Research Article  Open Access
Yanyan Song, Boyan Chang, Guoguang Jin, Zhan Wei, Bo Li, "An Approach for the Impact Dynamic Modeling and Simulation of Planar Constrained Metamorphic Mechanism", Shock and Vibration, vol. 2020, Article ID 8837838, 18 pages, 2020. https://doi.org/10.1155/2020/8837838
An Approach for the Impact Dynamic Modeling and Simulation of Planar Constrained Metamorphic Mechanism
Abstract
This paper studied the impact dynamic modeling of the planar constrained metamorphic mechanism (PCMM) during configuration transformation. Based on the dynamic theory of the multirigidbody system and the coefficient of restitution equation, a new method for dynamic modeling of PCMM considering impact motions generated by configuration transformation is presented, which can be treated as a theoretical foundation for performance design and dynamic control. Firstly, the topology theory based on the impact motion can be classified as the stable impact motion and the mobile impact motion, which is the prerequisite for dynamic modeling and simulation. Secondly, the stable and mobile impact dynamic models for PCMM are established according to the dynamic theory of the multirigidbody system. Then, using these models, the corresponding impulse solving models are deduced combining with the coefficient of restitution equation. Finally, the examples of the stable impact motion and the mobile impact motion are respectively given, and the configurationcomplete dynamic simulations are carried out. By comparing with the dynamic models without considering the impact motion, the dynamic characteristics of PCMM are analyzed. The theory and method proposed in this paper can be also applied in general planar robotic systems to deal with the problem of internal collision dynamics.
1. Introduction
Metamorphic mechanisms are members of the class of mechanisms that are able to change their configurations sequentially to meet different requirements [1]. Since the proposal of metamorphic mechanism in 1998 [2], it has been widely applied to various fields of engineering, such as bionic joint mechanism [3, 4], extendable/foldable flexible spacecraft mechanism [5], automated laying mechanism [6, 7], robot mechanism [8], and space metamorphic parallel mechanism [9]. The applications of the current metamorphic mechanisms are mainly based on taskorientated constrained metamorphic mechanisms [10], which have become the focus of analysis and research in the field of mechanism.
Based on the division method of the metamorphic mode, the metamorphic mechanisms have many ways to achieve configuration transformation [11]. Constrained metamorphic mechanism is a kind of mechanism, which realizes configuration transformation by using geometric constraints and/or force constraints to reduce the number of degrees of freedom (DOFs) of a multiDOF metamorphic mechanism to the number of driving links [12]. In the course of movement and work, the constraint types and the characteristics of metamorphic joints will change along with the continuous transformation of configurations. The internal impact is generated by configuration transformation, whose characteristics are very brief duration, high force levels reached, rapid dissipation of energy, and large accelerations and decelerations present [13]. In severe cases, it will directly affect stability, reliability, and safety of the system. It can be said that the characteristics of impact motion during configuration transformation directly determine whether the system can work safely and steadily or not in the constrained metamorphic mechanisms. Therefore, it is necessary to study the impact characteristics of the constrained metamorphic mechanism during configuration transformation.
Constrained metamorphic mechanism belongs to the multibody system; furthermore, the impact motion of the constrained metamorphic mechanism can be regarded as a typical collision dynamic problem of the multibody system with variable topological structures. The research on collision dynamic modeling methods of the multibody system can be divided into the following categories: impulsemomentum method, continuous model, and Lagrange multiplier method. In the impulsemomentum method, the colliding bodies are assumed to be rigid and no deformation occurs at the impact location. Duan and Zhang [14] introduced the concept of impact potential energy and investigated the rigidflexible coupling dynamics of a radially rotating flexible beam with impact. Jin et al. [15] proposed a method based on the impulse principle and the Gauss minimum constraint method to determine the system state variables after contact collision. Dong and Chen [16] analyzed the impact dynamics and the effect between the space manipulator endeffector and the satellite of the capture process with the momentum impulse method combining the momentum conservation principle. Deng et al. [17] used the impulsemomentum equation involving the restitution coefficient of the system to establish the impact dynamic model which can extrapolate the impact momentum on the drive component. Choi et al. [18] derived an analytical model of the restitution coefficient for the 3 DOF finger model colliding with a wall and showed that COR varied according to the colliding velocity and its contact area through the experiment. Although the impulsemomentum method has the advantages of high calculation efficiency and intuitionistic, it cannot calculate the collision process. In the continuous model, the impactinduced force is a function of the relative penetration of two bodies into each other. Machado et al. [19] presented a general and comprehensive study of some of the most relevant compliant contact force models for multibody system dynamics. Also, two simple planar multibody systems that included contactimpact scenarios were considered as examples of application to demonstrate the similarities of and differences between the contact force models used throughout this work. Bhalerao and Anderson [20] presented a complementaritybased recursive scheme to model intermittent contact for flexible multibody systems. Ahmadizadeh et al. [21] dynamically modeled the phenomenon of multiple impactcontacts based on the continuous contact force model for an open kinematic chain with rigid links and revolute joints. Korayem et al. [22, 23] studied the modeling of various contact theories for application in the manipulation of different biological micro/nanoparticles. Flores and Ambrósio [24] used a contact force model in contactimpact analysis in multibody dynamics and explicitly accounted for the deformation of the bodies during the impact process. The continuous model can objectively reflect the collision process, but the calculation form of collision force and the selection of relevant parameters are relatively difficult. Compared with the continuous model, the Lagrange multiplier method avoids the uncertainty caused by parameter selection and improves the reliability of the model. But, it is not easy to obtain a more general method to solve the velocity increments. To bridge the gap between accuracy and efficiency in the dynamic simulation of a flexible multibody system with contacts/impacts, Wang et al. [25] modeled the impact region using the finite element method. In addition, Hurmuzlu and Marghitu [26] studied the rigid body collision of planar, kinematic chains with an external surface while in contact with other surfaces. A. M. Shafei and H. R. Shafei [27] presented a systematic procedure for the dynamic modeling of a closedchain robotic system in both the flight and impact phases. Gattringer et al. [28] established an efficient dynamic model for rigid multibody systems with contact and impact by a recursive procedure. The above research studies are mainly aimed at the dynamic response of the multibody system colliding with its working environments and other multibody systems.
In this work, the impact dynamics of the constrained metamorphic mechanism during configuration transformation is mainly studied along with the impact dynamics between two internal components of the multibody system. Wang et al. [29] considered the effects of material parameters, control parameters, and internal impact excitation on dynamic performance of the mechanism system. Bruzzone and Bozzini [30] designed a novel microassembly system and tested the grasping stability of the metamorphic fingertips. Song et al. [31] studied the change of the 6R metamorphic mechanism from an unconstrained condition to a geometrically constrained condition to accomplish the transformation between different screw systems. Ye et al. [32] analyzed the configuration changes of the reconfigurable limb associated with the three distinct phases of the PMM (planar metamorphic mechanism) and identified the constraints exerted by the reconfigurable limb in various configurations. Until now, the configurationcomplete dynamic model of the metamorphic mechanism has been mainly established by incorporating both the topological structure change and the subconfiguration dynamic model [33], ignoring the impact motion generated by configuration transformation. It should be noticed that in order to keep favorable dynamic performance, the impact motion generated by configuration transformation should be taken into consideration in the dynamic modeling.
Therefore, to describe the influence of impact motion on the system’s stability when the configuration changes, the impact dynamics during configuration transformation need to be studied. In this paper, taking PCMM as an example, the dynamic models of its stable and mobile impact motions are established based on the topology theory and multibody system dynamics, and then the corresponding impulse solving models are deduced by combining the coefficient of restitution equation. Further, two examples of PCMM considering the impact motions generated by configuration transformation are given to illustrate the effect of impact motions. Meanwhile, the validity of the proposed method is verified.
2. Dynamic Analysis
The working process of PCMM can be roughly divided into the subconfiguration movement stage and the instantaneous configuration transformation stage. Therefore, the configurationcomplete dynamic equation of PCMM considering the impact motion during configuration transformation will be set up.
2.1. Dynamic Analysis in Subconfiguration Movement Stage
Under any working stage or working condition p, the corresponding topological structure of PCMM is called the pth configuration or configuration p. PCMM in any configuration p can be regarded as a conventional mechanism. Suppose the DOF of PCMM in configuration p is n and the independent generalized coordinate of PCMM is . Ignoring the influence of external disturbance such as friction, the dynamic equation of PCMM with any configuration p can be written by the Newton–Euler equation as a vector form:where is the generalized acceleration vector, is the inertia matrix which is symmetric positive definite, is the gravity, the Coriolis, and the centripetal force vector, is the generalized force vector, and is the generalized elastic and other generalized force vector.
2.2. Dynamic Analysis in Instantaneous Configuration Transformation Stage
For PCMM with c configurations, it is assumed that configuration is any configuration of PCMM. When PCMM is changed from configuration p to configuration p + 1, the impact motion occurs inside the system. There are mainly two situations as follows:(1)The moving component is merged with the frame(2)The moving component is merged with another moving component
To establish the instantaneous impact dynamic equation for configuration transformation of PCMM, the definitions are as follows.
When PCMM is changed from one configuration to the next,(1)According to the way of configuration transformation, if the moving component is merged with the frame, the impact motion generated by configuration transformation is named the stable impact motion and the generated internal impulse is named the stable impulse in this paper. Meanwhile, the dynamic equation of the system is named the stable impact dynamic equation.(2)Similarly, if the moving component is merged with another moving component, the impact motion generated by configuration transformation is named the mobile impact motion and the generated internal impulse is named the mobile impulse. At this time, the dynamic equation of the system is named the mobile impact dynamic equation.
It should be further pointed out that since the impact motion is generated instantaneously during the configuration transformation of PCMM, the impact dynamics is only studying the system state at a certain moment and not the system state throughout the time history.
2.2.1. Dynamic Analysis of the Stable Impact Motion
In this section, a dynamic model is established, which describes the dynamics of PCMM with a stable impact motion. In order to establish a complete theoretical system of impact dynamics of PCMM, it is very important to choose a reasonable topology structure. In this paper, it is assumed that the two adjacent components of PCMM are connected by rotating hinges, and the topology structure of PCMM can be considered as a tree system, as shown in Figure 1.
Assuming that the impact motion occurs instantaneously, the impact points are defined as and on the frame B_{0} and the moving component B_{1}, respectively. When the moving component B_{1} and the frame B_{0} merge, the stable impact motion occurs, and there are equal and opposite action and reaction forces at the impact points and . It is sometimes necessary to get more acquainted with the impact force of metamorphic components and the ideal constraint force of metamorphic joints for stability analysis of configuration transformation.
When the configuration of PCMM changes, the impulse generated by configuration transformation of the mechanism is zero [34]. However, when the moving component merges with the frame or the fixed base, the impulse acting on the moving component is not zero. To solve the impulse acting on the moving component B_{1}, the rotating joint O_{1} connecting the moving component B_{1} and the frame B_{0} can be released based on multibody systems dynamics [35, 36], and the stable impact motion system can be transformed into the multibody system f which is only subject to ideal constraints.
For the cutting of joints in the PCMM, that is to remove partial constraints in the system. The redundant joints removed are also called the cutoff joints. If the multibody system f is equivalent to the original stable impact motion system in dynamics, the constraint force acting on the adjacent components by the cutoff joint must be considered as an additional external force applied to the multibody system f. Therefore, based on the Newton–Euler equation, a dynamic equation of the multibody system f is established, and the stable impact dynamic equation is established combining the constraint equation of the cutoff joint O_{1}. And, the stable impact force of the metamorphic component B_{1} and the ideal constraint force of metamorphic joint O_{1} can be calculated by the stable impact dynamic equation. The detailed derivation process is as follows.
Assume that the generalized position vector of arbitrary configuration obtained by the cutting off joint is and is the number of DOFs in the multibody system . Then, position of the impact point can be written separately as expressed as a function with a generalized coordinate as
According to the kinematic relationship of the multibody system f, it is easy to obtain the following kinematic relationship between the velocity of the impact point on the moving component and the generalized velocity vector :where
When the system satisfies the conditions of configuration transformation , the stable impact force acting on the impact points and is immediately generated. According to the Newton–Euler equation, the multibody system f with the stable impact motion is subject to constraint forces at the cutoff joint and stable impact forces in addition to driven and elastic forces. Therefore, the dynamic equation of the multibody system f with the stable impact motion can be established aswhere is the generalized acceleration vector of the multibody system , is the inertia matrix of the multibody system , is the gravity, the Coriolis, and centripetal force vector of the multibody system , is the generalized force vector of the multibody system , is the generalized elastic and other generalized force vector of the multibody system , is the generalized constraint force vector of the cutoff joint , and is the generalized stable impact force vector.
According to the principle of virtual work, the generalized constraint force vector and the generalized stable impact force vector can be respectively expressed aswhere is the firstorder kinematic influence coefficient of the velocity vector of the cutoff joint O_{1} in the inertial coordinate system with respect to the generalized velocity in the multibody system f and is the constraint force at the cutoff joint O_{1}.
According to the Newton–Euler equation, the constraint force at the cutoff joint O_{1} can be expressed as the form of generalized acceleration vector in the stable impact motion system:where is the coefficient matrix of with respect to and is a column matrix.
According to the kinematic constraint equation at the cutoff joint O_{1}, that is, . The constraint force at the cutoff joint O_{1} can be expressed aswhere is the coefficient matrix of with respect to .
Combining equations (5)–(7) and (9), the stable impact dynamic equation of PCMM can be derived as
2.2.2. Dynamic Analysis of the Mobile Impact Motion
As shown in Figure 2, when the mobile impact motion occurs, the moving component merges with another moving component , and there are equal and opposite action and reaction forces at the impact points and . In order to obtain the mobile impact force of metamorphic components and the ideal constraint force of metamorphic joints, the rotating joint between the moving components and is cut off based on multibody system dynamics [35, 36]. Then, the mobile impact motion system is divided into two multibody systems with external impacts, which are respectively labeled as and , and the dynamic equations of the multibody systems and can be established.
In order to make the divided multibody systems and dynamically equivalent to the mobile impact motion system, the constraint force acting on the adjacent components by the cutting off joint must be regarded as an additional external force applied to the two multibody systems and .
It is assumed that the generalized position vectors of the multibody systems and are and , respectively, and and are the number of DOFs of the multibody systems and , respectively. Then, positions of the impact points and can be written separately as expressed as functions with generalized coordinates and as
According to the kinematic relationship of the multibody systems and , it is easy to obtain the following kinematic relationship between the velocity of the impact point on the moving component in the inertial coordinate system and the generalized velocity vector and the velocity of the impact point on the moving component in the inertial coordinate system and the generalized velocity vector :where
When the system satisfies the conditions of configuration transformation, the mobile impact force of the multibody system is immediately generated. Based on the Newton–Euler equation, the multibody systems and with mobile impact motion are subject to the constraint forces at the cutoff joint and the mobile impact forces in addition to driven and elastic forces. Therefore, the dynamic equations of the multibody systems and with mobile impact motion can be established aswhere is the generalized acceleration vector of the multibody system , is the inertia matrix of the multibody system , is the gravity, the Coriolis, and the centripetal force vector of the multibody system , is the generalized force vector of the multibody system , is the generalized elastic and other generalized force vector of the multibody system , is the generalized constraint force vector at the cutoff joint of the multibody system , and is the generalized mobile impact force vector of the multibody system .
According to the principle of virtual work, the generalized constraint force vector and the generalized mobile impact force vector of the multibody systems and at the cutoff joint can be respectively obtained:where is the firstorder kinematic influence coefficient of the velocity vector of the cutoff joint in the inertial coordinate system with respect to the generalized velocity in the multibody system , is the constraint force at the cutoff joint of the multibody system , , and .
According to the Newton–Euler equation, the constraint force at the cutoff joint can be deduced in the form of generalized acceleration vector aswhere is the generalized acceleration vector of the mobile impact motion system, is the coefficient matrix of with respect to , and is a column matrix.
Combining the kinematic constraint equation at the cutoff joint , it can be obtained aswhere is the coefficient matrix of with respect to and is a column matrix.
Substituting equation (18) into equation (17), the constraint force at the cutoff joint can be derived aswhere and .
Combining equations (14)–(16) and (19), the mobile impact dynamic equation of PCMM can be derived as
It is emphasized that with respect to PCMM with closedloop constraints, it can be transformed into multibody systems in the tree system by cutting off the metamorphic joints in the loop when PCMM is changed from one configuration to the next, so that its impact dynamic analysis can be carried out by the tree system theory mentioned above.
3. The Impulse Solving Model of Constrained Metamorphic Mechanism
Based on the dynamic equation in the subconfiguration movement stage, the system state variables before configuration transformation can be obtained. Aiming at the specific impact motion of mechanism, how to determine the internal impulse generated by configuration transformation instantaneously and the state variables of the system after configuration transformation is the basic research scope of the impact motion, and it is also an urgently solved core problem. In this paper, on the basis of the impact dynamic equations (10) and (20), the stable impulse solving model and the mobile impulse solving model can be, respectively, derived by combining the coefficient of restitution equation. The resulting system state variables after configuration transformation can be deduced according to variables before configuration transformation.
3.1. The Contact Impact Model
According to the classical collision theory, the contactimpact model has been developed with the following assumptions: (1) the impact time is infinitely small; (2) the position and orientation of all components remain unchanged during the process of configuration transformation; (3) the impact is a point contact; (4) the shape and the inertia of the component are unchanged during the process of configuration transformation.
In general, the impact is partially elastic, and is the coefficient of restitution. The normal vector of the impact point velocity increment is n along the contact surface, and the stable and mobile impact motion systems should satisfy the coefficient of restitution equation at the instant of configuration transformation as follows:where and are the velocities of impact points relative to the inertial coordinate system before configuration transformation and and are the velocity increments immediately after configuration transformation.
3.2. The Stable Impulse Solving Model
According to the basic assumption, the generalized positions of the system remain unchanged over a short duration where the time interval is small enough, so its generalized velocities are limited. The derived stable impact dynamic equation (10) is integrated over the time interval , and the result is obtained as
Taking the limit of equation (22) as tends to zero, it can be written aswhere is defined as the stable impulse at the impact point.
Then, the velocity increments of the generalized positions can be expressed aswhere
Based on the kinematics, the velocity increment of the impact point can be written as
According to the stable impact motion between the moving component and the frame, the absolute velocity and the velocity increment of the frame are always zero . Assuming that there is no friction between two impacting surfaces and substituting equation (26) into equation (21), it can be obtained as
In addition,
Then, the stable impulse of PCMM can be expressed as
Combining the initial condition of the system before configuration transformation, the generalized velocity of the system after configuration transformation can be obtained aswhere is the generalized velocity vector after configuration transformation and is the generalized velocity vector before configuration transformation.
3.3. The Mobile Impulse Solving Model
According to the basic assumption, the derived mobile impact dynamic equation (20) is integrated over the time interval , and the result is obtained as
Since the mobile impact motion is of short duration and generates a large mutual impact force, the generalized positions of PCMM are not significantly changed during configuration transformation and only the generalized velocities are changed. Based on the above analysis, equations (31) and (32) can be approximately written aswhere is defined as the mobile impulse at the impact point.
The derivation of (33) and (34) is based on the conservation of system momentum. Based on equation (34), the velocity increments of the generalized positions can be expressed in the multibody system aswhere
Based on the kinematics, the velocity increment of the impact point in the multibody system can be written as
Substituting equation (35) into equation (33), the velocity increment of the generalized coordinate in the multibody system can be expressed aswhere
Based on the kinematics, the velocity increment of the impact point in the multibody system can be written as
In addition,
Substituting equations (37), (40), and (41) into (21), the mobile impulse of PCMM can be derived aswhere .
Combining the initial condition of the system before configuration transformation, the generalized velocity of the system after configuration transformation can be obtained aswhere is the generalized velocity vector of the multibody system after configuration transformation and is the generalized velocity vector of the multibody system before configuration transformation.
According to the above derivation results, if the impulse of the impact point in the system and the velocity of each component before configuration transformation are known, we can calculate the velocity of each component after configuration transformation.
4. Dynamic Numerical Examples
For the sake of completeness, this section lists two typical examples to model and simulate the impact dynamics. One is an openloop constrained metamorphic mechanism and the other is a closedloop constrained metamorphic mechanism. To analyze the motion characteristics of the system before and after configuration transformation, the dynamic simulations of PCMM can be carried out by MATLAB. Since the impact dynamic equation of the system is nonlinear, it can be solved by using Runge–Kutta method to realize the configurationcomplete dynamic simulation of PCMM. The flow graph of numerical simulation is shown in Figure 3.
4.1. Simulation Example 1
In this case, the impact dynamics of the openloop threebar constrained metamorphic mechanism is analyzed in Figure 4. Symbols described in Figure 4 are explained as follows:(1): component i of the openloop threebar constrained metamorphic mechanism(2): joint O_{i} of the openloop threebar constrained metamorphic mechanism(3): the angle between component i and the xaxis(4): the equivalent moments acting on joint O_{i}
(a)
(b)
As shown in Figure 4, the openloop threebar constrained metamorphic mechanism is composed of component 1, component 2, component 3, and the frame. Assume that the motor is installed at the joint and the torsion spring is installed at the joint . If , the mechanism is in configuration 1 as shown in Figure 4(a); if , the component 2 merges with the component 3, and the mechanism is in configuration 2 as shown in Figure 4(b).
For the abovementioned metamorphic mechanism, which realizes the whole process of metamorphosis by constraints, it is required that the corresponding metamorphic joint of the corresponding configuration should be able to provide corresponding constraints in order to realize the configuration transformation in the working process. According to the existing working configuration, the joint is chosen as the metamorphic joint and its main realization form is shown in Figure 5. Symbols described in Figure 5 are explained as follows: a: a limited pin distributed on a circle
Figure 5 shows a limited rotation metamorphic joint [37]. The structure of the metamorphic joint is obtained by synthesizing the pinrestrained rotation metamorphic joint and the springrestrained rotation metamorphic joint. The component 2 and the component 3 are connected by torsion spring, and the component 2 contains a limited pin a distributed on a circle.
Then, the equivalent moments acting on each joint can be expressed as follows, and the geometric and physical parameters of the openloop threebar constrained metamorphic mechanism are shown in Table 1.

Assuming that the openloop threebar constrained metamorphic mechanism is transformed from configuration 1 to configuration 2 , the centroid point of component 3 is impacted with the centroid point of component 2. The normal vector of the impact point velocity increment is and the coefficient of restitution is 0.8. Based on the dynamics, the absolute angular velocity of each component before configuration transformation can be calculated as follows:
According to the mobile impulse solving model, the mobile impulse in the instantaneous configuration transformation can be obtained as
Based on equation (43), the absolute angular velocity of each component after configuration transformation can be calculated as follows:
In addition, constrained metamorphic operations of the mechanism are implemented by using the geometric constraint and the force constraint of the metamorphic joint to make it locked. Owing to the existence of the geometric constraint, the metamorphic joint is locked in instantaneous configuration transformation. Therefore, component 2 is merged with component 3 after configuration transformation, that is, , when considering constraint conditions of configuration transformation.
The numerical simulation results of each component are shown in Figures 6–9. In the conditions of considering and ignoring the impact motion during configuration transformation, the comparisons of the absolute angle of each component in the openloop threebar constrained metamorphic mechanism are shown in Figures 6(a)–6(c), respectively. Similarly, Figure 6(d) shows the angle of component 3 relative to component 2.
(a)
(b)
(c)
(d)
(a)
(b)
(c)
(a)
(b)
(c)
From Figures 6(a)–6(c), it can be seen that the motion trends of components considering the impact motion are exactly different from the motion trends ignoring the impact motion. Moreover, the motion amplitudes of each component considering the impact motion are larger than that of each component ignoring the impact motion, which indicates that the impact motion has a positive influence on each component. The motion law of component 3 relative to component 2 does not encounter changes, as shown in Figure 6(d), which is determined by the conditions of configuration transformation.
The comparisons of the absolute angular velocities are shown in Figures 7(a)–7(c), respectively. The absolute angular velocity of each component after configuration transformation has an obvious abrupt change, as shown in Figure 7, and it illustrates that the impact will occur in each joint with considering the impact motion during configuration transformation. In addition, both component 2 and component 3 are subjected to the mobile impact, and the abrupt change of absolute angular velocity of component 3 is obviously higher than component 2 with the same structural parameters, which is determined by the state variables of the system before configuration transformation.
Figure 8 compares and analyses the moments acting on the joints in the conditions of considering and ignoring the impact motion during configuration transformation. The moment at joint is related to the angular velocity of the component 1, so the moment changes abruptly after configuration transformation. The moments at joints and are only related to their absolute angular displacements, and there is no abrupt change in the whole movement process.
Figure 9 shows the variation of dynamic behavior for the system in the whole simulation process from the perspective of energy. As shown in Figure 9, kinematic energy of the system changes abruptly at the instant of configuration transformation. This is due to the impact of configuration transformation. Since potential energy is related to the absolute angular displacement, there is no abrupt change at the instant of configuration transformation.
4.2. Simulation Example 2
Taking the planar doublefolded metamorphic mechanism as an example [38], the types and constraints of metamorphic joints based on the kinematic characteristics of metamorphic joints are given. According to the working task, the planar doublefolded metamorphic mechanism (as shown in Figure 10) must complete the following two working requirements: horizontal folding and vertical folding:(1)Horizontal folding, as shown in Figure 10(a): horizontally pushing the left side of the singlelayer cardboard and rotating the second side of the left side along the second crease to the vertical position(2)Vertical folding, as shown in Figure 10(b): completing the rotation of the first surface around the first crease and coinciding with the second surface
(a)
(b)
Figure 11 shows the schematic diagram of the planar doublefolded metamorphic mechanism. According to the above requirements, force metamorphism is adopted at joint D, that is, when the mechanism is in configuration 1, the spring force is set at joint D, so that the relative moving resistance between the components 3 and 4 is larger than the motion resistance of the slider, and it keeps the components 3 and 4 relatively static. When the mechanism is in configuration 2, a geometric constraint is added at joint E, so that the slider moves to the specified position and stops moving when the mechanism meets the geometric limit. Its geometric and physical parameters are shown in Table 2.
 
Note. L_{AB} is the corresponding link length between joints A and B, L_{BC} is the corresponding link length between joints B and C, L_{CD} is the corresponding link length between joints C and D, L_{AEy} is the corresponding distance along the yaxis between joints A and E, is the mass of component i, J_{1} is the moment of inertia of component 1 around the center of mass, J_{BC} is the moment of inertia of component 2 around the joint C, J_{DC} is the moment of inertia of component 3 around the joint C, k is the spring constant, c is the damping constant, and is the initial angle of the spring. 
Assume that the motion law of component 1 can be written as follows:
In view of the abovementioned conditions, the numerical simulation is carried out, as shown in Figures 12–15. Figure 12 shows the change of impulse when the planar doublefolded metamorphic mechanism is transformed from configuration 1 to configuration 2.
(a)
(b)
From Figure 12, it can be seen that there is a macroimpact behavior in the whole simulation process. Since the impact is partially elastic and the impact point on the slider oscillates back and forth with the slider, the change of impulse moment in a macroimpact process is more intense, and there are multiple secondary impacts in a macroimpact process. In addition, the time interval of secondary impacts is becoming smaller and smaller. After several consecutive secondary impacts, the impulse moment of the slider becomes zero until the slider and the frame are completely merged, and the configuration transformation ends.
Figure 13 shows the variation of the slider position and slider velocity, respectively. From Figure 13, it can be seen that the impact motion considering the configuration transformation makes the slider velocity change complicatedly, and the change gradually decreases with time. After the slider and the frame are merged, velocity of the slider decreases to 0 and the mechanism enters the second configuration.
The variation of the driven moment is illustrated through Figure 14. It can be seen from the results in Figure 14 that the driven moment of the mechanism changes accordingly after the impact motion occurs. Comparing the displacement and velocity curves of the slider, the simulation results further illustrate the effectiveness of the model established.
Figure 15 shows the variation of dynamic behavior for the system in the whole simulation process from the perspective of energy. As shown in Figure 15, kinematic energy and potential energy of the system changes greatly at the instant of configuration transformation. This is caused by the impact of configuration transformation.
In addition, according to geometric and inertia parameters of the planar doublefolded metamorphic mechanism in Table 2, a threedimensional model is established in SolidWorks, as shown in Figure 16. The motion plugin of the SolidWorks software is used to carry out dynamic virtual simulation on it. The results are shown in Figure 17 and are compared with the numerical calculation results shown in Figure 13.
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(b)
From Figure 17, it can be found that the law of motion curve obtained by numerical calculation and virtual simulation is basically the same, but there is a slight deviation. This is due to the different calculation accuracy of MATLAB and SolidWorks at the time of configuration transformation.
5. Conclusion
The paper presents a new method of establishing impact dynamic models of the planar constrained metamorphic mechanism. Based on the dynamic modeling in the subconfiguration movement stage, the stable and the mobile impact dynamic equations of the planar constrained metamorphic mechanism are, respectively, established by considering the metamorphic forms and the constraint forms of the cutoff joint.
The stable and the mobile impulse solving models of the planar constrained metamorphic mechanism during configuration transformation are derived by the corresponding impact dynamic equation and the coefficient of restitution equation. The impulse and the generalized velocity increments are completely decoupled, which is beneficial to solve the abrupt change of the generalized velocity. Then, the system state variables after configuration transformation are calculated according to the initial conditions in configuration transformation, which provides an important basis and a precondition for the impact dynamic modeling of the planar constrained metamorphic mechanism and further improves its configurationcomplete dynamic models.
Using the proposed method, the openloop threebar constrained metamorphic mechanism and the planar doublefolded metamorphic mechanism are taken as examples to simulate the mobile impact motion and the stable impact motion, respectively. The results show, under the conditions of considering and ignoring the impact motion during configuration transformation, that the motion states of the openloop system after configuration transformation are obviously different and the motion states of the closedloop system during configuration transformation which are violent vibrations. In addition, the proposed impact dynamic modeling method of the planar constrained metamorphic mechanism not only provides a theoretical basis for our followup research work, but also can be applied to solve the internal collision dynamic problem of general planar robotic systems.
Nomenclature
DOF(s):  Degree(s) of freedom 
Superscript p:  Configuration p 
:  Independent generalized coordinate 
:  Inertial matrix 
:  Gravity, Coriolis, and centripetal force vector 
:  Generalized force vector 
:  Generalized elastic and other generalized force vector 
:  Position of the impact point i 
:  Position function of the impact point i in the multibody system 
:  Firstorder kinematic influence coefficient between the impact point i and generalized velocity in the multibody system 
:  Independent generalized coordinate of the multibody system 
:  Inertial matrix of the multibody system 
:  Gravity, Coriolis, and centripetal force vector of the multibody system 
:  Generalized force vector of the multibody system 
:  Generalized elastic and other generalized force vector of the multibody system 
:  Generalized constrained force vector of the cutoff joint 
:  Generalized stable impact force vector of the multibody system f 
:  Firstorder kinematic influence coefficient between the cutoff joint and generalized velocity in the multibody system 
:  Constraint force at the cutoff joint in the multibody system 
:  Stable impact force 
:  The coefficient matrix of with respect to 
:  A column matrix 
:  The coefficient matrix of with respect to 
:  Generalized mobile impact force vector of the multibody system 
:  Mobile impact force of the multibody system 
:  Velocity of impact point relative to the inertial coordinate system before configuration transformation 
:  Velocity increments immediately after configuration transformation 
:  Normal vector of impact point velocity increment 
:  Coefficient of restitution 
:  Stable impulse at the impact point 
:  Mobile impulse at the impact point. 
Data Availability
All data generated or analyzed during this study are included in this published article, and other pieces of information are available from the corresponding author upon reasonable request.
Conflicts of Interest
The authors declare that there are no conflicts of interest regarding the publication of this paper.
Acknowledgments
This study was partly supported by the National Natural Science Foundation of China (nos. 51275352 and 51475330), Natural Science Foundation of Tianjin (nos. 17JCQNJC03900 and 18JCQNJC05300), Tianjin Municipal Education Commission Research Program (2018KJ205), and Program for Innovative Research Team in University of Tianjin (TD135037).
References
 W. Zhang, X. Ding, and J. Liu, “A representation of the configurations and evolution of metamorphic mechanisms,” Mechanical Sciences, vol. 7, no. 1, pp. 39–47, 2016. View at: Publisher Site  Google Scholar
 J. S. Dai and J. Rees Jones, “Mobility in metamorphic mechanisms of foldable/erectable kinds,” Journal of Mechanical Design, vol. 121, no. 3, pp. 375–382, 1999. View at: Publisher Site  Google Scholar
 C. Valsamos, V. Moulianitis, and N. Aspragathos, “Index based optimal anatomy of a metamorphic manipulator for a given task,” Robotics and ComputerIntegrated Manufacturing, vol. 28, no. 4, pp. 517–529, 2012. View at: Publisher Site  Google Scholar
 C. Valsamos, V. C. Moulianitis, A. I. Synodinos, and N. A. Aspragathos, “Introduction of the high performance area measure for the evaluation of metamorphic manipulator anatomies,” Mechanism and Machine Theory, vol. 86, pp. 88–107, 2015. View at: Publisher Site  Google Scholar
 K. Xu, L. Li, S. Bai, Q. Yang, and X. Ding, “Design and analysis of a metamorphic mechanism cell for multistage orderly deployable/retractable mechanism,” Mechanism and Machine Theory, vol. 111, pp. 85–98, 2017. View at: Publisher Site  Google Scholar
 W. Zhang, F. Liu, Y. Lv, and X. Ding, “Design and analysis of a metamorphic mechanism for automated fibre placement,” Mechanism and Machine Theory, vol. 130, pp. 463–476, 2018. View at: Publisher Site  Google Scholar
 F. Liu, W. Zhang, K. Xu, H. Deng, and X. Ding, “A planar mechanism with variable topology for automated fiber placement,” in Proceedings of the 2018 International Conference on Reconfigurable Mechanisms and Robots (ReMAR), IEEE, Delft, Netherlands, June 2018. View at: Publisher Site  Google Scholar
 V. Charalampos, V. C. Moulianitis, and N. A. Aspragathos, “Kinematic synthesis of structures for metamorphic serial manipulators,” Journal of Mechanisms and Robotics, vol. 6, no. 4, Article ID 041005, 2014. View at: Publisher Site  Google Scholar
 D. Gan, J. Dias, and L. Seneviratne, “Unified kinematics and optimal design of a 3rRPS metamorphic parallel mechanism with a reconfigurable revolute joint,” Mechanism and Machine Theory, vol. 96, pp. 239–254, 2016. View at: Publisher Site  Google Scholar
 S. Li, H. Wang, X. Li, H. Yang, and J. S. Dai, “Taskorientated design method of practical constraint metamorphic mechanisms,” Journal of Mechanical Engineering, vol. 54, no. 3, pp. 26–35, 2018. View at: Publisher Site  Google Scholar
 P. Martín A, A. Butti, V. Tamellini, A. Cardona, and L. Ghezzi, “Topological synthesis of planar metamorphic mechanisms for lowvoltage circuit breakers,” Mechanics Based Design of Structures and Machines, vol. 40, no. 4, pp. 453–468, 2012. View at: Publisher Site  Google Scholar
 S. Li, H. Wang, Q. Meng, and J. S. Dai, “Taskbased structure synthesis of source metamorphic mechanisms and constrained forms of metamorphic joints,” Mechanism and Machine Theory, vol. 96, pp. 334–345, 2016. View at: Publisher Site  Google Scholar
 G. Gilardi and I. Sharf, “Literature survey of contact dynamics modelling,” Mechanism and Machine Theory, vol. 37, no. 10, pp. 1213–1239, 2002. View at: Publisher Site  Google Scholar
 Y. C. Duan and D. G. Zhang, “Rigidflexible coupling dynamics of a flexible robot with impact,” Advanced Materials Research, vol. 199200, pp. 243–250, 2011. View at: Publisher Site  Google Scholar
 G. Jin, G. Wu, B. Chang, and L. Chen, “Dynamic analysis of manipulator with contact impact,” Transactions of the Chinese Society for Agricultural Machinery, vol. 47, pp. 369–375, 2016. View at: Google Scholar
 Q.H. Dong and L. Chen, “Impact dynamics analysis of freefloating space manipulator capturing satellite on orbit and robust adaptive compound control algorithm design for suppressing motion,” Applied Mathematics and Mechanics, vol. 35, no. 4, pp. 413–422, 2014. View at: Publisher Site  Google Scholar
 Z. Deng, Q. Wang, Q. Quan, S. Jiang, and D. Tang, “Impact dynamics of a differential gears based underactuated robotic arm for moving target capturing,” Mechatronics, vol. 40, pp. 208–219, 2016. View at: Publisher Site  Google Scholar
 J. Choi, H. Ryu, and B. Yi, “Variable impact dynamics of a finger mechanism,” in Proceedings of the 2011 8th International Conference on Ubiquitous Robots and Ambient Intelligence, pp. 23–26, Incheon, South Korea, November 2011. View at: Publisher Site  Google Scholar
 M. Machado, P. Moreira, P. Flores, and H. M. Lankarani, “Compliant contact force models in multibody dynamics: evolution of the Hertz contact theory,” Mechanism and Machine Theory, vol. 53, pp. 99–121, 2012. View at: Publisher Site  Google Scholar
 D. Bhalerao and S. Anderson, “Modeling intermittent contact for flexible multibody systems,” Nonlinear Dynamics, vol. 60, no. 12, pp. 63–79, 2010. View at: Publisher Site  Google Scholar
 M. Ahmadizadeh, A. M. Shafei, and M. Fooladi, “A recursive algorithm for dynamics of multiple frictionless impactcontacts in openloop robotic mechanisms,” Mechanism and Machine Theory, vol. 146, pp. 1–20, 2020. View at: Publisher Site  Google Scholar
 M. H. Korayem and M. Taheri, “Modeling of various contact theories for the manipulation of different biological micro/nanoparticles based on AFM,” Journal of Nanoparticle Research, vol. 16, no. 1, pp. 1–13, 2014. View at: Publisher Site  Google Scholar
 M. H. Korayem, H. Khaksar, M. Taheri et al., “Modeling of contact theories for the manipulation of biological micro/nanoparticles in the form of circular crowned rollers based on the atomic force microscope,” Journal of Applied Physics, vol. 114, no. 18, Article ID 183715, 2013. View at: Publisher Site  Google Scholar
 P. Flores and J. Ambrósio, “On the contact detection for contactimpact analysis in multibody systems,” Multibody System Dynamics, vol. 24, no. 1, pp. 103–122, 2010. View at: Publisher Site  Google Scholar
 J. Y. Wang, Z. Y. Liu, and J. Z. Hong, “Partition method and experimental validation for impact dynamics of flexible multibody system,” Acta Mechanica Sinica, vol. 34, no. 3, pp. 482–492, 2018. View at: Publisher Site  Google Scholar
 Y. Hurmuzlu and D. B. Marghitu, “Rigid body collisions of planar kinematic chains with multiple contact points,” The International Journal of Robotics Research, vol. 13, no. 1, pp. 82–92, 1994. View at: Publisher Site  Google Scholar
 A. M. Shafei and H. R. Shafei, “Dynamic modeling of planar closedchain robotic manipulators in flight and impact phases,” Mechanism and Machine Theory, vol. 126, pp. 141–154, 2018. View at: Publisher Site  Google Scholar
 H. Gattringer, H. Bremer, and M. Kastner, “Efficient dynamic modeling for rigid multibody systems with contact and impact,” Acta Mechanica, vol. 219, no. 12, pp. 111–128, 2011. View at: Publisher Site  Google Scholar
 R. Wang, H. Chen, and J. Dai, “Dynamic stability study of a novel controllable metamorphic palletizing robot mechanism,” Journal of Mechanical Engineering, vol. 13, no. 19, pp. 39–47, 2017. View at: Publisher Site  Google Scholar
 L. Bruzzone and G. Bozzini, “A flexible joints microassembly robot with metamorphic gripper,” Assembly Automation, vol. 30, no. 3, pp. 240–247, 2010. View at: Publisher Site  Google Scholar
 Y. Song, X. Ma, and J. S. Dai, “A novel 6R metamorphic mechanism with eight motion branches and multiple furcation points,” Mechanism and Machine Theory, vol. 142, Article ID 103598, pp. 1–19, 2019. View at: Publisher Site  Google Scholar
 W. Ye, Y. Fang, K. Zhang, and S. Guo, “Mobility variation of a family of metamorphic parallel mechanisms with reconfigurable hybrid limbs,” Robotics and ComputerIntegrated Manufacturing, vol. 41, pp. 145–162, 2016. View at: Publisher Site  Google Scholar
 G. Jin, X. Ding, and Q. Zhang, “Research on configurationcomplete dynamics modeling and numerical simulation of metamorphic mechanism,” Acta Aeronautica et Astronautica Sinica, vol. 25, pp. 401–405, 2004. View at: Google Scholar
 S. Yang, G. Jin, J. Yun, and Z. Feng, “Research on impact motion in metamorphic mechanism,” China Mechanical Engineering, vol. 20, pp. 1608–1612, 2009. View at: Google Scholar
 K. S. Anderson and J. H. Critchley, “Improved “orderN” performance algorithm for the simulation of constrained multirigidbody dynamic systems,” Multibody System Dynamics, vol. 9, no. 2, pp. 185–212, 2003. View at: Publisher Site  Google Scholar
 J. Hong, Computational Dynamics of Multibody Systems, High Education Press, Beijing, China, 1999.
 Q. Yang, H. Wang, S. Li, and J. S. Dai, “Type synthesis of constrained metamorphic mechanisms with structural forms of metamorphic joints,” Journal of Mechanical Engineering, vol. 50, no. 13, pp. 1–8, 2014. View at: Publisher Site  Google Scholar
 B. Chang, G. Jin, and J. S. Dai, “Type synthesis of metamorphic mechanism based on variable constraint screw theory,” Journal of Mechanical Engineering, vol. 50, no. 5, pp. 17–25, 2014. View at: Publisher Site  Google Scholar
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Copyright © 2020 Yanyan Song et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.