Modeling and Power Quality Improvement of Grid Connected Induction Generators Driven by Turbo-Expanders

Nowadays, the energy crisis has forced the need to recover the energy which is normally wasted in industrial processes. Gas pressure reducing process in city or power plant gas stations is one of these processes in which the energy is wasted. This work is done by turbo-expanders in parallel with gas regulating valves. In electrical industry, these devices drive generators to produce electrical power from the main process. In this paper a model for turbo-expander is presented. This model which utilizes an online calculation method is more efficient and simpler than the older offline model which surmounts the need for making complicated lookup tables prior to calculation. Because of instantaneous varying of domestic consumptions, environment temperature and other effective parameters, turbo-expander inlet gas pressure and mass flow-rate vary with time and consequently the extracted power has time variant specification and causes some power quality issues such as voltage flicker, voltage sag, etc. So, this system is simulated and power quality issues are investigated for a fault occurring at the point of common coupling (PCC). Then, the flicker in electrical waveforms due to change in input pressure or mass flow rate is investigated. Since the power quality problems due to disturbances are considerable, a D-STATCOM is designed and connected at PCC and it is shown that the STATCOM has improved the power quality problems of the system.


Introduction
In natural gas industry, in order to reduce pipelines size and, then, losses, the gas is transmitted in high pressure levels. The typical pressure of gas in transmission pipelines is in the range of 200-1500 psi so for domestic or industrial consumptions such as power plants, it is necessary to reduce this pressure to the distribution levels. Usually, the pressure reduction is accomplished by mechanical valves at regulating stations where a large amount of latent energy of high pressure gas is wasted during the pressure reduction process [1]. Turbo-expanders can be installed in parallel with these regulating stations in order to recover this energy. Besides, they can reduce the gas pressure for downstream consumptions as well as old pressure regulators (mechanical valves). Moreover, the power extracted by turbo-expanders can drive electrical generators, compressors and other loads. In short, if there is a gas transmission and distribution network, it is possible to recover huge amounts of energy to produce electricity [2,3,4].
Since the gas consumption in domestic and industrial consumers is continuously varying, turbo-expander inlet mass flow-rate varies too. Moreover, turbo-expander inlet gas pressure and mass flow-rate can be affected by environment temperature, pressure drop in transmission pipelines, and some other parameters. Consequently, the turbo-expander output power variations are transferred by coupled generators to the power distribution network and cause voltage flicker at PCC [5,6]. As it is known, flicker can affect the normal operation of various devices, such as lamp illumination, TV representation, as well as, intensive care unit (ICU) and critical care unit (CCU) systems in hospitals; as a result, the flicker generated by the turbo-expander driven generator should be evaluated and mitigated, especially in weak power systems [7]. Moreover, it seems that a sharp drop in the inlet mass flow-rate or in the inlet pressure of turbo-expanders can cause other power quality issues. Also, we need to study the transient stability of the generator when a fault takes place in the power network.
Prior to this work, there has been some investigation on turbo-expander modelling for power system studies. In [8], turbo-expander was introduced for energy recovery in electrical form and some operational topologies of turbo-expander and electrical generators were presented. The basic rule of recoverable energy and variable efficiency of turbo-Connected Induction Generators Driven by Turbo-Expanders expander due to changes in inlet flow rate and pressure was studied in this paper. Then in [9,10], the same model was used for turbo-expander coupled with a synchronous generator to study mechanical oscillation of shaft and power quality issues of the generated power, but didn't provide any solution to overcome it. In these studies, for modelling the turbo-expander, it was required to form a lookup table which relates the change in passing gas enthalpy calculated from a thermodynamic software to the input pressure, output pressure and input constant temperature. This process is shortened in this paper and the temperature change of inlet gas can be easily included.
On the other hand, the generators used in installed turbo-expander systems such as Neka power plant are induction type and are not considered in previous studies. In this paper induction generator and power quality improvement equipment are studied.

Methodology
To study the system, first the expander turbine is modelled. Due to the effect of mass or input pressure variation on expander turbine efficiency, this efficiency variation is included in turbo-expander modelling. The old method for expander power calculation is an offline method. A newer online method is presented for power calculation and the results are compared.
Afterward a flicker meter is designed in software environment for power quality studies and voltage of PCC is investigated during system mechanical or electrical disturbances. To eliminate the voltage disturbances, a D_STATCOM is connected at PCC and it is shown that voltage flicker or voltage sags are decreased. Figure 1 shows a turbo-expander installation topology in parallel with the existing gas pressure regulating station at a city gate. The pipeline leading to the expander inlet is taken from a point of downstream of the monitoring regulator and upstream of the working regulator. The monitor regulator is, therefore, still able to provide back-up pressure control at the event of a malfunction. The turbo-expander nozzle control system is capable of holding turbine downstream pressure in an approximately constant value [10]. Figure 1. Schematic representation of gas regulating station and turbo-expander installation topology [11] Since the expansion process produces very cold gas in turbine downstream, if thermodynamical calculations indicate hydrate formation probability in the turbine downstream, gas preheating should be done. Figure 2 shows the modular model of turbo-expander-generator system. Considering this figure, first, the extractable power of the natural gas, , is computed, then the efficiency variation that is caused by inlet mass flow-rate and pressure deviation from their nominal values is considered and the net power delivered to the shaft, , , is calculated. And finally, is the delivered torque to the generator shaft.

Fluid (Gas) Power Computation
Turbo-expanders expand inlet compressed gas with the known pressure ratio in an isentropic process. In this type of expansion, the outlet gas temperature drops or in fact its enthalpy is reduced. With consideration of the first thermodynamic law, relation (1) gives applied power to the turbine shaft [8,12]; =̇× �ℎ , − ℎ , � (1) Where ̇ is mass flow-rate in kg/s, ℎ , and ℎ , are inlet and outlet specific enthalpies in kJ/kg and is the power of expanded fluid (gas) in kw.
To calculate the enthalpies, there is a need of a thermodynamic software and then, forming some lookup tables from input pressure and temperature and enthalpies according to figure 2[9, 10, 13].

Figure 2. Schematic diagram for enthalpies computation from inlet gas specifications
This process is time wasting and difficult to do. It is possible to use some thermodynamic rules to compute the output power of fluid expansion, directly from specifications of inlet and outlet gas and gas specific heat constants ( , ) [2,11,14].
Simulations show that this method is exactly in accordance with the old lookup table method.

Total Efficiency Computation
To consider the effect of mass and pressure variations on turbo-expander efficiency, relations (3) to (5) ought to be used [8,11]. (3) In these equations, P rated is the nominal pressure, P inlet is the gas inlet pressure, m rated is the turbine nominal mass flow-rate, m inlet is the turbine inlet mass flow-rate, and O.C. is the abbreviation of operation condition. Also, η lb is the turbine lower band efficiency, η ub is the turbine upper band efficiency, and finally η ltotal is the turbine overall efficiency regarding operation condition. w mill , in relation (5) is the delivered power from the turbo-expander to the turbine shaft. The block diagram of the proposed system is presented in figure 3.

Dynamic Model of Turbo-Expander
It is necessary to consider gas interaction with vanes in the dynamic model of turbo-expander. In fact, the amount of change appearing in the output mass flow-rate should be analysed for a small change in the turbine vessel mass flow-rate.
The mechanical part of turbo-expander is modelled as a second order model.

Generator Model
Induction or synchronous generators are usually con-nected to turbo-expander systems and each one has its benefits and problems. In this study induction generator is selected to simulate turbo-expander-generator installed in Neka power plant. The induction generator is squirrel-cage machine and its electrical part is represented by a fourth-order state-space model and the mechanical part by a second-order system [16]. The electrical generator parameters are listed in table 1.   Figure 5 shows the study system. Specification of this system is selected according to practical data which is taken from Neka power plant. In this system, the turbo-expander reduces natural gas pressure in parallel with a mechanical valve. A unit 10KV/20KV step-up transformer connects the generator to the power distribution network.

Turbo-Expander Power Calculation
In this section simulation is done to compare the new method of expander power calculation from equation (2) with the old method. Results in figure 6 show a very good conformity of the two methods. The relative error between the two methods is about 0.01%. Connected Induction Generators Driven by Turbo-Expanders

Flicker Study
Flicker is a phenomenon in which the power signal (50 or 60 Hz) is modulated with a 0.05 to 35 Hz envelope signal. This envelope variation is also called voltage fluctuation [17]. Because of turbo-expander generated power variations (due to gas pressure and the mass flow-rate time variant specification), it is required that the amount of flicker generation be studied and analysed. Short-term flicker-severity index is defined for a 10 min time interval.
= 1 indicates irritation limit of the human eye and the < 1 values are eye sensible light fluctuations [17].
It should be mentioned that flicker studies is done in steady-state conditions [7]. International Electrotechnical Commission (IEC) standard flicker meter is used for the short-term flicker-severity index computation. This tool is developed in the MATLAB environment based on IEC 61000-415 standard requirements [18,19]. On the basis of these standard recommendations, the short-term flicker severity , that is computed by this flicker meter should be in range (0.95-1.05) when a square wave signal modulates power signal. Block diagram of the designed flicker meter is shown in figure 7. The square wave signal variations and related results are given in table 2. In the simulation, inlet gas specifications are considered as inlet mass flow-rate 20 kg/s with 10% variance with respect to its mean value and inlet pressure 44 Bars with 5% variance with respect to its mean value. Figure 8 shows the inlet mass flow-rate and pressure waveforms for a 600 s time interval. Figure 8. The inlet mass flow-rate has 10% and inlet pressure has 5% variation with respect to their mean values Continuing the study, the turbo-expander inlet gas specifications were changed, and mass flow-rate has 5 to 40% variances from its mean value (20 kg/s). The values at the PCC with the above considerations are as figure 9. In this figure, the network parameters are constant ( = 90MVA, X/R= 7). With increase of mass flow-rate variance from its average value, the amount of flicker at the PCC increases seriously. In the other case, the mass flow-rate and pressure variance are supposed constant values of 10 and 5%, respectively, but the mean value of mass flow-rate changes from 10 kg/s to 30 kg/s with the same network parameters. Figure 10 shows the at PCC. It is seen that the deviation of average mass flow-rate from the turbo-expander nominal value (20 kg/s) will increase the amount of the produced flicker.

Voltage Sag
Voltage sags are short duration reductions in root mean square (RMS) voltage, caused by short circuits, overloads, and starting large motors. The interest in voltage sags is mainly due to the problems they cause on several types of equipment: adjustable-speed drives, process control equipment, and computers are notorious for their sensibility [20]. Since the simulated fault is three phase type, voltage of PCC during the fault will be around zero and induction generator starts to speed up. During the fault, the generator draws more reactive power from the network than the normal condition. After fault clearing, the generator restores its normal condition according to figure 11. This process takes about 2.2 seconds.

Power Quality Improvement Using D-STATCOM
D-STATCOM is one of the FACTS equipment that can improve the system power quality by reactive power injection. In this study a 3MVA D-STATCOM is used at 20KV PCC bus (according to figure 6) and its other parameters are listed in table 3.
Several works are done in the field of STATCOM control techniques. Some of these methods are based on non-linear techniques suitable for non-linear behaviour systems [21]. Some of them use the model free techniques such as fuzzy controllers which overcome problems related with system modelling or model complexity [22]. In this paper a linear control system is desired for the STATCOM system [23].    Figure 13 shows the flicker level on PCC for mass flow rate varying from 5% to 40% of nominal value and 5% change in pressure. It can be seen that D-STATCOM has truly restricted the flicker level to values under 0.05.

Average Mass Flow [Kg/Sec.] Short Term Flicker Sensitivity Index [Pst]
Without D-STATCOM Installation With D-STATCOM Installation Connected Induction Generators Driven by Turbo-Expanders Figure 14 shows a situation that deviation of mass flow rate and pressure with respect to their nominal values are 10% and 5% respectively. The flicker level is then measured versus mass flow rate average varying from 10kg/sec to 32 kg/sec. The same as the previous case, D-STATCOM has restricted the flicker level on PCC.

Conclusions
In this study, a modular model for turbo-expander-generator system is represented with a new simple method for turbo-expander power calculation that directly calculates output power of expander from inlet and outlet gas specifications. Also this method removes the need for making lookup tables in the same way that was done in previous studies. Also in previous studies synchronous generator was coupled with the turbo-expander, but in this work, simulations are done by induction generators that are more similar to real installed turbo-expander systems such as the system installed in Neka power plant.
To study power quality problems of turbo-expander coupled with induction generator, a flicker meter is developed in the MATLAB environment which measures the amount of produced flicker at the PCC. It is shown that this system can produce considerable amount of flicker on PCC due to variation of pressure and mass flow rate of inlet gas demanded by consumers. Also, because of the induction generator dynamic, voltage and frequency restoration consumes a relatively long time after a fault on PCC. In the next step, a D-STATCOM is used to improve power quality of the system and it is shown that both the flicker level and system restoration time are reduced by using the D-STATCOM.