Research Article  Open Access
Gang Li, Wen Wang, HongNan Li, "Experiment and Application of MarketBased Control for Engineering Structures", Journal of Applied Mathematics, vol. 2013, Article ID 219537, 12 pages, 2013. https://doi.org/10.1155/2013/219537
Experiment and Application of MarketBased Control for Engineering Structures
Abstract
An experimental study on the vibration control of a singledegreeoffreedom model is carried out to verify marketbased control (MBC) strategy effect. Results show that the MBC strategy can reduce both displacement and acceleration responses. Additionally, the MBC strategy is applied to a longspan bridge considering the travelling wave effect. Numerical simulations indicate that the displacement and acceleration responses of the longspan bridge with the travelling wave effect are smaller than those without, and the larger the velocity of travelling wave is, the better the control effect of MBC is. Based on the MBC theory and multimarketbased control (MMBC) presented here it is further applied to a largespace structure considering multiple dimensional features of structural model and ground motions. It is concluded that the MMBC strategy reduces the displacement response of the largespace structure, especially on vertical displacements, but has limited control effects on accelerations.
1. Introduction
The concept of structural control in civil engineering was first proposed in 1970s [1]. Since then, this technology has been developed greatly. According to the energy source (external or internal), structural control systems can be classified as passive, active, semiactive, or mixed control strategies. For active and semiactive control techniques, the control force is often determined by the control laws. Some typical control laws, that is, linear quadratic regulator (LQR), modal control, smart control, H_{2} and H∞, and so forth, have become hot research topics rapidly in recent years [2–5] For general structures, these control laws usually use a central computer responsible for the control of the entire system, but they exhibit limitation for large complex structures due to numerous degrees of freedom of the large complex structure. The marketbased control (MBC) as a special control theory introduces the price mechanism of free market economy into the field of structural control in civil engineering. The MBC is developed based on an analogy between the relations of control forceenergy sources and those of supplydemand in the market economy. The optimal problem of control force from actuator is transformed to that of allocation resources in the market.
The MBC concept was proposed by Clearwater [6]. It was applied to solve the optimal decentralized control problem of complex dynamic systems, allocate and coordinate the actions of different mechatronic systems, and develop a multiagent system for realizing the traffic intelligent control [7–9]. In addition, some prior research works about MBC used in various fields were carried out, such as the telecommunication, mechanism, and mission plan [10–12]. Application of the MBC in civil engineering to reduce the structural response under environmental loads has been carried out after the twenty first century [13–17].
However, previous researches mainly focused on ordinary structures, and few emphasized on applications of MBC in longspan and largespace structures. There are still existing problems in applications for these kinds of structures, such as travelling wave effect and multiple dimensions of ground motion. The structural control technology in longspan structure have drawn many researchers’ attention [18–21]. Because an earthquake excitation consists of superposition of a large number of waves carrying different characteristics, the different positions along a longspan structure are generally with different motions. Bridges as typical longspan structures; their control techniques considering multisupport and travelling seismic wave effects have been carried out by various researchers [22, 23]. These research results showed that control effect had an obvious distinction between uniform ground motion and differential ground motions. Largespace structures generally have thousands of degrees of freedoms and outstanding spatial characteristics; hence, multiple dimensional features, such as the spatial model and inputted ground motions, should be taken into account together. Additionally, theoretical researches have verified that the MBC is an effective control strategy, but experiments with the approach for model or actual structure have not been reported till now. Based on the above reason, a model test is carried out to validate the effectiveness of MBC in this paper, and the MBC strategy is applied to a longspan bridge considering the travelling wave effect and to a largespace structure considering multiple dimensional ground motion inputs, respectively.
2. Fundamental and Experiment
2.1. Basic Theory
The main objective of this study is to solve problems in structural control by the usage of MBC. In the MBC, power sources and controlled devices in a control system are abstracted to sellers and buyers in a free market. The relationship between the energy demand and supply in a control system corresponds to the supplydemand relation in the free market. The supplydemand relation is influenced by the equilibrium price, and the equilibrium price is certainly affected by the supplydemand relation in return. Take a virtual free market and singledegreeoffreedom system as an illustration to show the application of the MBC in structural control area.
The governing equation of motion for a SDOF system with controller can be expressed as where , , and represent the displacement, velocity, and acceleration of the SDOF system, respectively; and are the system mass and stiffness, respectively; denotes the viscous damping coefficient; is the controlling force from the actuator; is the environmental load.
The demand function is determined by its energy consumption , energy price , and responses of the dynamic system ; the sellers’ supply function is determined by its own original energy and energy price . Buyers and sellers both pursue their maximum interests at any time. This process has to be restricted by commodity quantities and virtual wealth . The relation is shown as follows:
In the free market, there is a general equilibrium rule between the supply and demand. The rule can be expressed as
Actually, the supplydemand relation is a core of the overall MBC theory. There have been several mathematical models reflecting the supplydemand relation by now, such as linearsupply and lineardemand model [14], linearsupply and powerdemand model [16], advanced linearsupply and powerdemand model, and linearsupply and exponentialdemand model [16]. Detailed introductions of these supplydemand models can be found in corresponding references. A simple relation of the supply function and price, linear model, is used here as And the advanced linearsupply and powerdemand model (ALPM) demand function is chosen to depict the relation of the demand and price as where is the parameter that reflects the energy supply, and are the storydisplacement and storyvelocity of the structural system and and are the weighting coefficients.
Substituting (4) and (5) into (3), an equilibrium price is obtained through solving (3) at any time step. The distribution of scarce resources reaches maximized benefits under the equilibrium price. The solution of (3) is called the Pareto optimal solution in economics [13]. Then, the control force is written as where is the gain coefficient related to the actuator.
Substitute (6) into (1); the MBC is implemented in the structural vibration control.
2.2. Experiment
A singledegreeoffreedom of structural model is made of steel and organic glass plates. The organic glass plate is chosen to model the floor of structure, and steel plates are as structural elements for resisting lateral force. Two piezoelectric ceramic thin plates are affixed on the surface of steel plates, one of which named the PZT1 is an exciting device at the beginning of experiment, and it becomes an actuator to control the structural response after the excitation and another of which named the PZT2 is a collecting sensor for the structural response. The structural model and piezoelectric ceramic thin plates are shown in Figure 1 and their parameters are listed in Tables 1 and 2.


The model vibrates under the excitation by the PZT1 at the beginning and the vibration makes the PZT2 deformed and results in electric signals change. The response of structural model is obtained from collecting and processing the electric signals. The PZT1 is an actuator during structural model vibration. The value of control force from the PZT1 is calculated by the MBC strategy based on the structural response status from the PZT2. The whole control process is shown in Figure 2.
Experimental devices include a PC with the MBC strategy, input and out control board, and piezoelectric driving device. All these devices are shown in Figures 3, 4, and 5.
The natural vibration frequency of model is 18.1 Hz through the sweptfrequency method. When the frequency of the environmental load equals natural frequency of the model, the vibration response of the structural model reaches maximum value. Thereby, the exciting load is defined as
Figures 6 and 7 show proportional acceleration and displacement responses of the structural model, respectively. The proportional acceleration is a signal measured directly from the PZT2. It can be transferred to an absolute acceleration through multipling a parameter related to the piezoelectric. In this study, the main objective of this experiment is focused on comparing the effectiveness of the MBC. Therefore, the proportional response is used here directly. It can be seen that the response of model controlled by the MBC has an obvious reduction than that of model with free vibration (FRE).
Figure 8 shows the relation of theoretical control force and time, which is equal to the ratio of actual force to gain coefficient. Figure 9 illustrates that the price has the same changing trend as the theoretical control force in time history. The change regularity of price in the market is consistent with that of control force from actuator illustrated efficiency of the MBC algorithm.
3. Application of the MBC in LongSpan Bridges
3.1. Governing Equation considering the Multiple Support
The equation of motion for the bridge considering multisupport is written as where , and are the mass, damping, and stiffness matrices, respectively; and are the control force vectors from actuator and environmental force; , and are the absolute acceleration, velocity, and displacement response vectors, respectively. Subscripts and stand for the structure and the support. Equation (8) can be rearranged as
The displacement is expressed by where and are the dynamic response and the pseudostatic response. Additionally, for the pseudostatic response of the structure, there is the following relation: where . Substituting (10) and (11) to (9), there is
The damping item has little influence on structural responses and can be neglected. Equation (12) is then simplified to
3.2. SupplyDemand Relation Model
In this section, linearsupply and exponent model [16] was used as control function.
The supply function is written as
The demand function is expressed by where is the parameter that reflects the energy supply of th actuator, andare the relative displacement and velocity at ends of the th actuator, and are the weighting coefficients, is the initial wealth of the th buyer, and is the equivalent price of the th actuator.
The equilibrium price is solved through defining (14) and (15) equal. Then, control force of the th actuator is expressed based on the price as follows:
3.3. Numerical Example
A longspan bridge shown in Figure 10 has 660 meters length. Bidirectional sliding bearings are set on the abutments and continuous piers. In order to analyze the control effect of the longspan bridge under the earthquake using the MBC strategy, The Taft earthquake record (July 21, 1951, the acceleration peak value is adjusted to 400 gal) is selected as an environmental load.
Planar beam elements are used to simulate piers and beams of the bridge. The longspan bridge is modeled with 70 finite elements and 197 freedoms. Figure 11 shows finite element divisions and some typical nodes numbers for convenient expression.
32 Magnetorheological dampers (MRDs) are installed on the abutments, I and IV piers. The modified boundary Hrovat algorithm [21] is used here for numerical simulations. The maximum force from a MRD is 2000 kN. Table 3 shows parameters of these MRDs, where is the cylinder diameter,is the effective length of the piston,is the diameter of the piston,is the gap spacing,is the apparent viscosity of the liquid, andis the maximum yield stress of the liquid.

The traveling wave speed as the known parameter is given during the dynamical time history analysis of the longspan bridge considering multiple supports. In order to find the rule of the response influenced by traveling wave, the velocities of traveling wave are set at 400 ms^{−1}, 1000 ms^{−1}, 3000 ms^{−1}, and infinity.
Figure 12 shows the price and displacement time history of the no. 6 node with the travelling wave speed at 3000 ms^{−1}. It can be seen from these figures that (a) the MBC strategy reduces displacement responses; (b) the displacement changing trend is consistent with the price response in whole time phase. The phenomena of the energy demand increasing by the displacement and velocity are also inflected from (4). It also means that the energy supply also increases by the displacement because of energy demand equaling to energy supply. In addition, it can be drawn from (6) that energy supply is proportional to the equivalent price. Therefore, both the displacement and equivalent price have the same changing trend.
(a)
(b)
Figures 13 and 14 indicate that forces of MRDs are dependent on not only the displacement but also velocity.
In order to validate the effectiveness of the MBC with various travelling wave speed, the reduction rate is defined as where and are responses of the bridge without and with actuators, respectively.
Figures 15 and 16 illustrate maximum displacement and acceleration comparisons of typical nodes with various traveling wave speeds. It is found that there are significantly differences of the responses of bridge among these travelling wave speeds. For the bridge without control, the displacement and acceleration responses at these nodes grow with the increase of travelling waves speeds. The greater the travelling wave speed is, the larger the reduction rate becomes. Therefore, effectiveness of the structural control using the MBC without considering the travelling wave effect is superior to that with consideration.
(a)
(b)
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(d) Consistent excitation
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(d) Consistent excitation
4. Application of the MBC in Large Space Structures
4.1. Basic Theory
A free market, which is a large unity, usually consists of many submarkets. The equilibrium price of commodity in each submarket is formed depending on its own supplydemand relation. However, the price tendency of each submarket is toward the whole equilibrium price. Thus, the price of whole market is a dynamic “cobweb” model, and price of each submarket has more or less influence on the price of the whole market. This theory based on multiple submarkets is called the multiple marketbased control (MMBC). The advantage of MMBC can realize the decentralized vibration control in the structural control area through the similarity between the submarket and substructure. In each substructure, the controlling force only depends on its own supplydemand relation. Only the supply and demand functions for the MMBC are introduced here, because the framework of MMBC is similar to that of the MBC.
The supply function of the th seller in the th submarket is expressed by
The demand function of the th buyer in the th submarket can be written as where and are relative displacement and velocity of the th seller in the th substructure, respectively; , , , and are the initial wealth, demand coefficient, and weighting coefficients of the th buyer in the th submarket; is the price in the th submarket; is the parameter that reflects the th seller in the th submarket.
Then, supplydemand relationship of whole market can be written as where is the number of the actuators, is the number of energy demand sources, and is the number of submarkets. The equilibrium price is solved from (20) through iterations. The controlling force is proportional to the energy supply at the price . The force from actuator can be drawn as where means the gain coefficient of controlling force from the th actuator of th substructure. Substituting (21) into the structure dynamic equation, application of the MMBC to structure may be realized.
4.2. Numerical Example
A reticulated shell structure (RSS) with 40 m span, 8 m high and 5 spanheight ratio is shown in Figure 17. It has four support positions at node Number 127, 140, 151, and 163. The RSS consists of two kinds of circular 4 mm thick steel tubes: one is 133 mm in diameter; another is 140 mm in diameter. The first one is used for string bar elements of RSS and the second is adopted for support bars. In order to validate the effectiveness of MMBC for the largespace structure in three dimensions, a 3dimensional finite element model is established and the El Centro earthquake record (NS, May 18, 1940, the acceleration peak value is adjusted to 400 gal) is inputted in the RSS along , , and directions. The MRDs are installed at node Number 133, 145, 157, and 169 shown in Figure 17. There are three MRDs, each is aligned with , , and directions at each nodal position. The RSS is distributed into three substructures named as the substructure, substructure, and substructure for the MMBC strategy application.
(a)
(b)
Figures 18 and 19 illustrate displacement and acceleration time history responses of the RSS with and without control. Tables 4 and 5 show the maximum response and reduction rate of typical nodes. It is obviously found from the above figures and tables that the displacement response can be controlled effectively, especially on the displacement in direction. However, the effectiveness of the acceleration controlling is limited. The reason is that the deformation of the RSS in direction is larger than that in and directions, and the acceleration response is not sensitive to such flexible RSS.


(a)
(b)
(c)
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Figures 20 and 21 show the price and control force time history of three various substructures. Since the price is a function of supplydemand model and responses of the RSS, it varies from different submarkets. In addition, the same regularity and changing trend between displacement and price in each substructure also is observed from these figures.
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(b)
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5. Concluding Remarks
In this paper, a vibration control experiment is carried out to validate the MBC effectiveness. The MBC is then applied to a longspan bridge considering the travelling wave effect. On the basis of MBC theory, the MMBC is presented here and applied to a largespace structure, taking into account the multiple dimensions of ground motions. The following conclusions are drawn in this study.(1)The experiment validates that the MBC is an effective control strategy offering significant controlling force and value to be applied in actual structures.(2)The travelling wave effect has a distinct influence on responses of the longspan bridge. The MBC strategy can reduce displacement and acceleration responses of the bridge both with and without the travelling wave effects. The greater the velocity of travelling wave of ground motion is, the larger the response of bridge is and the better the control effect is. Therefore, it is necessary to take the travelling wave effect into consideration during the analysis of vibration control of longspan structure using the MBC.(3)As the largespace structure is commonly flexible, especially in the vertical direction, the multiple dimensional responses and control effect of this kind of structure have to be considered. Numerical results have indicated that the displacement response of the largespace structure in the vertical direction are usually larger than those in horizontal directions, and the MMBC has better control effect on the displacement response than the acceleration response.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
Acknowledgments
This research work was jointly supported by the Natural Science Foundation of China (Grants no. 50808036, 91215302) and the Science Fund for Creative Research Groups of the National Natural Science Foundation of China (Grant no. 51121005).
References
 J. T. P. Yao, “Concept of structural control,” ASCE Journal of the Structural Division, vol. 98, no. 7, pp. 1567–1574, 1972. View at: Google Scholar
 T. T. Soong, Active Structure Control Theory and Practice, Longman Scientific & Technical, New York, NY, USA, 1990.
 J. N. Yang, J. C. Wu, and A. K. Agrawal, “Sliding Model control for nonlinear and hysterestic structures,” ASCE Journal of Engineering Mechanics, vol. 121, no. 12, pp. 1330–1339, 1995. View at: Publisher Site  Google Scholar
 L. Huo, G. Song, H. Li, and K. Grigoriadis, “H_{∞} robust control design of active structural vibration suppression using an active mass damper,” Smart Materials and Structures, vol. 17, no. 1, Article ID 015021, pp. 15–21, 2008. View at: Publisher Site  Google Scholar
 A. S. Ahlawat and A. Ramaswamy, “Multiobjective optimal structural vibration control using fuzzy logic control system,” ASCE Journal of Structural Engineering, vol. 127, no. 11, pp. 1330–1337, 2001. View at: Publisher Site  Google Scholar
 S. Clearwater, MarketBased Control: A Paradigm for Distributed Resource Allocation, World Scientific Publishing, Singapore, 1996.
 H. Voos, “Marketbased algorithms for optimal decentralized control of complex dynamic systems,” in Proceedings of the 38th IEEE Conference on Decision and Control (CDC '99), pp. 3295–3296, Phoenix, Ariz, USA, December 1999. View at: Google Scholar
 W. B. Jackson, C. Mochon, S. K. Van et al., “Distributed allocation using analog market wire computation and communication,” in Proceedings of the 7th Mechatronics Forum International Conference, Atlanta, Ga, USA, September 2000. View at: Google Scholar
 K. Prouskas, A. Patel, J. Pitt, and J. Barria, “A multiagent for intelligent network load control using a marketbased approach,” in Proceedings of the 4th International Conference on MultiAgent Systems (ICMAS '00), pp. 231–238, IEEE Computer Society, Boston, Mass, USA, July 2000. View at: Publisher Site  Google Scholar
 T. Alpcan, T. Başar, R. Srikant, and E. Altman, “CDMA uplink power control as a noncooperative game,” in Proceedings of the 40th IEEE Conference on Decision and Control (CDC '01), pp. 197–202, Orlando, Fla, USA, December 2001. View at: Google Scholar
 J. E. Hilland, R. R. Wessen, D. Porter, and R. S. Austin, “A marketbased conflict resolution approach for satellite mission planning,” IEEE Transactions on Engineering Management, vol. 48, no. 3, pp. 272–281, 2001. View at: Publisher Site  Google Scholar
 M. Bernardine and A. Stents, “Comparative study between centralized, marketbased, and behavioral multirobot coordination,” in Proceedings of the 2003 IEEE/RSL International Conference on Intelligent Robots and Systems, pp. 2297–2303, Las Vegas, Nev, USA, October 2003. View at: Google Scholar
 J. P. Lynch and K. H. Law, “Marketbased control of linear structural systems,” Earthquake Engineering and Structural Dynamics, vol. 31, no. 10, pp. 1855–1877, 2002. View at: Publisher Site  Google Scholar
 J. P. Lynch and K. H. Law, “Energy marketbased control of linear civil structures,” in Proceedings of the USKorea Workshop on Smart Structural Systems, Pusan, Korea, 2002. View at: Google Scholar
 L. Huo and H. Li, “Control law for marketbased semiactive timed liquid column dampers,” Chinese Journal of Applied Mechanics, vol. 22, no. 1, pp. 71–75, 2005. View at: Google Scholar
 Y. Li, Structural vibration control using MBC strategy [M.S. thesis], Dalian University of Technology, 2007.
 G. Li, Q. Liu, and H. Li, “Inelastic structural control based on MBC and FAM,” Mathematical Problems in Engineering, vol. 2011, Article ID 460731, 18 pages, 2011. View at: Publisher Site  Google Scholar
 H. J. Jung, B. F. Spencer Jr., and I. W. Lee, “Control of seismically excited cablestayed bridge employing magnetorheological fluid dampers,” ASCE Journal of Structural Engineering, vol. 129, no. 7, pp. 873–883, 2003. View at: Publisher Site  Google Scholar
 M. D. Symans and S. W. Kelly, “Fuzzy logic control of bridge structures using intelligent semiactive seismic isolation systems,” Earthquake Engineering & Structural Dynamics, vol. 28, no. 1, pp. 37–60, 1999. View at: Google Scholar
 S. J. Moon, L. A. Bergman, and P. G. Voulgaris, “Sliding mode control of cablestayed bridge subjected to seismic excitation,” Journal of Engineering Mechanics, vol. 129, no. 1, pp. 71–78, 2003. View at: Publisher Site  Google Scholar
 J. P. Ou, Structural Vibration ControlActive, SemiActive and Smart Control, Science Press, Beijing, China, 2003.
 S. M. Allam and T. K. Datta, “Seismic behaviour of cablestayed bridges under multicomponent random ground motion,” Engineering Structures, vol. 21, no. 1, pp. 62–74, 1999. View at: Google Scholar
 K. Soyluk, “Comparison of random vibration methods for multisupport seismic excitation analysis of longspan bridges,” Engineering Structures, vol. 26, no. 11, pp. 1573–1583, 2004. View at: Publisher Site  Google Scholar
Copyright
Copyright © 2013 Gang Li 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.