 Original Article
 Open access
 Published:
Simple PushType Wave Generating Method Using Digital Rotary Valve Control
Chinese Journal of Mechanical Engineering volume 33, Article number: 5 (2020)
Abstract
The important parameters to describe waves are their amplitude and length. In order to make it easier to improve wave amplitude and facilitate wave experiment, a simple pushtype wave generating method using digital rotary valve control was proposed and different wave amplitudes were generated by the new method. After the mathematical model of the new method had been established, numerical analysis based on the linear wave theory was carried out by means of Matlab/Simulink software tools, and experiments were conducted on the pushtype wave maker to ascertain the validity of the established model and the numerical simulation results. It shows that both experimental and theoretical results agree relatively well, and the plate motion frequency and amplitude of the pushtype wave maker can be continuously adjusted and the various required regular waves can be obtained. Although the wave amplitude and length descends with the increasing of working frequency, the wave amplitude can be improved conveniently by setting the axial opening width of the valve and the oil supply pressure of system. The wave length remains unchanged with the axial opening width and the oil supply pressure change. The research indicates that different regular waves can be easily generated by the new method and the wave amplitude can be further improved in a certain plate motion frequency range.
1 Introduction
The wave maker is one of the most important facilities in the research field of ocean engineering and hydraulic engineering. Its performance of wave simulation has an effect on the testing of sea keeping. As the wave maker plays an extremely important role in engineering research, the theory and implementation of wave generation have been attracting extensive attention for years. Scientists often perform laboratory experiments on the basis of pushtype wave makers, which move a wave plate to generate waves [1, 2]. Refs. [3, 4] facilitates the generation of arbitrary finiteamplitude waves at any distance from the wave maker. Moronkeji [5] performed experimental studies using electrically driven wave plates to improve plate amplitude. Teng et al. [6] reported a variation of the commonly used pushtype wave maker principle. By varying the speed and distance between the carriage and plate, waves of different amplitudes were generated. This method resolved the problem related to limiting the plate amplitude of pushtype wave makers. The study of Wu et al. [7] on long waves generated by a pushtype wave maker concludes that the method proposed by Wu et al. [8] was effective for generating solitary waves of stable height. The technology of generating white noise wave requires that wave amplitudes remain stable in a certain plate frequency range. White noise wave spectrum is basically flat in the floating objects test and this technology makes frequency response function more reliable in experiment analysis in a large frequency range [9].
The wave generator driven by electric motor is widely used in low load; for example, rocker flap wave maker. Conversely, the hydraulic wave generator could produce high torque with quickresponse and highaccuracy, thus it can be applied in pushtype wave maker in heavy load. Electrohydraulic servo technology was frequently adopted as a solution of highpower and highaccuracy vibration systems in recent years [10, 11]. To obtain the high flow, thrust, and frequency in these driving systems, a variety of electrohydraulic excitation devices with high thrust and high frequency were studied by many scholars, as a result, the AC servo hydraulic vibration technology, as well as the new electrohydraulic digital control technology, etc. were presented [12, 13]. Many scholars have been seeking new control elements to satisfy specific engineering requirements. For example, Hao et al. [14] utilized rotary valve structure to increase the wave frequency of exciter, and applied it to coal industry, metallurgical industry, construction industry, etc. Ruan et al. [15] proposed a high frequency electrohydraulic exciter with rotary valve and studied the frequency characteristic of electrohydraulic exciter, high frequency signal acquisition and control of typical excited wave forms. Ren et al. [16] studied vibration waveforms excited by an electrohydraulic exciter with a twodimensional rotary valve theoretically and experimentally. Other similar progresses include equilibrium hydraulic rotary valve with high pressure, large flow and electrohydraulic rotary valve studied at Zhejiang University [17, 18] and rotating shaft hydraulic rotary valve with good manufacturability designed by Marcus [19]. A fluid driven PWM valve based on a unidirectional rotary spool was presented, and it was found that the rotary valve reduced actuation power from a cubic dependence to a square dependence by eliminating motion reversals during transition [20]. Liu et al. [21, 22] designed a single stage rotary valve for application to high energy and variablefrequency vibration condition. The single stage rotary valve can be used to obtain the required vibration frequency and waveform by controlling the rotary velocity of spool, and thus meet different working requirements of tamping device.
In this paper, to make it easier to generate waves and improve wave amplitude in a certain plate frequency range, a simple pushtype wave generating method using digital rotary valve control was proposed [23] and developed, and the control system model was established, and different wave amplitudes and lengths were generated and further analyzed.
2 Working Principle and Test Rig
The working principle of the novel digital rotary valvecontrolled cylinder system is shown in Figure 1. It is composed mainly of a doubleacting hydraulic servo cylinder, a digital rotary valve, an electrohydraulic proportional axial variable piston pump, and a proportional relief valve. The wave experiment rig, as shown in Figure 1, includes a water tank (0.6 m wide×1.2 m high×12 m long), an electrohydraulic control system, a wave generation mechanism and a wave height meter.
The working principle and structure of the designed rotary valve are shown in Figure 2. It can be seen that 4 shoulders with same structure are designed and manufactured on the rotary valve spool. The rotary frequency of the spool can be controlled by a servo motor, and the axial displacement of the spool can be controlled by a linear stepper motor, thus the opening of the spool as well as the flow through the opening can be controlled. The valve ports are designed symmetrical, so that the opening area of the valve ports on the front shoulder 1 can change from zero to the maximum, and from the maximum to zero, then so can the opening area of the corresponding valve ports on the nearby shoulder 4 do. On the other hand, when one valve port is closed, another valve port on the opposite side of the same shoulder is just open, keeping the valve on working order.
When the valve core rotates to the specific angle as shown in Figure 2(a), oil flows from port P to port B, and then from port A to port T. In this case, the cylinder moves to the right. When the valve core rotates to another angle as shown in Figure 2(b), oil flows from P to A, and then from B to T, driving the cylinder to the left. With the change of servo motor’s speed, the frequency of the rotary valve core changes, leading to the change of wave maker’s working frequency. To meet higher flow for cylinder motion, linear flow and pressure control requirements, grooves in the valve core and windows in the sleeve are designed to be rectangular accordingly.
A test rig of wave experiment was established to validate the new working principle. By adjusting the stepper motor and the servo motor, we can control the axial displacement and the rotational speed of valve core respectively. Supply oil pressure can be set through the proportional relief valve. Consequently, the amplitude of wave plate becomes adjustable and the frequency of wave plate changeable. The experimental instruments are shown in Table 1. The main parameters of the new wave maker system are listed in Table 2. The operation parameters with instruments are listed in Table 3.
3 Mathematical Modelling
According to the Figure 1, the hydraulic transmission model is shown in Figure 3. The bottom of water tank is smooth and the hydrostatic depth is d. In the distal wave trough, there is no reflection, wave completely absorbed by the wave damper. Assume that the wave propagation direction is the positive x axis, the vertical direction is the positive z axis, the origin of the coordinate is on the surface of the water. The wave amplitude is much less than the wave length. Φ is the velocity potential function. The boundary value problem for the wave maker in the wave tank follows directly from the boundary value problem for twodimensional waves propagating in an inviscid, incompressible, irrotational fluid. Boundary value problem specification for periodic water waves is shown in Figure 3. According to the above assumptions, the potential flow theory and small amplitude wave theory [24,25,26], the equation of wave amplitude of the front plate a0 and plate amplitude e in different cycles is expressed as follows:
where H_{0} is the wave height, d is the depth of water, e_{1}, e_{2} are the amplitudes of plate motion distance from the bottom d_{1}, d_{2}, respectively, e is the amplitude of plate motion at water surface.
For pushtype wave maker, \( e_{1} = e_{2} = e,d_{1} = d,d_{2} = 0 \). According to the cylinder connection point of Figure 1, e (namely, the amplitude of wave plate) is equal to the motion displacement of hydraulic cylinder y_{p}, so:
The relation of the wave number k and the angular velocity of wave ω meets the dispersion formula: ω^{2} = 4π^{2} f^{2}_{j} = gktanh(kd) [1], where f_{j} is the working frequency of the wave plate, namely the hydraulic cylinder working frequency. k cannot be directly obtained from the above formula, where k can be solved by means of Matlab software tool . The parameter values of k and T_{1} used in the calculation are listed in Table 4.
The equivalent bridge of the rotary valvecontrolled cylinder system is shown in Figure 4. It is assumed that the system pressure p_{s} is constant, the total supply flow is q_{s}, q_{L} is the flow through the load and p_{L} is the pressure drop across the load.
The equations of flow through the orifices 1, 2, 3 and 4 are expressed as follows:
where p_{1} and p_{2} are the pressure of hydraulic cylinder two cavity respectively, C_{d} is the flow rate coefficient, ρ is the oil density, and S_{vi} (i = 1, 2, 3, 4) are orifice area of valve ports on the correspondent shoulder i.
Firstly, it is assumed that the connecting pipeline between rotary valve and hydraulic cylinder is short, thick and symmetrical enough, the dynamic loss and the pressure loss of the pipe can be ignored, the oil temperature and bulk modulus of hydraulic oil are constant, and the leakage of hydraulic cylinder is zero. When the cylinder moves to the right, the flow rate continuity equations of the chamber of the cylinder can be used.
The left chamber is
whereas the right chamber is
where V_{1} is the volume of forward chamber, V_{1} = V_{o1}+A_{p}y_{p}, V_{o1} is the initial volume of forward chamber, V_{2} is the volume of return chamber, V_{2} = V_{t} – (V_{o1}+A_{p}y_{p}), V_{t} is the total volume of cylinder chambers, β_{e} is the effective bulk modulus of oil and is assumed to be as constant in Low pressure test, A_{p} is the area of piston.
As the orifices are both matched and symmetrical, the flows in diagonally opposite arms of the bridge, as shown in Figure 4, are equal. Therefore, \( S_{{{\text{v}}1}} \left( \theta \right) = S_{{{\text{v}}3}} \left( {\theta +\uppi} \right), \) \( S_{{{\text{v}}4}} (\theta ) = S_{{{\text{v}}2}} (\theta +\uppi). \)
The equations of the flow through the orifices in a cycle are expressed as follows:
If the external leakage and internal leakage are zero, and p_{s} = p_{1}+p_{2}, p_{L} = p_{1}−p_{2}, the load flow of the cylinder is \( q_{\text{L}} = q_{\text{v1}}  q_{\text{v2}} \). That is,
The total open area is S_{vi} = 2x_{v}y_{vi}, where x_{v} is the axial opening width of the valve.
It is assumed that the opening circumferential conduction width of B and A are y_{v1} and y_{v4}, respectively. If y_{v1} is from zero to the maximum, then from the maximum to zero, after that, to enter the next opening port of nearby shoulder subsequently, y_{v4} is also from zero to the maximum, then from the maximum to zero, so the equations of y_{v1} and y_{v4} are:
where R is the radius of the spool shoulder, f is the rotational frequency of spool, and ω_{1} is the rotational angular velocity of valve spool.
Figure 2 shows that a single complete cycle of spool and the twice of oil reversing make hydraulic cylinder oscillating back and forth twice, so the relation between the working frequency of hydraulic cylinder and the rotational frequency of spool is\( f_{\text{j}} = 2f \).
The equation of motion for the cylinder is
where m_{t} is the equivalent mass, B_{c} is the total damping coefficient, and F_{L} is the force by the action of water on the plate. The system is greatly affected by the mass inertial force and the force by the action of water on the plate, the effect of other forces are so little that can be neglected when conducting actual calculation.
The wavefront equation of the twodimensional small amplitude propulsion wave with constant depth is
where \( \theta \) is the phase of the wave. The determination of the constants \( k \) and \( \omega \) is as follows:
(1) When x is increased or decreased by one wave length L, the wavefront height η should be constant. This must make
(2) When the time increments by one cycle T, the wave surface height of the same point should be constant, that is
Based on the above dispersion formula: ω^{2} = gktanh(kd) [1], substitute into Eqs. (16) and (17), so:
The relation between the working frequency of hydraulic cylinder and the rotational frequency of spool is \( f_{\text{j}} = 2f \), so: T = 1/\( f_{\text{j}} = 1/2f \).
4 Theoretical and Experimental Results
Figure 5 show the wave experiment and acquisition interface system of wave height meter. The distance between the wave height meter is X, the time difference of initial wave height data is \( \Delta t \). We can get L from the equation \( L = {X \mathord{\left/ {\vphantom {X {\Delta tf_{j} }}} \right. \kern0pt} {\Delta tf_{j} }} \) with the experimental data.
Test values in the wave experiment were compared with those obtained in the numerical analysis. It was assumed that the initial point of cylinder piston is in the middle with the maximum opening of valve port, and the cylinder to the right direction is positive to correspond to the hydraulic transmission model. The main factors and the control parameters for wave experiment can be obtained by continuously adjusting different input parameters (x_{v}, p_{s} and f_{j}), and analyzing output curves (y_{p}, L and a_{0}) in the solution process of mathematical models by means of Simulink software tool.
In the actual operation, because no feedbacks were used in the hydraulic control system, the cylinder piston rod was set to the leftmost position in each experiment and the valve port was set to closed at the same time. Therefore, the motion displacement of hydraulic cylinder in a cycle was 2y_{p}. The wave height H_{0} (2a_{0max}) of experimental data was measured by the wave height meter.
4.1 Influence of Different x _{v} and f _{j} on Wave Simulation
Figure 6 and Figure 7(a) show the y_{p}t and a_{0}t curves under different x_{v} at the working frequency of 1 Hz. From equation S = 2x_{v}y_{vi}, Figure 6 and Figure 7(a), S_{v} is determined by x_{v}, directly affecting y_{p} and a_{0}, Thus, x_{v} is the crucial factor for the motion amplitude of hydraulic cylinder and wave amplitude, and the bigger x_{v} is, the bigger S_{v}, y_{p} and a_{0} will be. Under the condition of 1.0 MPa (oil supply pressure), 1 Hz (Plate motion frequency, T_{1} = 1.54), 2.0 mm (Axial opening width), the maximum wave amplitude can reach to 64 mm. It can be seen from Figure 6 and Table 5 that test value and theoretical value in the maximum wave amplitude a_{0max} agree relatively well.
Figure 7(b) shows a_{0} and y_{p} under different work frequencies at 1.0 MPa oil supply pressure. From Figure 7(b), it can be seen that when work frequency is 1.6 Hz (T_{1} = 2), the maximum amplitude of the cylinder is 16 mm (x_{v} is set to 1 mm) or 21 mm (x_{v} is set to 2 mm), and a_{0max} is 32 mm (x_{v} is set to 1 mm) or 42 mm (x_{v} is set to 2 mm). When work frequency is 2 Hz (T_{1} = 2), the maximum amplitude of the cylinder is 12 mm (x_{v} is set to 1 mm) or 15 mm (x_{v} is set to 2 mm), and a_{0max} is 24 mm (x_{v} is set to 1 mm) or 30 mm (x_{v} is set to 2 mm). It can be also drawn from the curve of different work frequencies that the value of a_{0} can be determined by x_{v}. A larger value of x_{v} will lead to larger a_{0}.
Figure 7(c) shows the relationship between the working frequency and a_{0max} (H_{0}/2) under different x_{v}. The wave amplitude descends with the increase of the plate working frequency, the higher the working frequency, the smaller the wave amplitude. a_{01} (x_{v} is set to 2 mm) is higher than a_{02} (x_{v} is set to 1.5 mm), and a_{02} (x_{v} is set to 1.5 mm) is higher than a_{03} (x_{v} is set to 1 mm). The main comparison between theoretical and test values of a_{0max} under the same pressure are shown in Table 5. The test results under different x_{v} are in accordance with the theoretical calculation results, but the test values are slightly lower than the theoretical values.
Figure 7(d) shows the relationship between the working frequency and L under different x_{v}. The wave length descends with the increase of the plate working frequency, the higher the working frequency, the smaller the wave length. At the same frequency, the wave length remains unchanged with the axial opening width change. The main comparison between theoretical and test values of L under the same pressure are shown in Table 5. The test results under different x_{v} are in accordance with the theoretical calculation results.
4.2 Influence of Different p _{s} and f _{j} on Wave Simulation
Figure 8(a) shows y_{p} and a_{0} curves under different oil supply pressure. It can be seen from Figure 8(a), when f_{j} is set to 1 Hz, x_{v} is set to 1 mm, the maximum amplitude of the cylinder can reach to 25 mm under the pressure of 0.9 MPa, 31 mm under the pressure of 1.0 MPa, 36 mm under the pressure of 1.2 MPa, and a_{0max} can reach to 39 mm under the pressure of 0.9 MPa, 48 mm under the pressure of 1.0 MPa, 55 mm under the pressure of 1.2 MPa. Numerical curve shows that a_{0} can be controlled by the oil supply pressure. The higher the oil supply pressure, the larger the wave plate amplitudes and wave amplitudes. It can be seen from Figure 8 and Table 6 that test value and theoretical value in the maximum wave amplitude agree relatively well.
Figure 8(b) shows a_{0} at different work frequencies when x_{v} is set to 1 mm. It can be seen from the Figure 8(b) that when the work frequency is 1.6 Hz (T_{1} = 2), the maximum amplitude of the cylinder is 15 mm (p_{s} is set to 1.0 MPa) or 18 mm (p_{s} is set to 1.2 MPa), and a_{0max} is 30 mm (p_{s} is set to 1.0 MPa) or 36 mm (p_{s} is set to 1.2 MPa). When the work frequency is 2 Hz (T_{1} = 2), the maximum amplitude of the cylinder is 12 mm (p_{s} is set to 1.0 MPa) or 14 mm (p_{s} is set to 1.2 MPa), and a_{0max} is 24 mm (p_{s} is set to 1.0 MPa) or 28 mm (p_{s} is set to 1.2 MPa). It can be also drawn from the curve of different work frequencies that the value of a_{0} can be determined by p_{s}. The higher the p_{s}, the greater the a_{0}.
Figure 8(c) shows the relationship between the working frequency and the a_{0max} (H_{0}/2) under different supply pressure. a_{01} (p_{s} is set to 1.2 MPa) is higher than a_{02} (p_{s} is set to 1.0 MPa). The test results under different p_{s} are in accordance with the theoretical calculation results. It can be seen from Figure 7(c) and Figure 8(c), a_{0} descends with the increasing of working frequency. The main comparison between theoretical and test values of a_{0max} under the same x_{v} are shown in Table 6. Test values are slightly lower than the theoretical values. The differences between the test and theoretical values in Table 5 and Table 6 are mainly caused by water leaks from the gaps at both sides of the wave paddle.
Figure 8(d) shows the relationship between the working frequency and L under different supply pressure. At the same frequency, the wave length remains unchanged with the supply pressure change. The main comparison between theoretical and test values of L under the same x_{v} are shown in Table 6. The test results under different supply pressure are in accordance with the theoretical calculation results.
5 Conclusions
The experiment and analysis results show that the motion frequency and amplitude of pushtype wave maker can be continuously adjusted and the various required regular waves can be obtained conveniently. The axial opening width of the valve is the crucial factor for the plate amplitude and the wave amplitude. A larger value of the axial opening width lead to larger the wave plate amplitude and wave amplitude. The wave amplitude also depends on oil supply pressure, the higher the oil supply pressure, the greater the plate amplitude and the wave amplitude. At the same water depth, the working frequency of push plate determines wave number and wave length. Wave length is not affected by the axial opening width and the oil supply pressure. Although the wave amplitude and length descends with the increase of the working frequency, the wave amplitude can be easily improved by setting the axial opening width of the valve and the oil supply pressure of the system. These results indicate that different regular waves can be obtained conveniently by the new wave generating method, and the wave amplitude can be further improved in a certain plate frequency range. These facilitate convenient implementation of wave experiment. Based on the characteristics of high power electrohydraulic system, the new approach demonstrates its potential application to achieve highpower wave experiment with highpower wave maker system.
Considering the feasibility and practicability of the rotary valvecontrolled cylinder system applied to highpower wave experiment, future efforts will focus on practical application of the highpower wave maker. Future work includes vibration cylinder bias compensation with feedbacks, optimized and integrated design of the device.
Abbreviations
 A _{p} :

Area of piston
 a _{0} :

Wave amplitude
 B _{c} :

Total damping coefficient
 C _{d} :

Flow rate coefficient
 d :

Depth of water
 e :

Amplitude of wave plate (water surface)
 e _{1} :

Amplitude of plate distancing from the bottom d_{1}
 e _{2} :

Amplitude of plate distancing from the bottom d_{2}
 F _{L} :

Force by the action of water on the plate
 f :

Rotary frequency of spool
 f _{j} :

Working frequency of the wave plate
 g :

Gravitational acceleration
 H _{0} :

Wave height (2a_{0})
 k :

Wave number
 L :

Wave length
 m _{t} :

Equivalent mass
 p _{L} :

Pressure drop across the load
 p _{1}, p _{2} :

Pressure of hydraulic cylinder two cavity
 p _{s} :

System pressure
 q _{s} :

Total supply flow
 q _{L} :

Flow through load
 R :

Radius of spool shoulder
 T :

Ratio of wave amplitude and paddle amplitude
 S _{i} :

Orifice area of different valve ports
 V _{1} :

Volume of forward chamber
 V _{2} :

Volume of return chamber
 V _{o1} :

Initial volume of forward chamber
 V _{t} :

Total volume of cylinder chamber
 x _{v} :

Axial opening width of valve
 y _{p} :

Amplitude of wave plate (hydraulic cylinder)
 y _{vi} :

Opening circumferential conduction width
 β _{e} :

Effective bulk modulus of oil
 ρ :

Oil density
 ω :

Angular velocity of wave
 ω _{1} :

Rotational angular velocity of valve spool
 Φ :

Velocity potential function
References
R Dean, R Darymple. Water wave mechanics for engineers and scientists. World Scientific, 1991.
H A Schaffer. Secondorder wave maker theory for irregular waves. Ocean Engineering, 1996, 23(1): 4788.
C E Synolakis. Generation of long waves in laboratory. Journal of Waterway, Port, Coastal, and Ocean Engineering, 1990, 166(2): 252266.
D G Goring. Tsunamis—The propagation of long waves onto a shelf. Pasadena, California: California Institute of Technology, 1979.
A Moronkeji. Physical modelling of tsunami induced sediment transport and scour. Proceedings of the 2007 Earthquake Engineering Symposium for Young Researchers, 2007.
M H Teng, K Feng, T I Liao. Experimental study on long wave runup on plane beaches. Proceeding of the Tenth International Offshore and Polar Engineering Conference, Seattle, USA, 2000: 660664.
N J Wu, S C Hsiao, H H Chen, et al. The study on solitary waves generated by a pistontype wave maker. Ocean Engineering, 2016, 117(1): 114129.
N J Wu, T K Tsay, Y Y Chen. Generation of stable solitary waves by a pistontype wave maker. Wave Motion, 2014, 51(2): 240255.
H W Li, Y J Pang, Z Sun. Simulation of white noise irregular wave and focused wave in ocean basin. Huazhong University of Science and Technology, 2013, 41(1): 8992.
G SHEN, Z C ZHU, W D ZHU, et al. Realtime tracking control of electrohydraulic force servo systems using offline feedback control and adaptive control. ISA Transactions, 2017, 67: 356370.
G Shen, Z C Zhu, X Li, et al. Realtime electrohydraulic hybrid system for structural testing subjected to vibration and force loading. Mechatronics, 2016, 33: 4970.
Y Ren, X C Ji, J Ruan. Output characteristics of a horizontal type electrohydraulic excitation system with inertial loading: Modeling and experimentation. Journal of Mechanical Science and Technology, 2019, 33(11): 51575167.
Y Ren, H S Tang, J W Xiang. Experimental and numerical investigations of hydraulic resonance characteristics of the highfrequency excitation system. Mechanical System and Signal Processing, 2019, 131: 617632.
J G Hao, Y C Zhang. Study on the properties of a new electrohydraulic exciting system. Journal of Taiyuan University of Technology, 2003, 6: 706709.
W R Li, J Ruan, Y Ren, et al. Research on lowfrequency characteristics of onepole vibration cylinder controlled by 2D valve. Proc. 8th ICFP, 2013: 188192.
Y Ren, J Ruan. Theoretical and experimental investigation of vibration waveforms excited by an electrohydraulic type exciter for fatigue with a twodimensional rotary valve. Mechatronics, 2016, 33: 161172.
J Cui, F Ding, Q P Li. Novel bidirectional rotary proportional actuator for electrohydraulic rotary valves. IEEE Transactions on Magnetics, 2007, 43(7): 32543258.
J Cui, F Ding, Q P Li. Static torque characteristics of highpressure bidirectional rotary proportional solenoid. Journal of Zhejiang University, 2007, 41(9): 15781581.
B L Marcus. Rotary servo valve. U.S. Patent 5954093, Sept. 21, 1999.
H C Tu, M B Rannow, M Wang, et al. Design, modeling, and validation of a highspeed rotary pulsewidthmodulation on/off hydraulic valve. Journal of Dynamic Systems, Measurement and Control, 2012, 134(11): 112.
Y Liu, S K Cheng, G F Gong. Structure characteristics of valve port in the rotationspooltype electrohydraulic vibrator. Journal of Vibration and Control, 2017, 23(13): 21792189.
Y Liu, G F Gong, H Y Yang, et al. Regulating characteristics of new tamping device exciter controlled by rotary valve. IEEE/ASME Transactions on Mechatronics, 2016, 21(1): 497505.
Y Liu, S K Cheng, M J Zhu, et al. A wave machine based on hydraulic drive mode:China, 201410060768.8. 20140521.
J P Giesing. Twodimensional potential flow theory for multiple bodies in smallamplitude motion. AIAA Journal, 2015, 8(11): 19441953.
Q Zang, J Huang, Z Liang. Slosh suppression for infinite modes in a moving liquid container. IEEE/ASME Trans. on Mechatoronics, 2015, 20(1): 105114.
Y X Yu. Random wave and its application in engineering. Dalian: Dalian University of Technology Press, 2011.
Funding
Supported by National Natural Science Foundation of China (Grant Nos. 51605431, 51705456), Ningbo Municipal Natural Science Foundation of China (Grant No. 2019A610162), and Ningbo Major Scientific and Technological Projects (Grant No. 2017C110005).
Author information
Authors and Affiliations
Contributions
YL was in charge of the whole trial; JZ wrote the manuscript; RS and JC determined the subject discussed and wrote an outline; QX and FH assisted with revision and translation. All authors read and approved the final manuscript.
Authors’ Information
Yi Liu, received his PhD degree in mechanical engineering from Zhejiang University, China, in 2013. Since 2013, he has been an associate professor with Zhejiang University, Ningbo Institute of Technology. His current research interests include electrohydraulic control systems of vibration exciters and mechatronic systems design.
Jiafei Zheng, received the bachelor degree in machine design manufacture and automation from Ningbo Institute of Technology, Zhejiang University, China, in 2018. She became a graduate student with Soochow University, China. Her current research interests include wave simulation control, controlling and optimizing of the complex system, development of production management information system.
Ruiyin Song, born in 1974, is currently an associate professor at Ningbo Institute of Technology, Zhejiang University, China. He received his PhD degree from Zhejiang University, China, in 2006. His research interests include wave energy generation technology and wave simulation control.
Qiaoning Xu, received the PhD degree in mechanical engineering from Zhejiang University, China, in 2015. Since 2015, she has been in Zhejiang University of Technology, China. Her current research interests include fault diagnosis for hydraulic systems and electrohydraulic system control.
Junhua Chen, received his Ph.D. degree in mechanical engineering from Nanchang University, China, in 2011. Since 2018, He was the Vice Chairman of Ningbo Mechanical Engineering Society. His current research interests include marine equipment and mechatronics.
Fangping Huang, received his Master’s degree in mechanical engineering from Zhejiang University, China, in 2005. Since 2010, he has been an associate professor with Ningbo Institute of Technology, Zhejiang University. His current research interests include electrohydraulic control systems and mechatronic systems design.
Corresponding author
Ethics declarations
Competing interests
The authors declare that they have no competing interests.
Rights and permissions
Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.
About this article
Cite this article
Liu, Y., Zheng, J., Song, R. et al. Simple PushType Wave Generating Method Using Digital Rotary Valve Control. Chin. J. Mech. Eng. 33, 5 (2020). https://doi.org/10.1186/s1003301904294
Received:
Revised:
Accepted:
Published:
DOI: https://doi.org/10.1186/s1003301904294