Evolutionary Algorithms and Metaheuristics: Applications in Engineering Design and Optimization
View this Special IssueResearch Article  Open Access
Zhiyu Yang, Jixin Wang, Guangzong Gao, Xiangyun Shi, "Research on Optimized TorqueDistribution Control Method for Front/Rear Axle Electric Wheel Loader", Mathematical Problems in Engineering, vol. 2017, Article ID 7076583, 12 pages, 2017. https://doi.org/10.1155/2017/7076583
Research on Optimized TorqueDistribution Control Method for Front/Rear Axle Electric Wheel Loader
Abstract
Optimized torquedistribution control method (OTCM) is a critical technology for front/rear axle electric wheel loader (FREWL) to improve the operation performance and energy efficiency. In the paper, a longitudinal dynamics model of FREWL is created. Based on the model, the objective functions are that the weighted sum of variance and mean of tire workload is minimal and the total motor efficiency is maximal. Four nonlinear constraint optimization algorithms, quasinewton Lagrangian multiplier method, sequential quadratic programming, adaptive genetic algorithms, and particle swarm optimization with random weighting and natural selection, which have fast convergent rate and quick calculating speed, are used as solving solutions for objective function. The simulation results show that compared to nocontrol FREWL, controlled FREWL utilizes the adhesion ability better and slips less. It is obvious that controlled FREWL gains better operation performance and higher energy efficiency. The energy efficiency of FREWL in equipment transferring condition is increased by 13–29%. In addition, this paper discussed the applicability of OTCM and analyzed the reason for different simulation results of four algorithms.
1. Introduction
Hybrid wheel loader has raised much attention due to its green technology. It is considered to be the trend of future in the loader field [1–3]. Here are some released hybrid loader prototypes of several manufacturers, as shown in Table 1.
However, the energysaving method of these above loaders is energy management strategy [4–6]. Besides, its dynamic performance, passing performance, and operation efficiency have no obvious difference with conventional diesel driven wheel loader. Hence, optimized torquedistribution control method (OTCM) of front/rear drive axle or four wheels is essential to improve operation efficiency, providing a new energysaving strategy [7, 8]. Considering the cost and control technology, the configuration of front/rear axle independent drive is more possible to realize mass production than fourwheel drive, like massproduced electric vehicles Tesla Model S [9] and BYD QIN [10].
There are many technologies demanding prompt solution about OTCM for FREWL. Enlightened by the relative research in onroad vehicle field, tire energy dissipation [11], total motor efficiency [12], and motor power loss [13] are used as energy efficiency optimization objective. Tire workload reflects the utilization of road adhesion ability [14]. Through the control of tire workload, the operation performance of FREWL is obviously improved.
In this paper, the proposed OTCM for FREWL is to gain better operation performance and higher energy efficiency. In the primary stage of FREWL dynamics research, it is more urgent to study longitudinal dynamics than to study the lateral stability because FREWL is often operated in low speed. This paper assumes that FREWL only moves in the longitudinal direction. In Section 2, the dynamic model is created based on the configuration of FREWL. In Section 3, depending on the target to improve the operation performance and energy efficiency, objective functions are that the weighted sum of variance and mean of tire workload is minimal and the total motor efficiency is maximal. Then constraint conditions of the optimization control are listed. Four nonlinear optimization algorithms with constraints, quasinewton Lagrangian multiplier method (QNLM), sequential quadratic programming (SQP) [14, 15] adaptive genetic algorithms (AGA) [16, 17], and particle swarm optimization with random weighting and natural selection (PSORN) [18, 19], are introduced to solve the objective function. In Section 4, the effectiveness of OTCM is verified by simulation analysis. In Section 5, we discussed the applicability of OTCM and analyzed the reason for different simulation results of four algorithms.
2. Dynamical Model of FREWL
The distinctive transmission configuration of FREWL takes diesel generating set as main power source. Rectifier converts the alternating current generated by diesel generating set to a direct current which used to drive front motor, rear motor, and working motor. Supercapacitor is used as auxiliary source to effectively use braking energy and control diesel generating set in its high efficiency operating region. So diesel generating set can always operate in its high efficiency region. The transmission configuration of FREWL is shown in Figure 1.
A brief summary of the forces and torques in longitudinal dynamics is shown in Figure 2.
2.1. Wheel Vertical Load
Because FREWL operates in low speed, the influence of air resistance can be ignored. The wheel vertical load is, respectively, given bywhere is the distance from FREWL gravity center to front axle, is the distance from FREWL gravity center to rear axle, is the distance from the front axle to the tooth tip of bucket, , is the height of FREWL gravity center, is the mass, is the gradient of the slope, is the longitudinal acceleration, and are the vertical loads of front and rear wheels, is the vertical component of spading resistance on the tooth tip of bucket, and is the horizontal component of spading resistance on the tooth tip of bucket.
2.2. Tire Driving Torque and Wheel Longitudinal Force
The relationship between the longitudinal force and driving torque on each tire is given bywhere is the wheel rotational inertia, is the tire rolling radius, is the wheel angular acceleration, is the wheel longitudinal force, and is the tire driving torque. in subscript denotes the front or rear axle.
2.3. Motor Driving Torque
Suppose that longitudinal force and vertical load of the wheels in the same axle are equal; the relationship between the motor driving torque and tire driving torque is given bywhere is the motor driving torque, is the motor rotational inertia, is the motor angular acceleration, and is the reduction ratio from the motor to the wheels.
3. Optimal TorqueDistribution Control Method
OTCM consists of objective function, constraint conditions, and optimization algorithm.
3.1. Objective Function
3.1.1. Optimized TorqueDistribution Control Based on Tire Workload
The nonlinear optimization problem about enhancing operating performance can be formulated in this way. Because of the characteristic that the driving torque of both motors can be controlled online, the objective function is that the weighted sum of variance and mean of tire workload is minimal [5]. It can be defined as
From (2) and (3), tire workload of each wheel is defined aswhere is the tireroad friction coefficient of each wheel and is the reduction ratio. By the characteristic that the driving torque of both front motor and rear motor can be controlled online, the objective function can be set by the minimum of weighted sum of variance and mean of tire workload. Distribution coefficient is defined aswhere is the sum of driving torque of the front motor and rear motor, is the driving torque of the front motor, and is the driving torque of the rear motor. Tire workload of each wheel is defined aswhere is the tire workload of leftfront wheel, is the tire workload of the rightfront wheel, is the tire workload of leftrear wheel, and is the tire workload of rightrear wheel.
3.1.2. Optimized TorqueDistribution Control Based on Total Motor Efficiency
In order to improve the energy efficiency of the FREWL while transferring equipment, the objective function is that the total motor efficiency is maximal [12]. It can be defined aswhere is the efficiency of front motor, is the efficiency of rear motor, is the front motor speed, and is the rear motor speed. The relationship between motor efficiency , motor torque , and motor speed is shown in Figure 3.
3.2. Constraint Conditions
The total driving torque should satisfy expected accelerator position firstly, as is shown inwhere is the accelerator position and is the motor speed. The surface about the three parameters is shown as Figure 4.
Adhesion force is influenced by wheel vertical load and tireroad friction coefficient. Because the influence of the motor inertia moment and wheel inertia moment is tiny, it is appropriate to ignore them. So in pure longitudinal slip condition, the maximum driving torque is limited by
The motor driving torque and speed should be limited as follows:
The range of driving torquedistribution coefficient is given by
3.3. Optimization Algorithms
Nonlinear optimization algorithms are widely used to solve nonlinear optimization problems [28]. Each nonlinear optimization algorithm has its capabilities and limitations, which have a significant impact on the performance of OTCM. The common optimization algorithms for nonlinear constraints optimization problems are quasiNewton Lagrangian multiplier method (QNLM), sequential quadratic programming (SQP), adaptive genetic algorithms (AGA), and particle swarm optimization with random weighting and natural selection, (PSORN). The notable advantage that these four algorithms possess over their classic one is the fast solution speed, which satisfies the requirement of subsequent field test of FREWL.
3.3.1. QuasiNewton Lagrangian Multiplier Method
QuasiNewton method (QNM) is a special case of Newton method. The objective function is Taylor expanded in second order at , as shown in (14).
The derivative of (14) is
An approximate matrix is used to replace in (15). The BroydenFletcherGoldfarbShanno (BFGS) is used to update the , as shown in (16).
QuasiNewton method fails to solve the nonlinear constraints optimization problems. Thus Lagrangian multiplier (LM) is introduced into the problem. Inequality constraints are transformed into equality constraints by an auxiliary variable. Then with the original equality constraints, the Lagrangian function is transformed into where the iterative equation of the multiplier is The termination criterion of iteration iswhere is called a multiplier, is penalty factor, and is termination error ranging from 0 to 1.
The simulation parameters of the QNLM used in this paper are shown in Table 2. QNLM consists of QNM and LM. QNM and LM have their own maximum iteration number and termination error. The maximum iteration and termination error have influence on the computing accuracy and computing time. Penalty factor is used to penalize those individuals which do not satisfy the constraint condition for solving constrained optimization problems.

3.3.2. Sequential Quadratic Programming
SQP is an efficient method for nonlinear optimization with advantages of high computational efficiency and fast convergent rate. In SQP, positive definite matrix is used to seek the optimal solution of subquestion. The subquestion is described as
If the constraints and are satisfied, the calculation will be determined. , and 1 means the initial value. A point under Karush–Kuhn–Tucker (KKT) condition is obtained and the termination error is .
To some value function , the chosen penalty factor defines that is decreasing at the point . Suppose that is the tiniest nonnegative integer satisfying the following equation:where and .
From , , is given by
The least square multiplier is calculated by
The approximate matrix is the same as in (16).
The simulation parameters of the SQP used in this paper are shown in Table 3. SQP needs to solve a quadratic programming subproblem at every iteration step. It is necessary to set its and subproblem’s maximum iteration number and termination error. The values of maximum iteration number, termination error, and penalty factor are the same as the function in QNLM.

3.3.3. Adaptive Genetic Algorithms
AGA is another significant and promising variant of genetic algorithms. AGA adjusts probabilities of crossover and probabilities of mutation in order to maintain the genetic model and to accelerate the convergence speed. In AGA, the evolution usually starts from a population which consisted of randomly generated individuals. By Roulette strategy, individual fitness values are evaluated to judge if it agrees with the optimization criterion. The new individuals are generated by the optimal best mutation probability and the best crossover probability whose equations are shown inwhere is the maximum fitness value population, is the mean fitness value population, is the bigger fitness value in two individuals about to crossover, and is the fitness value of individuals about to mutate. , , , and are the constants.
The simulation parameters of AGA used in this paper are shown in Table 4. Among them, the lower bound and upper bound of independent variable and discrete precision determine the encoding length required for the binary encoding. The values for lower bound and upper bound depend on the constraints. The scale of population and the maximum ecology affect the accuracy and computing time. In order to analyze the advantages and disadvantages of the various algorithms as much as possible, the maximum evolution generations are the same with the maximum number of the same number of QNLM and SQP. The values of , , , and are usually based on different application objects. It generally requires that , .

3.3.4. Particle Swarm Optimization with Random Weighting and Natural Selection
Particle swarm optimization (PSO) based on natural selection is one of the improved algorithms, which is characterized by iteratively trying to improve a candidate solution. In each iteration, the worst half of the particles in the population is replaced by the best half of the particles while preserving the original historical optimal value. Therefore, it improves the optimization ability and solving speed and significantly reduces the algorithm premature convergence situation.
The inertia weight is an important parameter in the PSO which is used to control the ability of development and search. The core of avoiding falling into the local optimal is to determine a reasonable inertia weight. In order to accelerate up the convergence speed, the inertia weight is set as a random value. The equation to calculate the random is where is the random weight, and are the maximum and minimum of the inertia weight, and is the random number of standard state distribution.
The simulation parameters of the PSORN used in this paper are shown in Table 5. Acceleration constants and determine the influence of particle individual experience and group experience on the trajectory of particle movement, usually . Inertia weight can be used to control the algorithm development and search capabilities, which have different values according to different application problems. Dimension of search space has the same value as the number of its independent variables. Maximum particle position and minimum particle position are the boundary conditions of the algorithm, and the numerical value depends on the constraints of the actual problem. Maximum particle velocity determines the maximum distance that the particle can move in one flight, usually , .

4. Simulation Results
4.1. Simulation of OTCM Based on Tire Workload
Conditions of traveling, spading, and stacking on bumpy road are common for wheel loader. The paper establishes these three conditions to verify the improvement of the FREWL operation performance through OTCM based on tire workload. Condition 1 simulates the traveling condition, while condition 2 simulates the spading condition. Condition 3 simulates the stacking condition in bumpy road with slope. The simulation parameters are listed in Table 6.

From Figures 5 and 6, it is notable that in the first 2 s, namely, the starting stage, the longitudinal slip ratio of controlled FREWL is much smaller than nocontrol FREWL. The operation performance has significantly improved by OTCM. After 3 s, namely, the driving stage, the longitudinal ratio optimized by AGA is smoother than other three algorithms, so the operation performance of FREWL is the best.
Another parameter to evaluate the control effect is the driving distance of the controlled FREWL and nocontrol FREWL on bumpy road in the same time, which is shown in Figure 7. Table 7 shows the driving distance of the FREWL without spading. Controlled FREWL has better control to longitudinal slip ratio; thus it marches earlier and drives farther than nocontrol FREWL. The OTCM based on AGA has the best control effect, and the driving distance compared to nocontrol FREWL is increased by 18.68%. The control effect of other three optimization algorithms is basically the same; the driving distance is increased by 15.48% compared to the nocontrol FREWL.

Figures 8 and 9 show the longitudinal slip ratio of front and rear wheel in condition 2, respectively. Table 8 shows slip frequency of the front and rear wheel of the controlled FREWL and nocontrol FREWL. In whole simulation time, especially the starting stage, the control effect of OTCM based on SQP is the best. Only the rear wheel slips once.

Figure 10 shows the driving distance of FREWL in condition 2. Controlled FREWL utilizes adhesion ability better and slips less and also can go forward in a shorter period when encountering spading resistance, as shown in Table 9. In this case, FREWL controlled by QNLN, SQP, and PSORN can go forward in a shorter period and make significant improvement, but the control effect of OTCM based on AGA is undesirable.

Condition 3 simulates stacking condition that the FREWL operates on the bumpy road with 20° slope and encounters a continuous spading resistance after 5 s, and is gradually heavyloaded. Compared to conditions 1 and 2, condition 3 is more complicated. Figures 11 and 12 show the longitudinal slip ratio of front and rear wheel in condition 3. It is obvious that after 10 s the front wheel of nocontrol FREWL is basically in the slippery state. While the FREWL applies four optimization algorithms, the slippery time is much less. Among them, AGAcontrolled FREWL slips the least. The control effects of the other three algorithms are similar.
Figure 13 shows the driving distance of FREWL in condition 3. Since AGA is better in control of the longitudinal slip ratio of front/rear wheel in Figures 11 and 12, it drives farthest. The other three algorithms also have a good performance compared to nocontrol. This shows that FREWL, which applied OTCM based on tire workload, has better operation performance in stacking condition than nocontrol FREWL.
4.2. Optimized TorqueDistribution Control Based on Total Motor Efficiency
Two most common equipment transferring conditions are driving straightly on the bituminous road and reciprocating on bumpy road. This paper sets two conditions to simulate the improvement of energy efficiency of FREWL by OTCM while transferring equipment. The simulation parameters are listed in Table 10. Condition 4 is set to observe the energy efficiency of FREWL while driving straightly on the bituminous road. Condition 5 is set to observe the energy efficiency of FREWL while reciprocating on bumpy road.

Figure 14 shows the total motor efficiency of the FREWL when the FREWL is traveling on the bituminous road. Table 11 shows the maximum motor efficiency of the various optimization algorithms. The total motor efficiency optimized by OTCM based on QNLM fluctuates frequently and violently in the starting stage of simulation, which leads to calculation failure, which means that QNLM is not suitable for problems with strongnonlinearity. The results of other three optimization algorithms are better than nocontrol FREWL. The PSORN works best; the total motor efficiency is increased by 14.86% comparing to nocontrol FREWL. The results of SPQ and AGA are roughly the same; the total motor efficiency is increased by 13.64% comparing to nocontrol FREWL.

Figures 15 and 16 show longitudinal speed and total motor efficiency of FREWL in condition 5. Table 12 shows the maximum total motor efficiency of FREWL in the forward stage and the backward stage. The total motor efficiency of controlled FREWL is greatly improved compared to nocontrol FREWL when driving reciprocally. The results by OTCM perform better in backward stage than in forward stage. The solution of SQP is the best in forward stage; the total motor efficiency is increased by 15.24% at most. The result of AGA works best in backward stage; the total motor efficiency is increased by 29.12% at most.

4.3. Simulation Time
Simulation time is an essential factor to affect the practicability of the method. Table 13 shows the simulation time of the optimization algorithms under various conditions. The simulation step size is 0.001 s in the Simulink/Carsim platforms. Taking into account the actual real test, the sampling step is generally set to 0.01 s. Therefore, QNLM and SQP can be used in the online control, but AGA and PSORN cannot. Because QNLM fails in equipment transferring condition, SQP is comprehensively the best optimization algorithm for OTCM in actual test.

5. Discussion
In this paper, we study the OTCM of FREWL and prove that OTCM can improve the operation performance and energy efficiency of FREWL through five simulation conditions. In addition to five simulation conditions mentioned in this paper, this method is also adaptable to other operation and equipment transferring conditions of FREWL in longitudinal motion. The changed parameters are shown in Table 14. Tick “✓” means this parameter is changed in that situation and hyphen “—” means it is unchanged.

As can be seen from Table 14, in other conditions, all the changed parameters are taken into account in the dynamic model of FREWL. At the same time, the optimization algorithm and optimization goals do not change. Therefore, the method proposed in this paper is suitable for operation and equipment transferring conditions.
In the simulation case, compared to nocontrol FREWL, the FREWL controlled by four optimization algorithms have a great increase in the operation performance and energy efficiency. In the OTCM based on tire workload, the QNLM and SQP optimization solutions are almost identical, because their core algorithm is the BFGS algorithm, as shown in (16). PSORN and AGA are modern intelligent optimization algorithms, but their results are quite different because the optimal solution of PSORN is easy to fall into the local optimal solution. Comparing to PSORN, AGA increases the crossover probability and mutation probability when the optimal solution tends to local optimal solution, enhancing the ability to solve the global optimal solution. Thus, AGA generally has a better performance in most simulation conditions.
However, although the AGA has a better performance, it has the longest computing time because the movement of the whole population is more evenly moving to the optimal region. QNLM and SQP compute faster because they apply the traditional BFGS method. Among them, SQP needs to solve a quadratic programming subproblem at each iteration step, so the calculation time is longer than QNLM.
6. Conclusion
OTCM is a critical technology to improve the operation performance and energy efficiency of FREWL. The driving torque of front motor and rear motor of FREWL can be controlled independently. The objective function minimizes the weighted sum of variance and mean value of tire workload and maximizes the total motor efficiency. The results show that the operation performance and energy efficiency are obviously improved by OTCM. While the FREWL is operating, the frequency of slip is obviously reduced, and the adhesion ability is improved. While the FREWL is driving straightly in equipment transferring, total motor efficiency is improved by 14.86% at most. While the FREWL is driving reciprocally in equipment transferring, total motor efficiency is improved by 29.12% at most. Considering the simulation results and simulation time comprehensively, SQP is the most suitable one of the four optimization algorithms for field test of FREWL.
Conflicts of Interest
The authors declare that there are no conflicts of interest regarding the publication of this paper.
Acknowledgments
The authors acknowledge the funding support from National Natural Science Foundation of China, no. 51375202, and also acknowledge the support of Programs for Science Research and Development of Jilin Province, no. 20160101285JC.
References
 Z. Naiwei, D. Qunliang, J. Yuanhua, Z. Wei, and R. Youcun, “Modeling and simulation research of coaxial parallel hybrid loader,” Applied Mechanics and Materials, vol. 29–32, pp. 1634–1639, 2010. View at: Publisher Site  Google Scholar
 J. Wang, Z. Yang, S. Liu, Q. Zhang, and Y. Han, “A comprehensive overview of hybrid construction machinery,” Advances in Mechanical Engineering, vol. 8, no. 3, pp. 1–15, 2016. View at: Publisher Site  Google Scholar
 F. Wang, M. A. Mohd Zulkefli, Z. Sun, and K. A. Stelson, “Energy management strategy for a powersplit hydraulic hybrid wheel loader,” Proceedings of the Institution of Mechanical Engineers, Part D: Journal of Automobile Engineering, vol. 230, no. 8, pp. 1105–1120, 2016. View at: Publisher Site  Google Scholar
 P. Song, M. Tomizuka, and C. Zong, “A novel integrated chassis controller for full drivebywire vehicles,” Vehicle System Dynamics, vol. 53, no. 2, pp. 215–236, 2015. View at: Publisher Site  Google Scholar
 Y. Dai, Y. Luo, W. Chu, and K. Li, “Optimum tyre force distribution for fourwheelindependent drive electric vehicle with active front steering,” International Journal of Vehicle Design, vol. 65, no. 4, pp. 336–359, 2014. View at: Publisher Site  Google Scholar
 H. Fujimoto and K. Maeda, “Optimal yawrate control for electric vehicles with active frontrear steering and fourwheel drivingbraking force distribution,” in Proceedings of the 39th Annual Conference of the IEEE Industrial Electronics Society (IECON '13), pp. 6514–6519, IEEE, Vienna, AUSTRIA, November 2013. View at: Publisher Site  Google Scholar
 J. Kim, “Optimal power distribution of front and rear motors for minimizing energy consumption of 4wheeldrive electric vehicles,” International Journal of Automotive Technology, vol. 17, no. 2, pp. 319–326, 2016. View at: Publisher Site  Google Scholar
 A. Pennycott, L. De Novellis, A. Sabbatini, P. Gruber, and A. Sorniotti, “Reducing the motor power losses of a fourwheel drive, fully electric vehicle via wheel torque allocation,” Proceedings of the Institution of Mechanical Engineers, Part D: Journal of Automobile Engineering, vol. 228, no. 7, pp. 830–839, 2014. View at: Publisher Site  Google Scholar
 T. Cheong, S. H. Song, and C. Hu, “Strategic alliance with competitors in the electric vehicle market: tesla motor's case,” Mathematical Problems in Engineering, vol. 2016, Article ID 7210767, 10 pages, 2016. View at: Publisher Site  Google Scholar  MathSciNet
 H. He, J. Fan, Y. Li, and J. Li, “When to switch to a hybrid electric vehicle: a replacement optimisation decision,” Journal of Cleaner Production, vol. 148, pp. 295–303, 2017. View at: Publisher Site  Google Scholar
 Y. Suzuki, Y. Kano, and M. Abe, “A study on tyre force distribution controls for full drivebywire electric vehicle,” Vehicle System Dynamics, vol. 52, no. 1, pp. 235–250, 2014. View at: Publisher Site  Google Scholar
 Z.P. Yu, L.J. Zhang, and L. Xiong, “Optimized torque distribution control to achieve higher fuel economy of 4WD electric vehicle with four inwheel motors,” Journal of Tongji University, vol. 33, no. 10, pp. 79–85, 2005. View at: Google Scholar
 D. Wang and B. Wang, “Research on driving force optimal distribution and fuzzy decision control system for a dualmotor electric vehicle,” in Proceedings of the 34th Chinese Control Conference (CCC '15), pp. 8146–8153, IEEE, Hangzhou, China, July 2015. View at: Publisher Site  Google Scholar
 A. F. Izmailov, M. V. Solodov, and E. I. Uskov, “Globalizing stabilized sequential quadratic programming method by smooth primaldual exact penalty function,” Journal of Optimization Theory and Applications, vol. 169, no. 1, pp. 148–178, 2016. View at: Publisher Site  Google Scholar  MathSciNet
 M. A. Z. Raja, A. Zameer, A. U. Khan, and A. M. Wazwaz, “A new numerical approach to solve Thomas–Fermi model of an atom using bioinspired heuristics integrated with sequential quadratic programming,” SpringerPlus, vol. 5, no. 1, article 1400, 2016. View at: Publisher Site  Google Scholar
 J. Apolinar and M. Rodríguez, “Threedimensional microscope vision system based on micro laser line scanning and adaptive genetic algorithms,” Optics Communications, vol. 385, pp. 1–8, 2017. View at: Publisher Site  Google Scholar
 B. Bao, Y. Yang, Q. Chen, A. Liu, and J. Zhao, “Task allocation optimization in collaborative customized product development based on doublepopulation adaptive genetic algorithm,” Journal of Intelligent Manufacturing, vol. 27, no. 5, pp. 1097–1110, 2016. View at: Publisher Site  Google Scholar
 Y. Chen and M. S. Li, “A harmonic parameter estimation method based on Particle Swarm Optimizer with Natural Selection,” in Proceedings of the 1st International Conference on Information and Communication Technology Research (ICTRC '15), pp. 206–209, IEEE, Abu Dhabi, Arab Emipates, May 2015. View at: Publisher Site  Google Scholar
 Y. Hu, J. Lu, Y. Deng, and Z. Zhang, “MPPT algorithm based on particle swarm optimization with natural selection,” in Proceedings of the 3rd International Conference on Machinery, Materials and Information Technology Applications (ICMMITA '15), pp. 1814–1817, Atlantis Press, Qingdao, China, November 2015. View at: Publisher Site  Google Scholar
 H. Inoue, “Introduction of PC2008 hybrid hydraulic excavators,” Report, Komatsu, vol. 54, no. 161, pp. 1–6, 2008. View at: Google Scholar
 M. Ochiai and S. Ryu, “Hybrid in construction machinery,” in Proceedings of the 7th JFPS international symposium on fluid power, pp. 41–44, Toyama, Japan, September 2008. View at: Publisher Site  Google Scholar
 M. Ochiai, “Technical trend and problem in construction machinery,” Construction Machinery, vol. 38, no. 4, pp. 20–24, 2002. View at: Google Scholar
 S. Riyuu, M. Tamura, and M. Ochiai, “Hybrid construction machine,” Patent 2003328397, Japan, 2003. View at: Google Scholar
 J. Deere, “644K Hybrid Wheel Loader,” 2017, http://www.deere.com/wps/dcom/en_US/products/equipment/wheel_loaders/644k_hybrid/644k_hybrid.page. View at: Google Scholar
 J. Global, “L950 Wheel Loader,” 2017, https://mining.komatsu/productdetails/l950#!technology. View at: Google Scholar
 S. Hui and J. Junqing, “Research on the system configuration and energy control strategy for parallel hydraulic hybrid loader,” Automation in Construction, vol. 19, no. 2, pp. 213–220, 2010. View at: Publisher Site  Google Scholar
 N. Zhou, E. Zhang, Q. Wang et al., “Compound hybrid wheel loader,” Patent CN102653228A, China, 2012. View at: Google Scholar
 M. P. Aghababa, “3D path planning for underwater vehicles using five evolutionary optimization algorithms avoiding static and energetic obstacles,” Applied Ocean Research, vol. 38, pp. 48–62, 2012. View at: Publisher Site  Google Scholar
Copyright
Copyright © 2017 Zhiyu Yang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.