# Design and Modeling of a Novel Transformable Land/Air Robot

Authors: He Wang; Jiadong Shi; Jianzhong Wang; Hongfeng Wang; Yiming Feng; Yu You
Journal: International Journal of Aerospace Engineering
 (2019)

---

## Abstract

This paper describes a novel transformable land/air robot that is capable of terrestrial locomotion and aerial locomotion. What is unusual about the robot is that it can transform between the two modes of locomotion at will through the transformable mechanism, allowing the robot to overcome large obstacles in their mission environment. The wheel mechanism of the robot is shared by both terrestrial and aerial locomotion, instead of simply adding a quadrotor to a wheeled mobile robot. The objective of this paper is to design the robot and establish the kinematic and dynamic models for the transformable process. Herein, we focus on the design of the driving wheels and transformable mechanism. A series of experiments about the energy analysis and the transformation from aerial locomotion mode to terrestrial locomotion mode were performed with the physical prototype; the experiment results confirmed the validity of our design and the theoretical analysis that are helpful to optimize the key parameters in our design. Moreover, our work can provide a reference for the study of the flying car.


---

## Body

## 1. Introduction

The ability to explore areas that are risky and inaccessible to humans and easily deal with the complex terrains makes quadrotors an excellent choice in applications such as search and military surveillance [1, 2]. However, it is difficult for quadrotors to operate for an extended period of time and range because of their high-energy consumption [3, 4]; as we all know, terrestrial locomotion is more energy efficient. For these reasons, a robot that is capable of terrestrial and aerial locomotion can be better adapt to different environments at the same time can extend the operation time and range.There have been many successful attempts to create robots with terrestrial and aerial locomotion capabilities, and many approaches to combining aerial locomotion and terrestrial locomotion have been proposed [5, 6]. However, in order not to affect the operating capabilities of each mode of locomotion and the overall mobility of the robot, the two modes of locomotion should share part of their structure or actuators that can avoid the increasing weight and design complexity of the robot [7–10]. The HyTAQ connects a cylindrical cage to a quadrotor through two revolute joints, allowing the cage to roll freely with respect to the main quadrotor body. Moreover, the flight control system and commands used for aerial locomotion can be used to control the terrestrial locomotion. Compared to the aerial mode, there is no need to overcome the weight of the robot in the terrestrial mode, and therefore the robot reduces the power consumption [11–13]. Recently, some robots share part of their structure or actuators by undergoing a transformation when changing the modes or adjusting its shape by itself to adapt to the mode of locomotion. The robot [14–16] is a two-wheeled terrestrial locomotion robot that transforms into a helicopter. In the terrestrial locomotion mode, the rotors and stabilizer bar used for aerial locomotion are folded down along the length of the robot’s body. It transforms into its aerial locomotion mode by positioning itself on-end, with its long axis oriented vertically rather than horizontally, and unfolding its flight mechanisms. The rotors are attached to the rotor heads close to the drive shafts by passive hinges and thus unfold as the shafts begin to spin. Moreover, the researchers of the Deployable Air-Land Exploration Robot (DALER) propose a new approach, which is called “adaptive morphology”, where parts of the structure of the robot are shared between the different modes of locomotion, instead of simply adding a second locomotion structure to an existing robot. It uses its wings as whegs to move on the ground, and the structure could self-adjust the shape to adapt to the locomotion mode. The efficiency of locomotion in each mode of locomotion can be improved through adaptive morphology suitable for that mode [17, 18].Inspired by these works, we introduce a novel transformable land/air robot that is capable of terrestrial locomotion and aerial locomotion and enables to transform between the two modes of locomotion at will. It combines wheels with quadrotor, and the wheels are shared by both aerial and terrestrial locomotion, instead of simply adding a quadrotor to a wheeled mobile robot, and therefore avoid increasing weight and design complexity of the robot. The robot is primarily used on the ground, the intent of the aerial locomotion mode is to deal with the large obstacles, across complex terrain. Firstly, we described the outline of the platform’s structure, and detailed the design of the driving wheels and transformable mechanism. Secondly, we established the kinematic and dynamic models for the transformable process. Then the transformation and energy analysis experiments were performed with the physical prototype. Finally, conclusions are drawn in Section5.


## 2. Design of the Novel Transformable Land/Air Robot

There are three states of the robot in the process of motions. The full sequence is illustrated in Figure1, (a) represents the state of terrestrial locomotion, (b) and (d) represent the state of a transformable process between the two modes of locomotion, respectively, and (c) represents the state of aerial locomotion.Figure 1
The full sequence of motions.


### 2.1. Design of the Platform

The robot consists of three parts: running part, mode transformation part, and flying part. The running part realizes the stable running on the ground by adopting the architecture of two-wheel differential drive. The flying part realizes the stable flight by quadrotor mechanism. The mode transformation between the two modes of locomotion is directly driven by servos. Figure2 shows the configuration of the platform.Figure 2
Configuration of the platform.The control system of the robot is shown in Figure3. The communication between an operator and the robot is conducted wirelessly. The running part and mode transformation part are controlled by a microcontroller (STM32F407); the flying part is controlled by the APM2.8. The APM2.8 is composed of MCU and IMU which can provide the raw data of flight attitude and velocity, and the APM2.8 is mainly used for flight attitude control and navigation. The external GPS module can provide position information for the APM2.8. A Li-PO battery is used as the power supply. A microvideo camera mounted on the baseplate is equipped to take clear pictures and send to the control terminal real time.Figure 3
The control system of the transformable land/air robot.


### 2.2. Driving Wheel

The design of the driving wheel is very crucial. Figure4 shows the whole structure of the driving wheel. In the terrestrial locomotion mode, the carbon fiber brackets on both sides of the wheel do not rotate. The motor for running drives the gear train and further drives the gear ring to complete the terrestrial locomotion. Gear train and gear ring play an important role in reducing speed and increasing torque while transmitting motion. The external diameter of the gear ring is slightly larger than the rotors, allowing the wheels to protect the rotors from obstacles such as rubble and wall. The 0.5 mm gap between gear ring and carbon fiber bracket ensures the gear ring rotate smoothly. The carbon fiber brackets on both sides of the wheel are connected and supported through plastic studs, and its external diameter is slightly smaller than the gear ring, ensuring itself do not contact the ground. The gears at the edge of the wheels support and mesh with the gear ring to make the gear ring rotate smoother.Figure 4
Structure of the driving wheel.In aerial locomotion mode, the wheels are the mounting seat of the motor for flying. The rotors and its driving motors are installed at the center of the wheels, and they are cross distributed to control the flight attitude and position.


### 2.3. Transformable Mechanism

The transformable process between aerial locomotion and terrestrial locomotion is driven by the servo to rotate 180°, instead of turning over 90°. Figure5 shows the sequence of the transformable process, taking the transformation from terrestrial locomotion mode to aerial locomotion mode as an example. In the transformable process, in order to avoid the collision between the wheels and the baseplate, the rotational direction of the servo in diagonal direction is the same. The connection between the wheel and the servo is called transformable mechanism and it has a 135° angle (see Figure 6). Reference to the structure of the fast disassembly seat, as shown in Figure 6, the transformable mechanism consist of inter tube, outer tube, and quick-release clip, so the robot has the advantage of portability. The outer tube and motor for running are positioned on the same shaft center.Figure 5
Transformation sequence from terrestrial locomotion mode to aerial locomotion mode.Figure 6
Structure of the transformable mechanism: (a) driving wheel and (b) driven wheel.
(a)
(b)


## 2.1. Design of the Platform

The robot consists of three parts: running part, mode transformation part, and flying part. The running part realizes the stable running on the ground by adopting the architecture of two-wheel differential drive. The flying part realizes the stable flight by quadrotor mechanism. The mode transformation between the two modes of locomotion is directly driven by servos. Figure2 shows the configuration of the platform.Figure 2
Configuration of the platform.The control system of the robot is shown in Figure3. The communication between an operator and the robot is conducted wirelessly. The running part and mode transformation part are controlled by a microcontroller (STM32F407); the flying part is controlled by the APM2.8. The APM2.8 is composed of MCU and IMU which can provide the raw data of flight attitude and velocity, and the APM2.8 is mainly used for flight attitude control and navigation. The external GPS module can provide position information for the APM2.8. A Li-PO battery is used as the power supply. A microvideo camera mounted on the baseplate is equipped to take clear pictures and send to the control terminal real time.Figure 3
The control system of the transformable land/air robot.


## 2.2. Driving Wheel

The design of the driving wheel is very crucial. Figure4 shows the whole structure of the driving wheel. In the terrestrial locomotion mode, the carbon fiber brackets on both sides of the wheel do not rotate. The motor for running drives the gear train and further drives the gear ring to complete the terrestrial locomotion. Gear train and gear ring play an important role in reducing speed and increasing torque while transmitting motion. The external diameter of the gear ring is slightly larger than the rotors, allowing the wheels to protect the rotors from obstacles such as rubble and wall. The 0.5 mm gap between gear ring and carbon fiber bracket ensures the gear ring rotate smoothly. The carbon fiber brackets on both sides of the wheel are connected and supported through plastic studs, and its external diameter is slightly smaller than the gear ring, ensuring itself do not contact the ground. The gears at the edge of the wheels support and mesh with the gear ring to make the gear ring rotate smoother.Figure 4
Structure of the driving wheel.In aerial locomotion mode, the wheels are the mounting seat of the motor for flying. The rotors and its driving motors are installed at the center of the wheels, and they are cross distributed to control the flight attitude and position.


## 2.3. Transformable Mechanism

The transformable process between aerial locomotion and terrestrial locomotion is driven by the servo to rotate 180°, instead of turning over 90°. Figure5 shows the sequence of the transformable process, taking the transformation from terrestrial locomotion mode to aerial locomotion mode as an example. In the transformable process, in order to avoid the collision between the wheels and the baseplate, the rotational direction of the servo in diagonal direction is the same. The connection between the wheel and the servo is called transformable mechanism and it has a 135° angle (see Figure 6). Reference to the structure of the fast disassembly seat, as shown in Figure 6, the transformable mechanism consist of inter tube, outer tube, and quick-release clip, so the robot has the advantage of portability. The outer tube and motor for running are positioned on the same shaft center.Figure 5
Transformation sequence from terrestrial locomotion mode to aerial locomotion mode.Figure 6
Structure of the transformable mechanism: (a) driving wheel and (b) driven wheel.
(a)
(b)


## 3. Kinematic and Dynamic Modeling of the Transformable Process

The kinematic and dynamic modeling of aerial locomotion and terrestrial locomotion have been adequately described elsewhere in the literature [19–23]; thus, they are not described in this paper. Because the transformable process of the four wheels is basically the same, here, we only present the transformable process from aerial locomotion mode to terrestrial locomotion mode for the left-rear wheel as an example.


### 3.1. Kinematic Modeling

Now the research of kinematic modeling is relatively mature [24–26]; to realize the movement control and verify the kinematic characteristics of the robot, the equivalent angle-axis representation method [27] is used to describe the relationship between the pose of wheel and rotation angle of the servo in the transformable process. In order to express the coordinate system and kinematic parameters of the left-rear wheel more clearly, we simplified the wheel and the transformable mechanism, as shown in Figure 7. The wheel is assumed as the frame {C}, and the transformable mechanism is assumed as a link consists of L1 and L2.Figure 7
Simplified coordinate model of the wheel and the transformable mechanism.According to the rule of equivalent angle-axis representation and right hand, the frame {A} is fixed to the end of the servo shaft and it is considered the reference frame. The frame {B} is described as initially coincident with {A}. The origin of frame {C} is located in the point O, and the pose of wheel is described with the frame {C}. We describe the pose of the wheel in terms of frame {A}. Therefore, the transformable process can be simplified as the frame {C} rotates counterclockwise around the equivalent axis PQ in theYaQZa plane. In order to get the pose of the frame {C} relative to {A}, the frame {C} is translated to {B} and then {B} rotates counterclockwise around the equivalent axis PQ in the YaQZa plane.The translation matrix of the frame {C} relative to frame {B} is given as follows:(1)TCB=1000010−22L1001L2+22L10001.The equivalent rotation axis PQ in theYaQZa plane is given as
(2)K^=0−2222.The rotation matrix of the frame {B} relative to frame {A} is given as follows:(3)TBA=cosα−22sinα−22sinα022sinα12cosα+112cosα−1022sinα12cosα−112cosα+100001,where α is the rotation angle of the servo shaft in the transformable process; the angular velocity is a constant value.According to the homogeneous matrix transformation, the pose of the frame {C} relative to frame {A} is given as follows:(4)TCA=TBATCB=cosα−22sinα−22sinα−22L2sinα22sinα12cosα+112cosα−1−22L1+cosα−12L222sinα12cosα−112cosα+122L1+cosα+12L20001.Equation (4) describes the relationship between the wheel pose and the rotation angle of the servo shaft. Referring to the design model and physical prototype, the parameters are assigned as L1=36.5mm and L2=66.5mm. The wheel was initially in aerial mode. The position and the attitude in the aerial and terrestrial mode of the wheel were drawn in MATLAB, as shown in Figure 8. The direction of the arrow represents the trend of the transformable process.Figure 8
Position and attitude in the aerial and terrestrial mode of the wheel.From the simulation results, the wheel changed from parallel to the ground to perpendicular to the ground; position trajectory was consistent to our expectation. The simulation results confirmed the rationality of the transformable mechanism design and the kinematic modeling.


### 3.2. Dynamic Modeling

By the force analysis of the left-rear wheel using the isolation method in the transformable process, as shown in Figure9, we can calculate the servo output torque. In the transformable process, the wheel is not deformed.Figure 9
Force analysis of the transformable process.According to equation (4), we can get the pose of frame {C} and the position of the point O relative to the frame {A}; the position of the point O in ZA direction is given as
(5)ZO=22L1+cosα+12L2.Prototype experiments and design model of the robot show that the wheels contact the ground when the servo axis rotatesθ. Then the robot moves along the ZA direction, and the displacement and acceleration of the robot are given as follows:
(6)S=22L1+cosα+12L2−22L1+cosθ+12L2=cosα2−cosθ2L2,(7)a=S¨c=−L22cosα=−w2L22coswt,where w is the angular velocity of the servo shaft. In equation (7), the range of the α is from θ to π.The direction of the supporting force is opposite to the rotation direction of the gravity, given as(8)F=G+Ma4,where M is the mass of the robot; a is the acceleration of the robot in the ZA direction.The direction of frictional resistance is opposite to the rotation direction of the wheel, given as(9)f=μF4,where μ is the friction coefficient between the resin wheel and the ground.Figure10 shows the geometric relationship in the transformable process, which can help us calculate the arm of frictional resistance and supporting force clearly.Figure 10
The geometric relationship analysis of a certain angle in the transformable process.
(a)
(b)The arm of frictional resistance is given as follows:(10)H=h−S,Lf=L22+Hsinα/22sin34π−artanH/sinα/2L2,where h is the vertical distance from the point O to the ground in the terrestrial locomotion mode, and its value is 125 mm; α/2 is the angle between the wheel and the ground; H is the vertical distance from the point O to the ground.The arm of the supporting force is given as follows:(11)LF=XO+L=XO+Htanα/2cosα2,where XO is the position coordinates of point O; L is the vertical distance from point D to point O.The dynamic analysis of the transformation from terrestrial locomotion mode to aerial locomotion mode is divided into two steps. Next, we calculate the servo output torque referring to the above equations.Step 1 is from the aerial locomotion mode to the moment when the wheel contacts the ground. Neglecting the air resistance, the servo only needs to overcome the gravity of the wheel. The output torque is given as follows:(12)l=L2sinπ4,T1=mglsinπ4,where m is the mass of a wheel; l is the arm of gravity of the wheel; g is the gravity vector.Step 2 is from the wheel contacts the ground to the terrestrial locomotion mode; the servo needs to overcome the gravity of the robot and the frictional resistance. The output torque is given as follows:(13)T2=FLF+fLfsinπ4.


## 3.1. Kinematic Modeling

Now the research of kinematic modeling is relatively mature [24–26]; to realize the movement control and verify the kinematic characteristics of the robot, the equivalent angle-axis representation method [27] is used to describe the relationship between the pose of wheel and rotation angle of the servo in the transformable process. In order to express the coordinate system and kinematic parameters of the left-rear wheel more clearly, we simplified the wheel and the transformable mechanism, as shown in Figure 7. The wheel is assumed as the frame {C}, and the transformable mechanism is assumed as a link consists of L1 and L2.Figure 7
Simplified coordinate model of the wheel and the transformable mechanism.According to the rule of equivalent angle-axis representation and right hand, the frame {A} is fixed to the end of the servo shaft and it is considered the reference frame. The frame {B} is described as initially coincident with {A}. The origin of frame {C} is located in the point O, and the pose of wheel is described with the frame {C}. We describe the pose of the wheel in terms of frame {A}. Therefore, the transformable process can be simplified as the frame {C} rotates counterclockwise around the equivalent axis PQ in theYaQZa plane. In order to get the pose of the frame {C} relative to {A}, the frame {C} is translated to {B} and then {B} rotates counterclockwise around the equivalent axis PQ in the YaQZa plane.The translation matrix of the frame {C} relative to frame {B} is given as follows:(1)TCB=1000010−22L1001L2+22L10001.The equivalent rotation axis PQ in theYaQZa plane is given as
(2)K^=0−2222.The rotation matrix of the frame {B} relative to frame {A} is given as follows:(3)TBA=cosα−22sinα−22sinα022sinα12cosα+112cosα−1022sinα12cosα−112cosα+100001,where α is the rotation angle of the servo shaft in the transformable process; the angular velocity is a constant value.According to the homogeneous matrix transformation, the pose of the frame {C} relative to frame {A} is given as follows:(4)TCA=TBATCB=cosα−22sinα−22sinα−22L2sinα22sinα12cosα+112cosα−1−22L1+cosα−12L222sinα12cosα−112cosα+122L1+cosα+12L20001.Equation (4) describes the relationship between the wheel pose and the rotation angle of the servo shaft. Referring to the design model and physical prototype, the parameters are assigned as L1=36.5mm and L2=66.5mm. The wheel was initially in aerial mode. The position and the attitude in the aerial and terrestrial mode of the wheel were drawn in MATLAB, as shown in Figure 8. The direction of the arrow represents the trend of the transformable process.Figure 8
Position and attitude in the aerial and terrestrial mode of the wheel.From the simulation results, the wheel changed from parallel to the ground to perpendicular to the ground; position trajectory was consistent to our expectation. The simulation results confirmed the rationality of the transformable mechanism design and the kinematic modeling.


## 3.2. Dynamic Modeling

By the force analysis of the left-rear wheel using the isolation method in the transformable process, as shown in Figure9, we can calculate the servo output torque. In the transformable process, the wheel is not deformed.Figure 9
Force analysis of the transformable process.According to equation (4), we can get the pose of frame {C} and the position of the point O relative to the frame {A}; the position of the point O in ZA direction is given as
(5)ZO=22L1+cosα+12L2.Prototype experiments and design model of the robot show that the wheels contact the ground when the servo axis rotatesθ. Then the robot moves along the ZA direction, and the displacement and acceleration of the robot are given as follows:
(6)S=22L1+cosα+12L2−22L1+cosθ+12L2=cosα2−cosθ2L2,(7)a=S¨c=−L22cosα=−w2L22coswt,where w is the angular velocity of the servo shaft. In equation (7), the range of the α is from θ to π.The direction of the supporting force is opposite to the rotation direction of the gravity, given as(8)F=G+Ma4,where M is the mass of the robot; a is the acceleration of the robot in the ZA direction.The direction of frictional resistance is opposite to the rotation direction of the wheel, given as(9)f=μF4,where μ is the friction coefficient between the resin wheel and the ground.Figure10 shows the geometric relationship in the transformable process, which can help us calculate the arm of frictional resistance and supporting force clearly.Figure 10
The geometric relationship analysis of a certain angle in the transformable process.
(a)
(b)The arm of frictional resistance is given as follows:(10)H=h−S,Lf=L22+Hsinα/22sin34π−artanH/sinα/2L2,where h is the vertical distance from the point O to the ground in the terrestrial locomotion mode, and its value is 125 mm; α/2 is the angle between the wheel and the ground; H is the vertical distance from the point O to the ground.The arm of the supporting force is given as follows:(11)LF=XO+L=XO+Htanα/2cosα2,where XO is the position coordinates of point O; L is the vertical distance from point D to point O.The dynamic analysis of the transformation from terrestrial locomotion mode to aerial locomotion mode is divided into two steps. Next, we calculate the servo output torque referring to the above equations.Step 1 is from the aerial locomotion mode to the moment when the wheel contacts the ground. Neglecting the air resistance, the servo only needs to overcome the gravity of the wheel. The output torque is given as follows:(12)l=L2sinπ4,T1=mglsinπ4,where m is the mass of a wheel; l is the arm of gravity of the wheel; g is the gravity vector.Step 2 is from the wheel contacts the ground to the terrestrial locomotion mode; the servo needs to overcome the gravity of the robot and the frictional resistance. The output torque is given as follows:(13)T2=FLF+fLfsinπ4.


## 4. Experiments

The performance of the robot was evaluated in both indoor and outdoor environments, you can see in the accompanyingvideo. The terrestrial locomotion and aerial locomotion functions efficiently. Large obstacles can be avoided by flying over or running from the side, and for small obstacles within the obstacle climbing capability, the robot will run straight. Figure 11 shows the physical prototype in terrestrial and aerial modes and the state of mode transformation.Figure 11
Representations of the physical prototype state: (a) the terrestrial locomotion mode, (b) the state of mode transformation, and (c) the aerial locomotion mode.
(a)
(b)
(c)Table1 shows the dimensions of the physical prototype and the performance capabilities tested in both indoor and outdoor environments.Table 1
Prototype dimensions and performance capabilities.
Terrestrial mode
Aerial mode
Size (mm)
494×667×328
667×667×190
Rotor diameter (mm)
304.8
304.8
Wheel diameter (mm)
328
328
Weight (g)
3500
3500
Max velocity (m/s)
1.5
2
Max cargo load (g)
1500
1500
Max flight altitude (m)
\
20


### 4.1. Measurement Experiments of Servo Output Torque

In order to measure the output torque of the servo, the experiments about the transformation from aerial locomotion mode to terrestrial locomotion mode were performed with the physical prototype on different terrains including tiled floor, brick, and cement. You can find the experimental data in the accompanying materials. The friction coefficients between the resin wheel and the ground measured by dragging the wheel with a load cell on different terrains areutiled floor=0.16, ubrick=0.4, and ucement=0.545.According to the above dynamic models, the dynamic simulation results about the output torque were drawn in MATLAB, as shown in Figure12. The angular velocity of the servo is set as 0.314 rad/s.Figure 12
The dynamic simulation results of the output torque in the transformable process.From the simulation results, the transformable process was from 0 to 10 s, and it took about 5 seconds when the wheel touched the ground. So we can conclude that the wheel started to touch the ground when the servo shaft rotated about 90 degrees, and the output torque was maximum at this point. The simulation results were helpful for servo selection.We used digital oscilloscopes to measure and record the current real time, and the servo was powered by a 8.4 V dc power supply. Figure13 shows the current trend of the four servos on different terrains. In order to compare the experimental results with the theoretical value, the angular velocity of the servo is also set as 0.314 rad/s, and the experiment lasted for 20 s.Figure 13
Experimental current tendencies of the four servos on different terrains.According to the working principle of the servo and the relationship between the torque and the current, the output torque is calculated asT=KmI, where Kmis the coefficient of the torque and its value is 2.3 N·m/A. The output torque tendencies of a single servo are shown in Figure 14.Figure 14
Calculated the output torque tendencies of a single servo.Comparing Figures12 and 14, the experimental results have the same tendency with the dynamic simulation result, but there are some deviations between them. (1) The experimental results indicate the output torque of the servo is larger than what is predicted from theoretical analysis. We attribute this mostly to the uneven ground that are not modeled, and the servo efficiency is reduced due to long-term use. (2) The experimental results show that there is a longer adjustment time before the torque of the servo reaches its maximum value. According to the experiments, the time from about the fifth second to the maximum current value is the adjustment time of servo, the pose of the wheel did not change during this period. Future research will investigate these effects in the modeling process and optimize the current loop of the servo to speed up its response speed.


### 4.2. Energy Analysis

In order to compare the energy consumption in its terrestrial and aerial locomotion modes, we calculated the operating time and distance of the robot by measuring the current using the wireless galvanometer when the robot is moving at a constant speed.Table2 shows the experimental data, and Table 3 shows the calculated value of the operating time and distance. The weight of the prototype was 3.5 kg, and it was weighted to 4.2 kg in the experiment.Table 2
Experimental data in aerial and terrestrial modes.
Terrestrial mode
Aerial mode
Current (A)
0.5
16.5
Discharge capacity (mAh)
3200
3200
Velocity (m/s)
1.5
2Table 3
Calculated data of operating time and distance.
Terrestrial mode
Aerial mode
Operating time (s)
23040
698
Operating distance (m)
34560
1396The experimental results show that with the same battery the robot can fly about 23040 s and travels 34560 m and it can run 698 s and travels 1396 m. Therefore, the operating time increased about 33 times in the terrestrial mode, and the distance is still 25 times greater comparing to the aerial mode. Our robot takes account of the operating time and distance.


## 4.1. Measurement Experiments of Servo Output Torque

In order to measure the output torque of the servo, the experiments about the transformation from aerial locomotion mode to terrestrial locomotion mode were performed with the physical prototype on different terrains including tiled floor, brick, and cement. You can find the experimental data in the accompanying materials. The friction coefficients between the resin wheel and the ground measured by dragging the wheel with a load cell on different terrains areutiled floor=0.16, ubrick=0.4, and ucement=0.545.According to the above dynamic models, the dynamic simulation results about the output torque were drawn in MATLAB, as shown in Figure12. The angular velocity of the servo is set as 0.314 rad/s.Figure 12
The dynamic simulation results of the output torque in the transformable process.From the simulation results, the transformable process was from 0 to 10 s, and it took about 5 seconds when the wheel touched the ground. So we can conclude that the wheel started to touch the ground when the servo shaft rotated about 90 degrees, and the output torque was maximum at this point. The simulation results were helpful for servo selection.We used digital oscilloscopes to measure and record the current real time, and the servo was powered by a 8.4 V dc power supply. Figure13 shows the current trend of the four servos on different terrains. In order to compare the experimental results with the theoretical value, the angular velocity of the servo is also set as 0.314 rad/s, and the experiment lasted for 20 s.Figure 13
Experimental current tendencies of the four servos on different terrains.According to the working principle of the servo and the relationship between the torque and the current, the output torque is calculated asT=KmI, where Kmis the coefficient of the torque and its value is 2.3 N·m/A. The output torque tendencies of a single servo are shown in Figure 14.Figure 14
Calculated the output torque tendencies of a single servo.Comparing Figures12 and 14, the experimental results have the same tendency with the dynamic simulation result, but there are some deviations between them. (1) The experimental results indicate the output torque of the servo is larger than what is predicted from theoretical analysis. We attribute this mostly to the uneven ground that are not modeled, and the servo efficiency is reduced due to long-term use. (2) The experimental results show that there is a longer adjustment time before the torque of the servo reaches its maximum value. According to the experiments, the time from about the fifth second to the maximum current value is the adjustment time of servo, the pose of the wheel did not change during this period. Future research will investigate these effects in the modeling process and optimize the current loop of the servo to speed up its response speed.


## 4.2. Energy Analysis

In order to compare the energy consumption in its terrestrial and aerial locomotion modes, we calculated the operating time and distance of the robot by measuring the current using the wireless galvanometer when the robot is moving at a constant speed.Table2 shows the experimental data, and Table 3 shows the calculated value of the operating time and distance. The weight of the prototype was 3.5 kg, and it was weighted to 4.2 kg in the experiment.Table 2
Experimental data in aerial and terrestrial modes.
Terrestrial mode
Aerial mode
Current (A)
0.5
16.5
Discharge capacity (mAh)
3200
3200
Velocity (m/s)
1.5
2Table 3
Calculated data of operating time and distance.
Terrestrial mode
Aerial mode
Operating time (s)
23040
698
Operating distance (m)
34560
1396The experimental results show that with the same battery the robot can fly about 23040 s and travels 34560 m and it can run 698 s and travels 1396 m. Therefore, the operating time increased about 33 times in the terrestrial mode, and the distance is still 25 times greater comparing to the aerial mode. Our robot takes account of the operating time and distance.


## 5. Conclusions

In this paper, we designed a novel transformable robot that is capable of terrestrial locomotion and aerial locomotion and enables to transform between the two modes at will for overcoming obstacles. Firstly, we explained the outline of the platform and focus on analyzing the design of the driving wheel and transformable mechanism. Then, the kinematic and dynamic models about the transformable process were accurately established, which can provide an important reference to the key parameters design. Finally, a series of experiments about the running, mode transformation, and flying in both indoor and outdoor environments are performed. The experimental results show that the terrestrial locomotion and aerial locomotion function efficiently, and obstacles can be overcomed by flying over or running from the side. Moreover, the transformable experiments confirmed the validity of the kinematic and dynamic models that are important to transformable mechanism design and servo selection. The robot in the terrestrial mode can travel a distance almost 25 times greater and operate about 33 times longer compared to the aerial mode. The robot has a longer operating time and good mobility.Design optimization is a constant issue and requires a significant attention. In the future, we plan to optimize the transformable mechanism and the current loop of the servo to speed up its response speed, making the transformable process between aerial locomotion mode and terrestrial locomotion mode smoother and more stable. The ongoing research also continues to reduce the weight of the robot and improve both running and flying performance.



---

*Source: 2064131-2019-02-04.xml*