ISSN : 0970 - 020X, ONLINE ISSN : 2231-5039
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Thermogravimetric Studies on Non-isothermal Oxidative Pyrolysis of Lignocellulosic Materials

Viju Kumar V. G

Department of Chemistry, University College, Thiruvananthapuram, Kerala-695034, India

Corresponding Author E-mail : vgviju@gmail.com

DOI : http://dx.doi.org/10.13005/ojc/360421

Article Publishing History
Article Received on : 20 July 2020
Article Accepted on : 25 August 2020
Article Published : 28 Aug 2020
Article Metrics
ABSTRACT:

Inter species variations of lignocellulosic fibres were investigated in terms of the thermal degradation behaviour of ten different bamboo species using simultaneous TG-DTA analysis. The pyrolysis profiles under oxidative atmosphere shows that the thermal stability based on first stage of degradation is lowest for bambusa vulgaris and higher stability is attributed to dendrocalamus strictus and dendrocalamus membranaceus. The threshold temperature for active biomass pyrolysis for the first mass loss stage is between 220 oC – 240 oC.  Dendrocalamus membranaceus, bambusa nutans and bambusa vulgaris complete the decomposition process in two distinct stages and all others in three stages. The first stage, dominant below 340˚C, degrades polymeric chains forming active carbonaceous char which release volatile gases upon increase in temperature and  ~5% by weight of char  remains above 450 ˚C. The kinetic parameters of the solid state reactions were calculated using the Coats-Redfern integral method and are found to be highest for Bambusa vulgaris. The activation energy for the major mass loss stage in decomposition profiles ranges from 153.0 to 226.9 kJ mol-1. The stability in terms of DTG peak temperature is highest for dendrocalamus strictus, which possess the lowest values for kinetic parameters for the main decomposition stage. For the second stage, values of the kinetic parameters are found to be maximum for Bambusa vulgaris and the lowest for Bambusa nutans. Solid state kinetics were found to obey Mampel equation comprising the mechanism of random nucleation with single nucleus on each particle.

KEYWORDS:

Bamboo; Coats-Redfern; Kinetics; Lignocellulosic biomass; Pyrolysis; Thermogravimetry

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Introduction

Bamboo is a versatile, fast growing and renewable non-timber forest product which grows in comparatively hot and humid climates of subtropical and temperate zones of various parts of earth. Undesirable consequences of population growth in countries like India, demands sustainable and biodegradable materials for daily applications and where bamboo comes in to play.  Despite of its environmental importance and as a bioenergy feedstock, wide varieties of industrial applications of bamboo have been put forward by researchers such as rayon, plywood, reinforced boards, laminated flooring and food. High-performance adhesives and fiber engineering can be employed for durable lignocellulosic composites with high strength. Lignocellulosic biomass can also be incorporated with plastics, glass, metals and synthetic compounds to manufacture diverse products. It is possible to combine more than one materials in a synergic way so that a new engineering system can be evolved which is better than the constituent components with enhanced dimensional stability.1

The studies reveal that the bamboo consists of holocellulose (60-70%), cellulose (26-43%), hemicellulose and lignin (each amounted to about 20-30%), pentosans (20-25%), ash (1.7-5%), silica (~0.7%) and minor constituents like resins, tannins, waxes and trace amounts of inorganic salts. The composition of bamboo culm are comparable to that of common hardwood, but with greater alkaline extract, silica and ash contents.2 Lignocellulosic materials decompose thermally by two different mechanisms irrespective of the variations in their composition. The first mechanism, often found below 300˚C is associated with breakage of polymeric chains by bond fission, dehydration, formation of free radicals, carbonyl, carboxyl and hydroperoxide groups and release of gases such as CO and CO2. Finally the reactive carbonaceous char is yielded. Oxidation of the carbonaceous char and combustible volatile gasses leads to smoldering combustion and flaming combustion respectively.3, 4 The second mechanistic pathway, which operates above 300˚C, mainly consists of the fission of secondary bonds leading to some intermediate systems such as anhydromonosaccharides, which degrades into smaller systems, giving carbonized products.5 Temperature beyond 450°C, the char is predominant, and further decomposition results in the formation of volatiles and is designated as afterglow. The rate of formation of carbonaceous char decreases and tar forming reactions increases above 300˚C. The tar comprises of anhydro sugar derivatives which hydrolyses to reducing sugars. Levoglucosan and other volatile products evaporates in endothermic reaction which is followed by the exothermic combustion reactions.6 

The high percentage of volatiles is released from cellulose, which possess lowest heat of combustion and char yield. The whole wood releases next level of volatiles with higher heat of combustion and percentage of char formation. Bark exhibits higher heat of combustion as compared to wood with a high char and volatiles yield. Heat of combustion of lignin is the highest, giving out maximum char yield and the lowest yield of volatiles.4

Several researchers focused on the thermal behaviour of industrially useful wood species. But the thermal decomposition characteristics of bamboo species are less studied and not compared among species and the field is yet to be explored. Wiedemann studied the wood components in relation to the growth period of a tree using different thermoanalytical techniques.7 The composition of the stem varies according to the age, climate, soil constitution etc. So in order to make the study more scientific and reproducible, the bamboo samples were received from the bamboo plantation of JNTBGRI Thiruvananthapuram, India and the ten species of bamboo trees were of more or less same age and growing in the same terrain with similar growing conditions. The main objectives of this study is to increase the knowledge of the complex chemical mechanisms involved in the thermal degradation of lignocellulosic biomass giving special attention to ten varieties of bamboo. Such a comparison is not made elsewhere till the date.

Materials and Methods

The present investigation aims to assess the thermal stability of ten species of bamboo such as cephalostachyum pergracile (CP), bambusa pallida (BP), dendrocalamus brandisii (DB), dendrocalamus strictus (DS), dendrocalamus hamiltoni (DH), dendrocalamus gigantus (DG), dendrocalamus membranaceus (DM), bambusa nutans (BN), bambusa bambos (BB) and bambusa vulgaris (BV). The ten varieties of bamboo are approximately five years of age and all are cultivated in identical climate and soil conditions. The bamboo samples are collected from approximately three feet above the ground level of plant. The mode of preparation to obtain samples of each bamboo species is as follows. bamboo culms were split into pieces of 2.5 cm wide using a chisel. They were cut into small pieces about 8.0 cm long for the milling process. The separated bamboo strips were kept in water for 48 hours and then strips were removed and sliced longitudinally to extract the fibres. The clean samples are air dried at ambient laboratory conditions for approximately 10 days. Milling and homogenization was done to minimise the errors of thermal analysis procedure and get an average of each system. Bamboo samples were milled by a standard Whiley mill with a screen of 2 mm. Sieving was performed so as to get powder, approximately 40 (400 microns) – 60 (250 microns) mesh size (American Standard ASTM – E 11). Small particle size is preferred to check serious mass and heat transfer limitations. The wood powder (approximately 500 mg) of ten varieties of bamboo are separately treated in 10 mL distilled water, stirred and maintained at room condition for forty eight hours and oven dried at 70 °C.

The thermogravimetric analysis (TGA) was conducted in a Mettler Toledo thermal analyser. A linear heating rate of 10 Kmin-1 in dry dynamic air with a consistent flow rate (60 mLmin-1) is employed for all the samples in the temperature range of ambient to ~800 °C. For the interpretation of thermal behaviour, the data obtained from the TG, DTG (derivative thermogravimetry) and DTA (differential thermal analysis) experiments were used. Thermal decomposition kinetics and mechanism of samples were also investigated using these data.

Results and Discussion

Phenomenological Studies of Different Bamboo Species

The TG, DTG and DTA profiles of all the ten varieties of bamboo have been presented in Fig. 1 to 10. The data of the phenomenological aspects for the ten species of bamboo are tabulated in Table 1.

Table 1: Phenomenological data for the thermal decomposition of ten bamboo species

Sample

Plateau in
TG ( 0C)

Stage

Peak temperature in DTG ( 0C)

Peak width in DTG( 0C)

Peak temperature in  DTA   ( 0C)

Peak width in DTA              ( 0C)

Residue

Cephalostachyum pergracile

Up to 230

 

After 480

I

296

250-320

314

300-320

29.5

II

398

370-420

402

380-420

 

III

444

440-460

446

430-460

4.2

Bambusa pallida

Up to 240

 

 

After 480

I

278

240-310

312

280-330

32.3

II

398

380-430

404

380-430

 

III

450

430-470

457

430-490

6.5

Dendrocalamus brandisii

Up to 230

 

 

After 470

I

286

240-320

312

280-350

33.3

II

409

380-420

413

380-440

 

III

452

440-460

458

440-480

4.3

Dendrocalamus strictus

Up to 240

 

After 470

I

323

290-340

334

320-360

39.7

II

434

400-450

437

410-440

 

III

463

460-480

466

450-470

3.8

Dendrocalamus hamiltoni

Up to 240

 

 

After 480

I

289

250-320

319

280-340

40.9

II

414

370-430

418

380-420

 

III

456

440-470

459

440-470

5.5

Dendrocalamus gigantus

Up to 220

 

After 470

I

289

250-320

314

280-340

38.1

II

402

380-420

408

380-430

 

III

448

430-460

449

440-470

7.5

Dendrocalamus membranaceus

Up to 240

 

After 450

I

323

290-340

333

310-360

38.0

II

 

436

410-450

446

430-450

4.7

Bambusa nutans

Up to 240

After 460

I

321

290-330

321

300-370

35.8

II

426

390-430

436

420-440

 

III

430-450

456

440-460

3.8

Bambusa bambos

 

 

Up to 240

 

After 490

I

320

290-330

331

300-350

39.9

II

424

390-430

427

390-430

 

III

457

430-460

458

450-470

4.7

Bambusa vulgaris

 

 

Up to 220

After 470

I

276

260-310

306

260-320

34.4

II

 

441

410-450

443

420-470

8.5

(mass ~ 3mg, f = 100C min-1, atmosphere = dynamic air)

Since lignocellulosic material is a heterogeneous mixture of various constituent compounds, different fractions decompose at different temperature regimes. Maximum pyrolyzable fraction is attributed to biomass at a given temperature, independent of the time. So we depend upon global mass loss kinetics. Global kinetics can be extended for modeling complex solid state decomposition reactions where the complete spectrum of the hydrocarbon decomposition reactions are irrelevant. Global pyrolysis kinetics applied to bamboo is used to previse the overall rate of mass loss from the sample. Even if so many volatile products are discharged during decomposition, global kinetics shine light upon the key mechanistic stages in the overall decomposition process.

All the bamboo samples show a very small mass loss at 70 – 110°C and are due to desorption of moisture. In the case of CP, mass loss of 3.3% is observed below ~110 oC (Fig. 1). Before the active mass loss starts, small endothermic peak or region is found and is due to the melting or softening of waxy constituents in the sample. The threshold temperature for active wood pyrolysis for the bamboo species, CP is observed at 230°C. All the samples exhibit the onset temperature for the first mass loss stage in between 220 – 240°C. Except DM, BN and BV all other species undergo decomposition in three stages, and DM, BN and BV complete the decomposition process in two distinct stages.

Figure 1: TG-DTA profile of CP

Figure 1: TG-DTA profile of CP

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The sample of CP shows three DTG peaks with maxima at 296, 398 and 444°C. The largest DTG curve is found for the first decomposition stage. Hemicellulose and lignin fractions are degraded in the temperature regime 200 – 300 °C and 225- 450 °C, respectively. Dehydration reactions above 200°C are responsible for the decomposition of hemicellulose and lignin which produce high char quantity. Thermal degradation of cellulose can also be accelerated in presence of acids and oxygen. Volatilisation of laevoglucosan from cellulose is probably involved in the first stage of decomposition.

Of the three major lignocellulosic components, lignin fraction starts decomposing at lower temperature (160-170 oC). But the pyrolysis happens in an extensive temperature range with relatively low rates until ~900 oC. So, in the decomposition of biomass materials, lignin is mainly responsible for char production. Since hemicellulose also starts decomposing at lower temperatures compared to cellulose, it makes an appreciable contribution to the formation of char. Sharp exothermic DTA peaks are found at 314, 402 and 446 °C. For the first stage, especially, in the range from the commencement of the reaction to maximum mass loss rate, oxidation is weakly exothermic as evident by the difference between the DTG peak (296 oC) and DTA maximum (314 oC). In presence of air, the flaming of volatiles precedes, and produces high amount of heat than the glowing of solid residue. Since an oxidative atmosphere is maintained, the initial endothermic pyrolysis reaction is superimposed by strong exothermic oxidation. For the second and third stages the DTG maxima coincide with the corresponding DTA peaks. This indicates that the point of maximum mass loss rate is associated with the decomposition and oxidative gasification of char which is highly exothermic in nature. The sample of CP gives a char residue of 29.5% at the end set of the primary stage of pyrolysis. Approximately 67% of the lignocellulosic material excluding the initial moisture content was lost as volatiles in the oxidative atmosphere below ~360 oC. In the temperature range 240 – 360 oC, cellulose and hemicellulose fractions of bamboo are somewhat completely consumed. Above 410 oC, the mass loss rate is decreased and tends to reach constant mass. The major biomass components are almost completely decomposed below the final DTG peak commences and 11% of the sample remains at this point, which is stable char containing minor amounts of lignin, ash and decomposition products of cellulose and hemicellulose. The third stage of decomposition is indicated by the narrow DTG peak width of 430 – 460 oC and a mass loss of 5.0% is observed for this stage. The exothermic peak towards the end of the decomposition process is due the glowing combustion of high molecular weight chars and decomposition is complete at ~480oC leaving char residue of 4.2%. The similar observations were shown by Amutio et.al., in the oxidative pyrolysis of the bamboo species,where devolatization and char combustion occurs in the range 209 – 315 °C and 315 -333 °C respectively.8 Compared to inert atmosphere, the oxidizing atmosphere accelerates the devolatilization process. In thermogram, a peak which ends at a lower temperature has a shoulder due to char combustion. In the thermogram of  forest pinewood waste, the main peak ends at lower temperature and another second peak is found at higher temperature. Lu and Chen pointed out similar results in another experiment involving bamboo species.9

The sample of BP shows no significant loss of mass till ~220oC, and thereafter, it decomposes in three stages designated by DTG maxima at 278, 398 and 450oC (Fig. 2). The peak temperature of main decomposition stage for BP is reduced by 18oC compared to main stage decomposition of CP. It is due to the varying chemical composition of hemicellulose and cellulose. Since hemicellulose starts decomposing at much lower temperature than cellulose does, its higher percentage of former may shift DTG peak temperature to lower value. But for the second stage, both CP and BP show the same DTG peak temperature. After the main decomposition stage the residue remains is 32.3% and after the final stage it is 6.5%. BP shows constant mass after ~500oC.

Figure 2: TG-DTA profile of BP

Figure 2: TG-DTA profile of BP

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The species, DB is stable up to ~220oC (Fig. 3). DB decomposes in three stages as indicated by the DTG peaks at 286, 409 and 452oC and the corresponding exothermic DTA peaks at 312, 413 and 455oC. The first and second DTA peaks are spaced by temperature difference of 101oC for DB indicating that the char residue obtained at the end set of the first stage of decomposition resists oxidative gasification. But for CP and BP it was nearly 90oC indicating that the residue formed is comparatively more susceptible to oxidation or decomposition to volatiles. The residue remained after the first and third stages are 33.3 and 4.3%, respectively. The sample of DB attains a constant mass after ~470 oC.

Figure 3:  TG-DTA profile of DB

Figure 3:  TG-DTA profile of DB

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The sample of DS exhibits no significant mass loss up to ~240oC except small mass loss of 3.2% below 110oC due to desorption of moisture (Fig. 4). The three stages of thermal decomposition are denoted by the DTG maxima at 323, 434 and 463 oC. The shoulder near ~300oC at left hand side of the first DTG peak corresponds to the hemicellulose decomposition which commences at ~200 oC. This region corresponds to broad endothermic region in the DTA curve. The spacing between the first and second DTG maxima is about 111oC indicating the thermal stability of the residue formed at the end set of the first stage. A high char yield of 39.7% is observed after the first stage. The second stage of decomposition is denoted by exothermic DTA peak at 434 oC. The final stage is indicated by a small exothermic DTA peak at 466oC.

Figure 4: TG-DTA profile of DS

Figure 4: TG-DTA profile of DS

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The sample of DH is stable up to ~220 oC with no significant mass loss (vide Fig. 5). The three decomposition stages are indicated by DTG peaks at 289, 414 and 456 oC and corresponding exothermic DTA maxima at 319, 418, and 459 oC. The major DTG peaks are separated by 125oC showing the stability of the residue formed after the first stage. The residue left after the first stage is 40.9%.

Figure 5: TG-DTA profile of DH

Figure 5: TG-DTA profile of DH

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Like DH, the bamboo species DG is also stable up to ~220 oC and decomposes thereafter (Fig. 6). Both DH and DG show constant mass after ~470oC. The sample of DM undergoes decomposition in two stages indicated by DTG peaks at 323 and 436oC, respectively (Fig. 7) with two sharp exothermic peaks at 333 and 446oC. After the first decomposition stage the DTA profile shows a shoulder and is due to the decomposition of cellulose. The lignin undergoes endothermic fragmentation, but it is masked by strong exothermic process of char formation and oxidative reactions. The sample of BN (Fig. 8) also shows similar phenomenological data as that of BB (Fig. 9). The samples DS, DM, BN and BB show a shoulder near 300oC and all the four samples shows the first DTG peak with maximum mass loss rate in the narrow range of 320-323oC. The shoulder is due to the decomposition of hemicellulose as mentioned earlier. All other samples of bamboo without unique shoulder in DTG profile show DTG peak temperature ≤ 296oC. The pyrolysis of biomass involves early decomposition of hemicellulose (commences ~200oC), followed by pyrolysis of lignin and depolymerization of cellulose. The nature and amount of compounds formed during the decomposition of hemicellulose affects the decomposition mechanism of cellulose and lignin and trigger a set of simultaneous and consecutive reactions which pushes the peak to a higher temperature.

Figure 7: TG-DTA profile of DM

Figure 6: TG-DTA profile of DG

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Figure 7: TG-DTA profile of DM

Figure 7: TG-DTA profile of DM

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Figure 8: TG-DTA profile of BN

Figure 8: TG-DTA profile of BN

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Figure 9: TG-DTA profile of BB

Figure 9: TG-DTA profile of BB

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Apart from all other samples of bamboo, BV shows two well defined stages of decomposition as shown in Fig. 10. The sample of BV is stable up to ~220 oC. The first stage of decomposition is denoted by a large DTG peak at 276 oC. This sample gives the lowest DTG peak temperature among the ten bamboo species studied. The DTA peak temperature is observed at 306oC. For the first stage, especially in the range from commencement of reaction to maximum rate of weight loss, oxidation is weakly exothermic, indicated by the difference between DTG peak (276 oC) and DTA maximum (306 oC). Towards the end of first stage, the reactions are found to be highly exothermic. After the first stage, the sample loses mass in a slow manner. The second stage is indicated by DTG peak at 441oC and the process is exothermic which is evident from sharp DTA peak at 443 oC. This result is in tune with the observations made by Bada10. Bada proved that the bamboo variety (Bambusa multiplex) with the highest volatile matter has the lowest ignition temperature.

Figure 10: TG-DTA profile of BV

Figure 10: TG-DTA profile of BV

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Kinetic Studies of Different Bamboo Species

Solid state thermal decomposition reactions are often quite complex. Keeping the particle size of sample very small for TG analysis ignores heat transfer and diffusion process. The purging of gas in analyzer dissipates the volatile components instantly. So thermal decomposition process is deemed to be an irreversible reaction and fits the first order parallel reaction model. Zehui Jiang and coworkers found that the Coats-Redfern method is useful in determining the kinetic parameters of Moso bamboo pyrolysis.11 The kinetic parameters of the thermal degradation reactions of the ten bamboo samples were calculated by the Coats-Redfern integral method for each TG curve obtained at 10 Kmin-1 in present investigation.12 The kinetic parameters including order parameter, correlation coefficient, activation energy, pre-exponential factor and entropy of activation were evaluated for all the thermal decomposition stages.13 These values are tabulated and presented in table 2.

Table 2:  Kinetic parameters for the thermal decomposition of ten bamboo species 

Sample

Stage

Integral method/

Mechanism

Activation Energy,

E

(kJ mol-1)

Pre-exponential
factor,

A (s-1)

Entropy of activation DS
(J K-1mol-1)

Corr.

Coeff.

r

Cephalostachyum pergracile

I

Coats-Redfern; n=1.8

192.1

7.5×1015

53.6

0.9983

Random nucleation

145.5

1.6×1011

35.9

0.9979

II

Coats-Redfern; n=1.7

322.6

2.3×1023

195.4

0.9999

Random nucleation

249.4

2.2×1017

80.2

0.9924

Bambusa pallida

I

Coats-Redfern; n=2.0

194.5

2.5×1016

64.0

0.9985

Random nucleation

138.0

6.0×1010

43.6

0.9871

II

Coats-Redfern; n=1.7

256.9

1.1×1018

-93.8

0.9993

Random nucleation

206.2

7.3×1013

13.8

0.9962

Dendrocalamus brandisii

I

Coats-Redfern; n=1.9

179.5

5.7×1014

32.4

0.9978

Random nucleation

128.9

4.6×109

65.1

0.9878

II

Coats-Redfern; n=1.6

282.6

4.9×1019

125.2

0.9994

Random nucleation

233.6

5.0×1015

48.8

0.9961

Dendrocalamus strictus

I

Coats-Redfern; n=1.0

153.0

3.0×1011

-30.4

0.9960

Random nucleation

150.0

3.1×1011

-12.4

0.9960

II

Coats-Redfern; n=1.0

311.8

1.5×1021

153.4

0.9978

Random nucleation

301.8

1.7×1021

113.1

0.9978

Dendrocalamus hamiltoni

I

Coats-Redfern; n=1.8

181.2

6.4×1014

33.3

0.9976

Random nucleation

137.2

2.7×1010

50.5

0.9889

II

Coats-Redfern; n=1.7

301.8

3.8×1021

161.4

0.9991

Random nucleation

245.3

8.7×1016

72.4

0.9972

Dendrocalamus gigantus

I

Coats-Redfern; n=1.6

172.9

1.2×1014

19.6

0.9989

Random nucleation

144.7

1.9×1011

34.2

0.9953

II

Coats-Redfern; n=1.5

241.9

1.0×1017

74.1

0.9989

Random nucleation

203.7

6.6×1013

12.8

0.9969

Dendrocalamus membranaceus

I

Coats-Redfern; n=1.4

176.3

5.7×1013

13.1

0.9968

Random nucleation

153.8

4.1×1011

27.9

0.9949

II

Coats-Redfern; n=1.6

295.1

1.0×1020

131.4

0.9965

Random nucleation

233.6

1.7×1015

39.7

0.9886

Bambusa nutans

I

Coats-Redfern; n=1.3

189.6

9.1×1014

35.7

0.9985

Random nucleation

169.6

9.9×1012

11.8

0.9974

II

Coats-Redfern; n=1.1

240.3

1.6×1016

57.9

0.9984

Random nucleation

232.8

3.4×1015

45.2

0.9983

Bambusa bambos

I

Coats-Redfern; n=1.4

175.4

5.7×1013

12.6

0.9972

 

Random nucleation

152.1

3.0×1011

30.9

0.9957

II

Coats-Redfern; n=1.3

261.8

7.6×1017

90.3

0.9983

Random nucleation

237.8

8.4×1015

52.9

0.9974

Bambusa vulgaris

I

Coats-Redfern; n=2.0

226.9

4.8×1019

126.8

0.9990

Random nucleation

155.5

3.4×1012

10.2

0.9907

II

Coats-Redfern; n=1.3

429.8

4.0×1029

314.5

0.9999

 

Random nucleation

386.6

2.0×1026

251.3

0.9996

It has been already reported that pyrolysis of cellulose is endothermic while that of wood and lignin is endothermic initially but later becomes exothermic. The endothermic peaks are masked by strong exotherms due to an oxidative atmosphere, maintained in the experiment. Thus, trying to represent the full complexity of the hydrocarbon degradation process makes no sense and we depend upon global pyrolysis kinetics applied to bamboo is used to predict the overall rate of volatiles release (i.e., mass loss) from the solid. For all the samples two decomposition stages are evaluated since, the third stage, if exists, involve a mass loss of less than or equal to 5%. Thus determining kinetic parameters of the third stage is insignificant and process is simply the oxidation of residual char. So the present study concentrates on the first and second decomposition stages of all bamboo samples. For all the twenty decomposition stages of ten bamboo species, the order parameter ranges from 1.0 -2.0. Generally, the first stage of decomposition has higher order parameter compared to the second stage. The highest order parameter (2.0) is found for the first decomposition stage of BP and BV and the lowest for DS (1.0). The correlation coefficient for the first stage and second stage is greater than or equal to 0.9960 and 0.9965 respectively. The kinetic parameters show much higher values for the second stage in comparison with the first stage of decomposition. The activation energy for the primary decomposition stage ranges from 153.0 to 226.9 kJ mol-1. The lowest and highest value for energy of activation is found for DS and BV respectively. It is interesting to note that the stability in terms of DTG peak temperature is highest for dendrocalamus strictus (DS), which possess the lowest values for kinetic parameters for the main decomposition stage. The order parameter for both decomposition stages are unity for DS. Entropy of activation for main stage of DS alone is negative and for all other samples it is positive. Positive values of entropy of activation indicates that the activated complexes are less ordered than the corresponding reactants. So, the mass loss reactions are faster than  in the normal course. For DS, activation energy for the second stage of decomposition (311.8 kJ mol-1) is about two times higher than that obtained for the first stage (153.0 kJ mol-1). This indicates that with comparatively higher energy of activation, DS undergo very fast decomposition with high volatile evolution towards the end of decomposition, once activated. Also, the higher the activation energy, the higher is the sensitivity of Arrhenius parameter to temperature.

The kinetic parameters for the main stage of thermal decomposition are found to be highest for the species, Bambusa vulgaris (BV). The activation energy for the major mass loss stage for the bamboo samples are much lower than the activation energy of pure cellulose (table 3.2). The activation energy for major mass loss stage of different bamboo species decreases in the order BV > BP > CP > BN > DH > DB > DM > BB > DG > DS. The average activation energy of bamboo samples for the first stage of decomposition, excluding BV and DS, are 183±11 kJ mol-1. BV and DS show large deviation. The order parameter for the second stage of decomposition ranges from 1.0 to 1.7. For the second stage, values of the kinetic parameters are found to be maximum for the species Bambusa vulgaris and the lowest values are obtained for Bambusa nutans. For the second stage of decomposition, entropy of activation is positive for all samples. The average activation energy for the second stage is ~ 294 kJ mol-1.

Mechanism of Decomposition

Mechanism based kinetic equations elucidated by Satava have been employed to determine the mechanism of the decomposition for ten bamboo varieties and FR treated DS samples.14 The best linear plots obtained for each of the decomposition stages is chosen as the one, corresponding to the correct mechanism of the reaction for a particular decomposition stage. From the values of slope and intercept of the linear plots, the kinetic parameters were calculated and tabulated in table 2. It is found that the decomposition reactions of all these systems go along with the Mampel equation involving random nucleation with single nucleus on each particle.14 The kinetic parameters evaluated using these equations are mostly comparable with those utilizing the Coats-Redfern equation. Best fit model for the kinetics of bamboo pyrolysis is still in question as the process of degradation involve catalysis by metal compounds present in the bamboo matrix and the various secondary reactions owing to different physical and chemical characteristics of components such as cellulose, xylan and lignin.15

Conclusion

The thermal stability of ten varieties of bamboo of approximately same age and cultivated in the same land terrain were compared using simultaneous TG-DTA analysis. The thermochemical conversion reactions are found to be very useful techniques for biomass upgrading. The pyrolysis of lignocellulosic materials primarily involve a polymeric structure breakdown, converting the components into volatiles and char. Based on the thermal stability of species it can be best utilized for commercial purpose.

Thermal stability in terms of first stage of degradation is lowest for BV and higher stability is attributed to DS and DM. The onset temperature for active lignocellulosic pyrolysis for the first mass loss stage is between 220 oC – 240 oC.  DM, BN and BV complete the decomposition process in two distinct stages and all others in three stages. The first stage, dominant below 340˚C, decomposes polymers forming active carbonaceous char which release volatile gases upon increase in temperature leaving approximately 5% by weight of above 450 ˚C.

The kinetic parameters were calculated for the mass loss stages during slow decomposition of ten species of bamboo by the Coats-Redfern integral method. The kinetic parameters viz., energy of activation, pre-exponential factor and entropy of activation for the main stage of pyrolysis are found to be highest for BV.  The activation energy for major mass loss stage of different bamboo species decreases in the order BV > BP > CP > BN > DH > DB > DM > BB > DG > DS.

The first stage of decomposition has higher order parameter compared to the second stage. For all the twenty decomposition stages of ten bamboo species, the order parameter ranges from 1.0-2.0. The highest order parameter is found for the first decomposition stage of BP and BV and the lowest for DS.  Entropy of activation for main stage of DS alone is negative and for all others it is positive. For the second stage of pyrolysis, entropy of activation is positive for all samples. This indicates that the activated complexes are less ordered than the reactants, and evidently the decomposition reactions are presumed faster.

The decomposition reactions of all these samples obeys the Mampel equation indicating the mechanism of random nucleation with one nucleus on each particle.  The kinetic parameters calculated using the equations on the above-proposed mechanism for the samples are mostly comparable with those calculated using the Coats-Redferm equation.

Global pyrolysis kinetics applied to bamboo can be extended for predicting the overall volatile release rate from the solid and consequently the thermal stability and also shower light upon the mechanistic steps in the thermal degradation process.

Acknowledgement

The author gratefully acknowledge with thanks JNTBGRI, Thiruvananthapuram, India for providing the bamboo samples voluntarily and Department of chemistry, University of Kerala for granting access to thermogravimetric facility.

Declaration of Conflict of Interest

The author declare no conflict of interest.

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