Elsevier

Automatica

Volume 36, Issue 3, March 2000, Pages 363-378
Automatica

Drum-boiler dynamics

https://doi.org/10.1016/S0005-1098(99)00171-5Get rights and content

Abstract

A nonlinear dynamic model for natural circulation drum-boilers is presented. The model describes the complicated dynamics of the drum, downcomer, and riser components. It is derived from first principles, and is characterized by a few physical parameters. A strong effort has been made to strike a balance between fidelity and simplicity. Results from validation of the model against unique plant data are presented. The model describes the behavior of the system over a wide operating range.

Introduction

There are dramatic changes in the power industry because of deregulation. One consequence of this is that the demands for rapid changes in power generation is increasing. This leads to more stringent requirements on the control systems for the processes. It is required to keep the processes operating well for large changes in the operating conditions. One way to achieve this is to incorporate more process knowledge into the systems. There has also been a significant development of methods for model-based control, see Garcia, Prett and Morari (1989), Qin and Badgwell (1997) and Mayne, Rawlings and Rao (1999). Lack of good nonlinear process models is a bottleneck for using model-based controllers. For many industrial processes there are good static models used for process design and steady-state operation. By using system identification techniques it is possible to obtain black box models of reasonable complexity that describe the system well in specific operating conditions. Neither static models nor black box models are suitable for model-based control. Static design models are quite complex and they do not capture dynamics. Black box models are only valid for specific operating conditions.

This paper presents a nonlinear model for steam generation systems which are a crucial part of most power plants. The goal is to develop moderately complex nonlinear models that capture the key dynamical properties over a wide operating range. The models are based on physical principles and have a small number of parameters; most of which are determined from construction data. Particular attention has been devoted to model drum level dynamics well. Drum level control is an important problem for nuclear as well as conventional plants, see Kwatny and Berg (1993) and Ambos, Duc and Falinower (1996). In Parry, Petetrot and Vivien (1995) it is stated that about 30% of the emergency shutdowns in French PWR plants are caused by poor level control of the steam water level. One reason is that the control problem is difficult because of the complicated shrink and swell dynamics. This creates a nonminimum phase behavior which changes significantly with the operating conditions.

Since boilers are so common there are many modeling efforts. There are complicated models in the form of large simulation codes which are based on finite element approximations to partial differential equations. Although such models are important for plant design, simulators, and commissioning, they are of little interest for control design because of their complexity. Among the early work on models suitable for control we can mention Profos 1955, Profos 1962, Chien, Ergin, Ling and Lee (1958), de Mello (1963), Nicholson (1964), Thompson (1964), Quazza 1968, Quazza 1970, Caseau and Godin (1969), Kwan and Andersson (1970), McDonald and Kwatny (1970), Speedy, Bell and Goodwin (1970), Dolezal and Varcop (1970), McDonald, Kwatny and Spare (1971), Eklund (1971), Åström and Eklund (1972), Åström (1972), Bell (1973), Borsi (1974), Lindahl (1976), Tyssø, Brembo and Lind (1976), Bell, Rees and Lee (1977) and Morton and Price (1977). Boiler modeling is still of substantial interest. Among more recent publications we can mention Maffezzoni 1988, Maffezzoni 1992, Maffezzoni 1996, Klefenz (1986), Jarkovsky, Fessl and Medulova (1988), Unbehauen and Kocaarslan (1990), Höld (1990), Na and No (1992), Kwatny and Berg (1993), Na (1995).

The work presented in this paper is part of an ongoing long-range research project that started with Eklund (1971) and Bell (1973). The work has been a mixture of physical modeling, system identification and model simplification. It has been guided by plant experiments in Sweden and Australia. The unique measurements reported in Eklund (1971) have been particularly useful. A sequence of experiments with much excitation were performed on a boiler over a wide range of operating conditions. Because of the excitation used, these measurements reveal much of the dynamics of interest for control. Results of system identification experiments indicated that the essential dynamics could in fact be captured by simple models, see Åström and Eklund (1972). However, it has not been easy to find first principles models of the appropriate complexity. Many different approaches have been used. We have searched for the physical phenomena that yield models of the appropriate complexity. Over the years the models have changed in complexity both increasing and decreasing; empirical coefficients have been replaced by physical parameters as our understanding of the system has increased. The papers Åström and Eklund 1972, Åström and Eklund 1975, Åström and Bell 1988, Åström and Bell 1993 and Bell and Åström (1996) describe how the models have evolved. The models have also been used for control design, see Miller, Bentsman, Drake, Fahkfahk, Jolly, Pellegrinetti and Tse (1990), Pellegrinetti, Bentsman and Polla (1991), and Cheng and Rees (1997). Models based on a similar structure have been used for simulation and control of deaerators, see Lu, Bell and Rees (1997), and nuclear reactors, see Yeung and Chan (1990), Höld (1990), Irving, Miossec and Tassart (1980), Parry et al. (1995), Menon and Parlos (1992), Thomas, Harrison and Hollywell (1985), Schneider and Boyd (1985) and Kothare, Mettler, Morari, Bendotti and Falinower (1999).

Section snippets

Global mass and energy balances

A schematic picture of a boiler system is shown in Fig. 1. The heat, Q, supplied to the risers causes boiling. Gravity forces the saturated steam to rise causing a circulation in the riser-drum-downcomer loop. Feedwater, qf, is supplied to the drum and saturated steam, qs, is taken from the drum to the superheaters and the turbine. The presence of steam below the liquid level in the drum causes the shrink-and-swell phenomenon which makes level control difficult. In reality the system is much

Distribution of steam in risers and drum

To obtain a model which can describe the behavior of the drum level we must account for the distribution of steam and water in the system. The redistribution of steam and water in the system causes the shrink-and-swell effect which causes the nonminimum-phase behavior of level dynamics, see Kwatny and Berg (1993). One manifestation is that the level will increase when the steam valve is opened because the drum pressure will drop, causing a swelling of the steam bubbles below the drum level.

The

The model

Combining the results of 2 Global mass and energy balances, 3 Distribution of steam in risers and drum we can now obtain a model that gives a good description of the boiler including the drum level. The model is given by the differential equations , , , , and (16). In addition there are a number of algebraic equations. The circulation flow rate qdc is given by the static momentum balance (15), the steam flow rate through the liquid surface of the drum qsd by (18), and the drum level ℓ by Eq.

Step responses

To illustrate the dynamic behavior of the model we will simulate responses to step changes in the inputs. Since there are many inputs and many interesting variables we will focus on a few selected responses. One input was changed and the others were kept constant. The magnitudes of the changes were about 10% of the nominal values of the signals. To compare responses at different load conditions the same amplitudes were used at high and medium load.

Comparisons with plant data

Much of the model development was based on plant experiments performed with the P16-G16 unit at Öresundsverket in Malmö, Sweden in collaboration with Sydkraft AB. The experiments are described in Eklund (1971) and Åström and Eklund 1972, Åström and Eklund 1975. They were carried out in open loop with the normal regulators removed. The signals were filtered and sampled at a rate of 0.1 Hz. To ensure a good excitation of the process PRBS-like perturbations were introduced in fuel flow rate,

Conclusions

A nonlinear physical model with a complexity that is suitable for model-based control has been presented. The model is based on physical parameters for the plant and can be easily scaled to represent any drum power station. The model has four states; two account for storage of total energy and total mass, one characterizes steam distribution in the risers and another the steam distribution in the drum. The model can be characterized by steam tables and a few physical parameters.

The model is

Acknowledgements

The research has been supported by the Sydkraft Research Foundation and the Swedish National Board for Industrial and Technical Development under contract 97-04573. This support is gratefully acknowledged. We would also like to express our sincere gratitude to Sydkraft AB for their willingness to perform experiments on plants to increase our understanding of their behavior. Useful comments on several versions of the manuscript have been given by our colleagues J. Eborn, H. Tummescheit, and A.

Karl J. Åström is Professor and Head of the Department of Automatic Control at Lund University since 1965. He has broad interests in automatic control including, stochastic control, system identification, adaptive control, computer control and computer-aided control engineering. He has supervised 44 Ph.D. students, written six books and more than 100 papers in archival journals. He is a member of the Royal Swedish Academy of Engineering Sciences (IVA) and the Royal Swedish Academy of Sciences

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    Karl J. Åström is Professor and Head of the Department of Automatic Control at Lund University since 1965. He has broad interests in automatic control including, stochastic control, system identification, adaptive control, computer control and computer-aided control engineering. He has supervised 44 Ph.D. students, written six books and more than 100 papers in archival journals. He is a member of the Royal Swedish Academy of Engineering Sciences (IVA) and the Royal Swedish Academy of Sciences (KVA) and a foreign member of the US National Academy of Engineering and the Russian Academy of Sciences. Åström has received many honors including three honorary doctorates, the Callender Silver Medal, the Quazza Medal from IFAC, the Rufus Oldenburger Medal from ASME, the IEEE Control Systems Science Award and the IEEE Medal of Honor.

    Rod Bell is an Honorary Senior Research Fellow, a position he has held since February 1998. His previous position was Head of the Computing Department which he held since the beginning of 1994. He obtained his Ph.D. (Application of Optimal Control Theory to Industrial Processes) in 1972 from the University of New South Wales. He joined the academic staff at Macquarie University in 1972. He became interested in computers (hardware and software) in 1958 when he worked on one of the first digital computers in Australia, UTECOM at the University of New South Wales. His current research interests lie mainly in the Application of Control Theory to areas such as Industrial Processes (Power Stations in particular), National Economies, Management and Robotics. He is a member of IEEE. Among his personal interests are horse riding, growing waratahs, bush walking and restoring Jaguar cars.

    This paper was presented at IFAC 13th World Congress, San Francisco, CA, 1996. This paper was recommended for publication in revised form by Associate Editor T.A. Johansen under the direction of Editor S. Skogestad.

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