[0001] The present invention is for a heat radiation tube for furnaces and the like heating
purposes. The source of heat can be electrical resistance elements or a burner using
for example gas. Furnaces primarily means furnaces for heat treatment in industrial
processes.
[0002] Heat radiation tubes are mainly used in furnaces where the furnace atmosphere does
not allow direct heat. This can be due to that the atmosphere is harmful to the elements
which are being used for electrical heating or a wish to control the atmosphere in
the furnace whereby combustion gases are not allowed therein. Other reasons for the
use of radiation tubes instead of direct heating where such should be possible might
be for example that one wants to repair or exchange the heat source while the furnace
is being used. It will then be easier to do this in a separate space, e.g. inside
the radiation tube, than in the furnace chamber itself.
[0003] A heat radiation tube may comprise a cylindrical tube. A bottom is mounted in one
end of the tube. In the other end of the tube there is as a rule a flange for mounting
in the furnace wall. The tube can also have other arrangements, protrusions, etc.
for mounting in the furnace as well as distance pieces and the like. Mainly when heating
is obtained by combustion there may in the tube be inserts forming flow channels
for the combustion gases. There are also U-shaped radiation tubes.
[0004] Radiation tubes have hitherto mainly been used by furnace temperatures up to about
1100°C. The tubes are often made from an alloy mainly comprising nickel, chromium
and iron. The alloy composition is for example 40-60 weight % nickel, 15-20 % chrom
and 25-45 % iron. These radiation tubes, however, have certain drawbacks which are
of great importance in most application. On the surfaces of the tubes the outside
as well as the inside oxide layers are formed which are spalled off when they have
reached a certain thickness, which varies due to conditions in each application. Hereby
the oxide layers do not give protection against continuing attacks on the tubes. Downfalling
oxide flakes may cause problems if they get into contact with the products which are
present inside the furnaces. However, the greatest problems are caused by the oxide
flakes inside the tubes. If these are holding electrical elements for the heating
the flakes may cause short-circuiting between separate elements and between separate
parts of one element which brings with it an immediate interruption of the function
of the element or a considerably decreased life of the element. When an element is
exchanged, which means that element and element support is pulled out from the radiation
tube and after repair or exchange again is pushed into it,the supports may function
as scrapes and bring about heaps of oxides in most cases in the far end of the tube
which may cause difficulties by the repair work and function deficiencies.
[0005] Hitherto used radiation tubes do not have satisfactory mechanical properties by high
temperatures of use. Due to their own weight and the internal load the tubes tend
to sag. In order to compensate for this the tubes have to be turned 180° at regular
intervals. This can in most cases be made in connection with normal maintenance or
repair but it is still an important drawback and a factor which limits the possibilities
of use.
[0006] The object of the present invention is to avoid the above-mentioned drawbacks of
hitherto known radiation tubes and to make possible a higher temperature of use than
has hitherto been possible. This mainly refers to a higher constant temperature by
continuous use. The invention also makes it possible to have longer intervals between
stops for maintenance works. The much reduced or totally eliminated sagging of the
tubes means much for reliable function of the radiation tubes as well as easier maintenance.
[0007] Radiation tubes according to the invention are intended for use in furnaces and the
like heating purposes and are characterized therein that the tube is made from an
alloy of FeCrAl-type whereby a cylindrical part is a seamless tube. These radiation
tubes have important advantages compared to conventional tubes made by casting or
welding of plates from nickel chromium or iron-nickel-chromium-alloys. Radiation
tubes according to the invention can be used at temperatures up to 1250-1300°C.
[0008] At high temperatures FeCrAl-alloys at oxidizing conditions form a stable and adhering
layer of aluminium oxide on the surface of the material. This oxide is also more heat
resistant and resistant against chemical attacks than the layers which are formed
on nickel-chromium-alloys. This is particularly obvious in sulphur containing environments,
where rapid and severe attacks are obtained on nickel-chromium materials. If the
oxide layer is undamaged the FeCrAl-alloys are better also in carburating atmosphere.
In many applications it is therefore important to pre-oxidize the radiation tubes
according to the invention. This shall be done also if the intended temperature of
use is below 1100°C. Suitable pre-oxidation is for example heat treatment in air at
1100°C for at least 8 hours. The FeCrAl-alloy may also contain minor amounts of other
alloying components such as yttrium, titanium and zirkonium in amounts up to 0.2 weight
% of each. These additives influence the oxide layers as well as the structure and
properties of the material.
[0009] The cylindrical tube which is a main part of the radiation tube is seam-less and
preferably made by extrusion. The slab which is used for the extrusion is made in
a well-known way be casting or by power metallurgy. The shearing speed and other
conditions by extrusion are choosen to give the tubes a striped surface which means
that all of the outer surface of the tubes is rough with axially extending irregular
grooves and ridges, the size of which is chosen to optimize the properties of the
oxide layer, mainly its strength and elasticity, in order to avoid oxide spalling
by high temperatures and changing temperature.
[0010] Below the invention will be further described with reference to the accompanying
figures.
Fig. 1 shows electrically heated radiation tubes inside a furnace. One of the radiation
tubes is shown with part of the tube cut away in order to show the element.
Fig. 2 shows a cross section through a radiation tube which is heated by combustion
of gas.
Fig. 3 shows the surface of the cylindrical tube of a radiation tube.
Fig. 4 shows a cross section of the cylindrical tube.
[0011] Fig. 1 shows several radiation tubes (1, 2A, 2B) which have been mounted into a furnace,
whereof a brick wall (3) is shown. The radiation tubes have a sheath which is a cylindrical
tube (9) made from FeCrAl material. FeCrAl material means iron-chromium-aluminium-alloys
as described above. At the outer end of the tube is a wall (not shown) from the same
material. Into the wall (3) of the furnace is opened a hole which corresponds to the
tube and wherein the end of the tube is supported. For the not shown end of the tube
there is a corresponding support, for example a shelf or an opening in the furnace
wall. The distance between the walls of the furnace can be up to 2 meters and the
radiation tube is hanging unsupported therein between. Inside the tube there is an
electrical resistance element (4) which in the example shown is made from MoSi₂ of
the kind which is marketed under the trademark KANTHAL SUPER. The element is resting
on a ceramic support (5). The terminal parts (7) of the element pass through two plugs
(6, 8), which separate the hot atmosphere of the radiation tube from the surroundings
and support the terminal parts.
[0012] The radiation tube shown in Fig. 2 is intended to be heated by an indicated gas burner
(14). The combustion gases from the burner flow firstly through the insert (12), make
a turn at the wall (10) and flow back along the radiation tube (9). The latter has
a flange (11) for mounting to the furnace wall in a conventional way. Supports (13)
are welded to the insert.
[0013] The radiation tubes shown in figures 1 and 2 have dimensions chosen with respect
to the furnace wherein they are to be used. For example, the length of the tube may
be 1800 mm, its external diameter 200 mm and wall thickness 8 mm.
[0014] Figures 3 and 4 show the appearance of a radiation tube according to the invention.
Figure 3 is a photograph of the surface of the tube and figure 4 shows a cross section
of the same surface of the tube at about 50 times magnification. The striped appearance
of the surface is shown in the pictures. These crystal stripes are obtained by the
use of a sufficient high shearing speed at the extrusion process and can be essential
for the properties of the oxide layer.
1) Radiation for furnaces and the like heating purposes, characterized in that the tube is made from a FeCrAl alloy, whereby its cylindrical part is a seam-less
tube.
2) Radiation tube according to claim 1, characterized in that the tube is extruded.
3) Radiation tube according to any of the preceding claims, characterized in that the surface of the tube is rough having along the tube extending irregular grooves
and ridges.
4) Radiation tube according to any of the preceding claims, characterized in that its outer surface by pre-oxidation has been covered with an oxide layer comprising
mainly aluminum oxide.
5) Method of the production of tubes of alloys of FeCrAl type, characterized in that the tubes are obtained by extrusion.
6) Method according to claim 5, characterized in that the extrusion is made at such a shearing speed that the surface of the tube
is rough having along the tube extending grooves and ridges.