U.S. patent number 3,706,303 [Application Number 05/012,000] was granted by the patent office on 1972-12-19 for compact heat exchanger with high intensity burner.
This patent grant is currently assigned to Raytheon Company. Invention is credited to William H. Hapgood.
United States Patent |
3,706,303 |
Hapgood |
December 19, 1972 |
COMPACT HEAT EXCHANGER WITH HIGH INTENSITY BURNER
Abstract
A high intensity burner for burning a carbonaceous fuel in an
oxygen containing atmosphere has one or more ports through which
the fuel emerges and adjacent which complete combustion of the fuel
occurs within a limited combustion region at a temperature above
the dissociation temperature of CO.sub.2. A heat exchanger, which
is maintained at a temperature below the recombination temperature
of CO and O.sub.2, is located outside the limits of said combustion
region but sufficiently close to the burner ports so that, at the
normal operating velocity of the burned gases these gases would
reach the heat exchanger before the temperature of the gases had
dropped below the dissociation temperature and into the
recombination temperature range, except for the fact that a screen
is located between the limits of the combustion region and the heat
exchanger, and is heated by the gases, thereby extracting heat from
the gases, to a temperature at which it radiates energy, thus
reducing the temperature of such gases into the recombination
temperature range before they reach the heat exchanger.
Inventors: |
Hapgood; William H. (Brookline,
MA) |
Assignee: |
Raytheon Company (Lexington,
MA)
|
Family
ID: |
21752908 |
Appl.
No.: |
05/012,000 |
Filed: |
February 17, 1970 |
Current U.S.
Class: |
126/116R;
126/92R; 126/400; 122/356; 126/109; 431/329 |
Current CPC
Class: |
F23M
20/005 (20150115); F23M 9/06 (20130101) |
Current International
Class: |
F23M
13/00 (20060101); F23M 9/06 (20060101); F23M
9/00 (20060101); F24c 003/04 () |
Field of
Search: |
;126/116,110,11B,92,92B,91,109 ;122/356,367 ;431/10,328,329 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Myhre; Charles J.
Claims
What is claimed is:
1. In combination:
a burner adapted to burn a carbonaceous fuel, said burner having a
characteristic combustion region adjacent said burner, and a heat
exchanger adjacent said burner, said heat exchanger being adapted
to operate at a temperature below the recombination temperature of
carbon monoxide and oxygen, wherein the improvement comprises:
means intermediate said characteristic combustion region and said
heat exchanger for extracting heat energy from the combustion
products of said fuel to reduce the temperature of said products to
the recombination temperature of carbon monoxide and oxygen,
whereby, during operation of said combination, substantially all
carbon monoxide and oxygen in said products recombine to form
carbon dioxide before reaching said heat exchanger, said means
comprising a refractory perforate member interposed in the path of
the flow of said products from said combustion region to said heat
exchanger.
2. The combination of claim 1 in which the heat exchanger structure
presents heat conductive members adjacent said refractory member
and said refractory member is substantially insulated against any
high heat conductivity paths between it and all adjacent heat
conductive members, whereby said refractory member during operation
is heated by said products to a temperature at which it loses heat
substantially solely by radiation.
3. The combination of claim 1 in which said burner, said refractory
member and said heat exchanger are cylindrical in form and
concentrically arranged with respect to each other.
4. The combination of claim 1 in which said refractory member is
comprised of a refractory metal alloy.
5. The combination of claim 2 in which said refractory member is
supported by one or more heat insulating, sound absorbing members
supported by the adjacent heat exchange structure.
6. The combination of claim 5 in which said heat insulating members
are comprised of asbestos.
Description
BACKGROUND OF THE INVENTION
1. Field of the Invention
Compact heat exchangers with high intensity burners and with low CO
output.
2. Description of the Prior Art
A demand has arisen for very compact heat exchanger devices which
operate in conjunction with high intensity burners so as to provide
the capability of handling large amounts of heat energy within
limited spaces. While such high intensity burners can be made to be
very efficient, whereby all of the carbon content of the fuel
normally supplied to such burners is converted into CO.sub.2,
nevertheless, it has been found that if a relatively low
temperature heat exchanger is placed too close to the burner the
combustion products of the device will contain an undesirably high
CO content. If it were attempted to avoid this adverse result by
removing the heat exchanger to a greater distance from the burner,
compactness of the device would be sacrificed.
SUMMARY OF THE INVENTION
In the present invention the defects of the prior art have been
eliminated, without sacrificing the compactness of the structure,
by interposing at a critical location between the burner and the
heat exchanger, a screen made of a refractory material, such as a
refractory metal. The location is selected beyond the point at
which complete combustion of the fuel first occurs and sufficiently
ahead of the surface of the heat exchanger to permit complete
recombination of any dissociated CO.sub.2 to occur before the hot
gases reach such surface. The burner is operated at such high
intensity that at the point at which complete combustion is first
achieved, the temperature of the burned gases exceeds the
dissociation temperature of CO.sub.2. As the hot gases proceed
beyond that point they contact the screen which is heated by a
combination of conduction from the impacting gases and by radiation
from the hot gases in the combustion zone. The temperature of the
screen is such that it radiates substantial quantities of energy
which is absorbed by surrounding structures, thus dropping the
temperature of the screen to below such dissociation but still well
within the temperature range in which recombination of CO and
O.sub.2 occurs. The burned gases are reduced in temperature by the
screen so that they likewise drop into the recombination
temperature range and do not rise above the CO.sub.2 dissociation
temperature during the passage of such gases to the heat exchanger.
Once the gases drop into the recombination temperature range,
recombination of CO and O.sub.2 occurs with extreme rapidity so
that the screen may be placed quite close to the heat exchanger
without sacrificing the complete recombination of these elements.
The heat exchanger itself is maintained at a temperature below said
recombination temperature range. Therefore, if the hot gases were
permitted to reach the heat exchanger while still containing a
substantial amount of CO, the gases would be quenched and the
desired recombination would not occur.
BRIEF DESCRIPTION OF THE DRAWINGS
In the annexed drawings:
FIG. 1 is a vertical sectional view of a heat exchanger structure
incorporating this invention; and
FIG. 2 is a cross-sectional view taken along line 2--2 of FIG.
1.
DETAILED DESCRIPTION OF THE INVENTION
The burner 1 as shown in the drawings is a highly efficient, high
power burner which may be of the type as described and claimed in
the copending application of William H. Hapgood and Donald G.
Protopapas, Ser. No. 2,584 filed Jan. 13, 1970, now abandoned. Such
burner consists of a cylindrical shell 2, provided with a large
number of perforations 3 which serve as ports through which gas to
be burned issues. That gas, which may be a mixture of air and any
carbonaceous combustible material such as natural gas, gasoline,
methane, propane or the like, is supplied to the burner through an
inlet conduit 4. By any suitable system, such as that described in
said copending Hapgood-Protopapas application, the air-gas mixture,
preferably with up to 30 percent excess of air over the
stociometric level, is pumped into the conduit 4. Burners of this
type are capable of delivering large amounts of heat energy, for
example, at a rate in excess of 20,000 BTU per hour for each square
inch of burner surface. At upper levels of operation, the velocity
of the gas-air mixture as it emerges from the parts 3 may be in
excess of 1600 cm. per sec. Throughout the range of operation of a
burner of this type the outer limit of the flame structure of the
burner 1 will typically be one quarter inch to about one half inch
away from the surface of the burner. Whatever type of burner is
used, the outer limit of the flame structure is that at which
combustion of the fuel is first completed. What that distance is,
will depend upon the design of the burner and will be a definite
characteristic of the burner. The volume between the burner and
such characteristic distance will be designated as the
"characteristic combustion region" of the burner in the present
specifications and claims.
The heat generated by the burning of the fuel supplied to burner 1
is transferred to any convenient type of heat exchange structure
such as that designated generally at 5. This consists of a
plurality of tubes 6 arranged in a concentric cylindrical array
around the burner 1. These tubes 6 connect at their upper ends with
a header structure 7 and at their lower end with a header structure
8 provided with inlet and outlet pipes 9 and 10, whereby water to
be heated may be passed up and down in serial fashion through the
tubes 6. In order to increase the effectiveness and efficiency of
the transfer of heat from the hot gases into the water in the tubes
6, the tubes are embedded in a matrix 11 consisting of small
pellets of steel soldered to each other and to the tubes 6 and
filling the space between the tubes. The particular details of the
matrix 11 and of the header structures 7 and 8 form no part of this
invention and will not be described in greater detail herein. A
heat exchange structure of this kind is described in detail and is
claimed in my copending application Ser. No. 10,334, filed Feb. 11,
1970. The rate at which water is supplied through the heat exchange
structure is such that the maximum temperature reached by any part
of the structure will be well below the temperature range within
which CO will spontaneously combine with O.sub.2 to form CO.sub.2.
Such a temperature may be, for example, of the order of several
hundred degrees Farenheit and below about 1000.degree.F. While a
particular type of heat exchanger has been described, it will be
understood that any of the well-known types of heat exchangers
whose normal temperature of operation is below the recombination
temperature range of CO and O.sub.2 may be used.
With a high intensity burner, such as that described above, the
temperature of the gas within the characteristic combustion region
of the burner will reach a value of about 2800.degree.F or greater
which is above the temperature at which CO.sub.2 dissociates into
CO and O.sub.2. Therefore, as the hot gases pass out of the
characteristic combustion region, they will include a substantial
quantity of CO even though during the combustion process all of the
carbon in the gas will have been converted into CO.sub.2 which is
what occurs in a high efficiency, high intensity burner of the type
described above. Heretofore, the only way in which the hot gases
could lose energy before coming into contact with the heat
exchanger, was by radiation. However, the rate at which loss
occured was so slow that, at the normal velocities of the gas in
passing from the characteristic combustion region to the heat
exchanger, the temperature of the hot gas remained above the
recombination temperature of CO and O.sub.2 which is about
2500.degree.F. At that point, the heat exchanger extracted energy
from the hot gases so rapidly that the temperature of these gases
dropped through the recombination range so rapidly that there was
insufficient time for any substantial recombination to occur. This
could be considered a quenching action in which any recombination
tendency was quenched by the comparatively low temperature heat
exchanger.
In accordance with this invention the foregoing quenching action is
eliminated by mounting a perforated or grid-like screen 12 in the
space between the burner and the heat exchanger 5. The screen 12 is
made of coarse mesh of a refracting metal alloy such as that know
as "Kanthal" which is chrome-iron-aluminum-molybdnum alloy
containing about 65 percent iron, 30 percent chromium, 5 percent
aluminum and a trace of molybdenum. Of course, any refractory
material formed into a perforate screen around the burner 1 might
be used. For example, ceramic rods could be used as the material of
the screen 12.
The screen 12 is located just beyond the characteristic combustion
region of the burner 2. Where the depth of that region is about one
half inch, as in the example given above, the screen 12 may be
located about seven eighths inch from the surface of the member 2,
while the inner surface of the heat exchanger 5 might be about
another seven eighths inch beyond the screen. Thus, a convenient
location for the screen 12 is about half way between the outer
surface of the shell 2 and the inner surface of the heat exchanger
5, provided such location is outside of the characteristic
combustion region of the burner.
The combustion products of the burner 1 are forced to pass through
the heat exchanger by having the space between the burner 1 and the
heat exchanger 5 closed off by an upper plate 13 and a lower plate
14. The screen 12 is supported between these plates by means of a
refractory low heat conductivity block 15 secured to the plate 13
and another block 16 of similar material supported on the lower
plate 14. A convenient material for the blocks 15 and 16 is
asbestos, which also functions as a sound absorbing material to
absorb any undesired noises generated by the passage and burning of
the gases through the structure. The block 15 may be supported in
place by a plurality of clips 17 welded to the plate 15. The screen
12 is hung from the block 15 by means of a plurality of hooks 18
extending through the block 15. In this way very little, if any,
heat is conducted from the screen 12 by the supporting structure,
since it is desirable for the screen 12 to be maintained at a
substantially uniform temperature throughout. The lower end of the
screen 12 is stabilized by wires 19 projecting from the bottom of
screen 12 and lightly piercing the upper surface of the block 16.
It may not be necessary to secure the block 16 to the plate 14 but,
if desired, it can be secured in a manner similar to that used for
block 15.
The screen 12 receives some heat by radiation from the hot gases in
the characteristic combustion region, but it is heated principally
by the hot gases which emerge from that region and pass through the
perforations in the screen. As already indicated substantially no
heat is lost from the screen 12 by conduction to any adjacent
members and so it must lose heat by radiation. Therefore, the
temperature of screen 12 rises to a temperature of about
2500.degree.F which is substantially uniform throughout the screen.
This is the temperature at which the amount of heat supplied by hot
gases equals the heat lost from screen 12 by radiation. Thus, it
will be seen that the screen 12 uniformly cools the hot gases by
about 300.degree.F as they pass through the screen. This is
sufficient to drop the temperature of these gases to about
2500.degree.F which is within the recombination temperature range
for CO and O.sub.2. As a result, any CO in the hot gases rapidly
recombines with the O.sub.2 which was released by the previous
dissociation of CO.sub.2 and within a very short distance beyond
the screen 12 all the CO is thus been recombined, so that the hot
gases which reach the heat exchanger 5 are virtually free of
CO.
By virtue of the present invention, very compact, high power
density, highly efficient heat exchanger systems have been made
practicable with no loss in compactness or efficiency and which are
virtually free of any CO in their exhaust gases.
* * * * *