Research Article  Open Access
Liyue Fu, Aiguo Song, "Dynamic Characteristics Analysis of the SixAxis Force/Torque Sensor", Journal of Sensors, vol. 2018, Article ID 6216979, 11 pages, 2018. https://doi.org/10.1155/2018/6216979
Dynamic Characteristics Analysis of the SixAxis Force/Torque Sensor
Abstract
In this study, dynamic characteristics of a robot sixaxis wrist force/torque (F/T) sensor with crossbeam elastomer are analyzed by two methods of model identification, a method for simultaneous identification of order and parameters of the model (SIM) and a method based on the differential evolution (DE) algorithm. Firstly, by establishing the simplified mechanical model and finite element (FE) model, respectively, natural frequency of the sixaxis wrist F/T sensor is calculated. Secondly, dynamic calibration experiment is conducted. Lastly, two dynamic models of the sensor are identified by SIM and DE methods and the dynamic characteristics of the sensor, such as natural frequency and working band, are further analyzed. Comparing experimental values with the theoretical values, the results show that this sensor has a wide dynamic range with the first natural frequency at more than 1600 Hz, working bands (±5%) are more than 400 Hz, and the step response oscillation is intense. This study can provide a reference for the application of the sixaxis F/T sensor in the field of dynamic measurement.
1. Introduction
A sixaxis force/torque (F/T) sensor can measure the tangential force terms along , , and normal force term along axis (, , and ) as well as the moment terms about , , and axis (, , and ) simultaneously. Sixaxis F/T sensor can be used in robotics, aerospace, automotive, industrial areas [1]. Dynamic force measurement is more and more used in various industries, which make the dynamic performance analysis of sixaxis F/T sensors particularly important. In the field of micromachining, multiaxis F/T sensors are used to measure 3D machining forces which involve very high frequencies due to the high spindle speeds used during the process [2]. As research in vibrationbased damage identification increases, multiaxis F/T sensors with high dynamic ranges are used in realtime structural health monitoring [3]. With the quick development of the robot field and the needs of special areas, such as precise assembly, contour tracing, and twohand coordination [4], sixaxis F/T sensor has become one of the most important sensors in the field of the intelligent robot. When F/T sensor is used to sense the collision between robot and environment, it is necessary to detect the size and direction of the dynamic collision force [5]. As a detecting element in the force reflection control system, it should respond quickly to the load, namely, having excellent dynamic characteristics [6]. These applications demonstrate the importance of the research on the dynamic characteristics of the F/T sensor. This study arises from the demand for dynamic measurements in various industries.
The acquisition of the dynamic characteristics of the sixaxis F/T sensor is based on the dynamic calibration experiment. The dynamic calibration of a sixaxis F/T sensor is to obtain the relationship between the input and output of the sensor when performing varied sixaxis forces. Essentially, it is a process to acquire dynamic characteristics’ indices such as natural frequency, time constant, and damping ratio. Huang verified that the frequency band has the most influence for the sensor and test system and therefore becomes the most important practical index for dynamic calibration [7]. Regular incentives are impulse, step, and sinusoidal forces, and the corresponding calibration methods are called impulse response, step response, and frequency response methods, respectively [8]. Previously, the research on dynamic characteristics is mainly based on the impulse response method. Xu and Li used a pendulum to exert an impact force along one axis of a multiaxis wrist F/T sensor [9] and developed a dynamic test to compare the dynamic characteristics between the wrist sensor and a JR3® multiaxis F/T sensor [10]. However, only a few channels were utilized, since it is difficult to calibrate the torque, which cannot fully reflect the sixaxis wrist F/T sensor’s performance. Liu et al. developed a methodbased correlation wavelet for measuring the dynamic performance index, but the cantilever was tested, and the robot’s multiaxis wrist force sensor was only simulated [11]. In this study, the negative step excitation is constructed by cutting the rope of hanging weight to obtain the step response to carry out the dynamic calibration experiment of the sixaxis wrist F/T sensor.
There has been limited literatures on dynamic performance analysis of the multiaxis F/T sensor, but most of them are not comprehensive enough. Song et al. studied dynamic performance of the 2axis force sensor applied for the force feedback maglev control system by using an impulse stimulation method [12], yet dynamic indices were not attained. Xu and Zhu carried out the dynamic calibration experiment of the sixaxis wrist F/T sensor, without building the necessary difference equation model or transfer function model [13]. Ballo et al. employed a sixaxis F/T sensor for the frontal impact test on a Hybrid III 50th percentile dummy [14], but the dynamic analysis method was not given. Thus, the purpose of this paper is to analyze the dynamic characteristics of the sixaxis F/T sensor comprehensively.
The rest of this paper is organized as follows. Section 2 describes the mechanical structure of the F/T sensor. The mechanical model is established, and the relationship between the natural frequency and weight of the elastomer is obtained in Section 3. In Section 4, the first six natural frequencies and vibration modes are acquired by modeling and modal analysis of the sensor in ANSYS software. In Section 5, dynamic calibration experiment is conducted and the dynamic models are established by model identification. The methods of model identification used in this section are a method for simultaneous identification of order and parameters of the model (SIM) and a method based on the differential evolution (DE) algorithm. Furthermore, the dynamic performance indices of the sensor are achieved. Finally, the concluding remarks follow in Section 6.
2. Sensor Structure and Calibration Method
As shown in Figure 1(a), the prototype of the sixaxis wrist F/T sensor for the robot consists of four parts: pedestal, crossbeam elastomer, top cover, and calibration pillar. The sensor’s housing is designed as cylindrical structure to connect with the robotic arm and claws. Crossbeam elastomer is the core component of the sensor, and the performance of the sensor mainly relies on it. Figure 1(b) shows the structure of the crossbeam elastomer. It comprises of four crossbeams, four compliant beams, a central platform, and four rims, which are characterized by a compliant beam flexible link at the connection between a crossbeam and two rims. The force or torque is applied to the sixaxis F/T sensor through the calibration pillar which transmits the force or torque to the crossbeam elastomer by connecting with the central platform. Figure 2(a) illustrates the loading setup of sixaxis forces or torques. The calibration methods of various channels are depicted in Figures 2(b)–2(e).
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The excitation force applied to the sensor through the calibration pillar caused deformation of the crossbeam elastomer. Since the compliant beam is very thin, it can be regarded as the flexible link when the applied force is perpendicular to the plane of it and it can be regarded as the ideal rigid body when the applied force is parallel to the plane. Therefore, the force applied to the sensor leads to the bending deformation of two crossbeams whose deformation degree is proportional to the applied force and tension or compression deformation of the other two crossbeams whose deformation degree can be neglected. The resistive strain gauges attached to the bending crossbeams can detect the amplitude of the corresponding force.
3. Theoretical Analysis
3.1. Simplified Statics Model
To get the equivalent stiffness value of the flexible link of the crossbeam elastomer, simplified statics model is established. Figure 3(a) shows the schematic diagram of crossbeam elastomer, where represents the force applied to the elastomer along direction through central platform. Since its width (or height) is much less than the length, the crossbeam can be regarded as a slender beam. When the central platform is subjected to a tensile force along direction, bending occurs on crossbeams and and compliant beams and . The compliant beams and are considered as the roller support of the crossbeams and . As the compliant beams are laminated elements, compliant beams and are idealized as flexible bodies and crossbeams and are idealized as rigid bodies. Thus, the beam can be simplified as a simply supported beam with a fixed hinge at one end and a movable hinge at the other, whereas the beams and as cantilever beams. Figure 3(b) depicts the mechanical model of the whole crossbeam elastomer, where and are the displacement of midpoints of beams and , respectively, and and are shear forces on beams and , respectively. The simplified statics model of the crossbeams and is shown as Figure 3(c).
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According to the principle of the balanced force and moment, the supporting reaction forces of the supports are , where represents the force applied to the beam which is component of force and . The central platform can be regarded as a lumped mass owing to smaller size relative to the crossbeam, that is, the segment in Figure 3(d) can be concentrated on a point . The shear force and bending moment on an arbitrary section of the beam are as follows:
The deformation of the crossbeam can be expressed by the deflection and rotation angle of a point on this beam. As is shown in Figure 3(d), the point on this beam is shifted to the point under the action of the force , the distance between the two points along direction is deflection , and the angle at which the cross section turns relative to the original position is rotation angle . Both the bending moment and the shear force can cause the deformation of the beam [15]. where are are deflection and rotation angle brought on by bending moment, respectively, and and are deflection and rotation angle brought on by shear force, respectively. Based on the differential equation of the deflection and equations (1) and (2), the deflection and rotation angle of a point on this beam are derived [16]: where , , , and are undetermined coefficients whose values can be derived in virtue of boundary and continuous conditions. The final solution of the deflection of the beam is computed as follows: so that the midspan deflection, namely, the displacement of the beam , is shown as equation (5). In the same way, the displacement of the beam is summarized as equation (6). where and are the elastic modulus and shear modulus of the material, respectively, , and are the sectional area of the beams and , respectively, and and are the moment of inertia of the beams and , respectively. Based on the moment of inertia of a rectangular section, and can be expressed as equations (7) and (8), respectively.
The material of the crossbeam elastomer of the sixaxis wrist F/T sensor is aluminium alloy 2024. Parameters of the crossbeam elastomer are shown in Table 1, where and denote the width and thickness of crossbeam, respectively, and represent the height and length of compliant beam, respectively, and and are the elastic modulus and Poisson’s ratio of aluminium alloy 2024 which is used to make of the crossbeam elastomer. Moreover, equation (9) can be obtained according to the geometric characteristic of the deformation.

By substituting equations (5)–(8) to equation (9), the formula is derived as follows:
Subsequently, the equivalent stiffness coefficient is deducted as follows:
Substituting the parameters in Table 1 into equation (7), the equivalent stiffness coefficient can be calculated as
3.2. Simplified Dynamics Model
The sixaxis wrist F/T sensor is a multiple input and multiple output (MIMO) system. When the sensor is constrained on a foundation surface, the joint between the foundation surface and the pedestal is a rigid connection, and thus the inputoutput characteristics in any direction can be simplified as a single degreeoffreedom (DOF) system. When the sensor is mounted on the wrist of the robot, the whole mechanism consists of three components: the pedestal of the sensor, the crossbeam elastomer, and the robotic hand. Every component has one translation/rotation DOF in any direction of the sixaxis F/T sensor, so the mechanism is a 3DOF system. As shown in Figure 4, , , , and are the mass, displacement of the mass, equivalent stiffness, and damp, respectively, and subscripts , , and are the hand of the robot, the crossbeam elastomer, and pedestal of the sensor, respectively.
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Assuming that , , and are all compressed and the displacements of the mass change according to sinusoidal law, the displacements of the masses and the vibration equation are expressed as equations (13) and (14). Then, equation (13) is substituted with equation (14), and equation (15) is obtained. where is mechanical impedance matrix and can be denoted as the following form:
The eigenvalue of the matrix is the natural frequency of the system. Considering that the joint between robotic hand and the elastomer and the joint between robotic arm and the pedestal are rigid connections, the 3DOF system can be simplified to a singleDOF system as shown in Figure 4(a). Moreover, the mass is , and thus, the natural frequency of the system is resolved in equation (17). Obviously, in case of considering the equivalent mass of the robotic hand, mounted resonance frequency of the sixaxis wrist F/T sensor is diminished. In fact, the change of gripping workpiece mass, the mass, shape, and mass distribution of end effector will affect the dynamic characteristics of the sensor. Before testing and evaluating the dynamic properties of the wrist force sensor, it is necessary to determine the state of the sensor and the environment in which it is used. And the unified basis and meaningful results can be obtained under a uniform load.
In view of the equivalent stiffness coefficient and the mass of the crossbeam elastomer and calibration pillar (), the natural frequency of the sixaxis wrist F/T sensor in direction can be calculated to be 1642 Hz. Similarly, the natural frequencies of the sensor’s other channels can be solved as shown in Table 2.

4. Modal Analysis
Vibration modal is one of the intrinsic characteristics of elastic structures. The modal analysis of the elastomer is carried out in ANSYS software, and the inherent vibration properties of the sixaxis wrist F/T sensor are studied, including the undamped natural frequency, damped ratio, and vibration modal. The modal extraction method is set to block lanczos, and the number of extraction is 6. The results are shown in Table 3, and six vibration modes are shown in Figures 5(a)–5(f).

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5. Dynamic Calibration Experiment and Model Identification
5.1. Dynamic Calibration Experiment
The step response method is used to calibrate the sixaxis F/T sensor. The negative step excitation is constructed by cutting the rope of hanging weight to obtain the step response to carry out the dynamic calibration experiment of the sixaxis wrist F/T sensor. One end of the rope is hung on the calibration pillar, and the other end suspended the weight by a pulley. The rope is cut off at a given time, thus a negative step excitation is applied to the sixaxis F/T sensor. The cotton rope, fishing line, and ordinary plastic rope are, respectively, used to suspend weights during calibration experiment. Figure 6 shows the three ropes. The test results show that the fishing line has the best effect among the three ropes; hence, the fishing line with diameter of 0.4 mm is used in the dynamic calibration experiment. The step responses of the sensor have been acquired via a highspeed Smacq® USB4620 data acquisition card and transmitted to the host computer. The sampling frequency of this data acquisition card can be changed by software and set to 100 kHz in the dynamic calibration experiment. Figure 2(a) presents the experimental facilities.
The method of constructing step excitation by cutting the rope of hanging weight during dynamic calibration experiment is simple, but the step rise time is long. Force excitation can be generated in other ways, such as dynamic pressure generator based on a doubleacting pneumatic actuator [17].
5.2. Model Identification Based on the SIM Method
Based on the acquired input and output data, the dynamic models are established by model identification. The methods of model identification used in this paper are the SIM method and DE method. The SIM method is a method for simultaneous identification of order and parameters of the model. This method can directly calculate the minimum value of the index function corresponding to all the models of interest, and then the order is determined. Compared with the least square method, this approach has some important features, such as less calculation, simpler program, and more flexible applications. Meanwhile, the problem of numerical “morbid” caused by illconditioned regular equations in the least square method is avoided.
Let the differential equation of the sixaxis F/T sensor in channel is described as follows: where and are the input and output observations of the sensor, respectively, is a backward shift operator, is the fitting error, , and .
The negative step excitation constructed and step response acquired in experiment are shown in Figure 7. The relationship curve between the index function, described as the sum of squared residuals, and model order is depicted in Figure 8. It can be seen that the changes after is very slow, and thus the model order is 3. Then, the model parameter vector can be expressed as equation (19) by the SIM method model identification. The difference equation and transfer function of the sensor are shown in equations (20) and (21), respectively.
The negative step excitation constructed is used to get the model’s response. Figure 9(a) shows that the calculated values of the model fit well with the experimental response curve, and this model can be used. Bode diagram of this model is depicted in Figure 9(b).
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From the bode diagram and transfer function, we can see that the natural frequency of the model is 1720 Hz and the working bands of amplitude error within and within are 560 Hz and 414 Hz, respectively. Compared with the aforementioned theoretical analysis and modal analysis, this model identified by the SIM method is correct.
So the dynamic models from other channels can be also identified by the SIM method. The dynamic performance indices of the sensor can be obtained as shown in Table 4.

5.3. Model Identification Based on the DE Algorithm
Differential evolution (DE) algorithm is a kind of the optimization algorithm based on swarm intelligence theory, which is often used to solve the problem of optimization search in complex real space. The special memory ability of the DE algorithm enables it to dynamically track the current search situation to adjust its search strategy. It has strong global convergence ability and robustness and does not need the characteristics’ information of the problem. The parameter identification of the complex system can be realized.
The basic idea of the DE algorithm is that starting from a random initial population, a new individual is generated by summing weighted vector difference between any two individuals in the population and the third individual within the certain rules. By comparing to a predetermined individual, if the fitness of the new individual is better, the new individual will replace the old one in the next generation; otherwise the old remains. Through continuous iterative computation, we retain good individuals, eliminate inferior individuals, and guide the search process to approach the optimal solution.
Assumed to be a threeorder model, the discrete transfer function is expressed as equation (22) and parameters to be identified can be written as follows: . The ranges of these parameters are . In the DE algorithm, the mutation factor is 0.8, the cross factor is 0.7, the size of samples is 100, and the maximum of iterations is 500. After 60 steps of iteration, the best sample can be obtained as equation (23). Figures 10(a) and 10(b) depict the fitnessiteration relational curve and the model response, respectively.
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In the light of the transfer function identified by the DE algorithm, the bode diagram can be depicted as shown in Figure 11.
From Figure 11 and equation (23), it can be obtained that the natural frequency is 1680 Hz and the working bands of amplitude error within ±10% and within ±5% are 530 Hz and 395 Hz, respectively. These results agree with the model identified by the SIM method.
In the same way, the model identification results of , , and channels are shown as Figure 12. The transfer functions of the three channels are identified as equations (24)–(26). The dynamic performance indices are shown as Table 5.
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Combined with the aforementioned models, the dynamic performance indices are integrated into Table 6. It can be seen in the table that the analysis results of these models are consistent and the first natural frequency is more than 1600 Hz.

6. Conclusions
In this study, a systematic theoretical analysis, modal analysis, dynamic calibration experiment, and model identification are carried out for testing and verifying the sixaxis wrist F/T sensor. The SIM method and DE algorithm are used to identify the dynamic models. From Tables 2–6, the maximum difference among the aforementioned four models within 5.6% and the dynamic performance indices obtained by the identified models are consistent with the results from the theoretical analysis and thus showing the identified models are reasonable. The results from the dynamic analysis for the sixaxis wrist F/T sensor provide a theoretical basis for the application of the sensor in the dynamic working environment.
The results show that this sensor has a wide dynamic range with the first resonant frequency at more than 1600 Hz, working bands (±5%) are more than 400 Hz, and the step response oscillation is intense. To widen its working band and reduce the overshoot, it is necessary to add a compensation link to the sensor which will be the future work. In this dynamic calibration experiment, each channel is individually excited and only this channel’s responses are acquired simultaneously, so the coupling is weak and there are no decoupling in this experiment. However, the coupling is serious in actual dynamic applications, and dynamic decoupling of the sixaxis F/T sensor will also be the future work.
Data Availability
The data used to support the findings of this study are available from the corresponding author upon request.
Conflicts of Interest
The authors declare that there is no conflict of interest regarding the publication of this paper.
Acknowledgments
This work was supported by the National Key R&D Program of China (no. 2016YFB1001301), National Nature Science Foundation of China (no. U1713210), and Suzhou Science and Technology Planning Project (no. SGC201653).
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Copyright
Copyright © 2018 Liyue Fu and Aiguo Song. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.