ENERGY AND EXERGY ANALYSIS OF RICE STRAW GASIFICATION

 

I.S. DALMIS, B. KAYISOGLU, S. TUG†§   and   M.R. DURGUT

Mechanical Engng. Department, Tekirdağ Namık Kemal University, 59860 Corlu Tekirdag, Turkey.

Biosystem, Engng. Department, Tekirdağ Namık Kemal University, 59100 Tekirdag, Turkey

§ Vocational School of Technical Sciences, Tekirdağ Namık Kemal University, 59100 Tekirdag, Turkey

Corresponding author e-mail: idalmis@nku.edu.tr

 

 

Cite this article as: 

Dalmis, I.S., Kayisoglu, B., Tug, S., Durgut, M.R. (2022) “Energy and exergy analysis of rice straw gasification”, Latin American Applied Research 52(2), pp 111-117.

 


Abstract--  In this study, energy and exergy analyzes were performed in the gasification of rice straw pellets prepared in 5 different blends: PRF (reference sample with no additives), PVA3 (rice straw + 3% PVA), PML5 (rice straw + 5% molasses), PC5 (rice straw + 5% coal dust), and PC15 (rice straw + 15% coal dust). The average mass flow rates was measured in the gasification process. The tar and gas flow rates varied between 5.30g/s and 5.70g/s, 0.063g/s and 0.069g/s and between 0.424mol/s and 0.464mol/s, respectively. The heating value (LHV) of the pellets ranged from 12.45MJ/kg to 12.93MJ/kg. The calorific values of the obtained syngas samples were between 3885.5MJ/Nm3 and 4427.7MJ/Nm3. The energy efficiency of the pellet samples in gasification ranged from 53.44% to 58.01% and exergy efficiency varied from 49.19% to 53.48%. The lowest irreversibility value in the gasification process was 36.74kW in PC5 pellet, the highest irreversibility value was 44.21kW in PRF pellet. As a result of the thermodynamic analysis of the pellet samples in gasification, it was concluded that there is no need to add any additives in the pelletization of the rice straw.

Keywords-- irreversibility, biomass blends, ex-ergy analysis, rice straw, gasification.

I. INTRODUCTION

Biomass gasification is the most reliable and promising method nowadays to generate electricity because this process provides a sustainable and affordable alternative to fossil fuel-based process plants at small and medium levels (Kayisoglu et al., 2016; Khan, 2015, Parthasarathy et al., 2021). Gasification is a thermochemical process that can convert the biomass in a partial oxidation process at elevated temperature into syngas which contains such as H2, CO, CH4, and CO2 gases for thermal and power applications (Manatura et al., 2017; Rezaiyan and Cheremisinoff, 2005). Gasification reactions can be defined as a combination of pyrolysis reactions, followed by high temperature tar and coal reactions, followed by other primary gaseous reactions to obtain simple gas products (Parthasarathy et al., 2021). In the gasification process, the air is generally used due to its low cost. When the air is used in the gasification process of the biomass, a syn-gas with a heating value of 4-7MJ/Nm3 is obtained de-pending on the raw material. The higher heating value (12-28MJ/Nm3) can be obtained by using pure O2, but the cost of syngas production increases due to the cost of O2 production (Manatura et al., 2017).

The potential use of existing natural gas infrastructure as an energy carrier is considered as the major advantage. Syngas can be used as a green alternative to natural gas in households and fuel in transportation. Currently, several research institutes, including the Energy Research Center of the Netherlands (ECN), Center for Solar Energy and Hydrogen Research (ZSW) Baden Würtenberg, and Paul-Sherrer Institute (PSI) in Switzerland, are work-ing on developing biomass-to-SNG technology (Vitasari et al., 2011).

Experimental and theoretical studies were conducted (Singh et al., 2015) on a 50kWth downdraft gasifier with biomass blends of various quantities and qualities avail-able in rural areas, in which the effective utilization of biomass materials as blends can meet the rural energy demand have shown by the experimental and theoretical studies. Xiang et al. (2021) attempted to find a gasifier that is most suitable for the gasification of village-level solid wastes through the exergy analysis method. The results showed that the updraft fixed bed gasifier had higher exergy efficiency, and the gas produced by the downdraft fixed bed gasifier has a higher heating value.

Rice is one of the most important cereals consumed in the world after wheat. In recent years, rice production has increased in Turkey. The straws remaining on the sur-face of the field after the rice harvest is a problem for farmers. The silica content of rice straw is higher than other cereals. Therefore, it is difficult to break down the rice straws and very hard to decompose. Therefore, farmers are banned, although the rice straws remaining in the field are burned every year. This causes loss of energy and adverse environmental conditions. Evaluations of rice straws with the proper techniques and different methods have made a significant contribution to the country's economy and also will help reduce the impact of adverse environmental conditions. The gasification process of rice straw is one of these methods. The gasification of rice straw will be able to gain 75x109 MJ of energy in our country every year (Kayisoglu et al., 2016).

The lack of consensus on the evaluation of the performance of different stages of energy systems is one of the difficulties of measuring energy efficiency. In practice, energy efficiency has various performance indicators, such as thermodynamics or economics. Based on the second law (exergy analysis), thermodynamic indicators of process performance are commonly accepted as the most natural way to measure the performance of different processes, including but not limited to energy technology, chemical engineering, transportation, agriculture, etc. (Vitasari et al., 2011). Nowadays, energy analysis and exergy analysis have been integrated and applied to thermal performance evaluation of various gasification processes by many researchers. The exergy analysis of hydrogen production from biomass steam gasification was reviewed by Zhang et al. (2019), but they did not distinguish the type of gasifiers. The results indicated that the exergy efficiency initially increased and was finally decreased by both the steam to biomass ratio and steam flow rate. Mehrpooya et al. (2018) investigated 23 different kinds of biomass sources and analyzed the modeling and simulation of the biomass gasification process. The results showed that the highest (about 90.0%) exergy efficiency is the drying stage in all cases. Echegaray et al. (2016) investigated the gasification of peach pits exergetic efficiency. They utilized that thermodynamic indicators of process performance based on the second law (exergy analysis) in order to evaluate the effect of different operational parameters (temperature, supply air/stoichiometric air, supply steam/carbon ratio and moisture feed). The experiments shown that exergetic efficiency of the gasification process were decreases when the all considered operational parameters increase. Rodriguez et al. (2018) presented studies about the gasification of the lignocellulosic winery wastes in fluidized bed to obtain energy. The exergetic improvement potential (IP) and sustainability index (SI) variations with different operational variables were analyzed based on the exergy analysis. Gonzalez et al. (2020) worked on the exergy balance of an integrated biomass gasification power plant. The total destroyed exergy of biomass gasification and power generation processes showed a higher contribution and reaching values of 42.4% and 45.5% of the total destroyed exergy. Some researchers have also investigated in terms of the waste of gasification reactions. Echegaray et al. (2019) presents a thermodynamic model for describing the five wastes gasification behavior with char and tar formation. They considered that influence of variables process on the exergetic efficiency and sustainability index and declareted that the main problem for biomass gasification process is the tar often do to it produces soiling and equipment erosion, and an effective energy loss between 5 and 15%.

In this study, rice straw pellets prepared with different additives have been gasified with a micro-scale gasifier which was developed in our department. The main purpose of this paper is to compare rice straw pellets for their gasification efficiency using energy and exergy analysis methods.

II. EXPERIMENTAL SETUP
A. The Gasifier System

Experimental setup of the gasifier system includes adiabatic downdraft gasifier reactor, cyclone, gas cooling unit and condensation tank, vacuum pump and its service water tank, flare unit, measurement and control components,

Figure 1: Schematic view of the gasification system.

gas chromatography device (GC), and its components. The schematic view of the gasification unit is shown in Fig. 1. The system has a fixed bed reactor with an upper air inlet. The capacity of the reactor is 25kg of biomass. The gasifier reactor is a throatless type and the reactor diameter is 350mm. The height of the main reactor body is 840mm and is made up of stainless steel (AISI 310) material. Inner walls of the body have a refractive layer (Hycast 70) that is applied as 50mm. 1.5kW powered vacuum pump was used to create a gas flow in the line. Ash removal helix and gas cooler fan have 0.55kW powered motors.

Measurements were made from 7 points for temperature, 3 points for pressure, 2 points for flow rates. K-type thermocouples were used for temperature measurements. Air and gas flow rates were measured by orifice flow meters. Experimental data were collected and monitored by a Programmable Logic Controller (PLC) based moduler system. The control cabinet includes a 24VDC power supply, a 7-inch color touch-sensitive human-machine interface (HMI), a PLC CPU module, PLC expansion modules, relays and contactors. An USB flash drive plugged into HMI is used to save data. GC was used for the analysis of syngas produced in the gasifier operated at 0.2 Er ratio. The position of the GS was shown in Fig. 1.

B. Characteristics of Rice Straw Pellets

In this study, rice straws were chopped and blended with different additive materials like PVA, molasses, and coal dust. Five different samples were prepared and evaluated for the study. The proximate and ultimate analyses of the rice straw pellets were done in TUBITAK MAM Institute. The compositions of rice straw pellets used in this re-search are given in Table 1.

C. Syngas Analysis

The syngas sample with the help of a pipe from the main gas output line was taken and analyzed with Agilent 7890B GC model gas chromatography device. The de-vice gives volumetric percentages weight of gas compo-nents (H2, CO, CH4, CO2, and N2) contained in the syngas.

III. ENERGY AND EXERGY ANALYSIS

The schematic view of the gasification process using rice straw pellets is shown in Fig. 2 for evaluation energy and exergy analysis. Inputs of the system are biomass, air, ash screw, cooling fan, and vacuum pump and outputs are



Table 1. Composition of rice straw pellets

Code

Pellet Composition

PRF

No additive, reference pellet

PVA3

Rice straw + PVA %3

PML5

Rice straw + Molasses %5

PC5

Rice straw + Coal dust %5

PC15

Rice straw + Coal dust %15

Figure 2: Schematic view of the inlet and outlet flows of the gasification system.

 

syngas, tar, ash, and char. The syngas leaving the reactor is subjected to a cooling process. During the gasification process, the temperature of the gasifier was kept at 800°C and ER was adjusted as 0.2. In the gasification of the rice straw, when the core region temperature exceeds 800°C, vitrification and agglomeration occur in the reactor (Tuğ, 2016).

Equivalence Ratio ():

The important parameter in gasification is the equivalence ratio (), which is defined as the actual air-fuel ratio to the stoichiometric air-fuel ratio (Manatura et al., 2017):

,      (1)

where  and  are actual air-fuel ratio and stoichiometric air-fuel ratio, respectively.

Energy Balance:

The energy balance of the gasifier can be written as (Manatura et al., 2017):

,                      (2)

 

where , , , , ,  and  represent the energy flow rate of biomass, electricity, syngas, tar, ash, char, and loss part in kW, respectively. Electricity is the sum of the installed power of the electric motors that operate the vacuum pump, cooling fan, and ash screw used in the gasification system. =2.60kW in the gasification system.

Total energy flow is;

                                           (3)

where , ,  and  represent the kinetic, potential, physical, and chemical energy rates in kW, respectively.

Neglecting  and  Eq. (3) reduces to:

                    (4)

The physical (sensitive) energy is

(5)

where; ,  and  are gas flow rate in kmol/s, Enthalpy change in kJ/kmol, and constant pressure specific heat in kJ/kmolK, respectively.

Equaion (5) is suitable for air since it is heated before entering the gasifier. In this study, the air was not preheated, thus .

Constant pressure specific heat (𝐶𝑝) for each gas component can be calculated equations that are given in Table 2.

For the biomass and tar, their chemical energy can be evaluated as:

               (6)

where  is the heating value of biomass and tar in kJ/kg and  is the mass flow rate in kg/s.

The LHV of syngas in kJ kmol-1 is (Manatura et al., 2017):

                           (7)

where ,  and  represent a molar fraction of these gases in syngas, respectively.

The energy efficiency of the gasification can be calculated by the following equation

. (8)

Exergy analysis:

Exergy analyzes of biomass gasification using rice straw pellets as a feedstock were performed by the method applied by Szargut et al. (1988) and was evaluated with the following assumptions (Lewandowski and Kicherer, 1996):

·         The system is operated at a steady state.

·         Potential and kinetic energies are negligible.

·      Reference state (dead state) is set as  and 1atm.

·         Ash residue that remains behind the gasification process is negligible.

·         Syngas is assumed to be an ideal gas.

The exergy balance of the gasification can be defined as:

,                               (9)

where , ,  and  rep-resent the exergy of the biomass, vacuum pump, cooling fan, syngas, tar in kW, respectively.  is the irreversibility of the gasifier.

Chemical exergy () and physical exergy () are the sum of exergy () of syngas.

           (10)

Only chemical exergy was considered for biomass. The exergy of biomass can be defined as (Szargut et al., 1988):

,                            (11)

where  and  represent the lower heating value in kJ/kg and quality of fuel, respectively.  is the mass flow rate of biomass in kg/s.

The quality of fuel () can be expressed as:

          (12)

 

 


Table 2. Constant pressure specific heat ideal gas and temperature relations (Karamarkovic and Karamarkovic, 2010).

Gas

𝑪𝒑(𝒌𝑱/𝒌𝒎𝒐𝒍𝑲), =𝑻(𝑲𝒆𝒍𝒗𝒊𝒏)/𝟏𝟎𝟎

Range, K

Max. Error, %

N2

300-3500

0.43

O2

𝐶𝑝=37.432+0.20102−178.57+236.884

300-3500

0.30

H2

𝐶𝑝=56.505−702.74+1165.0−560.70

300-3500

0.60

CO

𝐶𝑝=69.145−0.704634−200.77+176.76

300-3500

0.42

H2O

𝐶𝑝=143.05+183.54−82.751−3.6989

300-3500

0.43

CO2

𝐶𝑝=−3.7357+30.529−4.1034 +0.024198

300-3500

0.19

CH4

𝐶𝑝=−672.87+439.74−24.8754+323.88

300-3500

0.15

 


Table 3. Specific absolute entropies of the syngas components

Substance

𝒔𝒐 (𝒌𝑱/𝒌𝒎𝒐𝒍𝑲)

N2

191.610

H2

130.684

CO

197.653

CO2

213.795

CH4

186.256

where , , and  are the molar fraction of carbon, hy-drogen, and oxygen, respectively.

The physical exergy of syngas is determined as:

(13)

For each gas component, the specific physical exergy in kJ/kmol is defined as:

                                    (14)

where  and  are the specific enthalpies in kJ/kmol and entropy in kJ/kmolK at the state (pressure,  (kPa) and temperature,  (K)). Moreover,  and  represent the specific enthalpy of formation and entropy at the reference state. When the temperature of the syngas is known, the  can be determined for each gas component as below:

      (15)

The entropy of each gas component in the syngas at the state condition can be calculated by:

                     (16)

where  is the universal gas constant and its value is 8.314kJ/kmolK.

Molar-specific absolute entropies of the components of the syngas at the reference state are given in Table 3.

The chemical exergy of syngas can be determined by the composition analysis of syngas and the flow rate. Its value is obtained from the following equation,

           (17)

where  represents the standard chemical exergy of the syngas compositions  that can be obtained from any thermodynamics book.

The exergy efficiency of the gasification can be calculated by the following equation:

. (18)

IV. RESULT AND DISCUSSION

Characterisation of samples:

Analysis results of pellet samples are displayed in Table 4 and Table 5. The  values of the pellet samples ranged from 12.45MJ/kg to 12.93MJ/kg, and the  values ranged from 13.53 to 13.98MJ/kg.  and  values are close to each other in all samples. Manatura et al. (2017) reported that in the rice husk pellets the LHV value was 14.17MJ/kg and the HHV value was 15.49MJ/kg. The heating value of the rice husk pellets is higher than the rice straw pellets. This is because the O/C ratios of the rice husk are lower than the rice straw. In their study, the O/C value of the rice husk pellets was reported as 0.92. In this study, O/C value of the rice straw pellets was around 0.87 on average (Table 3). The heat-ing value of fuels decreases nearly linearly with increasing O concentration (Lewandowski and Kicherer, 1996).

Gasification:

The tests were performed in triplicate and the calculations were made according to the average of the results. The average mass flow rates measured in the gasification process are given in Table 6 for each pellet sample. The mass, tar and gas flow rates varied between 5.30g/s and 5.70g/s, 0.063g/s and 0.069g/s and between 0.424mol/s and 0.464mol/s, respectively. In general, the tar flow rate was about 1.1% of the biomass flow rate. Similar results were found in the process of gasification with rice husks by Manatura et al. (2017). It was explained that updraft gasifiers produce more “tar” than downdrafts while “tar” production of fluidized beds was in between them. An average value of about 50g-tar/Nm3-syngas “tar” was measured in raw producer gases from updraft gasifiers which are higher than in any other gasifier. It was reported that an average “tar” loading of about 10g- tar/Nm3-syngas was measured in fluidized beds and CFBs (Graham and Bain, 1993). In this study, the tar production was about 6.6g-tar/Nm3-syngas on average.

The specific heat, enthalpy change, and entropy values of each gas component calculated as a function of gas temperature and pressure of syngas after cooling are given in Table 7.

 


Table 4. Proximate analysis of pellet samples

Pellet Samples

Moisture (wt%)

Ash (wt%)

Volatile matter (wt%)

Fixed Carbon (wt%)

 (MJ/kg)

 (MJ/kg)

PRF

7.01

17.21

61.61

14.18

12.77

13.85

PVA3

7.38

17.62

61.09

13.92

12.71

13.78

PML5

6.84

17.03

61.09

14.97

12.78

13.84

PC5

8.94

17.86

58.38

14.83

12.45

13.53

PC15

8.39

19.16

56.55

15.91

12.93

13.98

 

Table 5. Ultimate analysis of pellet samples (wt%)

Pellet Samples

C

H

N

S

O

H/C

O/C

PRF

39.90

4.89

1.24

0.20

35.27

0.12

0.88

PVA3

39.42

4.95

1.32

0.7

35.12

0.13

0.89

PML5

39.10

5.05

1.69

0.18

35.71

0.13

0.91

PC5

39.37

4.80

1.60

0.24

34.38

0.12

0.87

PC15

40.16

4.79

1.50

0.32

32.32

0.12

0.80

 

Table 7. Specific heat, enthalpy changes, and entropies of syngas components

Syngas components

Syngas Temperature (K)

Syngas Pressure (kPa)

Cp (kJ/kmolK)

h (kJ/kmol)

So (kJ/kmolK)

S (kJ/kmolK)

N2

338

99

29.19

1196.7

191.61

195.56

H2

339

99

29.05

1190.9

130.68

134.62

CO

340

99

29.09

1192.8

197.65

201.59

CO2

342

99

38.75

1588.8

213.80

218.98

CH4

345

99

37.58

1540.7

186.26

191.29

 

Table 8. Molar fraction (% dry basis) and LHV of syngas

Table 9. Energy balance of gasifier system in kW

 

PRF

PVA3

PML5

PC5

PC15

Biomass

78.95

73.03

78.89

71.71

78.29

Electricity

2.60

2.60

2.60

2.60

2.60

TOTAL INPUT

81.55

75.63

81.49

74.31

80.89

Chemical energy of syngas

43.17

41.27

43.70

42.53

42.62

Physical energy of syngas

0.55

0.54

0.59

0.57

0.61

Tar

2.34

2.27

2.48

2.41

2.56

Other loss

35.48

31.56

34.71

28.79

35.11

Energy efficiency (%)

53.62

55.27

54.35

58.01

53.44

 


Table 6. Mass flow rate biomass, tar, and syngas

Pellet

Biomass (g/s)

Tar (g/s)

 

Syngas (mol/s)

PRF

5.70

0.065

 

0.435

PVA3

5.30

0.063

 

0.424

PML5

5.70

0.069

 

0.464

PC5

5.30

0.067

 

0.451

PC15

5.60

0.071

 

0.477

 

Table 10.  and chemical exergy values of rice straw pellets

Pellet

 (kJ/kg)

 (-)

Exch (kJ/kg)

PRF

12770

1.1589

14799

PVA3

12710

1.1611

14758

PML5

12780

1.1657

14898

PC5

12450

1.1574

14410

PC15

12930

1.1442

14795

 

The molar fraction and  of syngas for each pellet sample are shown in Table 8. LHV of syngas samples varied between 3985.5kJ/Nm3 and 4427.7kJ/Nm3. The heating value is related to the molar fraction of hydrogen and nitrogen in syngas. As the hydrogen ratio increases, the heating value of the syngas also increases (Kartal and Ozveren, 2020). Conversely, if the nitrogen ratio in-creases, the heating value of syngas decreases. This situation is evident in Table 8.

Energy and exergy analyzes:

The energy balances of gasification of rice straw pellets are given in Table 9. The total energy input to the system ranged from 74.31kW to 81.55kW. Energy efficiencies of gasification of pellet samples varied between 53.44% and 58.01%. Manatura et al. (2017) found that the energy efficiency of the rice husk gasification was about 44%. They have externally applied heat energy to heat the air during the gasification process. So the efficiency was lower than our values. In the process of gasification of biomass, energy efficiency can vary widely depending on the type of biomass and the gasification process (Rodriguez, 2016). The gasifier was operated at optimum 0.2 ER ratio, excluding distribution, heat losses or other losses that result from operational activities (Onabanjo et al., 2016). The energy efficiency values of the gasification of pellet samples are close to each other.

The  and the exergy values of each pellet sample are displayed in Table 10. The  values changed between 1.1442 and 1.1657. Zhang et al. (2011) reported that  values for biomass changed between fuels in the range of 1.05-1.19. The beta values found in this study are within the specified limits. Manatura et al. (2017) also founded  value for the rice husk as 1.17. The  and the exergy values of the rice straw pellets were very close to each other in this study. There was no significant difference in the chemical exergy values of rice straw pellets. Ptasinski et al. (2007) expressed that the chemical exergy values of different biomass vary between 14760kJ/kg and 17129 kJ/kg. In this study, the chemical exergy values of rice straw pellets were close to the bottom of these limits (Table 10).


 

Table 11. Exergy balance of gasifier system in kW

 


Chemical exergy contained in the biomass is larger than its LHV and the chemical exergy contained in the product gas is smaller than its chemical energy. Ptasinski et al. (2007) explained larger chemical exergies than LHVs for biomass by the fact that polymers such as cellulose and hemicellulose are highly ordered structures, and work can be delivered if these are decomposed. Physical exergy values were very low in all samples. This is caused by the syngas which are subjected to cooling while leaving the system. However, even though there is no syngas cooling process, physical exergy is always smaller than chemical exergy. The reason is that the chemical exergy of the biomass is the main constituent of the total exergy and the contribution of physical exergy is much smaller. The solid biofuels with high oxygen content are regarded as high-quality fuels, for which a penalty is paid when decomposing them into small gaseous components. Also, the gas produced from solid bio-mass gasification has a lower temperature so that it contains less physical exergy (Zhang et al., 2011).

In pellet samples, total exergy efficiencies varied be-tween 49.19% and 53.48%. In all samples, the efficiency of exergy was lower than energy efficiency. The same results have been seen in researches related to biomass gasification. Zhang et al. (2011) have found that the energy efficiencies of biomass gasification are between 52.38% (rice husk, ER= 0.25) and 77.41% (wood chip, ER = 0.38), while those of polypropylene gasification are from 54.45% (ER = 0.20) to 58.43% (ER=0.35). The exergy efficiencies of biomass gasification are between 36.5% (rice husk, ER=0.25) and 50.19% (wood chip, ER=0.38). The exergy efficiencies of dry refinery sludge gasification are from 31.93% (ER=0.24) to 50.38% (ER=0.195). Energy and exergy efficiencies will be reduced by the increasing N2 which has low energy, and exergy values (Ahmed et al., 2014). The use of air in the gasification process results in high nitrogen content in the syngas. If pure oxygen is used, the gasification efficiency will be higher. However, the cost of gasification will also increase.

Irreversibility values of syngas samples were between 36.74kW and 44.21kW. The lowest irreversibility was in PC5 with 36.74kW and the highest irreversibility was in PRF with 44.21kW. The largest internal exergy losses (irreversibilities), the separation of carbon dioxide from methane, and drying of waste biomass take place in the methanation section in the gasifier (Vitasari et al., 2011). Although it is insufficient to compensate losses due to high moisture content and/or thermal losses, pre-heating air and/or bagasse may reduce irreversibility (Pellegrini and Oliveira, 2007).

V. CONCLUSIONS

In this study, the energy and exergy analysis of rice straw pellets in five different compositions was performed. Results of experiments showed that physical exergy values of syngas samples were very small due to the application of syngas cooling. In all pellet samples, energy efficiency was higher than exergy efficiency. However, there is no significant difference between them in terms of energy and exergy efficiency. For this reason, PVR pellet sample which does not have any additives can be recommended for rice straw gasification. Exergy analysis gives results concerning only thermodynamic efficiency. The total energy input to the system ranged from 74.31kW to 81.55kW. Energy efficiencies of gasification of pellet samples varied between 53.44% and 58.01%. The presented results in this research will be helpful in further process development of rice straw gasification. Because the gasification of rice straw has important technical problems. The high silicon content requires continuous control of the core region temperature in the reactor. However, in order to make a final judgment about process feasibility, it is also necessary to perform economic analysis and should be evaluated together with technical analysis.

ACKNOWLEDGEMENTS

We would like to thank TUBITAK for supporting this project that numbered 113O434. The gasifier used in this research was developed within the scope of the TUBITAK project.

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Received: July 16, 2021

Sent to Subject Editor: September 16, 2021

Accepted: November 22, 2021

Recommended by Subject Editor José L. Díaz de Tuesta