(10b) Modeling and Simulation of Downdraft Biomass Gasifier | AIChE

(10b) Modeling and Simulation of Downdraft Biomass Gasifier

Authors 

Sheth, P. - Presenter, Birla Institute of Technology and Science (BITS)
Babu, B. V. - Presenter, Birla institute of Technology and Science (BITS)

Abstract

Modeling of biomass
gasification implies the representation of chemical and physical phenomena
constituting all the four zones of the gasifier (pyrolysis, combustion,
reduction, and drying) in the mathematical form. The models of downdraft
biomass gasification can be categorized into two groups: (1) Equilibrium models
and (2) Combined transport and kinetic models. Kinetics-free equilibrium models
can predict the exit gas composition, given the solid composition and the
equilibrium temperature, but they cannot be used for reactor design (Di Blasi,
2000). An equilibrium model can not predict the concentration or temperature
profiles across the axis of gasifier and hence results generated using an
equilibrium model would give the same final composition for different lengths
of reduction zone of biomass gasifier. Hence, there is a need to develop a combined transport and
kinetic model which takes into account of the kinetics of homogeneous and
heterogeneous chemical reactions, transport of volatiles produced, heat and
mass transfer between solid and gaseous phase and pyrolysis reactions. In a
survey of gasifier manufacturers, it is reported that 75% of gasifiers offered
commercially were downdraft, 20% were fluid beds (including circulation fluid
beds), 2.5% were updraft, and 2.5% were of other types (Bridgwater, 2002).
Taking into account of the importance of downdraft biomass gasifier and its
commercial applications, it is essential to have a complete model for such a
configuration.

In the present study, a transient one-dimensional model is
developed for the throated close-top downdraft biomass gasifier. The model
takes into account of the pyrolysis, secondary tar reactions, homogeneous gas
reactions and heterogeneous combustion/gasification reactions. Eight gaseous
species namely O2, N2, CO2, CO, H2O,
H2, CH4 and tar are considered in the gas phase. In the
pyrolysis and combustion zone, the solid phase is a biomass, whereas in the
reduction zone it is charcoal. The developed model is divided into three parts
according to three prevailing zones in the gasifier: (1) pyrolysis, (2)
oxidation, and (3) reduction. Pyrolysis is a process by which a biomass
feedstock is thermally degraded in the absence of oxygen/air to produce solid
(charcoal), liquid (tar and other organics) and gaseous (H2, CO2,
CO, etc.) products. Released volatiles from each biomass particle flow downward
in packed pyrolysis bed. Rate of release of volatiles depends on the particle
size and temperature within a single particle. The drying zone is indirectly incorporated
in the developed model. The composition of volatiles is found using the
experimental data of Boroson et al. (1989), which predicts the release of
mainly water vapor from the pyrolyzing particle below 120 °C. Pyrolysis bed is modeled as a
stack of particles in one-dimension. To consider the temperature gradient, the
entire bed is divided into two subsystems, i.e., gas phase inside the
bed and the individual particles. To describe the chemical process of pyrolysis
in a single solid particle, an unsteady state one-dimensional variable property
model of transport phenomena is required. It should include heat (conductive,
convective and radiative modes), mass (diffusive and convective modes) and
momentum transport of the products formed within the solid (volatiles and
gases). The model developed and modified by Babu and Chaurasia (2004 a-d) is
used in the present study to model the single particle in the pyrolysis zone.
The single particle modeling equations are clubbed with the conservation
equation of the gaseous species flowing inside the bed of pyrolysis zone. The
volatile products generated in the pyrolysis zone flow downwards and enter into
the oxidation zone where a part of the volatiles gets oxidized. In complete
combustion, carbon present in biomass is completely converted to carbon dioxide
while hydrogen is converted to water vapor. It is an exothermic reaction and
yields temperatures in the range of 1000 °C to 1500 °C. In the present model,
complete combustion of biomass is assumed which is ensured by supplying excess
air (usually around 20% more than the stoichiometric requirement). It is
assumed that the tar present in the pyrolysed gas mixture completely gets
decomposed due to very high temperature present in the oxidation zone. The main
components of the gaseous mixture leaving the combustion zone are carbon
dioxide, water vapor, inert nitrogen, carbon monoxide, hydrogen and some amount
of low molecular weight hydrocarbons such as methane, ethane, ethylene etc. In
the reduction zone, the gaseous mixture passes through the hot porous charcoal
bed resting above the grate. The endothermic reactions are carried out where
the degree of temperature drop depends upon the extents of reactions. Giltrap
et al. (2003) developed a model of reduction zone of downdraft biomass gasifier
to predict the composition of producer gas under steady state operation. In our
earlier simulation study (Babu and Sheth, 2006), Giltrap's model (2003) was
modified by incorporating the variation of CRF along the reduction zone
of downdraft biomass gasifier. It is assumed that CRF is exponentially
increasing along the bed length of the reduction zone. Solid carbon in the form
of char is assumed to be present throughout the reduction zone.

The experimental data obtained in our
earlier study (Sheth and Babu, 2009) are used to validate the simulation
results of the complete combined transport and kinetic model. The fraction of initial
moisture content, air flow rate, temperature of the pyrolysis zone, and chemical
composition of the biomass are required as input data for the model to predict
the composition of producer gas. The variation of molar fraction of producer
gas components with time is predicted and compared with the experimental data.
It is found that the model predicted molar fraction of nitrogen decreases first
during the few initial minutes (5-10 min) of gasification. After that it
increases and attains a steady value (after 10-15 min). The molar amount of
nitrogen is constant for a particular flow rate of air as nitrogen acts as an
inert but its composition varies due to the changes in molar amount of other
components of gaseous mixture. It is found that the simulated molar fractions
of carbon monoxide and hydrogen increase first with time and subsequently decrease
and finally attain steady values. It is observed that the model predicted molar
fraction of methane is very less and almost remains constant; while the model
predicted molar fraction of carbon dioxide decreases initially and attains a
steady value.

The simulation results of the molar
composition of various components of the producer gas match well with the
experimental data of 10 minutes or higher from the start of an experimental run.
For the experimental data of 5 min and 10 min, the simulation results differ
more. This is because of the assumption taken in the model that all the gas
generated in pyrolysis or reduction zone travel downwards in the gasifier.
However, it is observed while carrying out the experiments that the gas
produced in the pyrolysis zone first travels upwards and occupies the empty
space above the biomass. After 5 - 10 minutes from the start of the run, the
accumulated gas builds up the pressure and the producer gas starts flowing
downwards. Because of this, the model predicts higher concentration of hydrogen
and carbon monoxide and lower concentration of nitrogen in comparison with the
experimental data for initial 5 -10 minutes from the start of a particular
experimental run. It is concluded from the present study that the developed
model can predict the performance of the biomass gasifier, a priori. The results of this study
are also useful in the design of a downdraft biomass gasifier.

References

Babu, B.V.,
Chaurasia A.S., 2004a. Parametric Study of Thermal and Thermodynamic
Properties on Pyrolysis of Biomass in Thermally Thick Regime. Energy Conversion
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Babu, B.V., Chaurasia A.S., 2004b. Dominant Design
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Babu, B.V., Chaurasia A.S., 2004c. Pyrolysis of
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Babu, B.V., Chaurasia A.S., 2004d. Heat Transfer and Kinetics in the
Pyrolysis of Shrinking Biomass Particle, Chemical Engineering Science, 59,
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Babu, B.V., Sheth, P.N., 2006.  Modeling and Simulation of Reduction Zone
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Boroson, M.L., Howard, J.B., Longwell, J.P., Peters, W.A., 1989. Product
Yields and Kinetics from the Vapor Phase Cracking of Wood Pyrolysis Tars.
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http://www.icheme.org/.../conferences/gasi/Gasification%
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Giltrap, D.L., McKibbin, R.;
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Sheth, P.N., Babu, B.V., 2009. Experimental studies on producer gas
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Zainal, Z.A., Ali, R., Lean, C.H., Seetharamu, K.N., 2001. Prediciton
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