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Environmental and Carbon Dioxide Issues
Pyrolysis Characteristics and Kinetics of Typical Municipal Solid Waste Components and Their Mixture: An Analytical TG-FTIR Study Yingyun Qiao, Fanfan Xu, Shili Xu, Dan Yang, Bo Wang, Xue Ming, Junhui Hao, and Yuanyu Tian Energy Fuels, Just Accepted Manuscript • DOI: 10.1021/acs.energyfuels.8b02571 • Publication Date (Web): 25 Sep 2018 Downloaded from http://pubs.acs.org on September 29, 2018
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Energy & Fuels
Pyrolysis Characteristics and Kinetics of Typical Municipal Solid Waste Components and Their Mixture: An Analytical TG-FTIR Study
Yingyun Qiao a, Fanfan Xu a, Shili Xu b, Dan Yang c, Bo Wang a, Xue Ming a, Junhui Hao a, Yuanyu Tian a, d, * a
State Key Laboratory of Heavy Oil Processing, China University of Petroleum (East
China), Qingdao 266580, RP China b
Shandong Hengyuan Petrochemical Co., Ltd., Linyi 251500, RP China
c
College of Science, China University of Petroleum (East China), Qingdao 266580,
RP China d
Key Laboratory of Low Carbon Energy and Chemical Engineering of Shandong
Province, Shandong University of Science and Technology, Qingdao 266580, RP China
* Corresponding Author. E-mail:
[email protected] (Y Tian) Address: State Key Laboratory of Heavy Oil Processing, China University of Petroleum (East China), Qingdao 266580, RP China
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Abstract: Recently, the renewed interest in the pyrolysis of municipal solid waste has
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been aroused. In this investigation, the pyrolysis behaviors and kinetics of typical
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municipal solid waste components and their mixture at high heating rates are studied
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by using Thermogravimetry-Fourier Transform Infrared spectrometer (TG-FTIR). The
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TG/DTG results presented the different pyrolysis behaviors of each components and
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their mixture. The main volatiles were generated from 250 °C to500 °C obtained by
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FTIR results. Moreover, the consistency between volatiles release and pyrolysis
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behavior was found through FTIR and TG. By comparing the experimental and
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calculated TG/DTG curves and volatiles released curves of mixed MSW, the
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interactions between individual components has been found, which performed as the
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interactions could accelerate the first pyrolysis reaction stage and postpone the second
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and third pyrolysis reaction stage. Based on the distributed activation energy model,
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the values of activation energy of individual components and their mixture were
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distributed between 123.73 kJ·mol-1 to 312.56 kJ·mol-1. Meanwhile, the frequency
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factor of them increased along with the activation energy. Overall, those findings can
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enrich a better comprehension of the MSW pyrolysis process.
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Keywords: Municipal solid waste; pyrolysis behavior; volatiles released; TG-FTIR;
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kinetic analysis
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1. Introduction In recently years, the alternate energy sources such as biomass and municipal
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solid waste (MSW) have been widely investigated due to the increasing depletion of
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fossil fuels. MSW mainly refers to the solid wastes produced in the daily life or in
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activities that provided services for daily life, which typically made up of polymer
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wastes, biomass wastes, kitchen wastes and other inorganic materials 1. With the
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growth of economy and expansion of urbanization, the amount of MSW has increased
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year by year. The World Bank estimated that by 2025, China’s solid waste generation
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will double to more than 500 million tons annually 2. Generally, MSW has a great
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potentiality in producing syngas, tar and char that are known as bioenergy since its
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heating value can be achieved 20.57 MJ·kg-1 3. Therefore, it can be used as the source
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of heat for power generation in waste incineration power plants. Alternatively, MSW
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can also be converted to petrochemical products or high value-added chemicals by
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thermochemical treatment.
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Incineration is the main traditional thermochemical treatment for MSW in the
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past two decades because of the mature technology. However, for some reasons such
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as the dioxins (PCDD/Fs) emission and the fly ash as by-products, the incineration
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has caused opposition by public 4. Several environment-friendly treatments for MSW
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have been received extensive attention from researchers and governments all over the
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world, where pyrolysis is the most effective and clean method to retrieve energy and
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produce chemicals from wastes. According to the definition, pyrolysis is a thermal
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conversion process which is commonly carried out in the inert atmosphere (absence of
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oxygen) 5. The advantages of pyrolysis are lower pollutant emissions, higher
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recycling rates and higher economic benefits when compared to incineration. In
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addition, there is almost no waste generated during pyrolysis process because that all
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components can convert into gases, liquid (bio-oil, tar) and solid (char). However, it is
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worth noting that the pyrolysis process is affected by various factors including
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material properties, experimental conditions and apparatuses. Hence, it is important to
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be aware of the thermal decomposition behaviors of all individual components and
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their mixture to further understand the MSW pyrolysis process. Several attempts have
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been made to study the pyrolysis behavior of MSW or typical MSW components at
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laboratory-scale 6-9. The common reactors or apparatuses used in laboratory-scale
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experiments are fluidized bed, fixed bed and thermogravimetric analyzer (TGA).
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However, the main purpose of the fluidized bed or fixed bed experiments is to obtain
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the products yield of gases, oil and char. That information provided is not sufficient
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for in-depth understanding and further study of MSW pyrolysis. Moreover, the critical
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information gained from TGA analysis is also limited, which could only explain the
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pyrolysis behavior such as weight loss and pyrolysis temperature interval 10. The
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volatile products of the MSW or typical components pyrolysis process is essential to
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investigate the pyrolysis characteristics. Recently, the hyphenated TGA techniques
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which can extract further information from thermal degradation process have attracted
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widespread interest. The Thermogravimetry coupled with Fourier Transform Infrared
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spectrometer (TG-FTIR) has been widely used in analyzing the solid wastes pyrolysis
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process due to its unique advantages 11. The composition of the volatile products
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(small molecular gases and typical functional groups of large gaseous products)
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released can be detected while the thermal weight loss behavior are also recorded at
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the same time. Thus, the pyrolysis characteristics and major volatile species can be
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acquired and the weight loss change can also be associated with the emission of
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specific volatiles. In this sense, the pyrolysis study of MSW or individual components
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can be conducted on TG-FTIR.
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Kinetic study is another important aspect of MSW pyrolysis process because the
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kinetic parameters can provide guidance for design and optimization of reactors 12.
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Since the multiple integral or differential formulas, there are various methods to
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calculate the kinetic parameters, which including model-fitting methods, model-free
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methods and distributed activation energy model (DAEM) method. Several kinetics
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studies on the pyrolysis of MSW or individual components have been investigated,
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but the parameters obtained are not quite consistent 13-16. Generally, model-fitting
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methods are more complicated than model-free methods since the kinetic parameters
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obtained with an assumption of reaction mechanism function. However, the activation
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energy is the only kinetic parameter that can be gained by using the model-free
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methods. The DAEM method is another poplar kinetic method in the calculation of
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kinetic parameters for coal, biomass and solid waste because its capability to describe
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the complicated pyrolysis process 11. It is well know that the DAEM method assumes
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that there are multiple independent parallel reactions occurred simultaneously in the
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pyrolysis process, while the kinetic parameters are not the same. Furthermore, all
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parallel reactions are regarded as irreversible first-order reaction in this method. This
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assumption is reasonable here because of the diversity and complexity of MSW or
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individual components. Therefore, DAEM method has been chosen to calculate and
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evaluate the kinetic of MSW or individual components during pyrolysis process. The principal objective of this work is to study the pyrolysis behaviors and
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kinetics of typical MSW components (plastics, rubber, textile, paper, poplar wood and
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kitchen wastes) and mixed MSW at high heating rates by means of TG-FTIR. Firstly,
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pyrolysis characteristics of individual components and mixed MSW were analyzed by
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TG analysis. Then, the composition and releasing characteristics of gas-phase
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products and functional groups were identified through infrared spectrum. By
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comparing the experimental and calculated values of mixed MSW, the interactions
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between the individual components were explored. Finally, the kinetic parameters and
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compensation effect were obtained by using DEAM method, which should be
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instructive for the design and optimization of MSW pyrolysis reactors.
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2. Materials and methods
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2.1. Materials
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Plastics (PE, PP and PVC), rubber, textile, paper, poplar wood and kitchen wastes
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(pork and rice) were chosen in this study. The plastics were purchased from Sinopec,
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China. The rubber was obtained from waste bicycle tires, the paper and textile were
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bought from market. In addition, the poplar wood was gathered from poplar trees in
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campus and the kitchen wastes were gained from canteen. The MSW sample were
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mixed by the ratio (plastics: rubber: textile: paper: poplar wood: kitchen wastes= 2: 1:
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1: 1: 1: 4) according to related literature 17. Some pre-treatments needed to be
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completed before the experiment starts. First, all samples were milled and sieved by
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grinder and sieve, which the particle size is less than 150 µm to prevent heat transfer
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effect in dynamic pyrolysis. Then, the samples were placed in oven with the
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temperature of 110 ℃ for 24h to eliminate the effects of moisture.
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2.2. Experiments
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The pyrolysis experiments of individual components and mixed MSW were
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carried out on the thermogravimetric analyzer (STA449 F3, NETZSCH, Germany)
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with a high-speed heating furnace, of which the heating rate is from 0 ℃·min-1
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to1000 ℃·min-1 and the maximum temperature is 1250 ℃. All samples were heated
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from 30 to 1000 ℃ under nitrogen (99.999% N2) atmosphere with 120 ml·min-1 (100
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ml·min-1 carrier gas and 20 ml·min-1 protective gas) at different heating rates of 50,
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100, 300, 500 and 700 ℃·min-1, respectively. In order to reduce heat transfer
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limitation, all samples were taken in platinum crucible for about 5 mg in this study.
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The release of volatiles during the entire pyrolysis process was detected by
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Fourier Transform Infrared spectrometer (TENSOR II, Bruker Optics, Germany). The
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output products from TGA were collected by FTIR through capillary bundle in
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transfer line with a constant temperature of 200 ℃ to prevent the volatiles
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condensation. In addition, FTIR analysis was conducted by the resolution of 4 cm-1
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with the spectrum at the range of 4000-440 cm-1. In order to eliminate the effect the
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background signal, it is necessary to measure the blank experiments before loading
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samples. However, the symmetrical molecules (N2, H2 and Cl2) and compounds with
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similar functional groups cannot be accurately identified by FTIR.
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2.3. Kinetic model (DAEM)
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The distributed activation energy model (DAEM) has been widely used in
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analyzing the activation energy and frequency factor of complicated reactions
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occurred in the entire pyrolysis process of fossil fuels 18, and later successfully applies
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to various raw materials such as coal, biomass and solid wastes 19. This model
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assumes that the pyrolysis of solid wastes include number of parallel first order
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irreversible reactions, which is written as follow:
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1 − / ∗ = (− ⁄ )() (1)
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Where V represents the volatile matter at time t and V* represents the effective
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volatile matter, T is the pyrolysis temperature as a function of time t. E and A are the
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activation energy and frequency factor, respectively.. Moreover, f(E) is the function of
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activation energy distribution curve and it satisfies the normalized condition as
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follow:
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( ) = 1
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(2)
The calculation of pyrolysis temperature T at any time t with the heating rate β is
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written as:
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= + t
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(3)
The Eq. (1) is simplified by an estimated method for f(E) and A provided by
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Miura and Maki 20, which is shown as:
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( ⁄ ! ) = ln( $⁄ ) + 0.6075 − ⁄$
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(4)
Thus, the kinetic parameters (E and A) can be obtained by plotting ln(β/T2) as a
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function of 1000/T with the specified values of V/V* under different heating rate
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conditions, of which the slope and intercept represent the value of E and A,
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respectively.
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3. Results and discussion
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3.1. Physicochemical parameters of materials
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The proximate and ultimate analysis of six kinds of components and mixed MSW
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are presented in Table 1. The proximate analysis was conducted based on the Chinese
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National Standards of GB/T 212-2008 and the ultimate analysis was done by using an
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elemental analyzer (Vario EL cube, Elementar, Germany). Moreover, the higher
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heating value (HHV=33.5C+142.3H-15.4O-14.5N) 21 and lower heating value
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(LHV=81C+342.5H-O/8+22.5S-6(9H+W)) 22 of components and their mixture are
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also given in Table 1.
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The rubber has the highest ash content and fixed carbon content among all
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components, while the plastics (PE, PP and PVC) have the highest volatile matter
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content. In addition, the ash content is relatively low of all components and mixed
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MSW when compared to other fractions of proximate analysis. It is well accepted that
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low ash content and high volatile matter content are suitable for pyrolysis due to the
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potential available energy is high 23. The carbon element content of PE and PP is more
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than 80%, other components are nearby 40% except rubber. Meanwhile, PE and PP
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has the highest hydrogen element content, while others are less than 9%. The nitrogen
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and sulfur content of all components are quite low except pork, which has the highest
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nitrogen element reach to 9.90%. It is worth mentioning that the chlorine content of
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PVC cannot be discovered due to the limitation of apparatus. The value of oxygen
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content of PVC in Table 1 contains a large amount of chlorine. Since the bond energy
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of C−O and C-H is lower than C-C, higher ratios of oxygen and hydrogen content
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compared with carbon in ultimate analysis could reduce the potential energy value 24.
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The definition of heating value is the energy or heat released by a unit of volume or
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mass of fuel when it is completely burned. The difference of higher heating value
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(HHV) and lower heating value (LHV) is whether to consider the latent heat of
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vaporization. As shown in Table 1, the HHV and LHV of all samples varies from 15
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to 50 MJ·kg-1. The heating values of PE, PP, rubber and mixed MSW are very high
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(more than 20 MJ·kg-1), while other components are distributed within the scope of
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15-20 MJ·kg-1. The heating value requirement for MSW incineration or pyrolysis is
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no less than 6500 KJ·kg-1 17, so all samples in this study meet the requirements of
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application.
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3.2. Pyrolysis analysis
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3.2.1. Pyrolysis analysis of individual components
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The TG and DTG curves obtained from TGA experiments of nine individual
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components at different heating rates (50, 100, 300, 500 and 700 ℃·min-1) are given
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in Fig. 1 and 2, respectively. Table S1 (Supporting Information) lists the pyrolysis
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characteristic parameters of individual components under different heating rate
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conditions.. The pyrolysis behavior of PE and PP are similar because of their similar
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chemical structure, of which are saturated straight-chain polymer. These was only one
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major pyrolysis reaction stage can be observed during the pyrolysis process of PE and
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PP from the TG/DTG curves. The pyrolysis interval of them was about 200 ℃, which
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is relatively narrow compared to other components. Another plastic component PVC
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had a distinct difference of pyrolysis characteristics because it was manufactured from
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the mixture of about 57% chlorine. There were two main reaction stages occurred in
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the pyrolysis process of PVC, which were the dehydrochlorination process in
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227-306 ℃ and the degradation process of remaining hydrocarbons in 399-683 ℃ 25. It
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can be observed that a significant peak at 204-660 ℃ and a weak peak at 665-998 ℃
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appeared in DTG curves of rubber component. According to the previous
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investigation 26, the primary pyrolysis of rubber was the main stage of the entire
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process, of which were the decomposition of plasticizer, natural rubber and synthetic
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rubber. The second stage was the secondary cracking reactions of products under high
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temperature condition. The pyrolysis process of textile showed that there was only
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one pyrolysis reaction that took place from 261 ℃ to 641 ℃. The main reaction of
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entire pyrolysis process was the decomposition of cellulose fibers and then the
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dewater and decarboxylation process occurred at about 450 ℃ 27. It is obviously that
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the pyrolysis of paper was two stage processes obtained from TG/DTG. The main
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weight loss occurred at 269-557 ℃ was the thermal decomposition reactions of plant
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fibers, which including cellulose, hemicellulose and lignin. The second stage from
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694 ℃ to 899 ℃ was the decomposition of the calcite and other additives which added
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in the papermaking process 28. There were two peaks can be found in DTG curves that
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the main pyrolysis reactions proceed from 230 ℃ to 669 ℃ for poplar wood, which is
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shown to be the decomposition of hemicellulose and cellulose, while the lignin
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thermal decomposition interval was wide without significant characteristic peaks. The
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pyrolysis of pork had only one reaction stage occurred at 190-647 ℃. At the initial of
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pyrolysis, low molecular weight compounds evaporated. With the temperature
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increased, the main degradation reactions occurred at about 360 ℃, which was the
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thermal decomposition of organic intermediates 29. It was only one main DTG peak
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can be found during the pyrolysis process of rice. The main reactions occurred at
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258-618 ℃ was the decomposition of starch and a small amount of protein.
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It is significant that there was a lateral offset in TG/DTG curves of Fig. 1 and
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2when the heating rates increased. The reason for this displacement can be attributed
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to the thermal lag, which is shown as a large difference between the temperatures of
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furnace samples under high heating rate conditions. Moreover, the heat transfer
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limitations was another factor for the lateral offset. With the increasing of heating
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rates, the reaction time became short, which directly lead to the difficult in the heat
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transfer from the boundary layer to the reacting surface 30. There also had a
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phenomenon that the residues after pyrolysis decreased with the heating rates
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increased except plastics and rubber component. High heating rates can result in rapid
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fragmentation of biomass and enhance the yield of volatiles. It can be explained that
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the increase of heating rates would shorten the pyrolysis reaction time, thus
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minimized the time available for secondary reactions such as tar cracking or
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repolymerization 31. Therefore, the weight loss of biomass pyrolysis process was
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higher under high heating rate conditions. Plastics and rubber basically have no tar
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generated under high temperature pyrolysis, so the weight loss is not affected by the
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heating rates.
244 245
3.2.2. Pyrolysis analysis of mixed MSW
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In this study, biomass and polymers are two main categories based on the
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complex composition of MSW. Paper, poplar wood and kitchen wastes belong to
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biomass, of which the main ingredients can be divided into cellulose, hemicellulose,
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lignin, starch and protein. Plastics, rubber and fibers are polymers, which consist of
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macromolecular compounds contained a high amount of hydrocarbons 16. Fig.3 shows
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the experimental and calculated TG/DTG curves for the mixed MSW pyrolysis
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process under different heating rates, of which the calculated curves was obtained
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from the linear combination of individual components. Table S2 in Supporting
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Information lists the comparison of experimental and calculated values for mixed
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MSW pyrolysis characteristic parameters. Two obvious peaks and one inconspicuous
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peak were presented in DTG curves at all heating rates, so it can be inferred that the
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pyrolysis process of mixed MSW could be distinguished into three reaction stages.
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From Fig. 3, the first stage occurred at about 240-390 ℃ was the main stage due to the
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absolute value of DTG is much high than that of other two stages. The thermal
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decomposition of biomass ingredients and textile was the main pyrolysis reaction in
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this stage. According to related literatures 32-34, the pyrolysis temperature interval for
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hemicellulose was 225-350 °C, cellulose was 325-375 °C, lignin was 250-600 °C,
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starch was 269-345 °C and protein was 220-500 °C respectively. At the initial of the
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first pyrolysis reaction stage, the hemicellulose first began to decompose because of
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the low polymerization degree. Meanwhile, the first pyrolysis reaction of protein also
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occurred in this stage. With the temperature increased, several primary polymerization
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reactions of cellulose and starch began. The peaks of DTG curves reached a
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maximum temperature values under different heating rates, then the decomposition of
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starch and cellulose became more intensified. In addition, the primary decomposition
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of rubber and dechlorination of PVC also happened. The second reaction stage was
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not prominent in TG/DTG curves owing to the components pyrolysis in this stage was
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not abundant. Lignin began to decompose in this stage due to the decomposition rate
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of lignin is relatively slow than that of cellulose and hemicellulose. At the same time,
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the second pyrolysis reaction stage of protein also took place. At the final of this stage,
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the initial chain scission reactions of plastics started. In the third pyrolysis reaction
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stage within the pyrolysis interval of 440-608 °C, the thermal decomposition of PE
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and PP was the major reactions. The thermal cracking or decomposition of the
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dehydrochlorinated PVC also occurred in this stage. However, there had slight
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fluctuations in TG/DTG curves when the pyrolysis temperature above 750 °C, this
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phenomenon resulted from the thermal decomposition of inorganic minerals
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contained in paper and rubber.
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There are obvious deviations between the experimental and calculated results of
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TG/DTG curves at different heating rates can be observed in Fig. 3. The peaks of
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experimental DTG curves in the first stage were observed to offset to the low
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temperature compared to calculated curves. And the corresponding DTG peak values
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of experimental were low than that of linear calculation. It meant that the individual
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components interacted during the pyrolysis process of mixed MSW in this stage, and
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this interaction had a positive effect on the reaction. Yang et al.35 conducted an
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in-depth investigation of hemicellulose, cellulose, and lignin in biomass, which had
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demonstrated that they have no apparent interaction during pyrolysis. Thus, the
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acceleration effect can be attributed to the generation of HCl during the
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dehydrochlorination process of PVC 36. The hydrogen chloride (HCl) could affect the
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decomposition of hemicellulose, cellulose and lignin through catalytic effect as a
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Lewis acid. It can not only make the reaction proceed at lower temperatures, but also
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enhance the reaction intensity. Analogously, the difference between the experimental
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and calculated results at the second reaction stage was similar to that of first stage.
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This phenomenon can also be explained by the dehydrochlorination of PVC, which
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can promote the reaction under the catalytic effect of HCl. However, as the pyrolysis
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temperature increased, the dehydrochlorination process ended and the reaction leveled
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off. The peaks of the third stage in experimental curves moved to the right
301
significantly compared to that of the calculated curves in Fig. 3. The main reactions
302
were the thermal degradation of plastics (PE, PP and PVC) in this stage according to
303
the pyrolysis characteristic parameters. Wu et al. 37 stated that the pyrolysis process of
304
PE/PVC blends were postponed than that of single component. Meanwhile, the same
305
retardation of PP in PVC/PP blends was found by Miranda et al. 38. Therefore, the
306
peak temperature of DTG curves would be delayed during the co-pyrolysis process of
307
mixed plastics. Similar to the individual components, the TG/DTG curves moved
308
toward higher temperatures zone along with the heating rates due to thermal lag and
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heat transfer limitations. The higher the heating rate is, the less obvious the second
310
pyrolysis stage will be. It is attributed to that the high heating rates would lead to the
311
decrease of reaction time, so the reaction of each component were not obvious or even
312
simultaneous.
313 314
3.3. FTIR analysis
315
3.3.1. FTIR analysis of individual components
316
TG-FTIR is commonly used to detect the gaseous products and typical functional
317
groups in volatiles from the pyrolysis process in real time. It can provide a judgment
318
to determine the species of pyrolysis products and deepen the understanding of
319
pyrolysis behaviors. A summary for infrared bands of gaseous products and typical
320
functional groups investigated in this study are presented in Table 2. Fig. 4 shows the
321
intensity via temperature profiles of the evolution of products during pyrolysis
322
process of individual components at 100 ℃·min-1. The absorption spectrum at a
323
particular wavenumber are linear depending on the concentration of volatiles
324
according to Lambert-Beer law, so the variation of absorbance intensity could reflect
325
the evolutionary tendency of gaseous products and typical functional groups.
326
As shown in Fig. 4 (a), there were several peaks of CO2 absorbance can be
327
observed in all individual components profiles. The main reactions for the formation
328
of CO2 occurred at around 250-450 °C, which were resulted from the destruction and
329
reforming of −C=O, −COOH and R−O−R 39. When the temperature reached 700 °C,
330
there had several significant peaks of paper and rubber. It can be owing to the
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decomposition of inorganic minerals (mainly CaCO3) or secondary cracking reactions
332
under high temperature conditions. Carbon dioxide is considered as one major
333
products during the biomass pyrolysis process, but there almost no release during
334
plastics pyrolysis. In addition, the generation of CO had a similar tendency with CO2
335
from 250 °C to 500 °C, but the intensity of individual components was quite different.
336
Since the secondary thermochemical decomposition of carbonyls and other volatiles,
337
there was only one obvious CO absorbance peak 40. The intensity of CO release of
338
paper, textile and poplar wood were slightly higher than other components. Fig. 4 (c)
339
depicts the intensity of CH4 release and two absorbance peaks at different temperature
340
range can be found. The first absorbance peak of CH4 release occurred at 300-500 °C.
341
This was caused by the decomposition of paper, textile, food wastes, poplar wood,
342
rubber and the first stage of PVC, of which the C-R bonds cracking and
343
recombination. Moreover, the demethylation of the methoxy groups (−O−CH3) can
344
also result in the formation of CH4 when the pyrolysis temperature above 400 °C. The
345
second absorbance peak main caused by the thermal cracking of PE and PP. The C−H
346
and C−R bonds generated from the depolymerization of PE, PP and PVC were broken
347
to form free radicals, which can undergo further recombination to form low molecular
348
gas such as methane 41. PE and PP had a much stronger intensity of CH4 release than
349
other components because of the high carbon and hydrogen content. As shown in Fig.
350
4 (d), one obvious absorbance peak of O−H was observed and it occurred in the range
351
of 260-500 °C. The O−H stretching vibration at the wavenumber of 3387 cm-1 related
352
to H2O, which was mostly generated by the cracking reaction of oxygen-containing or
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353
hydroxyl-containing functional groups 42. Fig. 4 (e) and (f) shows the absorbance
354
curves of C=O (mainly in aldehydes, ketones, esters) and C−O (mainly in alcohols,
355
ethers, phenols), and the similar trends occurred from 250 °C to 460 °C can be found.
356
Those two functional groups mainly appeared in the pyrolysis process of
357
hemicellulose and cellulose 43. Meanwhile, the release intensity of C=O and C−O of
358
individual components were slightly similar. The intensity of poplar wood was the
359
highest, whereas plastics and rubber almost no release. Overall, the evolution of
360
volatiles release were similar among biomass but quiet different between biomass and
361
plastics. Furthermore, the evolution of gaseous products and functional groups had
362
good consistency with pyrolysis characteristics of individual components, the main
363
functional groups generated from 250°C to 500 °C corresponded to all samples
364
pyrolysis between 200-600 °C.
365 366 367
3.3.2. FTIR analysis of mixed MSW The gaseous products and typical functional groups of volatiles in the mixed
368
MSW pyrolysis process at 100 ℃·min-1 are also detected by FTIR. Fig.5 gives the
369
comparison of products release with temperature of mixed MSW by experimental and
370
calculated data. It was not hard to find that the temperature of products release
371
corresponded to the temperature mentioned in mixed MSW pyrolysis process. As
372
shown in Fig. 5 (a), there were one main absorbance peak appeared before 400 ℃ and
373
two small absorbance peaks appeared after 400 ℃ of CO2 release, which can be
374
observed both in experimental and calculated profiles. The CO2 generated from mixed
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MSW pyrolysis was more than superposition result and the released temperature was
376
shifted to earlier. The main peak of CO absorbance occurred at about 300 ℃ from
377
experimental data, of which the calculated occurred at around 370 ℃ in Fig. 5(b),
378
which was contributed to the acceleration effect by interactions However, a small
379
obvious absorbance peak appeared at 505 ℃ was only found in experimental profile.
380
This phenomenon can be explained as the interaction between the various components
381
resulted in the pyrolysis reaction for CO generation in this stage. As presented in Fig.
382
5 (c)-(f), the evolution of other products release had a good consistency between
383
experimental and calculated profiles. However, the product concentration and release
384
temperature were slightly different. For CH4, the initial release temperature of first
385
pyrolysis stage was advanced and the third stage pyrolysis temperature was postponed
386
during mixed MSW pyrolysis when compared to calculated results. In addition, the
387
intensity of CH4 release was low than calculated result at the third stage of entire
388
pyrolysis process, which was caused by the interactions among plastics. Compared
389
with the calculated results, the initial release temperature of O−H,
390
was advanced from experimental results. The O−H and C=O concentration of
391
experimental results was slightly high than calculated results, while the C−O
392
concentration is low when compared to calculated result. Therefore, it can be inferred
393
that the interactions between the individual components were able to strengthen the
394
release of CO2, CH4, O−H and C=O, and they can inhibit the generation of CO and
395
C−O at the same time.
396
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397 398
3.4 Kinetic analysis Distributed activation energy model (DAEM) method has been widely applied in
399
calculating the kinetic parameters (activation energy Ea and frequency factor A) of the
400
pyrolysis process for solid wastes. Meanwhile, the iso-conversional method is one of
401
the most reliable way in accurate calculation of kinetic parameters 44, 45. In this study,
402
the conversion range 0.05-0.95 with the step size of 0.05 at different heating rates has
403
been chosen to investigate the kinetic.. Fig. 6 (a) displays the linear fit by plotting
404
ln(β/T2) vs 1/T for mixed MSW, Fig. 6 (b) shows the activation energy for all
405
components at different conversions and Fig 6 (c) and (d) exhibits the kinetic
406
compensation effect for rice and mixed MSW, respectively. In addition, the
407
compensation effect of other components are given in Fig. S1 (Supporting
408
Information). The kinetic parameters and compensation effect of different
409
components are listed in Table 3.
410
From Fig. 6 (a), all data points in the same conversion showed good correlation
411
with the fitting line except 0.05, 0.90 and 0.95. Obviously, the slopes and intercepts at
412
different conversions were not quite the same, which meant that the values of Ea and
413
A were mutative during the entire pyrolysis process. It might be attributed to the
414
complexity and diversity of MSW composition and the interaction between
415
components in the pyrolysis process. The same phenomenon also existed in individual
416
components, it can be explained that there were more than one single reaction
417
mechanisms during pyrolysis. And the competitive relations of those mechanisms
418
resulted in the decrease or increase of activation energy 46. As shown in Fig. 6 (b), the
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values of activation energy of most components was abnormal at low (V/V* < 0.1)
420
and high (V/V* > 0.9) conversion conditions. This was because that the minor errors
421
occurred in the baseline determination can greatly affect these parameters by using
422
iso-conversion model 47. All activation energy in the conversion range of 0.2~0.8 was
423
concentrated between the values of 100~300 kJ·mol-1 except PE, PP and part of pork.
424
Moreover, the frequency factor increased along with the activation energy. The mean
425
of activation energy (Ea), frequency factor (A) and correlation coefficient (R2) are
426
listed in Table 3. Due to the PVC, rubber, paper and mixed MSW had more than one
427
weight loss stage, it was classified into different stages to obtain the kinetic
428
parameters for a clearer understanding. The average activation energy of pork, PP and
429
PE were relatively high, which was shown as 321.63 kJ·mol-1, 312.56 kJ·mol-1 and
430
296.80 kJ·mol-1, respectively. The average activation energy of first reaction stage of
431
PVC and third reaction stage of Mixed MSW were the lowest with the values of
432
123.73 kJ·mol-1 and 146.72 kJ·mol-1. The values of average activation energy of other
433
components were around 200 kJ·mol-1. However, the correlation coefficient of kinetic
434
parameters for plastics and mixed MSW was low, while that of other components
435
were more than 0.97. The main reason for the low value of correlation coefficient was
436
the inevitable errors under low and high conversion in calculation process. Moreover,
437
the heating rate range (50-700 ℃·min-1) in this study was broad and the conversion
438
range (from 0.05 to 0.95 with 0.05 step size) for calculation was also wide. To obtain
439
more reliable kinetic parameters, the confidence interval (µ=0.99) is summarized in
440
Table 4. And the calculation formulas of the confidence interval index in Excel are
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441
listed in Table S3 (Supporting Information). The confidence interval is the estimated
442
interval of the population parameters constructed from the original data. Since the
443
lack of rigor, the confidence intervals can enhance the credibility of results in error
444
analysis of kinetic study 48. The 99% confidence intervals of Ea and A are selected in
445
this study are to provide the reference for related investigations.
446
Fig. 6 (c) and (d) shows the relationship between Ea and A for rice and mixed
447
MSW. Although the frequency factor A varied widely with the activation energy Ea,
448
they all demonstrated a strong linear relationship between the values of ln A and Ea,
449
which is known as “compensation effect” 49, 50. In many cases, the variation of these
450
parameters corresponds to the equation as ln A = a + bEa, of which a and b are
451
constants. Rice had only one main pyrolysis stage, so the compensation effect was
452
only one linear line. However, the compensation effect of mixed MSW seemed
453
slightly complicated and must be analyzed by the corresponding stages. This was also
454
suitable for other multi-stage reaction components such as PVC, rubber and paper
455
shown in Fig. S1. The equations obtained from compensation effect and their
456
correlation coefficient were summarized in the right column of Table 3. The existence
457
of kinetic compensation effect was confirmed by the high correlation coefficient
458
values.
459 460 461 462
4. Conclusion In this investigation, the TG/DTG curves of typical MSW components and mixed MSW at high heating rates were presented. Biomass components exhibited similar
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pyrolytic properties, which including the thermal decomposition of cellulose,
464
hemicellulose and lignin. Plastic components had the same pyrolysis tendency except
465
PVC. The pyrolysis process of mixed MSW had three different stages, of which the
466
first pyrolysis stage was the main stage. The interactions between different
467
components could promote the first pyrolysis stage, whereas the second and third
468
pyrolysis stage were suppressed. From FTIR analysis, the main volatiles generated at
469
the temperature interval of 250-500 °C. CO2 was the major gaseous product released
470
from the pyrolysis process except plastics, while CH4 released of plastics was higher
471
than other components. Moreover, the contradistinctive FTIR results suggested that
472
the interactions between the individual components can strengthen the release of CO2,
473
CH4, O−H and C=O and inhibit the release of CO and C−O. Through the calculation
474
of kinetic parameters and compensation effects, the DAEM was successfully
475
validated with experimental data. The activation energy values of individual
476
components and their mixture were distributed between 123.73 kJ·mol-1 to 312.56
477
kJ·mol-1. Such information obtained from this investigation can provide guiding
478
significance for industrial pilot or industrialization for MSW pyrolysis.
479 480 481
Acknowledgements The financial support of the National Natural Science Foundation of China
482
(21576294 and 21706287), Qingdao People's Livelihood Science and Technology
483
Project (16-6-2-51-nsh) and Independent Innovation Research Project of China
484
University of Petroleum (East China) (24720185022A) is gratefully appreciated by
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authors.
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(49)
(50)
126, 1037–1046. Ahmad, M.S.; Mehmood, M.A.; Taqvi, S.T.H.; Elkamel, A.;Liu, C.; Xu, J.; Rahimuddin, S.A.; Gull, M. Pyrolysis, Kinetics Analysis, Thermodynamics Parameters and Reaction Mechanism of Typha latifolia to Evaluate its Bioenergy Potential. Bioresour. Technol. 2017, 245, 491–501. Vyazovkin, S.; Burnham, A. K.; Criado, J. M.; Pérez-Maqueda, L. A.; Popescu, C.; Sbirrazzuoli, N. ICTAC Kinetics Committee Recommendations for Performing Kinetic Computations on Thermal Analysis Data. Thermochim. Acta 2011, 520 (1–2), 1–19. Hu, M.; Chen, Z.; Wang, S.; Guo, D.; Ma, C.; Zhou, Y.; Chen, J.; Laghari, M.; Fazal, S.; Xiao, B.; et al. Thermogravimetric Kinetics of Lignocellulosic Biomass Slow Pyrolysis Using Distributed Activation Energy Model, Fraser-Suzuki Deconvolution, and Iso-Conversional Method. Energy Convers. Manag. 2016, 118, 1–11. Pacheco, H.; Thiengo, F.; Schmal, M.; Pinto, J.C. A Family of Kinetic Distributions for Interpretation of Experimental Fluctuations in Kinetic Problems. Chem. Eng. J. 2018, 332, 1385-8947. Ye, G.; Luo, H.; Ren Z.; Ahmad, M.S.; Liu, C.; Tawab, A.; Al-Ghafari, A.B.; Omar, U.; Gull, M.; Mehmood, M.A. Evaluating the Bioenergy Potential of Chinese Liquor-industry Waste through Pyrolysis, Thermogravimetric, Kinetics and Evolved Gas Analyses. Energy Convers. Manag. 2018, 163, 13– 21. Narayan, R.; Antal, M. J. Thermal Lag, Fusion, and the Compensation Effect during Biomass Pyrolysis. Ind. Eng. Chem. Res. 1996, 35 (5), 1711–1721.
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638 639
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Table 1 Proximate and ultimate analysis of all samples. Samples
Plastics PE
Rubber PP
Textile
Paper
PVC
Poplar
Kitchen wastes
Mixed
wood
Pork
Rice
MSW
Proximate analysis (wt.%) Ad
-
-
-
18.74
2.70
12.59
2.70
3.70
2.38
4.32
Vd
99.98
99.97
97.23
59.52
87.55
73.84
79.81
90.56
81.33
84.55
FCd
0.02
0.03
2.77
21.74
10.21
13.57
17.49
5.74
16.29
14.13
84.13
38.64
69.94
44.51
41.05
45.39
43.63
44.17
53.76
Ultimate analysis (wt.%) C
85.47
H
14.21
14.96
4.77
5.78
6.73
6.16
6.24
8.30
6.92
8.77
N
0.08
0.23
0.14
0.40
0.37
0.04
0.18
9.90
1.24
2.01
0.24
0.24
0.11
1.42
0.91
0.35
1.99
0.96
1.07
0.98
3.72
44.78
39.81
43.50
33.51
44.22
30.16
S O
a
0.13
0.43
56.34
*
Heat value (MJ·kg-1)
640 641 642
HHV
48.84
49.37
19.64
31.02
17.54
16.38
17.36
19.84
17.65
25.55
LHV
43.64
43.91
17.97
29.41
17.23
15.95
17.28
19.79
17.39
24.08
A: ash; V: volatile matter; FC: fixed carbon; HHV: higher heating value; LHV: Lower heating value a d dry basis; by difference; * the result contains Cl.
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Table 2 The IR bonds for gaseous products and functional groups. Wavenumber/cm-1
Assignment
Possible compounds
2384 2180 3014 3200-3600 1650-1900 1080-1300
CO2 CO CH4 O−H Stretching C=O Stretching C−O Stretching
/ / / Water Carbonyl compounds Alcohols, phenols, esters
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645 646
Page 30 of 37
Table 3 Kinetic parameters and compensation effect of components. Components
Stage
Kinetic parameters Ea/kJ·mol
-1
A/min
Kinetic compensation effect -1
2
R
Equation
R2
Plastics PE
/
296.80
3.49E20
0.9347
ln A=0.1794Ea−5.9437
0.9985
PP
/
312.56
1.26E22
0.9456
ln A=0.1764Ea−4.2510
0.9995
PVC
1st
123.73
2.01E16
0.9457
ln A=0.2302Ea+9.0563
0.9981
2nd
206.70
1.13E22
0.9561
ln A=0.1152Ea+26.9677
0.9651
1st
183.28
1.13E14
0.9905
ln A=0.1475Ea+5.3247
0.9884
Rubber
2nd
203.55
4.93E10
0.9742
ln A=0.1978Ea−15.6413
0.9996
Textile
/
201.54
9.59E22
0.9726
ln A=0.2354Ea+5.4755
0.9990
Paper
1st
205.69
7.01E12
0.9695
ln A=0.2152Ea−5.0756
0.9993
2nd
198.43
1.87E12
0.9710
ln A=0.1680Ea−8.9273
0.9943
Poplar wood
/
186.95
1.38E15
0.9733
ln A=0.2305Ea−8.2324
0.9950
Pork
/
321.63
2.55E26
0.9738
ln A=0.1506Ea+12.3665
0.9972
Rice
/
234.57
1.08E21
0.9751
ln A=0.2312Ea−5.8004
0.9949
1st
163.30
3.15E15
0.9571
ln A=0.6211Ea−65.7391
0.9817
2nd
187.75
6.98E16
0.9357
ln A=0.1477Ea+11.0539
0.9681
3rd
146.72
9.98E10
0.9287
ln A=0.1317Ea+6.0037
0.9625
Kitchen wastes
Mixed MSW
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Table 4 The activation energy and frequency factor at the confidence interval of 0.99. Components
Stage
Kinetic parameters (µ=0.99) Ea/kJ·mol-1 A/min-1
/ / 1st 2nd 1st 2nd / 1st 2nd /
279.51−314.40 286.05−339.07 111.90−135.56 196.70−213.58 169.87−196.69 193.19−213.92 175.25−227.82 164.55−246.83 195.13−200.39 150.82−218.26
1.57E19−8.21E21 1.17E20−1.35E24 1.32E15−3.06E17 3.57E21−2.50E22 1.56E13−8.17E14 6.35E9−3.83E11 1.97E20−4.66E25 1.49E13−7.32E20 2.29E10−5.54E10 3.33E11−1.18E18
/ /
223.40−419.87 212.32−256.81
9.59E19−6.80E32 6.31E18−1.85E23
1st 2nd 3rd
160.40−166.20 166.59−208.91 136.47−156.97
5.21E14−1.94E16 3.07E15−1.59E18 2.59E10−3.85E11
Plastics PE PP PVC Rubber Textile Paper Poplar wood Kitchen wastes Pork Rice Mixed MSW
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50 °C•min-1
100 °C•min-1
300 °C•min-1
LDPE
PP
80
60
60
TG/%
80
60
40
40
20
0 400
600
800
1000
400
600
800
1000
200
Rubber
Textile
100
60
60
TG/%
60
TG/%
80
20
40
20
0 800
1000
40
400
600
800
1000
200
Poplar wood
Pork
100
60
TG/%
60
TG/%
60
20
40
20
0 800
1000
Rice
40
0 200
400
600
800
1000
Temparature/°C
200
400
600
Temparature/°C
650 651
1000
20
0 600
Temparature/°C
800
100
80
40
600
Temparature/°C
80
400
400
Temparature/°C
80
200
Paper
0 200
Temparature/°C
100
1000
20
0 600
800
100
80
40
600
Temparature/°C
80
400
400
Temparature/°C
100
TG/%
40
0 200
Temparature/°C
200
PVC
20
0 200
700 °C•min-1
100
80
20
649
500 °C•min-1
100
TG/%
TG/%
100
TG/%
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
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Fig.1. TG curves of individual components pyrolysis at different heating rates.
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1000
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50 °C•min-1
100 °C•min-1
0
0
-300
-300
300 °C•min-1
500 °C•min-1
700 °C•min-1
0
-900
-1
-600
DTG/%⋅min
-1
-600
DTG/%⋅min
DTG/%⋅min
-1
-100
-900
-200
-300 -1200
-1200
LDPE
-1500 200
400
600
800
-400
PP
-1500
1000
200
400
Temparature/°C
600
800
1000
PVC 200
400
Temparature/°C
600
800
1000
Temparature/°C 0
0
0
-150
DTG/%⋅min
-1
DTG/%⋅min
-1
DTG/%⋅min
-200
-1
-200
-100
-400
-300
-450 -300
-600
Rubber 200
400
600
800
1000
Textile 200
400
Temparature/°C
600
800
Paper
1000
200
400
Temparature/°C
600
800
1000
Temparature/°C
0
0
0
-100 -300
-300
-1
-200
DTG/%⋅min
-1
DTG/%⋅min
-1
-150
DTG/%⋅min
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
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-300
-400
-600
-900
-450 -500
Poplar wood
652
200
400
600
Temparature/°C
800
Pork
1000
200
400
600
800
Temparature/°C
1000
-1200
Rice 200
400
600
Temparature/°C
653 654
Fig.2. DTG curves of individual components pyrolysis at different heating rates.
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1000
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Experimental Calculated
100
50
0
-20
2nd 3rd
0
0 -25
-40
-1
-25
1st
TG/%
TG/%
2nd 3rd
0
40
25
DTG/%⋅min
25
1st
80
75 20
50
Experimental Calculated
100 40
75
DTG/%⋅min -1
-50
-50 -40
-75
50 °C•min 200
400
600
800
200
1000
400
Experimental Calculated
800
1000
Experimental Calculated
100 300
75
400
75
50
50
150
2nd
3rd
0
-25
2nd
3rd
0
0 -25
-200
-50
-1
-1
-150
1st
TG/%
1st 0
200
25
DTG/°C⋅min
25
TG/%
600
Temperature/°C
Temperature/°C
100
-50 -300
-75
300 °C•min
-75
-1
-1
-100
656
-1
100 °C•min
-100
-100
655
-80
-75
-1
DTG/°C⋅min
200
400
600
800
1000
-400
500 °C•min
-100 200
400
600
800
1000
Temperature/°C
Temperature/°C
Experimental Calculated
100
600
75 300
50
TG/%
25
1st
0
2nd
3rd
0
-25
-1
DTG/°C⋅min
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 34 of 37
-300 -50 -75
700 °C•min
-100
657 658 659
200
400
600
800
-1 -600
1000
Temperature/°C
Fig.3. The experimental and calculated TG and DTG curves of mixed MSW pyrolysis at different heating rates.
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PE PP PVC Rubber Textile Paper Poplar wood Pork Rice
Intensity
0.16
0.12
0.08
0.06
(b) CO
PE PP PVC Rubber Textile Paper Poplar wood Pork Rice
0.04
Intensity
(a) CO2 0.20
0.02
0.04
0.00
0.00
200
660
400
600
800
1000
200
400
Temerature/°C
(c) CH4
PE PP PVC Rubber Textile Paper Poplar wood Pork Rice
0.050
Intensity
0.3
0.025
0.000
0.2
300
350
400
450
500
550
600
800
1000
Temerature/°C PE PP PVC Rubber Textile Paper Poplar wood Pork Rice
(d) O−H 0.06
Intensity
0.4
0.03
0.1
0.0
0.00
200
661
400
600
200
1000
400
0.04
0.04
0.02
0.02
0.01
0.00
0.00 200
400
600
Temerature/°C
800
1000
800
1000
PE PP PVC Rubber Textile Paper Poplar wood Pork Rice
(f) C–O
0.03
Intensity
0.06
600
Temerature/°C PE PP PVC Rubber Textile Paper Poplar wood Pork Rice
(e) C=O
662 663 664
800
Temerature/°C
Intensity
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
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200
400
600
800
1000
Temerature/°C
Fig.4. The evolution of products with temperature in the pyrolysis process of individual components at heating rate of 100 ℃·min-1.
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0.16
Experimental Calculated
(a) CO2
0.05
Experimental Calculated
(b) CO
0.04 0.12
Intensity
Intensity
0.03 0.08
0.02
0.04
0.01
0.00
0.00
200
665
400
600
800
200
1000
400
Experimental Calculated
(c) CH4 0.05
600
800
1000
Temperature/°C
Temperature/°C
(d) O−H
Experimental Calculated
0.03
0.04
0.03
Intensity
Intensity
0.02
0.02
0.01
0.01 0.00
0.00 200
666
400
600
800
1000
200
Temperature/°C
0.020
600
800
1000
Temperature/°C Experimental Calculated
(f) C−O
Experimental Calculated
(e) C=O
400
0.009
0.015
Intensity
0.006
Intensity
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 36 of 37
0.010
0.003 0.005
0.000
667 668 669
0.000 200
400
600
Temperature/°C
800
1000
200
400
600
800
1000
Temperature/°C
Fig. 5. The comparison of products release with temperature of mixed MSW by experimental and calculated data at heating rate of 100 ℃·min-1.
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(a) -6.0
700 °C⋅min
600
-1
(b)
-1
500 °C⋅min
300 °C⋅min 100 °C⋅min
-1
2
ln(β/T )
-7.5
500
-1
-1
-7.0
Ea (kJ⋅mol )
-6.5
-8.0
50 °C⋅min
-8.5
-1
v/v*=0.05
-9.0
PE PP PVC Rubber Textile
Paper Poplar wood Pork Rice MSW
400
300
200
0.3 0.7
-9.5
100
0.95 -10.0 1.1
670
1.2
1.3
1.4
1.5
1.6
1.7
1.8
1.9
0.0
2.0
0.2
0.4
0.6
0.8
1.0
V/V*
1000/T
(d) Mixed MSW
(c) Rice
40
56
2nd Stage 36
1st Stage
52
32 48
ln A
ln A
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
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ln A=0.2312Ea-5.8004
ln A=0.6211Ea-65.7391 2 R =0.9817
28
3rd Stage
2
R =0.9945
44
ln A=0.1317Ea+6.0037 2 R =0.9625
24
20
40
200
671 672 673 674
ln A=0.1477Ea+11.0539 2 R =0.9681
220
240
260
280
100
120
140
160
180
200
220
-1
-1
Ea(kJ⋅mol )
Ea(kJ⋅mol )
Fig.6. Kinetic study by DAEM: (a) Arrhenius plots for mixed MSW, (b) Activation energy values, (c) Kinetic compensation effect for rice, (d) Kinetic compensation effect for mixed MSW.
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