# Design, Analysis, and Experiment for Rescue Robot with Wheel-Legged Structure

Authors: Meng Ning; Bilun Xue; Zefeng Ma; Changhong Zhu; Zihao Liu; Cuncai Zhang; Yao Wang; QiuJu Zhang
Journal: Mathematical Problems in Engineering
 (2017)

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## Abstract

A wheel-legged rescue robot design with strong environmental adaptability is proposed. The design presented is aimed at helping rescue workers complete their missions, such as environmental and personnel search, quickly and accurately. So it has broad application prospects. In order to achieve the advantages of simple structure, easy control, small occupation space, and wide motion range, a wheel-legged rescue robot is designed in this paper, and the robot can realize three kinds of motion states, which include wheel state, rotation center lifting process, and leg state. Then the motion states are analyzed in detail, which provides a reference for motion control. Considering the wheel state and leg state share the same structure to contact with the ground, the effect of the stiffness of wheel-legged structure to the motion performance is analyzed. Then the experiment is carried out to prove the feasibility of the structure design. This study offers a design and quantitative analysis for wheel-legged rescue robot. Furthermore, a basis for future control research and engineering applications is established.


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## Body

## 1. Introduction

The complex and dangerous environment after the disaster can cause serious danger to the life safety of rescue workers. Rescue robot can perform many tasks instead of rescue workers, such as environmental monitoring and personnel search, and it can improve the rescue efficiency and information accuracy. So the rescue robot has broad application prospect [1–4]. Because the postdisaster environment is very complex, the adaptability of complex environment is the basic function of the rescue robot.According to the different movement forms, rescue robots can be divided into four categories: tracked rescue robot [5–8], wheeled rescue robot [9], multilegged rescue robot [10, 11], and snake-like rescue robot [12, 13]. However, the movement environment and function of the above four kinds of robots have some limitations. In order to solve the above problems, many researchers have studied the wheel-legged robot connecting the high obstacle capability of multilegged robot and high mechanical efficiency of wheeled robot. According to the different structure form, wheel-legged structure of the robot can be divided into series structure, similar parallel structure, and simplified structure. The leg of mammals and insects has three parts: thigh (femur), calf (tibia), and foot (tarsus); thus, the leg can be considered as a series mechanism [14]. Many wheel-legged structures were designed by mimicking biological leg structure and have the advantages of high flexibility. For example, California Institute of Technology designed a six-wheel-legged mobile robot ATHLETE in 2008. Each leg of this robot has six DOF (degrees of freedom), and each wheel-legged can change posture flexibly to adapt to different terrain or across obstacles [15, 16]. Amar et al. [17] designed a wheel-legged robot, and each leg has three DOF. An electrical actuator with a ball screw is mounted on each sliding joint. Besides, many scientific research institutions [18–21] have carried out in-depth research on the structure design and performance analysis of this type of wheel-legged robots. Similar parallel structure has the advantages of high load capacity and rigidity, and some research institutions also have studied this type of robot. For example, Wang et al. [22] designed a wheel-legged rescue robot, and the leg is a (2-VPS+U)R series-parallel mechanism. Alamdari et al. [23] explored the use of various candidate articulated leg-wheel subsystem designs (based on the four-bar mechanism) to enhance locomotion capabilities of land-based vehicles. Besides, Luo et al. [24] and Siegwart et al. [25] also studied this type of wheel-legged robots. For some wheel-legged robots, wheel structure can directly change into leg structure, which is totally different from the biological legs. For example, Kim et al. [26] designed a wheel-leg hybrid robot which utilizes a novel transformable wheel that combines the advantages of both circular and legged wheels. Tadakuma et al. [27] and Chen et al. [28] also have studied this type of robot.Although many robots with different wheel-legged structures have been designed and the movement performances have been analyzed, the wheel-legged robots still have the disadvantages of complex structure, difficult control, large space required for wheel-legged translation, and limited movement environment. This limits the practical application of the wheel-legged rescue robots. In order to solve the above problems, a new wheel-legged rescue robot is designed and the motion states are analyzed to provide a reference for motion control. Considering the wheel state and leg state share the same structure to contact with the ground, the elastic deformation of the wheel-legged structure is also analyzed. The experimental results prove the feasibility of the structural design and lay the foundation for further research on control methods.


## 2. Structure Design

### 2.1. Structure Design of Wheel-Legged Rescue Robot

The common series wheel-legged structure and similar parallel structure are shown in Figure1. In Figure 1(a), link A1B1 and link B1C1 are connected by hinge, and the wheels are added at the end of the leg. In Figure 1(b), links A1B1, B1D1, D1C1, and C1A1 consist of four-bar wheel-legged structure. In Figure 1, the solid line and dotted line represent the wheel state and leg state of the robot, respectively. It can be known from Figure 1 that the robot needs a large space when the motion state is converted between the wheel state and leg state, and this limits the application of rescue robot in narrow space.Figure 1
Common wheel-legged structures. (a) Series wheel-legged structure. (b) Four-bar wheel-legged structure.
(a)
(b)Considering the arc leg, which is a part of circle, also can make multilegged robot walk, the transformation process from wheel state to leg state is shown in Figure2. When the left half arc structure and the right half arc structure form a circle, the robot is in the wheel state. And when the left half arc structure rotates around the rotation axis and fits in the right half arc structure, the robot is in the leg state. This kind of wheel-legged structure is simpler than other wheel-legged structure, and the transformation process between wheel state and leg state takes up small space. In particular, when the motion process of the robot changes from wheel state to leg state, the rotational center needs to be raised. So the wheel-legged robot has three kinds of motion states: wheel state, rotation center lifting process, and leg state.Figure 2
Transformation process from wheel state to leg state. (a) Wheel state. (b) Transformation process. (c) Leg state.The drive schematic of wheel-legged structure is shown in Figure3. Motor 1 is fixedly connected with gear 1, and motor 2 is fixedly connected with gear 3. Gear 1 rotates under the drive of motor 1. Because gear 2 is engaged with gear 1, gear 2 is driven to rotate by gear 1. Gear 2 is connected with the fixing link through connecting plate, and the fixed link fixedly connected with the wheel. So the robot can realize the wheel movement by the driving of motor 1. Motor 2 is fixedly connected with gear 3, and gear 3 is engaged with the rack. At this time, the position of the rotation center can be lifted by the driving of motor 2. In particular, the fixed link and rack are fixed to the base plate. So when the robot is in the wheel state, the fixed link rotates, and the rack also rotates. At this time, gear 3 rotates inevitably. Motor 2 should match the motion of motor 1 when the robot is in wheel state. After the rotation center being lifted to specified location, the upper contact point contacts with the lower contact point. The circuit of the motor 3 is connected. Then the left half arc structure rotates by the driving of motor 3 until two half arc structures are fit together. When the rescue robot is in the leg state, the legs swing under the action of motor 1 and motor 2. The overall structure diagram of wheel-legged rescue robot is shown in Figure 4.Figure 3
Drive schematic of wheel-legged structure. (a) Main view of main structure. (b) Postview of main structure.
(a)
(b)Figure 4
Overall structure diagram of wheel-legged rescue robot. (a) Robot in wheel state. (b) Robot in leg state.
(a)
(b)


### 2.2. Application Range of Wheel-Legged Rescue Robot

One of the biggest characteristics of the wheel-legged robot with semicircle legs is that it can not only move on the rugged road (Figure5(a)), but also move in water (Figure 5(b)). This is what other wheel-legged robots, whether the series wheel-legged structure or similar parallel wheel-legged structure, do not have. When the wheel-legged robot moves on land in leg state, the wheel-legged structure can either turn clockwise or counterclockwise. And when the robot moves in the water, the wheel-legged structure can only turn counterclockwise. At this time, the wheel-legged structures are equivalent to the oars. This has greatly broadened the applications scope of robot.Figure 5
Movement environment of wheel-legged rescue robot. (a) Moving on rough terrain. (b) Moving in the water.
(a)
(b)


## 2.1. Structure Design of Wheel-Legged Rescue Robot

The common series wheel-legged structure and similar parallel structure are shown in Figure1. In Figure 1(a), link A1B1 and link B1C1 are connected by hinge, and the wheels are added at the end of the leg. In Figure 1(b), links A1B1, B1D1, D1C1, and C1A1 consist of four-bar wheel-legged structure. In Figure 1, the solid line and dotted line represent the wheel state and leg state of the robot, respectively. It can be known from Figure 1 that the robot needs a large space when the motion state is converted between the wheel state and leg state, and this limits the application of rescue robot in narrow space.Figure 1
Common wheel-legged structures. (a) Series wheel-legged structure. (b) Four-bar wheel-legged structure.
(a)
(b)Considering the arc leg, which is a part of circle, also can make multilegged robot walk, the transformation process from wheel state to leg state is shown in Figure2. When the left half arc structure and the right half arc structure form a circle, the robot is in the wheel state. And when the left half arc structure rotates around the rotation axis and fits in the right half arc structure, the robot is in the leg state. This kind of wheel-legged structure is simpler than other wheel-legged structure, and the transformation process between wheel state and leg state takes up small space. In particular, when the motion process of the robot changes from wheel state to leg state, the rotational center needs to be raised. So the wheel-legged robot has three kinds of motion states: wheel state, rotation center lifting process, and leg state.Figure 2
Transformation process from wheel state to leg state. (a) Wheel state. (b) Transformation process. (c) Leg state.The drive schematic of wheel-legged structure is shown in Figure3. Motor 1 is fixedly connected with gear 1, and motor 2 is fixedly connected with gear 3. Gear 1 rotates under the drive of motor 1. Because gear 2 is engaged with gear 1, gear 2 is driven to rotate by gear 1. Gear 2 is connected with the fixing link through connecting plate, and the fixed link fixedly connected with the wheel. So the robot can realize the wheel movement by the driving of motor 1. Motor 2 is fixedly connected with gear 3, and gear 3 is engaged with the rack. At this time, the position of the rotation center can be lifted by the driving of motor 2. In particular, the fixed link and rack are fixed to the base plate. So when the robot is in the wheel state, the fixed link rotates, and the rack also rotates. At this time, gear 3 rotates inevitably. Motor 2 should match the motion of motor 1 when the robot is in wheel state. After the rotation center being lifted to specified location, the upper contact point contacts with the lower contact point. The circuit of the motor 3 is connected. Then the left half arc structure rotates by the driving of motor 3 until two half arc structures are fit together. When the rescue robot is in the leg state, the legs swing under the action of motor 1 and motor 2. The overall structure diagram of wheel-legged rescue robot is shown in Figure 4.Figure 3
Drive schematic of wheel-legged structure. (a) Main view of main structure. (b) Postview of main structure.
(a)
(b)Figure 4
Overall structure diagram of wheel-legged rescue robot. (a) Robot in wheel state. (b) Robot in leg state.
(a)
(b)


## 2.2. Application Range of Wheel-Legged Rescue Robot

One of the biggest characteristics of the wheel-legged robot with semicircle legs is that it can not only move on the rugged road (Figure5(a)), but also move in water (Figure 5(b)). This is what other wheel-legged robots, whether the series wheel-legged structure or similar parallel wheel-legged structure, do not have. When the wheel-legged robot moves on land in leg state, the wheel-legged structure can either turn clockwise or counterclockwise. And when the robot moves in the water, the wheel-legged structure can only turn counterclockwise. At this time, the wheel-legged structures are equivalent to the oars. This has greatly broadened the applications scope of robot.Figure 5
Movement environment of wheel-legged rescue robot. (a) Moving on rough terrain. (b) Moving in the water.
(a)
(b)


## 3. Motion States Analysis

### 3.1. Wheel State

The rescue robot needs to overcome all kinds of obstacles, which include road resistance, which is caused by unevenness of the road surface and slope of the ground, and inertia resistance, which is caused by overcoming the inertia of the robot.Road resistance can be shown as [29](1)RR=Rf+Ri=μ1·mg+μ2·sin⁡θ·mg,where Rf is the rolling resistance, which is related to the type of road, the velocity, and the structure of the tire. μ1 is the rolling resistance coefficient. Ri is the slope resistance. θ is the angle of slope. μ2 is the slope resistance coefficient, and it is greater than 1.Inertia resistance includes the inertia force and inertia moment. The robot is composed of many parts, and the inertia force and inertia moment of each part are not the same. For easy calculation, the inertia resistance can be shown as(2)RI=μ3·ma,where m and a are the total mass and the acceleration of the center of mass, respectively. μ3 is the equivalent coefficient, and it is greater than 1. At this time, the resistance of the wheel-legged rescue robot in wheel state can be shown as(3)R=RR+RI.According to the structural characteristics, the torque of motor 1 can be shown as(4)M1=μ4·R·D2·i1i2,where D is the diameter of the wheel, i1 is the number of teeth of gear 1, and i2 is the number of teeth of gear 2. μ4 is the safety factor, and it is also greater than 1.When the rescue robot is in the wheel state, in addition to motor 1, motor 2 also should work at the same time. So the speed of the two motors should be matched. The rotation relationship between motor 1 and motor 2 can be shown in Figure6. If gear 3 does not rotate and only the rack rotates from position 1 to position 2, the relative position of gear and rack changes, which can lead to the rotation center of wheel-legged changes. At this time, the wheel turns into a “cam.” According to geometric relationship, the relationship between the speeds of the two motors can be expressed as(5)n3=n1·i1i2,where n1 is the speed of motor 1 and n3 is the speed of motor 3. The rotation directions of the two motors are the same.Figure 6
Rotation relationship between motor 1 and motor 2.


### 3.2. Rotation Center Changing Process

The rotation center can be changed under the action of motor 2, and it is also the change process of movement state between wheel state and leg state. When the trunk is lifted, the torque can be shown as(6)Mt2=μ5·14mg·rg3,where m is the mass of robot; rg3 is the radius of gear 3. μ5 is the safety factor, and it is greater than 1. When the trunk moves downwards, motor 2 plays a limiting role. Besides, when the left half arc structure rotates, motor 3 is mainly to overcome the inertia resistance, and the torque of the motor 3 can be calculated according to (3).


### 3.3. Leg State

There are two walking ways when the robot is in wheel state: arcuate part of the wheel-legged structure touches the ground first and endpoint of the wheel-legged structure touches the ground first. For the former, the motion sequence can be shown in Figure7(a). When the robot walks on the horizontal ground, the midpoint of the semicircle arc lands first, and then the structure rotates clockwise until the end point contacts with the ground. This movement mode is suitable for the robot to move on a relatively flat ground, and it has the advantage of high efficiency. For the latter, the motion sequence can be shown in Figure 7(b). The endpoint of the semicircle arc lands first, and then the structure rotates around the landing point until the diameter is perpendicular to the ground. This movement mode is suitable for the stepped road because the endpoint of the semicircle arc is not easy to slide.Figure 7
Walking ways of the rescue robot. (a) Arcuate part of the wheel-legged structure lands first. (b) Endpoint of the wheel-legged structure lands first.
(a)
(b)In order to analyze the driving torque of the wheel-legged structure when the robot is in the walking process, force analysis should be conducted. For the first walking way, the moment balance equation is(7)M+FS1×dS1+mlg×dS2+Fc1×dc1+Mc1=0,where M is the driving torque, FS1 is the force of the trunk to the leg, and ml is the mass of the wheel-legged structure. Fc1 and Mc1are inertia force and inertia moment, respectively. d is the vector from the point of force to the contact point between the wheel-legged structure and the ground. To simplify the calculation process, consider the speed of the leg in the swing phase is large and the speed of the leg in support phase is small, regardless of the inertia force and inertia moment. And safety factor can be introduced. According to the geometric relationship, (7) can be simplified as(8)M=μ6FS1·rcos⁡α+mlg·lS1·cos⁡π2-β,where lS1=r2-2cos⁡α; β=sinα/2-2cosα. r is the radius of the wheel-legged structure, and α is rotation angle of leg. μ6 is the safety factor.For the second walking way, the moment balance equation is the same as (7). In particular, gravity always does negative work for the first walking way, and gravity does positive work and then does negative work for the second walking way. The driving torque of the robot with the second walking way can be shown as(9)M=FS1·2rcos⁡α+msg·2r·sin⁡π4-α.The initial angle can be expressed as(10)α0=arcsin⁡hr,where h is the height of step. Suppose the mass of trunk of robot is 40 Kg, ml = 0.5 Kg, h = 0.1 m, and r = 0.2 m. The variation law of driving force is shown in Figure 8. Horizontal axis represents the rotation angle, and vertical coordinate represents torque. It can be known from Figure 8 that average torque of the robot in the second walking way is greater than average torque in the first walking way.Figure 8
Variation law of driving torque in leg state.After knowing the driving torque, the motion speed of the robot also can be obtained. For the first walking way, the relationship between motor speed and motion speed of robot is(11)vx=rθ˙sin⁡θ+rvy=rθ˙cos⁡θ.For the second walking way, the relationship between motor speed and motion speed of robot can be shown as(12)vx=2rθ˙sin⁡θvy=2rθ˙cos⁡θ.When the speed of motor is 1 rad/s, the relationship between the rotation angle of the wheel-legged structure and the speed of the robot can be shown in Figure9. In the leg state, the robot has both the speed along the horizontal direction and the speed along the vertical direction. When the robot moves in the second walking way, the speed along the vertical direction is greater, and this also shows that the robot is more suitable for ladder-type pavement with the second walking way.Figure 9
Variation law of speed in leg state.Based on the analysis results of the wheel state, rotation center changing process, and leg state, motion law of wheel-legged structure and motor torques can be obtained. In different motion states, the required motor torque is also different. After a comprehensive consideration, the model of motor 1 and motor 2 is maxon RE35, and the rated torque is 2.5 Nm. The model of motor 3 is GA12YN20, and the rated torque is 0.7 Nm.In particular, when the robot is in leg state, it also can move in the water. At this time, each leg is affected by the force of water on it. The force balance equation can be shown as(13)Fd+Fcd+Ft=0ld⊥×Fd+Mcd+Md=0,where Md is motor torque, Mcd and Fcd are inertia force and inertia moment, respectively, Fd is the force of water on wheel-legged structure, Ft is the force of trunk on wheel-legged structure, and ld⊥ is acting arm. For the wheel-legged rescue robot, it suffers friction, pressure difference resistance, wave resistance, and air resistance. Because the velocity is not great, the friction of water and air resistance is very small. The pressure difference resistance is proportional to the square of the velocity of robot. The wave resistance is introduced due to the wave of water. In order to simplify the calculation, it can be considered proportional to the speed of the robot. The force balance equation of robot can be written as(14)md1+md2dvddt=-avd-kvd2+Fd,where md1 is the mass of robot, md2 is the mass of load, and vd is the velocity of robot. a and k are coefficients of wave resistance and pressure difference resistance, respectively. Fd is the force of the water to the robot. The calculation method of Fd is different when the underwater environment is different. For example, the wave force in the regular wave can be written as [30](15)Fd=ρV1+K33ωeωω2k1e-ω2/gHζaeiωet,where ρ is the density of water, V is the drainage volume, and K33 is the vertical and longitudinal additional mass coefficients. ωe and ω are encounter frequency and wave circle frequency, respectively. k1 is reduction coefficient, which represents the influence of the ratio of the length of the underwater robot and the effective wavelength on the wave force. ζa is amplitude of regular wave.


## 3.1. Wheel State

The rescue robot needs to overcome all kinds of obstacles, which include road resistance, which is caused by unevenness of the road surface and slope of the ground, and inertia resistance, which is caused by overcoming the inertia of the robot.Road resistance can be shown as [29](1)RR=Rf+Ri=μ1·mg+μ2·sin⁡θ·mg,where Rf is the rolling resistance, which is related to the type of road, the velocity, and the structure of the tire. μ1 is the rolling resistance coefficient. Ri is the slope resistance. θ is the angle of slope. μ2 is the slope resistance coefficient, and it is greater than 1.Inertia resistance includes the inertia force and inertia moment. The robot is composed of many parts, and the inertia force and inertia moment of each part are not the same. For easy calculation, the inertia resistance can be shown as(2)RI=μ3·ma,where m and a are the total mass and the acceleration of the center of mass, respectively. μ3 is the equivalent coefficient, and it is greater than 1. At this time, the resistance of the wheel-legged rescue robot in wheel state can be shown as(3)R=RR+RI.According to the structural characteristics, the torque of motor 1 can be shown as(4)M1=μ4·R·D2·i1i2,where D is the diameter of the wheel, i1 is the number of teeth of gear 1, and i2 is the number of teeth of gear 2. μ4 is the safety factor, and it is also greater than 1.When the rescue robot is in the wheel state, in addition to motor 1, motor 2 also should work at the same time. So the speed of the two motors should be matched. The rotation relationship between motor 1 and motor 2 can be shown in Figure6. If gear 3 does not rotate and only the rack rotates from position 1 to position 2, the relative position of gear and rack changes, which can lead to the rotation center of wheel-legged changes. At this time, the wheel turns into a “cam.” According to geometric relationship, the relationship between the speeds of the two motors can be expressed as(5)n3=n1·i1i2,where n1 is the speed of motor 1 and n3 is the speed of motor 3. The rotation directions of the two motors are the same.Figure 6
Rotation relationship between motor 1 and motor 2.


## 3.2. Rotation Center Changing Process

The rotation center can be changed under the action of motor 2, and it is also the change process of movement state between wheel state and leg state. When the trunk is lifted, the torque can be shown as(6)Mt2=μ5·14mg·rg3,where m is the mass of robot; rg3 is the radius of gear 3. μ5 is the safety factor, and it is greater than 1. When the trunk moves downwards, motor 2 plays a limiting role. Besides, when the left half arc structure rotates, motor 3 is mainly to overcome the inertia resistance, and the torque of the motor 3 can be calculated according to (3).


## 3.3. Leg State

There are two walking ways when the robot is in wheel state: arcuate part of the wheel-legged structure touches the ground first and endpoint of the wheel-legged structure touches the ground first. For the former, the motion sequence can be shown in Figure7(a). When the robot walks on the horizontal ground, the midpoint of the semicircle arc lands first, and then the structure rotates clockwise until the end point contacts with the ground. This movement mode is suitable for the robot to move on a relatively flat ground, and it has the advantage of high efficiency. For the latter, the motion sequence can be shown in Figure 7(b). The endpoint of the semicircle arc lands first, and then the structure rotates around the landing point until the diameter is perpendicular to the ground. This movement mode is suitable for the stepped road because the endpoint of the semicircle arc is not easy to slide.Figure 7
Walking ways of the rescue robot. (a) Arcuate part of the wheel-legged structure lands first. (b) Endpoint of the wheel-legged structure lands first.
(a)
(b)In order to analyze the driving torque of the wheel-legged structure when the robot is in the walking process, force analysis should be conducted. For the first walking way, the moment balance equation is(7)M+FS1×dS1+mlg×dS2+Fc1×dc1+Mc1=0,where M is the driving torque, FS1 is the force of the trunk to the leg, and ml is the mass of the wheel-legged structure. Fc1 and Mc1are inertia force and inertia moment, respectively. d is the vector from the point of force to the contact point between the wheel-legged structure and the ground. To simplify the calculation process, consider the speed of the leg in the swing phase is large and the speed of the leg in support phase is small, regardless of the inertia force and inertia moment. And safety factor can be introduced. According to the geometric relationship, (7) can be simplified as(8)M=μ6FS1·rcos⁡α+mlg·lS1·cos⁡π2-β,where lS1=r2-2cos⁡α; β=sinα/2-2cosα. r is the radius of the wheel-legged structure, and α is rotation angle of leg. μ6 is the safety factor.For the second walking way, the moment balance equation is the same as (7). In particular, gravity always does negative work for the first walking way, and gravity does positive work and then does negative work for the second walking way. The driving torque of the robot with the second walking way can be shown as(9)M=FS1·2rcos⁡α+msg·2r·sin⁡π4-α.The initial angle can be expressed as(10)α0=arcsin⁡hr,where h is the height of step. Suppose the mass of trunk of robot is 40 Kg, ml = 0.5 Kg, h = 0.1 m, and r = 0.2 m. The variation law of driving force is shown in Figure 8. Horizontal axis represents the rotation angle, and vertical coordinate represents torque. It can be known from Figure 8 that average torque of the robot in the second walking way is greater than average torque in the first walking way.Figure 8
Variation law of driving torque in leg state.After knowing the driving torque, the motion speed of the robot also can be obtained. For the first walking way, the relationship between motor speed and motion speed of robot is(11)vx=rθ˙sin⁡θ+rvy=rθ˙cos⁡θ.For the second walking way, the relationship between motor speed and motion speed of robot can be shown as(12)vx=2rθ˙sin⁡θvy=2rθ˙cos⁡θ.When the speed of motor is 1 rad/s, the relationship between the rotation angle of the wheel-legged structure and the speed of the robot can be shown in Figure9. In the leg state, the robot has both the speed along the horizontal direction and the speed along the vertical direction. When the robot moves in the second walking way, the speed along the vertical direction is greater, and this also shows that the robot is more suitable for ladder-type pavement with the second walking way.Figure 9
Variation law of speed in leg state.Based on the analysis results of the wheel state, rotation center changing process, and leg state, motion law of wheel-legged structure and motor torques can be obtained. In different motion states, the required motor torque is also different. After a comprehensive consideration, the model of motor 1 and motor 2 is maxon RE35, and the rated torque is 2.5 Nm. The model of motor 3 is GA12YN20, and the rated torque is 0.7 Nm.In particular, when the robot is in leg state, it also can move in the water. At this time, each leg is affected by the force of water on it. The force balance equation can be shown as(13)Fd+Fcd+Ft=0ld⊥×Fd+Mcd+Md=0,where Md is motor torque, Mcd and Fcd are inertia force and inertia moment, respectively, Fd is the force of water on wheel-legged structure, Ft is the force of trunk on wheel-legged structure, and ld⊥ is acting arm. For the wheel-legged rescue robot, it suffers friction, pressure difference resistance, wave resistance, and air resistance. Because the velocity is not great, the friction of water and air resistance is very small. The pressure difference resistance is proportional to the square of the velocity of robot. The wave resistance is introduced due to the wave of water. In order to simplify the calculation, it can be considered proportional to the speed of the robot. The force balance equation of robot can be written as(14)md1+md2dvddt=-avd-kvd2+Fd,where md1 is the mass of robot, md2 is the mass of load, and vd is the velocity of robot. a and k are coefficients of wave resistance and pressure difference resistance, respectively. Fd is the force of the water to the robot. The calculation method of Fd is different when the underwater environment is different. For example, the wave force in the regular wave can be written as [30](15)Fd=ρV1+K33ωeωω2k1e-ω2/gHζaeiωet,where ρ is the density of water, V is the drainage volume, and K33 is the vertical and longitudinal additional mass coefficients. ωe and ω are encounter frequency and wave circle frequency, respectively. k1 is reduction coefficient, which represents the influence of the ratio of the length of the underwater robot and the effective wavelength on the wave force. ζa is amplitude of regular wave.


## 4. Structural Stiffness Analysis

Because the disaster environment is very complex, the rescue robot should have good buffering performance. Otherwise, whether the robot is in the wheel state or in the leg state, the wheel-legged structures of the robot may have rigid collision with the ground frequently and further lead to a series of problems. Considering the wheel state and leg state share the same structure to contact with the ground, the effect of structural stiffness of wheel-legged structure in wheel state and leg state on motion performance is analyzed.


### 4.1. Structural Stiffness in Wheel State

The wheel should be elastic wheel, which means that hub should be able to achieve deformation under external force. In addition to the elastic deformation of the wheel, the tire can also achieve elastic deformation, so the motion of the robot on the rough road surface can be simplified to a two-DOF vibration system in the vertical direction.According to Lagrange equation, motion equations of equivalent vibration system can be expressed as [31, 32](16)m2z¨2=kz1-z2+cz˙1-z˙2m1z¨1=cz˙2-z˙1+kz2-z1-ktz1-q,where z1 and z2 are vertical displacement of wheel and body, m2 is the mass of robot, k is the equivalent stiffness coefficient of wheel, c is the damping of wheel, m1 is the mass of wheel, and kt is the equivalent stiffness coefficient of tyre. q is the input of road roughness, and it is harmonic exciting force. The output can be written as z1=z10eiωt+φ and z2=z20eiωt+φ. Inserting them into (16), it can be written as(17)z2-ω2m2+iωc+k=z1iωc+kz1-ω2m1+iωc+k+kt=z2iωc+k+qkt.At this time, the frequency response function can be shown as(18)z2z1=iωc+k-ω2m2+iωc+kz1q=A2ktA3A2-A12z2q=z2z1·z1q=A1ktA3A2-A12,where A1=iωc+k; A2=-ω2m2+iωc+k; A3=-ω2m1+iωc+k+kt. The amplitude frequency characteristics of the robot relative to road surface are obtained:(19)z2q=γ1-λ22+2ξλ2Δ,where Δ=1-λ21+γ-λ2/μ2-1+2λξ2γ-1/μ+1λ22. λ is the frequency ratio, μ is mass ratio of body and wheel, and ξ is damping ratio. According to the calculation results of the three-dimensional software (Solidworks), m1 = 0.5 Kg, m2 = 40 Kg. According to the vibration model of the car, kt = 200000 N/m [33]. The amplitude frequency characteristics of robot body with different k can be shown in Figure 10(a). As can be seen from Figure 10(a), the reduction of the spring stiffness coefficient can effectively reduce the resonance peak. But the increase of the spring stiffness coefficient can shock absorption. Amplitude frequency characteristics of body acceleration to road surface velocity can be written as(20)z¨2q˙=z2ω2qω=ωz2q.Figure 10
Amplitude frequency characteristics of equivalent vibration system. (a) Amplitude frequency characteristics of displacement input and displacement output. (b) Amplitude frequency characteristics of body acceleration to road surface velocity. (c) Amplitude frequency characteristics of relative dynamic load on road surface velocity.
(a)
(b)
(c)The amplitude frequency characteristics of relative dynamic load on road surface velocity can be shown as(21)FdGq˙=m2z¨2m2gq˙=1gz¨2q˙.The amplitude frequency characteristics of body acceleration to road surface velocity and relative dynamic load on road surface velocity can be shown in Figures10(b) and 10(c), respectively. The trends are almost the same. In low-frequency section and resonance section, the bigger k is, the better the ride comfort is. And in high frequency section, the smaller k is, the better the ride comfort is.It can be known from Figure10 that the decrease of stiffness coefficient can effectively reduce the resonance peak. But it may reduce shock absorption effect. Besides, the smaller stiffness may produce greater friction because the wheel deformation can make the contact of the wheel with the ground change from point contact to line contact.


### 4.2. Structural Stiffness in Leg State

When the rescue robot is in leg state, the buffering performance is also important. The arc leg is a compliant mechanism, and it is hard to analyze the buffering performance because the arc leg introduces geometric nonlinearities. The pseudo-rigid-body model used in this study can simplify large-deflection analysis [34–36]. For the first walking way (the midpoint of the arc leg lands first), the leg structure which plays a role in buffering can be considered to be 1/4 circles. At this time, the 2R model is used, and the pseudo-rigid-body model is shown in Figure 11(a). The equivalent rotation pair at AL2 is RL11, and equivalent rotation pair at AL3 is RL21. AL1 is the connection point between the trunk and the leg, and AL3 is the landing point. So the arc leg can be equivalent to 2-DOF serial mechanism, and torsion spring is used in each rotation pair. The coordinate origin of the fixed coordinate system o0-x0y0 coincides with the landing point. The direction of the x0-axis is horizontal to the right, and the direction of the y0-axis is perpendicular to the ground and is upward.Figure 11
Pseudo-rigid-body model of arc leg. (a) First walking way. (b) Second walking way.
(a)
(b)Suppose the trunk moves only in the vertical direction. The coordinate ofAL1 is (-R, R-h1). In triangle AL1AL2AL3, the length of AL1AL3 can be shown as (22)s=R-h12+R2.The rotation angles of linkAL1AL2 relative to link AL2AL3 can be shown as(23)γ1=π-arccos⁡l112+l212-s22·l11·l21-γ10.The rotation angles of linkAL2AL3 relative to horizontal direction can be written as(24)γ2=arctan⁡R-h1R-arccos⁡l212+s2-l1122·l21·s-γ20,where h1 is the trunk movement distance, R is the radius of wheel-legged structure, and l11 and l21 are the length of link AL1AL2 and link AL2AL3. γ10 and γ20 are initial angles. In order to obtain the mechanical properties of buffering process, the force analysis also can be conducted. The force and torque balance equation of each link can be shown as(25)Fi-Fi+1+Fci+mig=0(26)Mi-Mi+1-ri+1×Fi+1+ri×Fi+rci×Fci+mig=0,where r is the vector of the coordinate system origin to the point of force. Fi and Mi are the force and moment of link li-1 to li, and Fi+1 and Mi+1 are the force and moment of link li+1 to li. Fci and Mci are the inertia force and inertia moment, respectively. When i=2 or 3, Mi represents the torque generated by the torsion springs. When i=3, F3 represents the force of the ground to the leg. To simplify the calculation process, regardless of the mass of the legs, the mass of the robot remains concentrated in the trunk. Spring damping is also not considered. At this time, the support force of the ground to the wheel-legged structure can be written as(27)FxFy=-l1·sin⁡γ1l1·cos⁡γ1l2·sin⁡γ2l2·cos⁡γ2-1M1-M2M2+M3,where M2=k11·γ11, M3=k21·γ21. ki1 is the torsional stiffness coefficient.For the second walking way, the pseudo-rigid-body model is shown in Figure11(b). The equivalent rotation pairs at BL2, BL3, and BL4 are RL12, RL22, and RL32, respectively. For the 1/4 circles, it is still the 2-DOF serial mechanism. In particular, considering the complexity of the environment, the end point of the leg is likely to fall into the soft soil or crevice. So BL4 can be seen as fixed point. The attitude of link BL1BL2 is unchanged in buffering process.In triangleBL2BL3BL4, the length of BL2BL4 can be shown as(28)s=T12+T22,where T1=l4·sin⁡γ40-l1·sinγ10-h-h1; T2=2R·cosφ-l4·cosγ40-l1·cosγ10. li is the length of BLiBLi+1. θ10 is the angle between link BL1BL2 and x0-axis, and θ40 is the angle between link BL4BL5 and x0-axis. φ is the initial inclination angle of wheel-legged structure.At this time, the rotation angles of linkl(i-1)1 relative to link li1 can be shown as(29)γ2=π-arccos⁡l222+l322-s22·l22·l32-γ20(30)γ3=π-arccos⁡l322+s2-l2222·l32·s+arctan⁡T2T1+π2-θ40-γ30(31)γ1=arccos⁡l122+l222-ss22·l12·l22-γ10,where (32)ss=l4·sinθ40+l3·sinθ3+h+h12+2R·cosφ-l4·cosθ40-l3·cosθ32.θ3 is the angle between link BL3BL4 and x0 axis.According to (25)-(26), the support force of the ground to the leg can be obtained.In order to analyze the mechanical properties, the stiffness coefficient of equivalent torsion springs should be further determined. When the external forces the wheel-legged structure suffers are the same and the deformation is also the same, the relationship between equivalent torsion spring stiffness coefficient and equivalent stiffness coefficient of leg can be determined according to experiment.If the landing ground is rigid,BL4 can be seen as fixed point. It can be simplified as a revolute pair. So pseudo-rigid-body model has four DOF. At this time, the kinematics can be analyzed according to the same method. Because the equivalent model has four DOF and only 3 constraints can be contained, including the position and posture of end link, the angle of each link cannot be determined directly, and kinematic relationship can be written as(33)γ1γ2γ3=fiγ4.Equation (33) shows that γ1, γ2, and γ3 can be expressed with γ4. In order to further solve γ4, the force balance equation can be added according to (25)-(26). Considering kinematics and dynamics equations synthetically, the equations can be simplified as(34)fγ4=0.Thenγ4 can be obtained, and other unknown numbers also can be obtained. Suppose R = 0.1 m. The relationship between h and k can be shown in Figure 12. It can be known from Figure 12 that the torsional spring coefficient decreases with the increase of deformation.Figure 12
Relationship betweenh and k1.The forces of the wheel-legged structure to the trunk of the robot with different maximum buffer distance can be shown in Figure13. Figures 13(a) and 13(b) show the force along x0-axis and y0-axis with the first walking way, and Figures 13(c) and 13(d) show the force along x0-axis and y0-axis with the second walking way. It can be known from Figure 13 that the force the trunk suffers gradually increased with the increase of deformation of wheel-legged structure. At the same time, larger torsional spring coefficients correspond to greater forces. For the different walking way, the force the trunk suffers along x0-axis is larger with the second walking way, but the force the trunk suffers along y0-axis is smaller with the second walking way.Figure 13
Support force of the ground to the leg. (a) Support force alongx0-axis with the first walking way. (b) Support force along y0-axis with the first walking way. (c) Support force along x0-axis with the second walking way. (d) Support force along y0-axis with the second walking way.
(a)
(b)
(c)
(d)It can be known from the above analysis that smaller stiffness of the wheel-legged structure can make the change trend of the force the trunk suffers more stable in leg state, but it will require the larger torque of the drive motor in the same case because the motor also needs to overcome the deformation. Besides, small stiffness will increase the deformation of the structure. Considering the effect of stiffness on the motion performance when the robot is in wheel state and leg state, the structural stiffness should be considered synthetically.


## 4.1. Structural Stiffness in Wheel State

The wheel should be elastic wheel, which means that hub should be able to achieve deformation under external force. In addition to the elastic deformation of the wheel, the tire can also achieve elastic deformation, so the motion of the robot on the rough road surface can be simplified to a two-DOF vibration system in the vertical direction.According to Lagrange equation, motion equations of equivalent vibration system can be expressed as [31, 32](16)m2z¨2=kz1-z2+cz˙1-z˙2m1z¨1=cz˙2-z˙1+kz2-z1-ktz1-q,where z1 and z2 are vertical displacement of wheel and body, m2 is the mass of robot, k is the equivalent stiffness coefficient of wheel, c is the damping of wheel, m1 is the mass of wheel, and kt is the equivalent stiffness coefficient of tyre. q is the input of road roughness, and it is harmonic exciting force. The output can be written as z1=z10eiωt+φ and z2=z20eiωt+φ. Inserting them into (16), it can be written as(17)z2-ω2m2+iωc+k=z1iωc+kz1-ω2m1+iωc+k+kt=z2iωc+k+qkt.At this time, the frequency response function can be shown as(18)z2z1=iωc+k-ω2m2+iωc+kz1q=A2ktA3A2-A12z2q=z2z1·z1q=A1ktA3A2-A12,where A1=iωc+k; A2=-ω2m2+iωc+k; A3=-ω2m1+iωc+k+kt. The amplitude frequency characteristics of the robot relative to road surface are obtained:(19)z2q=γ1-λ22+2ξλ2Δ,where Δ=1-λ21+γ-λ2/μ2-1+2λξ2γ-1/μ+1λ22. λ is the frequency ratio, μ is mass ratio of body and wheel, and ξ is damping ratio. According to the calculation results of the three-dimensional software (Solidworks), m1 = 0.5 Kg, m2 = 40 Kg. According to the vibration model of the car, kt = 200000 N/m [33]. The amplitude frequency characteristics of robot body with different k can be shown in Figure 10(a). As can be seen from Figure 10(a), the reduction of the spring stiffness coefficient can effectively reduce the resonance peak. But the increase of the spring stiffness coefficient can shock absorption. Amplitude frequency characteristics of body acceleration to road surface velocity can be written as(20)z¨2q˙=z2ω2qω=ωz2q.Figure 10
Amplitude frequency characteristics of equivalent vibration system. (a) Amplitude frequency characteristics of displacement input and displacement output. (b) Amplitude frequency characteristics of body acceleration to road surface velocity. (c) Amplitude frequency characteristics of relative dynamic load on road surface velocity.
(a)
(b)
(c)The amplitude frequency characteristics of relative dynamic load on road surface velocity can be shown as(21)FdGq˙=m2z¨2m2gq˙=1gz¨2q˙.The amplitude frequency characteristics of body acceleration to road surface velocity and relative dynamic load on road surface velocity can be shown in Figures10(b) and 10(c), respectively. The trends are almost the same. In low-frequency section and resonance section, the bigger k is, the better the ride comfort is. And in high frequency section, the smaller k is, the better the ride comfort is.It can be known from Figure10 that the decrease of stiffness coefficient can effectively reduce the resonance peak. But it may reduce shock absorption effect. Besides, the smaller stiffness may produce greater friction because the wheel deformation can make the contact of the wheel with the ground change from point contact to line contact.


## 4.2. Structural Stiffness in Leg State

When the rescue robot is in leg state, the buffering performance is also important. The arc leg is a compliant mechanism, and it is hard to analyze the buffering performance because the arc leg introduces geometric nonlinearities. The pseudo-rigid-body model used in this study can simplify large-deflection analysis [34–36]. For the first walking way (the midpoint of the arc leg lands first), the leg structure which plays a role in buffering can be considered to be 1/4 circles. At this time, the 2R model is used, and the pseudo-rigid-body model is shown in Figure 11(a). The equivalent rotation pair at AL2 is RL11, and equivalent rotation pair at AL3 is RL21. AL1 is the connection point between the trunk and the leg, and AL3 is the landing point. So the arc leg can be equivalent to 2-DOF serial mechanism, and torsion spring is used in each rotation pair. The coordinate origin of the fixed coordinate system o0-x0y0 coincides with the landing point. The direction of the x0-axis is horizontal to the right, and the direction of the y0-axis is perpendicular to the ground and is upward.Figure 11
Pseudo-rigid-body model of arc leg. (a) First walking way. (b) Second walking way.
(a)
(b)Suppose the trunk moves only in the vertical direction. The coordinate ofAL1 is (-R, R-h1). In triangle AL1AL2AL3, the length of AL1AL3 can be shown as (22)s=R-h12+R2.The rotation angles of linkAL1AL2 relative to link AL2AL3 can be shown as(23)γ1=π-arccos⁡l112+l212-s22·l11·l21-γ10.The rotation angles of linkAL2AL3 relative to horizontal direction can be written as(24)γ2=arctan⁡R-h1R-arccos⁡l212+s2-l1122·l21·s-γ20,where h1 is the trunk movement distance, R is the radius of wheel-legged structure, and l11 and l21 are the length of link AL1AL2 and link AL2AL3. γ10 and γ20 are initial angles. In order to obtain the mechanical properties of buffering process, the force analysis also can be conducted. The force and torque balance equation of each link can be shown as(25)Fi-Fi+1+Fci+mig=0(26)Mi-Mi+1-ri+1×Fi+1+ri×Fi+rci×Fci+mig=0,where r is the vector of the coordinate system origin to the point of force. Fi and Mi are the force and moment of link li-1 to li, and Fi+1 and Mi+1 are the force and moment of link li+1 to li. Fci and Mci are the inertia force and inertia moment, respectively. When i=2 or 3, Mi represents the torque generated by the torsion springs. When i=3, F3 represents the force of the ground to the leg. To simplify the calculation process, regardless of the mass of the legs, the mass of the robot remains concentrated in the trunk. Spring damping is also not considered. At this time, the support force of the ground to the wheel-legged structure can be written as(27)FxFy=-l1·sin⁡γ1l1·cos⁡γ1l2·sin⁡γ2l2·cos⁡γ2-1M1-M2M2+M3,where M2=k11·γ11, M3=k21·γ21. ki1 is the torsional stiffness coefficient.For the second walking way, the pseudo-rigid-body model is shown in Figure11(b). The equivalent rotation pairs at BL2, BL3, and BL4 are RL12, RL22, and RL32, respectively. For the 1/4 circles, it is still the 2-DOF serial mechanism. In particular, considering the complexity of the environment, the end point of the leg is likely to fall into the soft soil or crevice. So BL4 can be seen as fixed point. The attitude of link BL1BL2 is unchanged in buffering process.In triangleBL2BL3BL4, the length of BL2BL4 can be shown as(28)s=T12+T22,where T1=l4·sin⁡γ40-l1·sinγ10-h-h1; T2=2R·cosφ-l4·cosγ40-l1·cosγ10. li is the length of BLiBLi+1. θ10 is the angle between link BL1BL2 and x0-axis, and θ40 is the angle between link BL4BL5 and x0-axis. φ is the initial inclination angle of wheel-legged structure.At this time, the rotation angles of linkl(i-1)1 relative to link li1 can be shown as(29)γ2=π-arccos⁡l222+l322-s22·l22·l32-γ20(30)γ3=π-arccos⁡l322+s2-l2222·l32·s+arctan⁡T2T1+π2-θ40-γ30(31)γ1=arccos⁡l122+l222-ss22·l12·l22-γ10,where (32)ss=l4·sinθ40+l3·sinθ3+h+h12+2R·cosφ-l4·cosθ40-l3·cosθ32.θ3 is the angle between link BL3BL4 and x0 axis.According to (25)-(26), the support force of the ground to the leg can be obtained.In order to analyze the mechanical properties, the stiffness coefficient of equivalent torsion springs should be further determined. When the external forces the wheel-legged structure suffers are the same and the deformation is also the same, the relationship between equivalent torsion spring stiffness coefficient and equivalent stiffness coefficient of leg can be determined according to experiment.If the landing ground is rigid,BL4 can be seen as fixed point. It can be simplified as a revolute pair. So pseudo-rigid-body model has four DOF. At this time, the kinematics can be analyzed according to the same method. Because the equivalent model has four DOF and only 3 constraints can be contained, including the position and posture of end link, the angle of each link cannot be determined directly, and kinematic relationship can be written as(33)γ1γ2γ3=fiγ4.Equation (33) shows that γ1, γ2, and γ3 can be expressed with γ4. In order to further solve γ4, the force balance equation can be added according to (25)-(26). Considering kinematics and dynamics equations synthetically, the equations can be simplified as(34)fγ4=0.Thenγ4 can be obtained, and other unknown numbers also can be obtained. Suppose R = 0.1 m. The relationship between h and k can be shown in Figure 12. It can be known from Figure 12 that the torsional spring coefficient decreases with the increase of deformation.Figure 12
Relationship betweenh and k1.The forces of the wheel-legged structure to the trunk of the robot with different maximum buffer distance can be shown in Figure13. Figures 13(a) and 13(b) show the force along x0-axis and y0-axis with the first walking way, and Figures 13(c) and 13(d) show the force along x0-axis and y0-axis with the second walking way. It can be known from Figure 13 that the force the trunk suffers gradually increased with the increase of deformation of wheel-legged structure. At the same time, larger torsional spring coefficients correspond to greater forces. For the different walking way, the force the trunk suffers along x0-axis is larger with the second walking way, but the force the trunk suffers along y0-axis is smaller with the second walking way.Figure 13
Support force of the ground to the leg. (a) Support force alongx0-axis with the first walking way. (b) Support force along y0-axis with the first walking way. (c) Support force along x0-axis with the second walking way. (d) Support force along y0-axis with the second walking way.
(a)
(b)
(c)
(d)It can be known from the above analysis that smaller stiffness of the wheel-legged structure can make the change trend of the force the trunk suffers more stable in leg state, but it will require the larger torque of the drive motor in the same case because the motor also needs to overcome the deformation. Besides, small stiffness will increase the deformation of the structure. Considering the effect of stiffness on the motion performance when the robot is in wheel state and leg state, the structural stiffness should be considered synthetically.


## 5. Experiments

The control flow chart is seen in Figure14. When the leg state is needed for the robot, the current state should be determined. If the robot is already in the leg state, the terrain conditions should be determined, and the two different gates can be chosen. On the contrary, if the robot is in the wheel state, motor 2 works to make the trunk lifted. When the trunk is lifted to the specified position, motor 3 works to make the left half arc structure of the wheel rotate. At this time, the motion state of the robot changes. When the wheel state is needed for the robot and the robot is already in the wheel state, motor 1 and motor 2 work together, and the robot moves forward. When it encounters obstacles, the motion state can be changed from wheel state to leg state. When the wheel state is needed but the robot is in the leg state, the motor works to make the left half arc structure of the wheel rotate, and when the leg structure changes to the wheel structure, motor 2 works to make the center of rotation from the eccentric position to the wheel center. According to the above control method, the robot can realize the conversion of the leg state and wheel state.Figure 14
Control flow chart.The wheel-legged rescue robot is shown in Figure15. The control hardware is located on the trunk of the robot. Attitude conversion process from wheel state to leg state is shown in Figure 16. First, the trunk of the robot is lifted with the driving of the motor. Then the right half arc structure rotates by the driving of motor 3 until it fits with the left half arc structure. At this time, the rescue robot is in the leg state.Figure 15
Wheel-legged rescue robot.Figure 16
Conversion process from wheel state to leg state.The robot can achieve different leg movement states according to the different terrain environment. When the robot walks on a rough road, the gait is shown in Figure17. In the walking process, the two wheel-legged structures which are in a diagonal position move simultaneously. And there are two wheel-legged structures in the support phase, the other two wheel-legged structures in the swing phase. This kind of gait makes the robot move fast, but it cannot get over the high obstacles.Figure 17
Gait 1 of the robot (walk on rough road).
(a)
Gait sequence diagram
(b)
Motion diagram of the robotWhen the robot encounters a high barrier to climb, the gait is shown in Figure18. The height of the obstacle is 15 cm. First, two wheel-legged structures which are in front of the robot are on the edge of the obstacle in turn. Then the robot climbs the obstacle with the driving of motor 1 and motor 2. In particular, the height of the obstruction cannot be higher than the diameter of the wheel. The robot may move slowly with this kind of gait, but the obstacles it can climb can be higher than gait 1.Figure 18
Gait 2 of the robot (overcoming a barrier).
(a)
Gait sequence diagram
(b)
Motion diagram of the robotIn addition, because the wheels are elastic, the robot can reduce the vibration and impact in the rugged environment, and the robot can achieve a smooth movement. Therefore, the robot has good performance and can adapt to the complex and changeable postdisaster environment.


## 6. Discussion

A new wheel-legged rescue robot is designed in this paper. For the mechanical structure, the wheel of the robot can rotate 180° around the vertical axis and turn into a semicircular structure. Because it does not require any space other than the space occupied by the robot with wheel state during the state change process, it has the advantage of small occupation space. Moreover, compared with the series leg structure and similar parallel leg structure, the structure of semicircle arc leg is simpler and easier to control. This provides a new idea for the design of wheel-legged robot. For the movement state analysis, it provides a reference for motors selection and control. For the structural stiffness analysis, considering the wheel state and leg state share the same structure to contact with the ground and the effects of structural stiffness on the performance of robot with wheel state and leg state are different, the research results can provide a basis for wheel stiffness design. The above research results provide a useful reference for mechanism design, parameter selection, and control strategy.However, there are still many problems for the wheel-legged rescue robot. For example, there is no waterproof structure, intelligent control algorithm is not studied, and the kinematic performance when the robot is in sea wave is not analyzed. All this needs further improvement.


## 7. Conclusion

This paper focuses on the design and analysis for a wheel-legged rescue robot. Considering the existing wheel-legged robot has the disadvantages of complex structure, difficult control, large space required for wheel-legged translation, and limited movement environment, a novel wheel-legged rescue robot is designed, and the wheel becomes semicircular leg by the rotation of half wheel along vertical axis. The robot can carry out a variety of motion states and can move on land or in waves. Based on the analysis results of motion states and the effect of structural stiffness of wheel-legged structure on motion performance, the prototype of wheel-legged rescue robot is designed, and the experiments show that the robot has good performance. The present study provided a basis for designing the wheel-legged rescue robot. Further extensions to this work include the design for waterproof structure, research on intelligent control method, and the test in real postdisaster environment.



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*Source: 5719381-2017-11-06.xml*