a) Introduction
Since the first cupola patent
was taken out in England in the late eighteenth century, the furnace has
remained the predominant melting unit in iron foundries on a tonnage basis.
Over the two intervening centuries, the basic operations of coke fired cupola
have remained relatively unchanged, although the understanding of the process
involved has improved considerably.
The conventional cupola has
been perceived as a relatively low cost plant which, particularly for smaller
foundries, is capable of achieving the appropriate quantity of iron, especially
grey iron. Thus the status of the furnace was virtually unchallenged in iron
foundries until the late 1950s, early 1960s.
At that time, electric
furnaces, particularly coreless induction types, began to make inroads into the
market. This market penetration has accelerated in recent years with the
development of more efficient and powerful solid state powered equipment. The
introduction of electric furnaces was promoted by environmental concerns, by
the ability to produce more easily a
range of alloys, by increasing customer expectations regarding quality, and
improvements of both electric furnace equipment and associated refractory
systems. Many of the small to medium sized electric furnace plants installed in
recent years have been justified on this basis, even though capital costs may
be higher than for a simple cupola plant.
The introduction of
environmental legislation requiring rigorous control of emissions to the
external atmosphere has been perceived to mitigate against cupola melting in
favour of electric melting, the latter being considered by most foundrymen to
be cleaner. However, this is not necessarily true, since deterioration of scrap
quality, the need to control workplace environment and the continued scrutiny
and tightening of outside emission limits apply whatever the melting unit.
Various recent waste regulations mean that the dumping of waste from furnace
emission control systems will become more difficult and expensive, and the use
of the cupola to reprocess such material will become a more important benefit
in the future.
The largest melting cost item
is charge metallic and the ability to process lower quality scrap through a
cupola, due to its refining action and greater tolerance of included
non-metallic material, is of considerable benefit, particularly for tonnage
applications. This is why large tonnage outputs of a restricted range of
unalloyed cast irons are almost invariably produced from cupolas. Such plants
may include hot blast facilities and will for the most part be fitted with fume
cleaning plant of sufficient efficiency to satisfy the appropriate
environmental requirements. These cupola installations will employ electric
holding furnaces to allow for optimum operation of the prime cupola melter.
Most iron foundries have had to
consider either upgrading their emission control equipment or changing their
melting practice to ensure compliance with the relevant requirements. The
choice in reality has been between fitting dry bag filtration systems or
changing to induction furnace operation. These options are expensive, but
installing suitable emission control equipment on an existing cupola plant has
no economic justification other than keeping the company out of Courts and
allowing them to continue in business.
The majority of cupola plants are based on conventional cold
blast units, which may or may not be fitted with improvements such as automatic
blast control, oxygen enrichment, and divided blast equipment. In addition, the
higher output furnaces, especially where long campaign operation is involved,
have for many years been largely of the hot blast type. However, relatively
recently, the impending legislation on emissions and to a lesser extent waste,
the increased interest in long campaign operation and the ever present need to
reduce costs – both capital and operating – have all conspired to ensure that
cupola technology has not become stagnant. The following sections attempt to
review the current status of the cupola furnace.
b) Conventional Cold Blast
Cupola Operation
The conventional cold blast
cupola is a vertical shaft furnace operating on the counter-current principle.
Cold charge materials are fed into the top of the unit and are preheated by the
products of combustion of coke as they descend and melt before being tapped out
near the base (see Exhibit Q).
An incandescent coke bed is
established in the lower part of combustion air (blast air) introduced via a
series of tuyeres arranged in this area to ensure that appropriate combustion
conditions are generated. Blast pressure, velocity and disposition are
important and require adequate control if the correct bed conditions and
temperature distribution are to be maintained.
The cupola furnace is not a
“dead melting” furnace in that the melting process is accompanied by a number
of compositional changes – carbon and sulphur pick-up, and oxidation losses of
silicon and manganese.
Pick-up of carbon depends on a
number of factors including:
initial carbon content of the charge mixture
the tapped silicon and phosphorus levels
the amount and quality of the coke
coke bed temperature
cupola well depth
method of tapping
metal tapping temperature.
Clearly some of these factors
are inter-related.
Sulphur pick-up in turn is
governed by a number of factors, notably the sulphur content of the coke, slag
basicity and charge make-up and composition.
There is invariably some
oxidation loss of silicon during cupola melting, normally between 10% and 20%
of the charged level of element. The actual figure will vary depending on the
melting conditions, with high tapping temperatures favouring a reduction in
losses and the presence of steel scrap and high silicon briquette additions
having the opposite effect. Manganese is subject to oxidation losses of the
order of 20–25% of the charged level, although again melting conditions will
have an influence on the practical values achieved.
The cupola is refractory lined
and as the melting campaign proceeds, the refractory is mechanically and
chemically eroded until the remaining thickness is insufficient to allow for
continued safe operation. This erosion situation limits the melting campaign
and usually requires the provision of two
furnaces in an installation. One will be melting while he second unit is being
repaired. Eroded lining material, together with coke ash, dirt from the charge
materials and appropriate fluxes (usually limestone) results in the formation
of an acid slag which is tapped either with or separate to the metal.
From the above, it can be
observed that there are a number of areas of possible improvements that could
be explored when considering the limitations of the conventional cold blast
cupola. These include:
increasing coke bed and metal tapping temperatures
improving carbon pick-up and reducing sulphur pick-up
reducing silicon manganese oxidation losses
increasing campaign length
increasing melting rates.
In addition, the increasingly
stringent emission and waste regulations have resulted in the development of
re-use systems to minimise their effects on the foundry’s operations and costs.
These factors have resulted in considerable research and
development of a wide variety of cupola technology in an effort to improve the
performance of the furnace.
c) Divided Blast Cupola
The divided blast cupola, a
development of the balanced blast cupola of earlier years, was developed in the
early 1970s and became very popular as a means of improving the performance of
many cold blast cupola plants installed years before and struggling to meet
increasing quality standards. It also became popular in new installations at
that time.
In the balanced blast system,
however, the cupola is provided with two rows of tuyeres set 900 mm apart and
the air blast is controlled in both areas. A distribution of 50/50 between the
two rows of tuyeres appears to give the best results independent of the amount
of charge coke or blast rate. Control can be obtained by using separate fans
for each row of tuyeres or by installing proportioning control equipment in the
ducts from a single fan (see Exhibit R).
The system enables a higher
metal tapping temperature and higher carbon pick-up to be obtained for a given
coke charge or a reduction in charge coke and an increase in melting rate
whilst maintaining a given tapping temperature. It is necessary to recognise
that all of these advantages cannot be obtained at the same time.
Exhibit S shows the relationship between coke consumption,
metal temperature and melt rate. The divided blast cupola may be further
enhanced by the use of oxygen applied to the lower row of tuyeres.
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