Abstract:
Blast furnace is a moving bed noncatalytic reactor, used widely
for producing pig iron. Burden feed consisting of iron ore, coke and
flux enters the furnace from top and moves downwards. While the hot
air blast introduced through the tuyeres at the bottom of furnace,
moves upwards. Many transfer and rate processes take place during the
countercurrent sojourn of gas and solids in the furnace. Overall
process of making pig iron requires large amount of heat, which is
supplied by the hot gases produced during the combustion of coke with
hot air blast. Due to the increasing emphasis on energy conservation
and pollution control, there is a need to understand and analyse the
blast furnace process so that the problems associated with its
operation, design and control could be solved.
Mathematical modelling is an attractive tool for the analysis and
simulation of systems as the models are based upon fundamental laws of
conservation of mass, momentum and energy. Properly formulated models
provide sufficient insight about the processes occuring in the system
and also assist in quantifying them. Thus, it is desirable to develop a
mathematical model of the complex blast furnace process.
In the present thesis, a One-dimensional mathematical model of the
shaft region of blast furnace has been developed. The shaft encompasses
stack, belly and bosh. Its model consists of ten nonlinear partial
differential equations (time-dependent convection equations), one
ordinary differential equation and four algebraic equations. In the
model eight chemical reactions have been considered, which also include
the reaction of SiO gas with carbon dissolved in molten pig iron. This
model is capable of predicting the behaviour and performance under
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unsteady state as well as steady state operations. For its numerical
solution, initial and boundary conditions, and appropriate constitutive
relationships are required.
In view of the above, a procedure for computing the material and
energy balances of a blast furnace has been developed and programmed.
The program calculates the boundary conditions of the proposed
mathematical model by using the generally available plant data and also
computes the parameters of streams, which are difficult to measure and
are normally not known. During the process few significant results and
relationships have also been obtained, which are mentioned below.
A methodology for computing the molar flow rate of SiO gas
formed in the combustion zone.
An empirical relationship for calculating the melting
temperature of coke ash for the specified Al 0 and SiO
contents.
Simplified relationships for the direct calculation of
adiabatic flame temperature, tuyere gas temperature, and top
gas temperature.
Besides, it has been clearly demonstrated by computations that the
tuyere gas temperature is approximately 250 K less than the adiabatic
flame temperature. Hence, it is not advisable to use adiabatic flame
temperature in place of tuyere gas temperature in modelling studies.
Constitutive relationships play an important role in modelling and
simulation of engineering systems. For blast furnace process, their
number is quite large. Correlations for various parameters used in the
model have been discussed and derived. Their limitations have also been
pointed out. Further, the heat of reaction varies with temperature,
and there exists wide variation in temperature within the furnace.
Therefore, the correlations for heats of reactions as a function of
temperature have been derived so that the effect of variation in heats
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of reactions on the behaviour of furnace could be studied.
The model has been transformed into steady state model by setting
time derivatives equal to zero. Resulting model equations consist of
eleven nonlinear ordinary differential equations. In the present work,
it was decided to obtain the numerical solution of the model under
steady state conditions only. These model equations constitute a
Boundary Value Problem (BVP), which is generally difficult to solve in
comparison to an Initial Value Problem (IVP). Since developed model
consists of many adjustable parameters pertaining to the
maldistribution of gas and solids, and uncertainties associated with
the constitutive relationships, therefore, the model equations have
been solved as an IVP and the iterations have been stopped by matching
the calculated and given boundary conditions at one of the end. A
computer program has been developed for the simulation of steady state
model. It has been our experience that the numerical solution of the
model is very sensitive to the adjustable parameters and slight
variation in their values might lead to nonconvergence of the
numerical scheme adapted to solve it as a BVP.
An industrial blast furnace was selected for testing the model
predictions. Its dimensions and four sets of operating data were taken
from the literature. In order to ascertain the correctness of the
proposed model, longitudinal profiles of all the process variables,
namely compositions, fractional conversions, temperatures and pressure
have been computed, and are in accordance with those reported in the
literature. These have also been explained on the basis of assumptions
underlying the model.
It has been observed that the change in heats of reactions as a
result of variation in temperature has appreciable effect on the model
predictions in higher temperature zones (1000 K or above) . Therefore,
it is necessary to account for this effect in the model. This
conclusion is in contrast to most of the earlier modelling studies in
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which heats of reactions were considered constant and taken at the
reference temperature (298 K).
It is our view that the proposed model may be used for the
analysis of blast furnace process and optimization of its productivity,
provided actual plant data could be made available for estimating the
adjustable parameters of the model. Then the model may also be used for
studying its dynamic behaviour and developing suitable control
strategies.