BACKGROUND OF THE INVENTION
Field of the Invention:
[0001] The present invention relates to a combustion device having a ceramic burner.
Description of the Related Art:
[0002] There has heretofore been known a combustion device having a burner which is supplied
with a mixture of a fuel gas and air added at a predetermined ratio and burns the
supplied mixture in total primary combustion. The burner comprises a ceramic burner
having a ceramic plate which is porous to make itself resistant to thermal shocks.
The ceramic plate has a number of small-diameter burner ports defined therein and
extending from a surface of the plate to the opposite surface thereof.
[0003] In combustion devices, it has been general practice to apply a voltage is between
a burner and a frame rod and detect a flame current flowing through flames produced
by the burner for detecting an ignition. If a flame current in excess of a predetermined
level is detected, then it is confirmed that the mixture has well been ignited. If
the flame current falls below the predetermined level while the mixture is being combusted
by the burner, then the burner is determined as suffering a flame failure. Since the
ceramic burner is electrically nonconductive and no current flows therethrough, however,
it is difficult to detect an ignition on the ceramic burner based on the flame current.
[0004] In view of the above drawback, it has been proposed to construct a ceramic burner
of an electrically conductive ceramic material. One example of electrically conductive
ceramic material is lithia-based ceramics such as petalite (LiAlSi
4O
10), for example.
[0005] A study by the inventors of a ceramic burner of petalite has revealed that when a
voltage is applied between the ceramic burner of petalite and the flame rod, a produced
flame current largely varies depending on the surface temperature of the ceramic burner.
Specifically, the flame current that flows between the ceramic burner of petalite
and the flame rod is as small as if the burner were made of an electrically nonconductive
material when the surface temperature of the ceramic burner is low, and therefore
it takes a considerable period of time until the flame current reaches a level high
enough to be detected. The ceramic burner of petalite is further disadvantageous in
that when burning conditions are changed while the mixture is being combusted or the
mixture is re-ignited after the combustion of the mixture has been stopped, the flame
current suffers a large overshoot, and will be stabilized after a long period of time.
If the overshoot of the flame current is large, then the flame current tends to be
too large to detect an ignition or a flame failure, and hence an ignition or a flame
failure cannot be detected until the flame current becomes stabilized.
[0006] Japanese laid-open utility model publication No. 1-67466 and Japanese utility model
publication No. 5-18606 disclose combustion devices in which an electrically conductive
layer is placed on a surface of a ceramic burner where flames are produced. According
to the disclosed combustion devices, a flame rod is disposed in confronting relation
to the electrically conductive layer where flames are produced by the ceramic burner,
and a voltage is applied between the electrically conductive layer and the flame rod.
Alternatively, a voltage is applied between the electrically conductive layer and
a heat exchanger which is employed in place of the flame rod. The publications referred
to above state that the disclosed arrangement allows a flame current flowing through
the flames to be detected to detect an ignition.
[0007] It is known that a deposited film of nickel is disposed as the electrically conductive
layer on the surface of the ceramic burner. However, the deposited film of nickel
cannot withstand use over a long period of time because nickel is poor in heat resistance.
[0008] If a deposited film of platinum or palladium which is highly resistant to heat is
used instead of the deposited film of nickel, then it can be of stable service for
a long period of time. Using such a deposited film of platinum or palladium inevitably
results in an increase in the cost of the combustion device because these materials
are precious metals and expensive.
[0009] Another solution is to use a deposited film of silicon carbide (SiC) instead of the
deposited film of nickel. Silicon carbide is highly heat-resistant in air and can
be utilized as an electrically conductive material as it is an intrinsic semiconductor.
Therefore, silicon carbide is suitable for use as an electrically conductive material
deposited on a ceramic burner surface. A deposited film of silicon carbide can be
produced when silicon dioxide and carbon or silicon and carbon react with each other
and then the reaction product is baked.
[0010] If a film of silicon carbide is to be deposited on a porous ceramic plate of a ceramic
burner, however, since a high-temperature heat-treatment process is necessary to produce
the deposited film of silicon carbide, the porous ceramic plate is rendered dense,
and its resistance to thermal shocks is lowered. If the above reaction product is
baked at a temperature which is not sufficiently high to make the porous ceramic plate
dense, then it is difficult to produce a deposited film of silicon carbide.
[0011] The process of baking silicon carbide requires an additive of boron, carbon, or the
like. However, a deposited film of silicon carbide produced with an added impurity
tends to suffer reduced strength at high temperatures. Therefore, it is not easy to
establish proper baking conditions. Furthermore, inasmuch as silicon carbide deteriorates
if oxidized while being baked, the baking facility needs to be evacuated to prevent
silicon carbide from being oxidized. Accordingly, the baking facility is complex and
large in scale, tending to increase the cost of the combustion devices.
SUMMARY OF THE INVENTION
[0012] It is therefore an object of the present invention to provide a combustion device
which includes a ceramic burner having an electrically conductive layer that is highly
resistant to heat, relatively inexpensive, and can easily be manufactured.
[0013] To achieve the above object, there is provided in accordance with the present invention
a combustion device comprising a ceramic burner comprising a porous ceramic plate
having a plurality of burner ports defined therein, an electrically conductive layer
disposed on a surface of the ceramic burner where flames are produced, an electric
conductor disposed in facing relation to the electrically conductive layer, and ignition
detecting means for detecting a flame current flowing through the flames to detect
an ignition when a voltage is applied between the electrically conductive layer and
the electric conductor, the electrically conductive layer being made of an electrically
conductive perovskite-type metal oxide.
[0014] The ceramic plate of the ceramic burner can be manufactured inexpensively as a thermal-shock-resistant
ceramic plate which is made of porous ceramics produced by baking particles of a fire-resistant,
low-expansion ceramic material. The fire-resistant, low-expansion ceramic material
may be cordierite, spodumene, aluminum titanate, mullite, zirconia, zircon, magnesia
(including spinel and forsterite), alumina (including corundum), calcia, chromium
oxide, dolomite, sillimanite, silica stone, zircon mullite, a mixture of alumina and
zirconia, a mixture of alumina and zircon, or a mixture of two or more of the above
materials, or the like.
[0015] The ceramic burner may be constructed of a dense ceramic plate. The dense ceramic
plate may be manufactured by baking particles of a low-expansion ceramic material
such as petalite, spodumene, eucryptite, aluminum titanate, zirconium potassium phosphate,
or the like. However, the baking temperature is relatively high and a certain amount
of energy is required to achieve the relatively high baking temperature. The electrically
conductive layer may be formed on the dense ceramic plate by vacuum evaporation, CVD,
or the like. However, it is necessary to roughen the surface of the dense ceramic
plate for the purpose of increasing the bonding strength between the ceramic plate
and the electrically conductive layer.
[0016] Consequently, if the dense ceramic plate is used, the cost of manufacture of the
dense ceramic plate and the cost of manufacture of the electrically conductive layer.
According to the present invention, the porous ceramic plate is used for reducing
the cost of manufacture of the ceramic burner.
[0017] The perovskite-type metal oxide is represented by a general formula ABO
3 where A and B represent metals and O represents oxygen. Some perovskite-type metal
oxides exhibit metallic electric conductor properties or semiconductor properties.
According to the present invention, the electrically conductive layer is formed of
a perovskite-type metal oxide which exhibits metallic electric conductor properties
or semiconductor properties. The perovskite-type metal oxide may be represented by
the above general formula where the metal A or a portion of the metals A, B is replaced
with another metal.
[0018] The electrically conductive layer is produced by coating the ceramic plate with an
aqueous slurry comprising a powder of electrically conductive perovskite-type metal
oxide mixed with a solvent such as water or the like, drying the slurry, and baking
the dried slurry. Since the perovskite-type metal oxide itself is inexpensive and
does not require any special device for avoiding its oxidization because it is already
an oxide. Therefore, the cost of manufacture of the combustion device is relatively
low. The perovskite-type metal oxide is highly resistant to heat as it is already
an oxide.
[0019] Preferably, the electrically conductive layer uniformly covers the surface of the
porous ceramic plate, and the electrically conductive perovskite-type metal oxide
enters surface pores in the ceramic plate.
[0020] The electrically conductive layer can exhibit uniform electric conductivity by uniformly
coating the surface of the ceramic plate therewith. When the perovskite-type metal
oxide is baked as described above, the perovskite-type metal oxide and the ceramic
plate jointly make up a solid solution at their contacting surfaces. Therefore, the
electrically conductive layer and the ceramic plate are firmly bonded to each other.
Since the perovskite-type metal oxide entering the surface pores and the ceramic plate
jointly make up the solid solution as described above, the electrically conductive
layer is securely anchored to the ceramic plate.
[0021] The electrically conductive layer should preferably comprise particles of the electrically
conductive perovskite-type metal oxide which have diameters ranging from 0.04 to 5
µm. The diameters referred to herein are those of the particles of the electrically
conductive perovskite-type metal oxide after it has been baked.
[0022] If the particle diameters of the baked electrically conductive perovskite-type metal
oxide were less than 0.04 µm, then it would be difficult for the electrically conductive
layer to uniformly cover the surface of the ceramic plate. If the particle diameters
of the baked electrically conductive perovskite-type metal oxide were greater than
5 µm, the solid solution would be difficult to form, and the electrically conductive
layer would easily be peeled off the ceramic burner.
[0023] In order to uniformly cover the surface of the ceramic plate, the electrically conductive
layer should preferably have a thickness ranging from 10 to 300 µm. If the thickness
of the electrically conductive layer were smaller than 10 µm, then the ceramic plate
would be liable to be exposed and the electrically conductive layer would not exhibit
uniform electric conductivity. If the thickness of the electrically conductive layer
exceeded 300 µm, then the electrically conductive layer would tend to crack due to
thermal expansion upon baking, and would easily be peeled off the ceramic burner.
[0024] Preferably, the electrically conductive layer contains an inorganic binder ranging
from 1 to 20 weight % of the total amount thereof, and the electrically conductive
layer is bonded to the porous ceramic plate by the inorganic binder. Since the electrically
conductive layer contains the inorganic binder, particles of the perovskite-type metal
oxide are firmly bonded to each other or to the ceramic plate by the inorganic binder.
The electrically conductive layer which contains the inorganic binder is effective
to lower a baking temperature at which to bake the perovskite-type metal oxide and
increase the range of baking temperatures at which the baked perovskite-type metal
oxide acts as the electrically conductive layer. Therefore, it is made easy to establish
a desired baking temperature.
[0025] The inorganic binder may be borosilicate glass, soda lime glass, etc. If the content
of the inorganic binder were less than 1 weight % of the total weight of the electrically
conductive layer, then the inorganic binder would fail to act as a binder. If the
content of the inorganic binder were greater than 20 weight % of the total weight
of the electrically conductive layer, then the resistance of the electrically conductive
layer would be too large.
[0026] The electrically conductive perovskite-type metal oxide should preferably comprise
La
1-xSr
xMnO
3 because it exhibits electric conductivity and can easily be manufactured.
[0027] Furthermore, since La
1-xSr
xMnO
3 has a high emissivity, the electrically conductive layer on the surface of the ceramic
burner is effective to lower the temperature of flames, thus reducing nitrogen oxides
emitted upon combustion by the ceramic burner. Moreover, because La
1-xSr
xMnO
3 has a catalytic action for fully oxidizing methane contained in a town gas at low
temperatures, it is capable of further reducing nitrogen oxides emitted upon combustion
by the ceramic burner.
[0028] The above and other objects, features, and advantages of the present invention will
become apparent from the following description when taken in conjunction with the
accompanying drawings which illustrate preferred embodiments of the present invention
by way of example.
BRIEF DESCRIPTION OF THE DRAWINGS
[0029]
FIG. 1 is a schematic cross-sectional view of a combustion device according to the
present invention;
FIG. 2 is a graph showing flame currents detected between an electrically conductive
layer and a flame rod in response to input powers in a predetermined range in the
combustion device according to the present invention;
FIG. 3 is a graph showing temperature-dependent changes in the electric conductivity
of an electrically conductive perovskite-type metal oxide in the combustion device
according to the present invention;
FIG. 4 is a graph showing changes in flame currents in response to input powers in
a ceramic burner of the combustion device according to the present invention and other
ceramic burners;
FIG. 5(a) is a graph showing time-dependent changes in flame currents in the ceramic
burner of the combustion device according to the present invention and the other ceramic
burners at the time an excess air ratio is 1.4 and the combustion device is set to
a maximum combustion capability;
FIG. 5(b) is a graph showing time-dependent changes in flame currents in the ceramic
burner of the combustion device according to the present invention and the other ceramic
burners at the time an excess air ratio is 1.4 and the combustion device is set to
a minimum combustion capability;
FIG. 6(a) is a graph showing time-dependent changes in flame currents in the ceramic
burner of the combustion device according to the present invention and the other ceramic
burners at the time an excess air ratio is 1.1 and the combustion device is set to
a maximum combustion capability;
FIG. 6(b) is a graph showing time-dependent changes in flame currents in the ceramic
burner of the combustion device according to the present invention and the other ceramic
burners at the time an excess air ratio is 1.1 and the combustion device is set to
a minimum combustion capability;
FIG. 7(a) is a graph showing time-dependent changes in flame currents in the ceramic
burner of the combustion device according to the present invention and the other ceramic
burners at the time burning conditions are changed during combustion;
FIG. 7(b) is a graph showing time-dependent changes in flame currents in the ceramic
burner of the combustion device according to the present invention and the other ceramic
burners at the time the mixture is extinguished after combustion and then re-ignited;
and
FIG. 8 is a graph showing the relationship between contents of an inorganic binder
in an electrically conductive layer, baking temperatures, and electric resistances
of the electrically conductive layer in the combustion device according to the present
invention.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT
[0030] FIG. 1 shows a combustion device 1 according to the present invention which comprises
a ceramic burner 3 housed in a casing 2 and a heat exchanger 5 also housed in the
casing 2 for heating water supplied from a water supply pipe 4 with the ceramic burner
3 thereby to produce hot water. The combustion device 1 has a hot water supply pipe
6 for supplying hot water produced by the heat exchanger 5 to various places including
a kitchen, a washroom, a bathroom, etc.
[0031] The ceramic burner 3 has a thermal-shock-resistant ceramic plate made of porous ceramics
produced by baking particles of cordierite which is a fire-resistant, low-expansion
ceramic material. The ceramic plate has a number of small-diameter burner ports 3a
defined therein and extending from a surface of the plate to the opposite surface
thereof. The ceramic burner 3 has an electrically conductive layer 7 disposed on a
surface thereof facing the heat exchanger 5, the electrically conductive layer 7 comprising
a coated layer of an electrically conductive perovskite-type metal oxide.
[0032] The combustion device 1 also has a frame rod 8 disposed between the ceramic burner
3 and the heat exchanger 5, and an ignition detector 9 for detecting an ignition by
the ceramic burner 3. The ignition detector 9 detects an ignition by detecting a flame
current that flows through flames F when a voltage is applied between the electrically
conductive layer 7 and the flame rod 8 to ignite a mixture of a fuel gas and air supplied
to the ceramic burner 3.
[0033] The porous ceramic plate which is produced by baking particles of cordierite has
surface pores each having a size ranging from 3 to 200 µm. The porous ceramic plate
with such surface pores has a good level of resistance to thermal shocks.
[0034] Electrically conductive perovskite-type metal oxides which exhibit metallic electric
conductor properties include, for example, SrTiO
3, BaTiO
3, LaTiO
3, CaVO
3, SrVO
3, CaCrO
3, SrCrO
3, CaFeO
3, SrFeO
3, SrCoO
3, LaNiO
3, etc. Electrically conductive perovskite-type metal oxides which exhibit semiconductor
properties include, for example, CaTiO
3, BaVO
3, LaCrO
3, CaMnO
3, LaMnO
3, BaFeO
3, LaFeO
3, BaCoO
3, SrNiO
3, BaNiO
3, LnCrO
3 (Ln = Pr, Nd, Sm, Eu), etc. Electrically conductive perovskite-type metal oxides
which exhibit metallic electric conductor properties and semiconductor properties
include, for example, LaCoO
3, etc.
[0035] The electrically conductive perovskite-type metal oxides may exhibit metallic electric
conductor properties or semiconductor properties by replacing a portion of the metal
A or B with another metal in the above general formula. Such electrically conductive
perovskite-type metal oxides include, for example, La
1-xSr
xMnO
3, La
1-xCa
xMnO
3, La
1-xSr
xCoO
3, La
1-xSr
xCrO
3, La
1-xCa
xCrO
3, La
1-xSr
xFeO
3, Y
1-xMg
xCrO
3, Y
1-xCa
xCrO
3, Y
1-xSr
xCrO
3, Y
1-xBa
xCrO
3, Gd
1-xCa
xCrO
3, LaCr
1-yMn
yO
3, LaCr
1-yMg
yO
3, etc. Furthermore, the perovskite-type metal oxides may exhibit metallic electric
conductor properties and semiconductor properties by replacing a portion of the metal
A or B with another metal in the above general formula. Such perovskite-type metal
oxides include, for example, Gd
1-xSr
xCo
1-yMn
yO
3, La
1-xCa
xCr
1-yCo
yO
3, etc. In the above general formula, each of x and y represents a number which is
equal to or greater than 0 and less than 1.
[0036] The perovskite-type metal oxide can be produced by mixing an oxide or carbonate of
a metal so that the metal is of such an amount as to constitute the oxide stoichiometrically,
and then baking the mixture at a predetermined temperature. The produced perovskite-type
metal oxide is crushed into a powder having a particle diameter ranging from 0.005
to 0.3 µm, and waster is added to the powder to produce a slurry. The slurry is coated
on the surface of the ceramic burner 3 by spraying, dried at a predetermined temperature,
and then baked at a predetermined temperature. When thus baked, the particles of the
perovskite-type metal oxide have diameters in the range from 0.04 to 5 µm, providing
an electrically conductive layer 7 which has a thickness ranging from 10 to 300 µm
and uniformly covers the ceramic burner 3.
[0037] When the slurry is baked into the electrically conductive layer 7, the perovskite-type
metal oxide and the ceramic burner 3 jointly make up a solid solution. Therefore,
the electrically conductive layer 7 is firmly bonded to the ceramic burner 3. As described
above, the ceramic burner 3 comprises a porous ceramic plate having surface pores
each having a size ranging from 3 to 200 µm. Because the slurry contains the perovskite-type
metal oxide powder with the particle diameter ranging from 0.005 to 0.3 µm, the particles
of the perovskite-type metal oxide powder uniformly cover the surface of the ceramic
plate 3 and enter the surface pores of the ceramic plate. When the particles of the
perovskite-type metal oxide powder which have entered the surface pores of the ceramic
plate are baked, the produced electrically conductive layer 7 is securely anchored
to the ceramic burner 3.
[0038] If the particle diameter of the perovskite-type metal oxide powder were smaller than
0.005 µm, then the particles of the perovskite-type metal oxide powder would enter
the surface pores too deeply, failing to produce a electrically conductive layer 7
of uniform thickness. If the particle diameter of the perovskite-type metal oxide
powder were greater than 0.3 µm, then when the perovskite-type metal oxide powder
is baked, it would not form particles having diameters in the range from 0.04 to 5
µm, failing to securely anchor the electrically conductive layer 7 to the ceramic
burner 3.
[0039] The electrically conductive layer 7 may also firmly be bonded to the ceramic burner
3 by roughening the surface of the porous ceramic plate to adjust the surface roughness
thereof, rather than adjusting the particle diameter of the perovskite-type metal
oxide.
[0040] Inventive Examples of the present invention will be described below.
[Inventive Example 1]
[0041] In Inventive Example 1, La
0.7Sr
0.3MnO
3 was used as the electrically conductive perovskite-type metal oxide.
[0042] A powder of La
2O
3, a powder of SrCO
3, and a powder of Mn
2O
3 were mixed at a molar ratio of 0.7 : 0.3 : 1, and 200 g of ethanol was added to the
mixture. The mixed components were mixed by a ball mill in a wet process. After the
mixture was dried, it was molded by a uniaxial hydraulic press. The molded product
was preliminarily baked at 1100°C for 12 hours in an electric furnace, and then crushed
into a powder by an automatic mortar in a dry process. The powder was then baked at
1300°C for 12 hours in an electric furnace, and then crushed into a powder by an automatic
mortar in a dry process.
[0043] The baked powder was analyzed by an X-ray diffraction process. As a result, it was
confirmed that the baked power had an LaMnO
3-based crystalline structure.
[0044] To the powder, there were added water of the same weight as the powder and a dispersant
(tradename: Seruna D-305 manufactured by Chukyo Yushi) in 0.5 weight % of the powder.
The components were mixed by a ball mill in a wet process, and dried into an La
0.7Sr
0.3MnO
3 powder having an average diameter of 0.2 µm. An analysis of the powder with an energy-distributed
X-ray analyzer confirmed that the proportions of the constituents of the powder were
La : Sr : Mn = 0.7 : 0.3 : 1 (molar ratio).
[0045] To the La
0.7Sr
0.3MnO
3 powder, there were added water in 20 - 50 weight % of the powder and a dispersant
(tradename: Seruna D-305 manufactured by Chukyo Yushi) in 0.5 weight % of the powder.
The components were mixed into a slurry by a ball mill in a wet process. The slurry
was then sprayed onto the surface of a ceramic plate by a commercially available atomizer,
producing a film on the surface of the ceramic plate. The film was then dried at 110°C
for 2 hours in a drier, and thereafter baked at 1080°C for 1 to 3 hours in an electric
furnace. As a result, a ceramic burner 3 having an electrically conductive layer 7
made of La
0.7Sr
0.3MnO
3 with a particle diameter of 2 µm and having a thickness of 110 µm was produced.
[0046] The electrically conductive layer 7 was formed so as to cover the surface of the
ceramic burner 3 uniformly with La
0.7Sr
0.3MnO
3. Because particles of La
0.7Sr
0.3MnO
3 entering the surface pores of the ceramic burner 3 were baked, the electrically conductive
layer 7 and the ceramic burner 3 were firmly bonded to each other.
[0047] Then, the ceramic burner 3 was installed in the combustion device 3 shown in FIG.
1, and a mixture of a fuel gas and air was supplied to the combustion device 3 and
ignited. A voltage of 120 V was applied between the electrically conductive layer
7 and the flame rod 8, and flame currents detected by the flame detector 9 in response
to input powers in a predetermined range were measured. The measured flame currents
are shown in FIG. 2.
[0048] As can be seen from FIG. 2, with the electrically conductive layer 7 according to
Inventive Example 1, the flame detector 9 detected flame currents ranging from 40
to 160 µA with respect to input powers ranging from 8 to 24 kW. Usually, a flame current
of 1 µA is needed for the ignition detector 9 to detect an ignition, and a flame current
of 0.1 µA is needed for the ignition detector 9 to detect a flame failure. Since the
flame currents produced by the electrically conductive layer 7 according to Inventive
Example 1 are much greater than 1 µA, they are in a range large enough for the ignition
detector 9 to detect an ignition.
[0049] Temperature-dependent changes in the electric conductivity of La
0.7Sr
0.3MnO
3 of the electrically conductive layer 7 are shown in FIG. 3. A review of FIG. 3 reveals
that La
0.7Sr
0.3MnO
3 according to Inventive Example 1 suffers only small changes in the electric conductivity
even at high temperatures, and is hence stable.
[0050] Then, the ceramic burner 3 was installed in the combustion device 3 shown in FIG.
1, and a mixture of a fuel gas and air with an excess air ratio of 1.4 was supplied
to the combustion device 3 and ignited. A voltage of 120 V was applied between the
electrically conductive layer 7 and the flame rod 8, and flame currents detected by
the flame detector 9 in response to input powers in a predetermined range were measured.
The measured flame currents are shown in FIG. 4.
[0051] The excess air ratio represents the ratio of an amount of air to be actually mixed
with the fuel gas to a theoretical or stoichiometric amount of air, which is assumed
to be "1", required for the complete combustion of a given amount of fuel gas. The
excess air ratio is indicated as a dimensionless number.
[0052] A ceramic burner 3 (Conventional Example) which was manufactured in the same manner
as with Inventive Example 1 except that it had no electrically conductive layer 7
was installed in the combustion device 3 shown in FIG. 1, and flame currents were
measured in the same conditions as with Inventive Example 1. Furthermore, a ceramic
burner (Comparative Example) made of electrically conductive ceramics of petalite
and having no electrically conductive layer 7 was installed in the combustion device
3 shown in FIG. 1, and flame currents were measured in the same conditions as with
Inventive Example 1. The measured flame currents are also shown in FIG. 4.
[0053] As can be seen from FIG. 4, the ceramic burner 3 with the electrically conductive
layer 7 according to Inventive Example 1 allowed the flame detector 9 to detect flame
currents large enough to detect an ignition irrespective of the magnitude of input
powers even under such conditions that the excess air ratio is 1.4 and the mixture
is air-rich.
[0054] The ceramic burner 3 according to Conventional Example was an electric nonconductor,
and did not allow the flame detector 9 to detect almost any flame currents irrespective
of the magnitude of input powers. With the ceramic burner 3 according to Comparative
Example, under such conditions that the mixture was air-rich and the temperature of
the ceramic burner 3 was relatively low, detected flame currents were reduced to the
same level as with the ceramic burner 3 according to Conventional Example as the input
power was increased.
[0055] The ceramic burner 3 according to Inventive Example 1 was installed in the combustion
device 3 shown in FIG. 1, and a supplied mixture was ignited while the excess air
ratio and the combustion capability of the combustion device 3 were varied. A voltage
of 120 V was applied between the electrically conductive layer 7 and the flame rod
8, and time-dependent changes in flame currents detected by the flame detector 9 were
measured. The measured changes are shown in FIGS. 5(a), 5(b), 6(a), and 6(b).
[0056] The ceramic burner 3 according to Conventional Example and the ceramic burner 3 according
to Comparative Example were installed in the combustion device 3 shown in FIG. 1,
and time-dependent changes in flame currents detected by the flame detector 9 were
measured under the same conditions as those with the ceramic burner 3 according to
Inventive Example 1. The measured changes are also shown in FIGS. 5(a), 5(b), 6(a),
and 6(b).
[0057] Specifically, FIG. 5(a) shows time-dependent changes in flame currents at the time
the excess air ratio is 1.4 and the combustion device is set to a maximum combustion
capability. In FIG. 5(a), the temperature of the ceramic burner is relatively low.
FIG. 5(b) shows time-dependent changes in flame currents at the time the excess air
ratio is 1.4 and the combustion device is set to a minimum combustion capability.
In FIG. 5(b), the temperature of the ceramic burner is higher than the temperature
of the ceramic burner in FIG. 5(a).
[0058] FIG. 6(a) shows time-dependent changes in flame currents at the time the excess air
ratio is 1.1, making the mixture gas-rich, and the combustion device is set to a maximum
combustion capability. In FIG. 6(a), the temperature of the ceramic burner is higher
than the temperature of the ceramic burner in FIG. 5(b). FIG. 6(b) shows time-dependent
changes in flame currents at the time the excess air ratio is 1.1 and the combustion
device is set to a minimum combustion capability. In FIG. 6(b), the temperature of
the ceramic burner is highest.
[0059] It can be understood from FIGS. 5(a), 5(b), 6(a), and 6(b) that the electrically
conductive layer 7 according to Inventive Example 1 allowed the flame detector 9 to
detect flame currents large enough to detect an ignition within a very short period
of time irrespective of burning conditions.
[0060] The ceramic burner 3 according to Conventional Example was an electric nonconductor,
and did not allow the flame detector 9 to detect almost any flame currents irrespective
of burning conditions, as can be seen from FIGS. 5(a), 5(b), 6(a), and 6(b). With
the ceramic burner 3 according to Comparative Example, as can be seen from FIG. 5(a),
under such conditions that the temperature of the ceramic burner 3 was relatively
low, substantially the same flame currents as those with the ceramic burner 3 according
to Conventional Example were detected. As can be seen from FIGS. 5(b), 6(a), and 6(b),
the ceramic burner 3 according to Comparative Example allowed the flame detector 9
to detect flame currents sufficiently large to detect an ignition and a flame failure
under such conditions that the temperature of the ceramic burner was high. However,
it took 0.5 to 2.0 minutes until the flame currents grew large enough for the flame
detector 9 to detect.
[0061] The ceramic burner 3 according to Inventive Example 1 was installed in the combustion
device 3 shown in FIG. 1, and a voltage of 120 V was applied between the electrically
conductive layer 7 and the flame rod 8. Time-dependent changes in flame currents detected
by the flame detector 9 were measured when the burning conditions were varied during
combustion or at the time the mixture was extinguished after combustion and then re-ignited.
The measured changes are shown in FIGS. 7(a) and 7(b).
[0062] The ceramic burner 3 according to Conventional Example and the ceramic burner 3 according
to Comparative Example were installed in the combustion device 3 shown in FIG. 1,
and time-dependent changes in flame currents detected by the flame detector 9 were
measured under the same conditions as those with the ceramic burner 3 according to
Inventive Example 1. The measured changes are also shown in FIGS. 7(a) and 7(b).
[0063] FIG. 7(a) shows time-dependent changes in flame currents measured when the mixture
was combusted for 15 minutes with an excess air ratio of 1.1 and a minimum combustion
capability of the combustion device 1, and then the excess air ratio remained unchanged
and the combustion device 1 set to a medium combustion capability. FIG. 7(b) shows
time-dependent changes in flame currents measured when the mixture was combusted for
15 minutes with an excess air ratio of 1.1 and a minimum combustion capability of
the combustion device 1, and then the mixture was extinguished, the combustion device
1 was completely cooled, and thereafter the mixture was re-ignited with an excess
air ratio of 1.1 and a medium combustion capability of the combustion device 1.
[0064] As can be seen from FIGS. 7(a) and 7(b), with the ceramic burner 3 with the electrically
conductive layer 7 according to Inventive Example 1, flame currents suffered only
a slight overshoot, and normal flame currents were recovered within a very short period
of time, irrespective of burning conditions.
[0065] With the ceramic burner 3 according to Comparative Example, however, flame currents
exhibited a large overshoot immediately after burning conditions were changed, as
shown in FIG. 7(a). The flame currents were out of scale for 4 seconds immediately
after the burning conditions were changed. It took 20 to 25 minutes until normal flame
currents were restored and stabilized after the overshoot. With the ceramic burner
3 according to Comparative Example, furthermore, immediately after the mixture was
extinguished after combustion and then re-ignited, flame currents exhibited a large
overshoot, as shown in FIG. 7(b), and it took 20 to 25 minutes until normal flame
currents were restored and stabilized after the overshoot. The ceramic burner 3 according
to Comparative Example did not allow the ignition detector 9 to detect an ignition
until normal flame currents were restored after the overshoot.
[0066] Since the ceramic burner 3 according to Conventional Example is an electric nonconductor,
it did not allow the flame detector 9 to detect almost any flame currents irrespective
of burning conditions.
[Inventive Example 2]
[0067] In Inventive Example 2, La
0.7Sr
0.3MnO
3 was used as the electrically conductive perovskite-type metal oxide, and the electrically
conductive layer 7 contained borosilicate glass as an inorganic binder.
[0068] First, an La
0.7Sr
0.3MnO
3 powder was produced in the same manner as with Inventive Example 1. The borosilicate
glass was crushed into a powder by a ball mill in a wet process.
[0069] To the La
0.7Sr
0.3MnO
3 powder, there were added water in 20 - 50 weight % of the powder, a dispersant (tradename:
Seruna D-305 manufactured by Chukyo Yushi) in 0.5 weight % of the powder, and the
borosilicate glass powder. The components were mixed into a slurry by a ball mill
in a wet process. The added amount of the borosilicate glass powder was 4 weight %
of the total amount of an electrically conductive layer 7 to be formed from the slurry.
[0070] The slurry was then sprayed onto the surface of a ceramic plate by a commercially
available atomizer, producing a film on the surface of the ceramic plate. The film
was then dried at 110°C for 2 hours in a drier, and thereafter baked at 950°C for
1 hour in an electric furnace, thus producing an electrically conductive layer 7 having
a thickness of 120 µm.
[0071] The electrically conductive layer 7 was formed so as to cover the surface of the
ceramic burner 3 uniformly with La
0.7Sr
0.3MnO
3. Because particles of La
0.7Sr
0.3MnO
3 entering the surface pores of the ceramic burner 3 were baked, the electrically conductive
layer 7 and the ceramic burner 3 were firmly bonded to each other. The electrically
conductive layer 7 contained the borosilicate glass in 4 weight % of the total amount
thereof. As a result, the particles of La
0.7Sr
0.3MnO
3 were bonded to each other or to the ceramic burner 3 by the binder of borosilicate
glass, bonding the electrically conductive layer 7 and the ceramic burner 3 further
firmly.
[0072] Five slurries containing La
0.7Sr
0.3MnO
3 were prepared in the same manner as described above except that the borosilicate
glass powder was added in different amounts. Specifically, the borosilicate glass
powder was added in 0 weight %, 2 weight %, 4 weight %, 10 weight %, and 20 weight
% of the total amount of electrically conductive layers 7 to be formed from the slurries.
[0073] The produced slurries were then sprayed onto the surfaces of ceramic plates by a
commercially available atomizer, producing films on the surfaces of the ceramic plates.
The films were then dried at 110°C for 2 hours in a drier, and thereafter baked at
880 to 1100°C for 1 to 3 hours in an electric furnace. As a result, ceramic burners
3 having electrically conductive layers 7 having a thickness of 120 pm and containing
no borosilicate glass and 2 weight %, 4 weight %, 10 weight %, and 20 weight % of
borosilicate glass with respect to the total amount of the electrically conductive
layers 7 were produced.
[0074] In order to check ranges of baking temperatures in which the La
0.7Sr
0.3MnO
3 powder bonded to the ceramic burner 3 by baking acts as the electrically conductive
layer 7, minimum baking temperatures T
1 for preventing the formed electrically conductive layer 7 from being peeled off and
temperatures T
2 at which the resistance of the electrically conductive layer 7 is infinitely large
were measured. These measured temperatures T
1, T
2 and ranges d of the baking temperatures (d = T
2 - T
1) are shown in Table 1 below.
[0075] Changes in the resistance of the electrically conductive layers 7 which contained
0 weight %, 2 weight %, 4 weight %, 10 weight %, and 20 weight % of the total amount
of electrically conductive layers 7, with respect to the baking temperatures are shown
in FIG. 8.
Table 1
Added amount (wt %) |
T1 |
T2 |
d |
0 |
1060 |
1100 |
40 |
2 |
880 |
1000 |
120 |
4 |
880 |
990 |
110 |
10 |
880 |
970 |
90 |
20 |
880 |
920 |
40 |
[0076] As can be seen from Table 1 and FIG. 8, adding the borosilicate glass is effective
to lower the minimum baking temperature at which the La
0.7Sr
0.3MnO
3 powder can be baked and increase the range of baking temperatures at which the baked
La
0.7Sr
0.3MnO
3 powder acts as the electrically conductive layer 7. Therefore, it is made easy to
establish a desired baking temperature.
[0077] Insofar as the content of the borosilicate glass is in the range from 1 to 20 weight
% of the total amount of the electrically conductive layer 7, the resistance of the
electrically conductive layer 7 can be controlled by appropriately establishing a
desired baking temperature. If the content of the borosilicate glass exceeded 20 weight
% of the total amount of the electrically conductive layer 7, then the resistance
of the electrically conductive layer 7 would become excessive regardless of the baking
temperature.
[0078] In Inventive Example 2, borosilicate glass was used as the inorganic binder. However,
soda lime glass may also be used as the inorganic binder to obtain the same advantages
as described above.
[Inventive Example 3]
[0079] In Inventive Example 3, La
0.7Sr
0.3FeO
3 was used as the electrically conductive perovskite-type metal oxide.
[0080] A ceramic burner 3 having an electrically conductive layer 7 was manufactured in
exactly the same manner as with Inventive Example 1 except that an Fe
2O
3 powder was used instead of the Mn
2O
3 powder in Inventive Example 1.
[0081] The ceramic burner 3 having the electrically conductive layer 7 with La
0.7Sr
0.3FeO
3 according to Inventive Example 3 was installed in the combustion device 1 shown in
FIG. 1. Flame currents sufficiently large to detect an ignition between the electrically
conductive layer 7 and the flame rod 8 were obtained as with the ceramic burner 3
having the electrically conductive layer 7 with La
0.7Sr
0.3MnO
3 according to Inventive Example 1.
[Inventive Example 4]
[0082] In Inventive Example 4, La
0.5Sr
0.5CoO
3 was used as the electrically conductive perovskite-type metal oxide.
[0083] A ceramic burner 3 having an electrically conductive layer 7 was manufactured in
exactly the same manner as with Inventive Example 1 except that a powder of La
2O
3, a powder of SrCO
3, and a powder of Co
3O
4 were mixed at a molar ratio of 0.5 : 0.5 : 1, and the powder was baked at a temperature
of 1200°C after the preliminary baking.
[0084] The ceramic burner 3 having the electrically conductive layer 7 with La
0.5Sr
0.5CoO
3 according to Inventive Example 4 was installed in the combustion device 1 shown in
FIG. 1. Flame currents sufficiently large to detect an ignition between the electrically
conductive layer 7 and the flame rod 8 were obtained as with the ceramic burner 3
having the electrically conductive layer 7 with La
0.7Sr
0.3MnO
3 according to Inventive Example 1.
[Inventive Example 5]
[0085] In Inventive Example 5, La
0.5Ca
0.5CrO
3 was used as the electrically conductive perovskite-type metal oxide.
[0086] A ceramic burner 3 having an electrically conductive layer 7 was manufactured in
exactly the same manner as with Inventive Example 1 except that a powder of La
2O
3, a powder of CaCO
3, and a powder of Cr
2O
3 were mixed at a molar ratio of 0.5 : 0.5 : 1, and the powder was baked at a temperature
of 1500°C after the preliminary baking.
[0087] The ceramic burner 3 having the electrically conductive layer 7 with La
0.5Ca
0.5CrO
3 according to Inventive Example 5 was installed in the combustion device 1 shown in
FIG. 1. Flame currents sufficiently large to detect an ignition between the electrically
conductive layer 7 and the flame rod 8 were obtained as with the ceramic burner 3
having the electrically conductive layer 7 with La
0.7Sr
0.3MnO
3 according to Inventive Example 1.
[Inventive Example 6]
[0088] In Inventive Example 6, La
0.6Sr
0.4CrO
3 was used as the electrically conductive perovskite-type metal oxide.
[0089] A ceramic burner 3 having an electrically conductive layer 7 was manufactured in
exactly the same manner as with Inventive Example 1 except that a powder of La
2O
3, a powder of SrCO
3, and a powder of Cr
2O
3 were mixed at a molar ratio of 0.6 : 0.4 : 1, and the powder was baked at a temperature
of 1500°C after the preliminary baking.
[0090] The ceramic burner 3 having the electrically conductive layer 7 with La
0.6Sr
0.4CrO
3 according to Inventive Example 6 was installed in the combustion device 1 shown in
FIG. 1. Flame currents sufficiently large to detect an ignition between the electrically
conductive layer 7 and the flame rod 8 were obtained as with the ceramic burner 3
having the electrically conductive layer 7 with La
0.7Sr
0.3MnO
3 according to Inventive Example 1.
[Inventive Example 7]
[0091] In Inventive Example 7, La
0.2Ca
0.8MnO
3 was used as the electrically conductive perovskite-type metal oxide.
[0092] A ceramic burner 3 having an electrically conductive layer 7 was manufactured in
exactly the same manner as with Inventive Example 1 except that a powder of La
2O
3, a powder of CaCO
3, and a powder of Mn
2O
3 were mixed at a molar ratio of 0.8 : 0.2 : 1.
[0093] The ceramic burner 3 having the electrically conductive layer 7 with La
0.2Ca
0.8 MnO
3 according to Inventive Example 7 was installed in the combustion device 1 shown in
FIG. 1. Flame currents sufficiently large to detect an ignition between the electrically
conductive layer 7 and the flame rod 8 were obtained as with the ceramic burner 3
having the electrically conductive layer 7 with La
0.7Sr
0.3MnO
3 according to Inventive Example 1.
[Inventive Example 8]
[0094] In Inventive Example 8, Gd
0.8Sr
0.2Co
0.9Mn
0.1O
3 was used as the electrically conductive perovskite-type metal oxide.
[0095] A ceramic burner 3 having an electrically conductive layer 7 was manufactured in
exactly the same manner as with Inventive Example 1 except that a powder of Gd
2O
3, a powder of SrCO
3, a powder of Co
3O
4, and a powder of Mn
2O
3 were mixed at a molar ratio of 0.6 : 0.4 : 1, and the powder was baked at a temperature
of 1500°C after the preliminary baking.
[0096] The ceramic burner 3 having the electrically conductive layer 7 with Gd
0.8Sr
0.2Co
0.9Mn
0.1O
3 according to Inventive Example 8 was installed in the combustion device 1 shown in
FIG. 1. Flame currents sufficiently large to detect an ignition between the electrically
conductive layer 7 and the flame rod 8 were obtained as with the ceramic burner 3
having the electrically conductive layer 7 with La
0.7Sr
0.3MnO
3 according to Inventive Example 1.
[0097] Although certain preferred embodiments of the present invention has been shown and
described in detail, it should be understood that various changes and modifications
may be made therein without departing from the scope of the appended claims.