributed under the terms of the Creative Commons Attribution Non-Commercial License (http://creativecommons.org/licenses/by-nc/3.0), which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited. | |
This study deals with object transportation using multiple mobile robots. Each robot is assumed to have a mechanism to couple with an object. The mechanism is operated by pushing and pulling forces without an actuator and becomes a free joint after coupling. The transportation operation is conducted as follows. The mobile robots first couple with the object using pushing motions. Then, they transport the object to the goal position. Finally, they decouple from the object using pulling motions after arriving at the destination. In this study, we focus on coupling and decoupling operations and discuss the configurations of the object and robots for coupling and decoupling. First, we formulate a kinematic model and static equilibrium equation for the object and n robots and then show that there exists a configuration, in which the robots can push and pull one another for coupling and decoupling while maintaining static equilibrium. Such a configuration is a singular configuration and is usually regarded as undesirable in terms of motion control. It is demonstrated through numerical examples using two, three, and four robots that the singular configuration is appropriate for coupling and decoupling operations.
Keywords: Object transportation, Multiple robots, Coupling and decoupling, Singular configuration, Mobile robot |
In ports, warehouses, factories, and restaurants, mobile robots carrying goods or food are common. However, most of these robots are designed to handle objects with limited size, shape, and weight. Furthermore, the process of loading goods or food onto the robots requires human intervention. The common action of moving refrigerators or furniture in our daily lives is a pushing or pulling motion, and through this motion, we can move large and heavy objects with relatively small force without additional measures for transportation. This study deals with object transportation using multiple mobile robots, which makes the transport of objects in different sizes, shapes, and weights possible through pushing and pulling motions.
Many studies have been conducted in the fields of modern logistics and automated transportation on multirobot cooperation [1]–[15]. Cooperative operation by multiple robots is important when handling bulky and heavy objects because these tasks may be too arduous or dangerous for individual robots or humans. Techniques, such as pushing, grasping, and caging, have proven to be reliable methods for multirobot cooperation to address such challenges [1][2].
The movement of target objects by multiple robots directly applying pushing forces has been demonstrated [3]-[6]. The effectiveness of this method lies in the distribution of the required forces, thereby reducing the burden on individual to manipulate large objects. Grasping technology relies on the ability of robots to grasp an object securely and then move it collaboratively. This method is suitable for objects that are easily held and require precise handling. It has been shown that the grasping approach ensures operational stability and efficiency, and prevents the object from falling or overloading. The caging method uses multiple robots to form an enclosed structure and transport objects. This approach is particularly suitable for objects with irregular shapes or the ones, which are difficult to directly grasp [10]-[14].
Implementing robotic transportation in the real world provides many advantages; however, there are challenges, including precise control, environmental adaptability, inter-robot communication, and decision-making [15]. The size, shape, and weight of objects, along with environmental factors, such as terrain and space constraints, also influence transportation approaches.
This study considers the multi-robot cooperative object transportation, as shown in Figure 1, to handle objects of various sizes, shapes, and weights. Unlike pushing, grasping, and caging methods, robots use a mechanism to couple with an object, which makes transportation control easier. The mechanism is operated by applying pushing and pulling forces without an actuator, which become a free joint after coupling. The transportation operation is conducted as follows. The mobile robots first couple with the object using pushing motions. Then, they transport the object to the goal position, and finally decouple from the object using pulling motions after arriving at the destination.
In this study, we focus on the coupling and decoupling operations and discuss the configurations of an object and robots for coupling and decoupling. Sections 2 and 3 present the formulation of the kinematic model and static equilibrium equation, respectively. In Section 4, it is shown that there exist configurations, in which the robots can push and pull one another for coupling and decoupling without generating a moment on the object. These configurations are singular configurations and are usually regarded as undesirable in the motion control aspect. Numerical examples are presented and discussed in Section 5 to verify the coupling and decoupling configurations.
Assume that the mechanism shown in Figure 2 is used for coupling and decoupling. Coupling is achieved by pushing when the gates are in contact with the axis attached to the object, and decoupling is achieved by the reverse action.
Consider an object in contact with n mobile robots, as shown in Figure 3. Let v_{o} ∈ ℜ^{2} and ω_{o} ∈ ℜ be the linear and angular velocities of the object, respectively, r_{i} ∈ ℜ^{2} (i = 1, 2, ⋯ , n) be the position vector pointing from the center of mass of the object to the contact point with the robot i, and v_{ci} ∈ ℜ^{2} be the velocity of the contact point. Because v_{ci} = v_{o} + Er_{i}ω_{o}, we get
(1) |
where,
(2) |
The contact point velocities can also be obtained from the linear and angular velocities of each robot. Let v_{Ri} ∈ ℜ^{2} and ω_{Ri} ∈ ℜ be the linear and angular velocities of the robot i, respectively (refer to Appendix A.1 for obtaining v_{Ri} and ω_{Ri} from the angular velocities of the wheels) and l_{ci} ∈ ℜ^{2} is the position vector pointing from the center of mass of the robot to the end of the coupling mechanism, i.e., the contact point. From Figure 4 and v_{ci} = v_{Ri} + El_{ci}ω_{Ri}, we get
(3) |
where,
O_{2} is a 2 × 2 zero matrix, and O is a 2 × 1 zero vector.
From Equations (1) and (3), we can obtain the velocity constraints as:
(4) |
Here, to consider only the pushing and pulling motions for coupling and decoupling, the angular velocities ω_{Ri} are moved to the left side of Equation (4), and the following kinematic model can be obtained.
(5) |
where,
Let f_{o} ∈ ℜ^{2} and m_{o} ∈ ℜ be the force and moment generated on the object, respectively, f_{Ri} ∈ ℜ^{2} and m_{Ri} ∈ ℜ be the force and moment of the robot i, respectively (refer to Appendix A.2 for obtaining f_{Ri} and m_{Ri} from the torques of the motors attached at the wheels), and f_{ci} ∈ ℜ^{2} (i = 1, 2, ⋯ , n) be the force generated at the contact point. From Figure 5, we obtain the following static equilibrium equation for the object as:
(6) |
where,
(7) |
This relation can be expressed for all the robots as:
(8) |
where,
Combining the τ_{o} in Equation (6) and equations related with m_{Ri} in Equation (8), the static equilibrium condition for pushing and pulling can be obtained as:
(9) |
where,
As shown in Figures 1 and 2, coupling and decoupling are performed using pushing and pulling motions. Thus, such actions must be achieved without generating a moment on the object; otherwise, the motion of the object becomes unstable, and the robots can detach from the object.
From Equation (5), when rank(A) < min(2n, 3 + n), there exists
(10) |
This indicates that there exists a certain contact force f_{c} that maintains static equilibrium without exerting force and moment on the object (τ_{o} = 0) and moments on the robots (m_{Ri} =0). Thus, it can be concluded that a configuration satisfying the following conditions is appropriate for pushing and pulling one another for coupling and decoupling.
(11) |
In this case, the contact force f_{c} can be obtained as:
(12) |
where, h is the basis of Ker(A^{T}) and γ is a real number. In addition, the force and moment exerted by each robot to accomplish coupling and decoupling can be obtained using Equation (8).
Consider Cases (a) and (b), as shown in Figure 6. Table 1 presents the values of r_{i} and l_{ci}. From Equation (5), if two robots are used, i.e., n = 2, we have:
r_{i} | l_{ci} | |
---|---|---|
Figure 6(a) | ||
Figure 6(b) |
(13) |
First, in the case of Figure 6(a), rank(A) = 3 < min(4, 5) and dimKer(A_{T}) = 1, thus, this configuration is a singular configuration, and certain contact forces exist to push and pull each other while maintaining static equilibrium. Equation (12) gives f_{c} = (-0.7071, 0, 0.7071, 0)^{T}γ; the robots can pull each other for decoupling if γ is a positive real number and push for coupling if γ is a negative. Equation (8) yields the forces and moments of the robots to exert f_{c} : τ_{R} = (-0.7071, 0, 0, 0.7071, 0, 0)^{T}γ , where, γ is positive for decoupling (pulling) and negative for coupling (pushing).
Next, in the case of Figure 6(b), rank(A) = 3 < min(4, 5), dimKer(A^{T}) = 1 , and f_{c} = (–0.7071, 0, 0.7071, 0)^{T}γ . It is known that this configuration is singular and appropriate for coupling and decoupling. For this case, the force and moment of the robots are τ_{R} = (-0.7071, 0, 0, 0.7071, 0, 0)^{T}γ. However, if r_{2} is changed to (0.4, 0)^{T} as shown in Figure 7, rank(A) = 4 = min(4, 5) and dimKer(A^{T}) = 0. Hence, the configuration is not singular, and there are no contact forces for static equilibrium. Figure 7 shows that the contact forces exert a moment on the object in this configuration.
The four configurations and parameter values are given in Figure 8 and Table 2, respectively. If three robots are used (n = 3), we obtain:
Figure 8 | r_{i} | l_{ci} |
---|---|---|
(a) | ||
(b) | ||
(c) | ||
(d) |
(14) |
Checking the case of Figure 8(a), rank(A) = 5 < min (6, 6), dimKer(A^{T}) = 1 , f_{c} = (–0.5, –0.2887, 0.5, –0.2887, 0, 0.5774)^{T}γ , and τ_{R} = (–0.5, –0.2887, 0, 0.5, –0.2887, 0, 0, 0.5774, 0)^{T}γ, where, γ is positive for decoupling and negative for coupling. The configuration is singular, and robots can push and pull one another for coupling and decoupling. In this case, the contact forces meet at the center of mass of the object. Unlike this, Figure 8(b) is the case when the contact forces meet at another place. This configuration is proper for coupling and decoupling; we can confirm this by rank(A) = 5 < min (6, 6) , dimKer(A^{T}) = 1, f_{c} = (–0.3536, –0.3536, 0.3536, –0.3536, 0, 0.7071)^{T}γ, and τ_{R} = (–0.3536, –0.3536, 0, 0.3536, –0.3536, 0, 0, 0.7071, 0)^{T}γ.
In case of Figure 8(c), rank(A) = 5 < min (6, 6) , dimKer(A^{T}) = 1 , f_{c} = (0.7071, 0, –0.7071, 0, 0, 0)^{T}γ , and τ_{R} = (0.7071, 0, 0, –0.7071, 0, 0, 0, 0, 0)^{T}γ, where, γ is positive for coupling and negative for decoupling. This configuration has a local singular configuration and is appropriate for the coupling and decoupling of Robots 1 and 2. However, Robot 3 cannot exert a contact force for coupling and decoupling.
In addition, if a robot must be decoupled from the object, the configuration shown in Figure 8(d) can be used. In this case, rank(A) = 5 < min (6, 6) , dimKer(A^{T}) = 1 , f_{c} = (0.3536, –0.3536, –0.3536, –0.3536, 0, 0.7071)^{T}γ , and τ_{R} = (0.3536, –0.3536, 0, –0.3536, –0.3536, 0, 0, 0.7071, 0)^{T}γ . When γ is a positive, Robot 3 can decouple from the object by pulling motion, while the other robots push the object.
When we use four robots (n = 4),
(15) |
From rank(A^{T}) + dimKer(A^{T}) = 8 , it can be known that dimKer(A^{T}) ≠ 0 even if rank(A) = rank(A^{T}) = 7 = min(8,7); this means that the robots can push and pull one another for coupling and decoupling at any configuration; however, there is a configuration, at which specific robot(s) cannot exert a contact force for coupling and decoupling like Robot 3, as shown in Figure 8(c). This result can be applied to cases, in which more than four robots are used.
In this study, we discussed the coupling and decoupling configuration of an object and robots for cooperative object transport. The following conclusion were drawn:
Our future work will involve conducting experimental verification and developing a path-following control method for multirobot cooperative object transportation.
Conceptualization, J. -K. Choi; Methodology, J. -K. Choi; Software, J. -K. Choi and H. Tian; Formal Analysis, J. -K. Choi, H. Tian and Y. -S. Ha; Investigation, J. -K. Choi and H. Tian; Resources, J. -K. Choi and H. Tian; Data Curation J. -K. Choi and H. Tian; Writing-Original Draft Preparation, J. -K. Choi and H. Tian; Writing-Review & Editing, J. -K. Choi, H. Tian and Y. - S. Ha; Visualization, J. -K. Choi and H. Tian; Supervision, J. -K. Choi.
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Consider a mobile robot with wheels on the right and left sides. Let ω_{ri} , ω_{li} , v_{ri} , v_{li} , L and r be the angular velocities of the right and left wheels, linear velocities generated by the angular velocities, distance between the center of mass and center of the wheel, and radius of the wheels, respectively. From v_{ri} = rω_{ri} and v_{li} = rω_{li}, we can obtain the linear and angular velocities of the robot i :
(A.1) |
Let τ_{ri}, τ_{li}, f_{ri} and f_{li} be the torques generated by the motors attached at the right and left wheels, and forces by the torques, respectively. Because
(A.2) |
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