01.12.2020  Original Article  Ausgabe 1/2020 Open Access
Analysis of Power Matching on Energy Savings of a Pneumatic Rotary Actuator ServoControl System
 Zeitschrift:
 Chinese Journal of Mechanical Engineering > Ausgabe 1/2020
1 Introduction
The problem of energy shortages has become increasingly significant with the rapid development of society. In addition to discovering new energy sources, energy conservation is the most effective and important measure to fundamentally solve the energy problem [
1]. Energy saving has increasingly become a hot topic of concern. Energy has always been a constraint to economic development, which makes energysaving research more urgent and practical [
2]. Currently, pneumatic technology is widely used in various fields of industry, and has become an important technical means of transmission and control [
3,
4]. The use of existing technology to improve the energy utilization rate of energyconsuming equipment is an important energysaving method [
5].
However, the energy efficiency of pneumatic technology is relatively low [
6]. Therefore, improving the efficiency of energy utilization and reducing the energy loss of pneumatic systems have become the concern of scholars all over the world [
7,
8].
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Pneumatic systems have three aspects of energy wastage [
9,
10]: (1) gas and power losses during compressor gas production, (2) pressure loss in the gas supply pipeline, and (3) gas leakage from the gas equipment [
11]. Accordingly, many methods are available to solve these problems. For the pressure loss in the air source, the timing of opening and closing of multiple air compressors can be optimized, and the gas production process of the air compressors can also be optimized, such as making full use of the expansion of compressed air to reduce unnecessary power consumption [
12]. In order to reduce pressure loss in the pipeline, the method of reducing the pressure in the gas supply pipeline can be adopted [
13]. When necessary, a supercharger can be added in front of the terminal equipment. For gas leakage from the gas equipment, optimizing the component structure is usually implemented to solve this problem. The pneumatic servocontrol system precisely controls the angle of rotation; however, energy loss still occurs in the system. For this system, reducing the gas supply pressure is the most effective way of reducing the energy loss. Determining the critical pressure and reducing the gas supply pressure as much as possible while ensuring normal operation of the system are the key. The powermatching method can solve the optimization problem of the gas supply pressure based on the power required by the system [
14]. In flow compensation, different compensation controllers can also be designed to match the flow and the system to realize the purpose of energy savings [
15,
16]. Problems arise with regard to the high energy consumption and poor controllability of the rotary system of a hydraulic excavator due to throttle loss and overflow loss in the control valve during frequent acceleration and deceleration with large inertia. Therefore, Huang et al. [
17] proposed the flow matching of a pump valve joint control and an independent measurement method of the hydraulic excavator rotary system to improve the energy efficiency of the system and reduce throttle loss. Xu et al. [
18] designed a dynamic bypass pressure compensation circuit of a load sensing system, which solved the problems of pressure shock and energy loss caused by excessive flow and improved the efficiency and controllability of the system. Kan et al. [
19] analyzed the basic characteristics of a hydraulic transmission system for wheel loaders using numerical calculation and adopted the optimal design method of a powermatching system. This improved the efficient working area of the system and average efficiency in the transportation process, and reduced the average working fuel consumption rate. Yang et al. designed an electrohydraulic flowmatching controller with shunt ability to improve the dynamic characteristics and energysaving effect and improve the stability of the system [
20]. Guo et al. [
21] used genetic algorithm to optimize the parameters of an asynchronous motor to achieve energy savings and consumption reduction, which proved the effectiveness and practicability of the power matching method of an electric pump system. Wang et al. [
22] matched an engine and a generator to achieve efficiency optimization and obtained a common high efficiency area. They proposed a partial power tracking control strategy. Lai et al. [
23] proposed a parameter matching method for an accumulator in a parallel hydraulic hybrid excavator and optimized the parameter matching process of the main components such as the engine, accumulator, and hydraulic secondary regulatory pump using genetic algorithm to reduce the installed power. Yan et al. [
24] focused on the problem in which the flow of a constant displacement pump could not match with the changing load, resulting in energy loss. They proposed an electrohydraulic flowmatching steering control method, which used a servo motor to drive a constant displacement pump independently to reduce the energy consumption of the system. At present, many studies on energy savings are conducted using the power matching method in the hydraulic system, but only few focus on the pneumatic system [
25].
In the present study, a method of reducing the gas supply pressure is implemented to reduce energy loss of a pneumatic rotary actuator servocontrol system. The output and load characteristic curves of the system are derived, and the power source characteristic curve is matched to determine the optimal gas supply pressure. Finally, the experiment verifies the energysaving effect under this gas supply pressure.
Through theoretical analysis and experimental verification of the application platform of the pneumatic rotary actuator, a method of function matching and energy optimization method for the pneumatic rotary actuator under normal working conditions is proposed for the first time.
2 Experimental Platform
Figure
1 shows the schematic diagram of the pneumatic rotary actuator servocontrol system.
×
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As a gas source, the air compressor provides power to the system. The air filter, air regulator, and air lubricator are used to filter and clean the gas. When the driving voltage signal of the proportional directional control valve is given, the proportional valve controls the flow and direction of the gas, and then controls the rotary motion of the pneumatic rotary actuator. The rotary encoder measures the angular displacement and transmits the TTL (Transistor–Transistor Logic) level signals to the data acquisition card. The data acquisition card is installed in the industrial personal computer which calls the program of the upper computer, samples the encoder signal, and outputs a 0–10 V voltage signal through the controller calculation. The driving voltage signal output by the controller further regulates the flow and direction of the proportional directional control valve to reduce the angle error. After continuous iteration, the angle error of the system decreases and tends to stabilize.
Figure
2 shows the experimental platform of the pneumatic rotary actuator servocontrol system. The round steel passes through the pneumatic rotary actuator and is connected to the rotary encoder through the coupling. The pneumatic rotary actuator is horizontally installed.
×
By selecting the MPYEM5010B model proportional valve with a smaller range, we can more easily ensure the control accuracy of the system. The SMC MSQA30A pneumatic rotary actuator is adopted. The actuator has a highprecision ball bearing and belongs to a highprecision actuator type. The rotating platform of the actuator contains many symmetrical threaded holes for easy introduction of loads. A highprecision rotary encoder is used, and the 20000P/R resolution corresponds to an accuracy of 1.8 × 10
^{−2}°, which satisfies the highprecision measurement for the rotation angle. In addition, the air compressor and the filter, regulator, and lubricator (F. R. L.) units satisfy the gas supply pressure of at least 0.8 MPa. The digital I/O port and analog output port of the dataacquisition card must meet the experimental requirements, and the higher digit counter in the dataacquisition card improves the system response speed. The models and parameters of the components are listed in Table
1.
Table 1
Models and parameters of the components
Component

Model

Parameter


Air compressor

PANDA 75030L

Maximum supply pressure: 0.8 MPa

F. R. L. units

AC300003

Maximum working pressure: 1.0 MPa

Proportionaldirectional control valve

FESTO MPYE5M5010B

3position 5way valve, 0–10 V driving voltage

Pneumatic rotary actuator

SMC MSQA30A

Bore: 30 mm; stroke: 190°

Rotary Encoder

GSS06LDHRAG20000Z1

Resolution: 20000P/R

Dataacquisition card

NI PCI6229

32bit counter; from − 10 V to + 10 V output voltage

Industrial personal computer

ADVANTECH IPC610H

Standard configuration

In some experimental tests, measuring the flow rate, pressure, and temperature of the gas is necessary, which can be performed using a flow sensor, a pressure transmitter, and a temperature transmitter (thermocouple), respectively. The flow rate in the inlet and outlet is measured using a flow sensor in the FESTO SFAB series with a range of 2–200 L/min, and the flow rate of the leak port is measured using a flow sensor with a range of 0.1–5 L/min in the SFAH series. The MIKP300 pressure transmitter has high accuracy and fast response and can accurately measure the pressure changes. A thermocouple is used as a temperature transmitter to measure the gas temperature. To prevent signal interference, a temperature isolator is added to the circuit for the temperature signal transmission. The models and parameters of the test components are listed in Table
2. The circuit connection of the experimental platform is shown in Figure
3.
Table 2
Models and parameters of the test components
Component

Model

Parameter


Pressure transmitter

MIKP300

Range: 0–1.0 MPa; accuracy: 0.3% FS

Flow sensor 1

FESTO SFAB200UHQ82SVM12

Range: 2–200 L/min; accuracy: 3% o.m.v. + 0.3% FS

Flow sensor 2

FESTO SFAH5UQ6SPNLKPNVBAM8

Range: 0.1–5 L/min; accuracy: 2% o.m.v. + 1% FS

Temperature transmitter (thermocouple)

TTK36 (K type, diameter: 0.1 mm)

Range: 0–260°; accuracy: 0.4% FS

Temperature isolator

SLDTR2P11

Response time: ≤ 10 ms; accuracy: 0.1% FS

×
The schematic diagram of the valvecontrolled cylinder system is constructed according to the experimental platform, as shown in Figure
4. The system consists of Chamber
a and Chamber
b. The dashed lines represent the boundaries of the chambers. Figure
4 shows the gasflow mechanism when the spool moves to the right, and
\(\dot{m}_{\text{a}}\),
\(\dot{m}_{\text{b}}\) represent the mass flow rates of Chamber
a and Chamber
b, respectively.
\(p_{\text{a}}\),
\(p_{\text{b}}\) and
\(T_{\text{a}}\),
\(T_{\text{b}}\) represent the corresponding pressure and temperature of Chamber
a and Chamber
b, respectively.
\(p_{\text{s}}\) is the gas supply pressure,
\(p_{\text{e}}\) is the atmospheric pressure, and
\(\theta\) is the rotation angle of the pneumatic rotary actuator.
×
3 Power Characteristic Matching
3.1 Output Characteristics of the ValveControlled Cylinder
The output characteristic of the valvecontrolled cylinder system refers to the relationship between the total load moment and angular velocity when the power source is known. The output characteristic can be obtained by the following method.
When supply pressure
\(p_{\text{s}}\) is relatively low, i.e., when
\(0.1013\;{\text{MPa}} \le p_{\text{s}} \le 0.4824\;{\text{MPa}}\), the condition is satisfied, i.e.,
\({{p_{a} } \mathord{\left/ {\vphantom {{p_{a} } {p_{s} }}} \right. \kern0pt} {p_{s} }} > b = 0.21\), where
\(b\) denotes the critical pressure ratio. The gas flow in the proportional–directional control valve is a subsonic flow. Here, the mass flow equation through the proportional valve is [
26]
where
\(S_{\text{e}}\) is the effective area of the proportional valve orifice,
\(R\) is the gas constant,
\(T_{\text{s}}\) is the gas supply temperature, and
\(\kappa\) is the isentropic index.
$$\dot{m}_{\text{a}} = \frac{{S_{\text{e}} p_{\text{s}} }}{{\sqrt {RT_{\text{s}} } }}\sqrt {\frac{2\kappa }{\kappa  1}\left[ {\left( {\frac{{p_{\text{a}} }}{{p_{\text{s}} }}} \right)^{{\frac{2}{\kappa }}}  \left( {\frac{{p_{\text{a}} }}{{p_{\text{s}} }}} \right)^{{\frac{\kappa + 1}{\kappa }}} } \right]} ,$$
(1)
$$\dot{m}_{\text{b}} = \frac{{S_{\text{e}} p_{\text{b}} }}{{\sqrt {RT_{\text{s}} } }}\sqrt {\frac{2\kappa }{\kappa  1}\left[ {\left( {\frac{{p_{\text{e}} }}{{p_{\text{b}} }}} \right)^{{\frac{2}{\kappa }}}  \left( {\frac{{p_{\text{e}} }}{{p_{\text{b}} }}} \right)^{{\frac{\kappa + 1}{\kappa }}} } \right]} ,$$
(2)
When the opening of the proportional–directional control valve is maximum, the mass flow rates of the two chambers are maximum, which can be expressed as
where
\(C\) is the flow coefficient and
\(r\) is the radius of the orifice.
$$\dot{m}_{\text{amax}} = \frac{{C\uppi r^{2} p_{\text{s}} }}{{\sqrt {RT_{\text{s}} } }}\sqrt {\frac{2\kappa }{\kappa  1}\left[ {\left( {\frac{{p_{\text{a}} }}{{p_{\text{s}} }}} \right)^{{\frac{2}{\kappa }}}  \left( {\frac{{p_{\text{a}} }}{{p_{\text{s}} }}} \right)^{{\frac{\kappa + 1}{\kappa }}} } \right]} ,$$
(3)
$$\dot{m}_{\text{bmax}} = \frac{{C\uppi r^{2} p_{\text{b}} }}{{\sqrt {RT_{\text{s}} } }}\sqrt {\frac{2\kappa }{\kappa  1}\left[ {\left( {\frac{{p_{\text{e}} }}{{p_{\text{b}} }}} \right)^{{\frac{2}{\kappa }}}  \left( {\frac{{p_{\text{e}} }}{{p_{\text{b}} }}} \right)^{{\frac{\kappa + 1}{\kappa }}} } \right]} ,$$
(4)
Under adiabatic condition,
\({{p_{\text{a}} } \mathord{\left/ {\vphantom {{p_{\text{a}} } \rho }} \right. \kern0pt} \rho }_{\text{a}}^{\kappa } = {{p_{\text{s}} } \mathord{\left/ {\vphantom {{p_{\text{s}} } {\rho_{\text{s}}^{\kappa } }}} \right. \kern0pt} {\rho_{\text{s}}^{\kappa } }}\) and
\({{p_{\text{b}} } \mathord{\left/ {\vphantom {{p_{\text{b}} } \rho }} \right. \kern0pt} \rho }_{\text{b}}^{\kappa } = {{p_{\text{c}} } \mathord{\left/ {\vphantom {{p_{\text{c}} } {\rho_{\text{c}}^{\kappa } }}} \right. \kern0pt} {\rho_{\text{c}}^{\kappa } }}\), where
\(\rho_{\text{a}}\),
\(\rho_{\text{b}}\),
\(\rho_{\text{s}}\), and
\(\rho_{\text{e}}\) represent the gas density in Chamber
a, gas density in Chamber
b, gas supply density, and atmospheric density respectively. For the pneumatic rotary actuator, these can be obtained from the mass flowrate formulas:
where
\(A\) is the effective area of a single piston,
\(d_{\text{f}}\) is the pitch diameter of the gear, and
\(\dot{\theta }\) is the angular velocity of the pneumatic rotary actuator.
$$\dot{m}_{\text{amax}} = \rho_{\text{a}} \cdot 2A \cdot \frac{1}{2}d_{\text{f}} \dot{\theta } = \frac{{\rho_{\text{a}} }}{{\rho_{\text{s}} }}\rho_{\text{s}} Ad_{\text{f}} \dot{\theta } = \left( {\frac{{p_{\text{a}} }}{{p_{\text{s}} }}} \right)^{{\frac{1}{\kappa }}} \frac{{p_{\text{s}} }}{{RT_{\text{s}} }}Ad_{\text{f}} \dot{\theta },$$
(5)
$$\dot{m}_{\text{bmax}} = \rho_{\text{b}} \cdot 2A \cdot \frac{1}{2}d_{\text{f}} \dot{\theta } = \frac{{\rho_{\text{e}} }}{{\rho_{\text{b}} }}\rho_{\text{b}} Ad_{\text{f}} \dot{\theta } = \left( {\frac{{p_{\text{e}} }}{{p_{\text{b}} }}} \right)^{{\frac{1}{\kappa }}} \frac{{p_{\text{b}} }}{{RT_{\text{s}} }}Ad_{\text{f}} \dot{\theta },$$
(6)
The dynamic equation of the pneumatic rotary actuator can be expressed as follows:
where
\(f\) is the total load moment.
$$p_{\text{a}}  p_{\text{b}} = \frac{f}{{d_{\text{f}} A}},$$
(7)
Combining Eqs. (
3)–(
6) yields
\(p_{\text{a}}\) and
\(p_{\text{b}}\). Substituting the expressions of
\(p_{\text{a}}\) and
\(p_{\text{b}}\) into Eq. (
7) yields
$$p_{\text{s}} \left[ {1  \frac{{A^{2} d_{\text{f}}^{2} \dot{\theta }^{2} (\kappa  1)}}{{2C^{2}\uppi^{2} r^{4} \kappa RT_{s} }}} \right]^{{\frac{\kappa }{\kappa  1}}}  \frac{{p_{\text{e}} }}{{\left[ {1  \frac{{A^{2} d_{\text{f}}^{2} \dot{\theta }^{2} (\kappa  1)}}{{2C^{2}\uppi^{2} r^{4} \kappa RT_{s} }}} \right]^{{\frac{\kappa }{\kappa  1}}} }} = \frac{f}{{d_{\text{f}} A}}.$$
(8)
Eq. (
8) is the expression of the output characteristic curve of the valvecontrolled cylinder. The known parameters in the equation are shown in Table
3.
Table 3
Known parameters in Eq. (
8)
Parameter

Value


A (m
^{2})

3.4636 × 10
^{−4}

d
_{f} (m)

0.014

κ

1.4

C

0.6437

r (m)

1.00 × 10
^{−3}

R (J/(kg·K))

287

To extend and improve the influence of the output characteristics of the system, the influence law of the fixed parameters is also theoretically analyzed. Figure
5 shows the output characteristic curves. The following characteristics can be found in plane
\(\dot{\theta }{  }f\):
(1)
Figure
5(a) shows that when pressure
\(p_{\text{s}}\) increases from 0.3 MPa to 0.4 MPa, the curve is a parabola and
\(p_{\text{s}}\) is a variable parameter. Increasing
\(p_{\text{s}}\) makes the whole parabola move to the right while the shape does not change.
(2)
Figure
5(b) shows that when the maximum opening area of the valve increases from
\(\uppi r^{2}\) to
\(2\uppi r^{2}\), the whole parabola becomes wider but the vertices remain the same.
(3)
Figure
5(c) shows that the increase in effective working area
\(A\) of the piston makes the top of the parabola move to the right and the parabola simultaneously becomes narrower.
×
We can see from Eq. (
8) that when
\(\dot{\theta }\) = 0, the maximum total load moment can be expressed as
$$f_{\text{max} } { = }Ad_{\text{f}} \left( {p_{\text{s}}  p_{\text{e}} } \right).$$
(9)
When
\(f\) = 0, the maximum angular velocity is
$$\dot{\theta }_{\text{max} } { = }\sqrt {\frac{{2C_{1}^{2}\uppi^{2} r^{4} \kappa RT_{s} }}{{A^{2} d_{\text{f}}^{2} (\kappa  1)}}\left[ {1  \left( {\frac{{p_{\text{e}} }}{{p_{\text{s}} }}} \right)^{{\left( {\frac{\kappa  1}{2\kappa }} \right)}} } \right]} .$$
(10)
3.2 Load Characteristic
The load characteristic refers to the relationship between the moment required for the load to move and the position, velocity, and acceleration of the load itself [
27]. The load characteristic can be expressed by the angular velocity–moment curve.
The load characteristic is related to the form of load movement. When the load sinusoidally moves, the motion of the load is expressed as
where
\(\theta_{\text{m}}\) is the maximum angular value of the load motion and
\(\omega\) is the sinusoidal motion frequency of the load.
$$\theta = \theta_{\text{m}} \sin \omega t,$$
(11)
The angular velocity and acceleration of the load are
$$\dot{\theta } = \theta_{\text{m}} \omega \cos \omega t,$$
(12)
$$\ddot{\theta } =  \theta_{\text{m}} \omega^{2} \sin \omega t.$$
(13)
The total load moment of the pneumatic rotary actuator is
where
\(m_{\text{p}}\) is the mass of a single piston and
\(J\) is the moment of inertia of the pneumatic rotary actuator.
\(F_{\text{f}}\) is the friction force and can be represented by the Stribeck friction model.
where
\(F_{\text{s}}\) is the maximum static friction,
\(F_{\text{c}}\) is the Coulomb friction,
\(\dot{\theta }_{\text{s}}\) is the critical Stribeck velocity, and
\(\sigma\) is the viscous friction coefficient.
$$\begin{aligned} f & = \left( {\frac{1}{2}m_{\text{p}} d_{\text{f}}^{2} + J} \right)\ddot{\theta } + \frac{1}{2}d_{\text{f}} F_{\text{f}} \\ & { = }  \left( {\frac{1}{2}m_{\text{p}} d_{\text{f}}^{2} + J} \right)\theta_{\text{m}} \omega^{2} \sin \omega t \\ & \quad + \frac{1}{2}d_{\text{f}} \left[ {F_{\text{c}} {\text{sign(}}\dot{\theta }) + (F_{\text{s}}  F_{\text{c}} )e^{{  \left( {{{\dot{\theta }} \mathord{\left/ {\vphantom {{\dot{\theta }} {\dot{\theta }_{\text{s}} }}} \right. \kern0pt} {\dot{\theta }_{\text{s}} }}} \right)^{2} }} {\text{sign(}}\dot{\theta }) + \sigma \dot{\theta }} \right], \\ \end{aligned}$$
(14)
$$F_{\text{f}} = F_{\text{c}} {\text{sign(}}\dot{\theta }) + (F_{\text{s}}  F_{\text{c}} )e^{{  \left( {{{\dot{\theta }} \mathord{\left/ {\vphantom {{\dot{\theta }} {\dot{\theta }_{\text{s}} }}} \right. \kern0pt} {\dot{\theta }_{\text{s}} }}} \right)^{2} }} {\text{sign(}}\dot{\theta }) + \sigma \dot{\theta },$$
(15)
Combining Eqs. (
12)–(
14) yields
$$\begin{array}{*{20}l} { \left[ \begin{gathered} \frac{{f  \frac{1}{2}d_{{\text{f}}} F_{{\text{c}}} {\text{sign(}}\dot{\theta })  \frac{1}{2}d_{{\text{f}}} (F_{{\text{s}}}  F_{{\text{c}}} )e^{{  \left( {{{\dot{\theta }} \mathord{\left/ {\vphantom {{\dot{\theta }} {\dot{\theta }_{{\text{s}}} }}} \right. \kern\nulldelimiterspace} {\dot{\theta }_{{\text{s}}} }}} \right)^{2} }} {\text{sign(}}\dot{\theta })}}{{\left( {\frac{1}{2}m_{{\text{p}}} d_{{\text{f}}}^{2} + J} \right)\theta _{{\text{m}}} \omega ^{2} }} \hfill \\  \frac{{\frac{1}{2}d_{{\text{f}}} \sigma \dot{\theta }}}{{\left( {\frac{1}{2}m_{{\text{p}}} d_{{\text{f}}}^{2} + J} \right)\theta _{{\text{m}}} \omega ^{2} }} \hfill \\ \end{gathered} \right]^{2} } \\ { \quad + \left( {\frac{{\dot{\theta }}}{{\theta _{{\text{m}}} \omega }}} \right)^{2} = 1.} \\ \end{array}$$
(16)
3.3 Power Source Characteristics and Matching
The power source characteristic refers to the characteristic of the flow and pressure provided by the power source, which can be expressed by the flow–pressure curve. The air compressor used in this work can be approximately regarded as a constantpressure source for a quantitative pump. Therefore, the power source characteristic curve is shown in Figure
7, where
\(\dot{m}_{\text{s}}\) is the gas supply mass flow,
\(p_{\text{s}}\) is the gas supply pressure,
\(\dot{m}_{\text{L}}\) is the driving mass flow, and
\(p_{\text{L}}\) is the driving pressure.
×
The output and power source characteristics of the valvecontrolled cylinder should envelope the load characteristic curve. To minimize unnecessary energy consumption, the output characteristic curve should be tangent to the load characteristic curve, and the power source characteristic curve should be tangent to the output characteristic curve in the
faxis direction and the load characteristic curve in the
\(\dot{\theta }\)axis direction, as shown in Figure
8.
×
In this manner, the maximum total load moment is obtained, i.e.,
\(f_{\text{max} }\) = 0.96 N·m. The optimum gas supply pressure can be obtained from Eq. (
9), i.e.,
\(p_{\text{s}} { = }{{f_{\text{max} } } \mathord{\left/ {\vphantom {{f_{\text{max} } } {d_{\text{f}} A}}} \right. \kern0pt} {d_{\text{f}} A}} + p_{\text{e}} { = 0} . 3 3 6 7\;{\text{MPa}}\).
4 Experimental Verification of the Energy Savings
To verify the calculation results presented in the previous section, lowspeed uniformmotion experiments of the pneumatic rotary actuator were carried out using 0.6 and 0.3367 MPa supply pressure. The total energy and effective energy consumed by the valvecontrolled cylinder system were measured and calculated. In the experiment, the inputangle signal was set as the slope signal, and Chamber
a was used as the intake chamber. The motion curve of the uniformvelocity period was considered, and the angular strokes in the two experiments were the same. Two flow sensors were used to measure the volume flow of the gas supply pipeline and the Chamber
a port. Temperature sensors were used to measure the gas temperature of the gas supply pipeline and Chamber
a.
Figures
9 and
10 show the system response curves at gas supply pressure values of 0.6 and 0.3367 MPa, respectively, including the angle curve, gas supply flow curve, gas supply temperature curve, pressure curve of Chamber
a, volumeflow curve of Chamber
a, and temperature curve of Chamber
a. Figures
9(f) and
10(f) show that the temperature in Chamber
a changed with the change in the velocity, which first increased, then decreased, and then entered a stable stage.
×
×
The total power consumed by the pneumatic system is expressed as [
28,
29]:
where
\(\dot{V}_{\text{s}}\) is the volume flow through the gas supply pipeline, and its numerical variation curves are shown in Figures
9(b) and
10(b). The
\(T_{\text{s}}\) curves are shown in Figures
9(c) and
10(c).
$$P_{\text{T}} = p_{\text{s}} \dot{V}_{\text{s}} \left[ {\ln \frac{{p_{\text{s}} }}{{p_{\text{e}} }} + \frac{\kappa }{\kappa  1}\left( {\frac{{T_{\text{s}}  T_{\text{e}} }}{{T_{\text{e}} }}  \ln \frac{{T_{\text{s}} }}{{T_{\text{e}} }}} \right)} \right],$$
(17)
The effective power of the pneumatic rotary actuator can be expressed as
where
\(\dot{V}_{\text{a}}\) is the volume flow into Chamber
a, and its numerical variation curves are shown in Figures
9(e) and
10(e). The
\(T_{\text{a}}\) curves are shown in Figures
9(f) and
10(f).
$$P_{\text{E}} = p_{\text{a}} \dot{V}_{\text{a}} \left[ {\ln \frac{{p_{\text{a}} }}{{p_{\text{e}} }} + \frac{\kappa }{\kappa  1}\left( {\frac{{T_{\text{a}}  T_{\text{e}} }}{{T_{\text{e}} }}  \ln \frac{{T_{\text{a}} }}{{T_{\text{e}} }}} \right)} \right],$$
(18)
By substituting the data in Figures
9 and
10 into Eqs. (
17) and (
18), the total and effective power of the pneumatic system at different supply pressure values can be obtained, as shown in Figure
11. The total and effective energy consumed by the pneumatic system can be obtained by integrating the data shown in Figure
11 using the Origin software.
×
The actual work done by the gas on the pneumatic rotary actuator is equal to the sum of the rotational kinetic energy of the rotating platform, the kinetic energy of the cylinder piston, and the work done by the piston to overcome the friction force, which can be expressed as
where
\(y\) is the displacement of the actuator piston and
\(\dot{\theta }\) is replaced by the average value of the angular velocity.
$$\begin{aligned} {\text{W}} & = \frac{1}{2}J\dot{\theta }^{2} + \frac{1}{2} \cdot 2m_{\text{p}} \cdot (\dot{y})^{2} + F_{\text{f}} y \\ & { = }\frac{1}{2}\left( {J + \frac{1}{2}m_{\text{p}} d_{\text{f}}^{2} } \right)\dot{\theta }^{2} + \frac{1}{2}F_{\text{f}} d_{\text{f}} \theta , \\ \end{aligned}$$
(19)
The calculation results are described as follows. When the gas supply pressure is 0.6 MPa, the total energy consumed by the system is 195.552 J, the effective energy is 32.666 J, and the actual work done by the pneumatic rotary actuator is 3.513 J. When the gas supply pressure is 0.3367 MPa, the total energy consumed by the system is 32.207 J, the effective energy is 9.481 J, and the actual work done is 3.517 J. In both cases, the actual work of the pneumatic rotary actuator is almost the same, and when the gas supply pressure is 0.3367 MPa, the energy consumption is greatly reduced.
5 Further Discussions
According to the matching method of the power characteristics, for the constantpressure source servo system with a quantitative pump, we need to calculate the optimal airsupply pressure required for manually adjusting the airsupply pressure to the optimal pressure. Matching efficiency
η represents the ratio of the power output of the pneumatic system to the input power of the gas source. The matching efficiency is expressed as
$$\eta = \frac{{p_{\text{L}} \dot{m}_{\text{L}} }}{{p_{\text{s}} \dot{m}_{\text{s}} }}.$$
(20)
Figure
7 shows that the matching efficiency of this method is low. The adaptive power source can adaptively change the gas supply pressure or flow to meet the system requirements and improve the matching efficiency. It can be divided into the following three types [
30].
(1)
Flow adaptive power source
This power source can adaptively adjust the supply flow from the power source according to the system flow demand to reduce the loss in the flow. The characteristic curve is shown in Figure
12(a). The matching efficiency is expressed as
$$\eta = \frac{{p_{\text{L}} \dot{m}_{\text{L}} }}{{p_{\text{s}} \dot{m}^{\prime}_{\text{s}} }} \approx \frac{{p_{\text{L}} }}{{p_{\text{s}} }}.$$
(21)
×
(2)
Pressure adaptive power source
This power source can adaptively adjust the gas supply pressure of the power source according to the system pressure demand to reduce the pressure loss. The characteristic curve is shown in Figure
12(b). The matching efficiency is expressed as
$$\eta = \frac{{p_{\text{L}} \dot{m}_{\text{L}} }}{{p^{\prime}_{\text{s}} \dot{m}_{\text{s}} }} \approx \frac{{\dot{m}_{\text{L}} }}{{\dot{m}_{\text{s}} }}.$$
(22)
(3)
Power adaptive power source
This power source can adaptively adjust the gas supply pressure and flow from the power source according to the system pressure and flow demand to minimize the loss in power.
\(\dot{m}_{\text{s}}^{'}\) denotes the airsupply flow. The characteristic curve is shown in Figure
12(c). The matching efficiency is expressed as
$$\eta = \frac{{p_{\text{L}} \dot{m}_{\text{L}} }}{{p^{\prime}_{\text{s}} \dot{m}^{\prime}_{\text{s}} }} \approx 1.$$
(23)
Therefore, the power adaptive power source demonstrates better energysaving effect, and its matching efficiency is closer to 100%.
6 Conclusions
Power matching of the pneumatic rotary actuator involves optimizing the relevant parameters of the pneumatic rotary actuator system based on the premise of satisfying the normal operation of the pneumatic rotary actuator, realizing the power demand and output matching, and achieving energy savings. In this study, the derivation process of the outputpower and load characteristics of the pneumatic rotary actuator servocontrol system is described. The employed air compressor is regarded as a constantpressure source of the quantitative pump, and the power characteristics of the system are matched. The following conclusions are obtained.
(1)
The minimum gas supply pressure obtained by the powermatching method represents the optimal gas supply pressure. The optimum gas supply pressure is 0.3367 MPa.
(2)
By comparing the systemresponse experiments at 0.6 and 0.3367 MPa, the total energy consumed by the system generates savings of 163.345 J. This value verifies that the system under the optimal gas supply pressure can significantly reduce energy loss.
(3)
According to the characteristic curves of the adaptive power sources, the matching efficiency of the power adaptive power source is higher than that of the flow and pressure adaptive power sources.
Acknowledgments
The authors would like to thank Henan Polytechnic University and Beihang University for providing the necessary facilities and machinery to build the prototype of the pneumatic servo system. The authors are sincerely grateful to the reviewers for their valuable review comments, which substantially improved the paper.
Competing Interests
The authors declare no competing financial interests.
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