[TECHNICAL FIELD]
[0001] The present invention relates to a metal base plate material for a heat exchange
plate.
[BACKGROUND ART]
[0002] Plate-type heat exchangers utilizing condensation heat transfer of working media
are known. Heat exchange plates to be built into the plate-type heat exchangers are
usually formed into complex shapes such as a herringbone shape and the like to improve
heat exchange efficiency and/or mechanical durability. In general, such heat exchange
plates are manufactured by press forming metal base plate materials.
[0003] To further improve the heat exchange efficiency of a heat exchange plate, a method
in which a plurality of minute ridges is provided on a surface of a metal base plate
material before press forming has been proposed (Patent Document 1). In Patent Document
1, two kinds of ridges are symmetrically formed on a surface of a metal flat plate
material before press forming in such a way as to be angled in a V-shape, and a gap
is provided between these two kinds of ridges. This enables agitation of a vapor of
a working medium, thereby accelerating condensation of the working medium, and enables
a condensate of the working medium to be efficiently discharged.
[0004] Since the two kinds of ridges provided on the surface of the base plate material
in Patent Document 1 form the symmetrical V-shape with the gap between the two kinds
of ridges, the condensate flowing down on the surface of the base plate material is
guided by the two kinds of ridges to be concentrated on a space between the ridges,
and the flow slows down when passing the gap between ends on the downstream side of
the ridges. Hence, a new approach needs to be devised to properly disperse the condensate
on the plate material surface and discharge the condensate more efficiently.
[PRIOR ART DOCUMENTS]
[PATENT DOCUMENTS]
[0005] Patent Document 1: Japanese Unexamined Patent Application, Publication No.
2015-161449
[SUMMARY OF THE INVENTION]
[PROBLEMS TO BE SOLVED BY THE INVENTION]
[0006] The present invention has been made in view of the above-described circumstances,
and an object of the present invention is to provide a metal base plate material for
a heat exchange plate which can properly disperse a condensate of a working medium
and efficiently discharge the condensate.
[MEANS FOR SOLVING THE PROBLEMS]
[0007] An aspect of the invention made to solve the above problems is a metal base plate
material for a heat exchange plate to be built into a plate-type heat exchanger, wherein
at least one surface is provided with a plurality of strip-shaped first regions and
a plurality of strip-shaped second regions, which are provided alternately and in
parallel; the strip-shaped first regions each have a plurality of first ridges arranged
substantially parallel to each other and at substantially equal intervals such that
an angle of intersection with a longitudinal direction is greater than or equal to
10° and less than or equal to 25°; the strip-shaped second regions each have a plurality
of second ridges arranged substantially parallel to each other and at substantially
equal intervals and angled to face the plurality of the first ridges in a crosswise
direction; the first regions are separated from the second regions adjacent thereto
by gap regions therebetween, respectively, at substantially equal intervals; and when
one orientation of longitudinal directions of the first regions and the second regions
is defined as a downstream direction, first ends on a downstream side of the plurality
of the first ridges and second ends on a downstream side of the plurality of the second
ridges are positioned differently from each other in the longitudinal directions.
[0008] Since the metal base plate material has the gap regions between the first regions
and the second regions and ends (the first ends and the second ends) of two kinds
of ridges (the first ridges and the second ridges) are arranged to be positioned differently
from each other in the longitudinal directions of the first regions and the second
regions, concentration of a condensate on a space between the ends of the two kinds
of ridges can be reduced and the condensate can be properly dispersed. Furthermore,
since the two kinds of ridges of the metal base plate material, which are inclined
in opposite directions from each other with respect to the longitudinal directions,
are arranged such that the angles of intersection with the longitudinal directions
of the first regions and the second regions are greater than or equal to 10° and less
than or equal to 25°, slowdown of a downward flow of the condensate can be curbed,
enabling efficient discharge of the condensate.
[0009] It is preferred that an average distance between the plurality of the first ridges
is greater than or equal to 0.1 mm and less than or equal to 1.0 mm, an average distance
between the plurality of the second ridges is greater than or equal to 0.1 mm and
less than or equal to 1.0 mm, and an average distance between the first regions and
the second regions is greater than or equal to 0.2 mm and less than or equal to 4.0
mm. In the metal base plate material, since the average distance between the first
ridges, the average distance between the second ridges, and the average distance between
the first regions and the second regions are properly adjusted in this manner, the
condensate can be efficiently discharged.
[0010] An amount of positional difference longitudinally between the first ends and the
second ends is preferably greater than or equal to 0.1 mm and less than or equal to
5.8 mm. In the metal base plate material, since the amount of positional difference
longitudinally between the first ends and the second ends is properly adjusted in
this manner, the condensate can be properly dispersed.
[0011] An angle of intersection of the second ridges with the longitudinal direction of
the second regions is preferably equal to an absolute value of the angle of intersection
of the first ridges. This is because amounts of downward flow of the condensate in
the first regions and the second regions are effectively balanced.
[EFFECTS OF THE INVENTION]
[0012] The metal base plate material for a heat exchange plate of the present invention
can properly disperse a condensate of a working medium and efficiently discharge the
condensate.
[BRIEF DESCRIPTION OF THE DRAWINGS]
[0013]
FIG. 1 is a schematic plan view showing a part of a surface of a metal base plate
material of an embodiment of the present invention.
FIG. 2 is a schematic perspective cross-sectional view showing a part of a cross-section
taken along an A-A line around the surface of the metal base plate material in FIG.
1.
[DESCRIPTION OF EMBODIMENTS]
[0014] Embodiments of the metal base plate material for a heat exchange plate according
to the present invention will be described in detail below with reference to the drawings.
Metal base plate material
[0015] A metal base plate material 1 in FIG. 1 is a metal base plate material for a heat
exchange plate to be built into a plate-type heat exchanger. A material for the metal
base plate material 1 is not particularly limited, but for example, titanium is used.
The metal base plate material 1 is a flat plate material serving as a material for
manufacturing a heat exchange plate, and when it is to be built into a plate-type
heat exchanger, it is formed into the heat exchange plate by press forming. As the
metal base plate material 1, a rectangular plate with long sides of 1,200 mm, short
sides of 800 mm, and an average thickness of greater than or equal to 0.5 mm and less
than or equal to 1.0 mm is used, although there is no particular limitation.
[0016] A plurality of strip-shaped first regions 2 and a plurality of strip-shaped second
regions 3 are provided alternately and in parallel on a surface of the metal base
plate material 1. It is to be noted that the surface having the first regions 2 and
the second regions 3 is at least one surface of the metal base plate material 1, and
may be one side of the metal base plate material 1 or both sides of the metal base
plate material 1.
First Regions
[0017] The first regions 2 are strip-shaped regions provided on the surface of the metal
base plate material 1. The plurality of the first regions 2 is provided such that
the first regions 2 are substantially parallel to each other. Each of the first regions
2 has a plurality of first ridges 21 arranged substantially parallel to each other
and at substantially equal intervals such that the angle of intersection with a longitudinal
direction is θ
1.
[0018] The lower limit of an average width Z
1 in a crosswise direction of the first regions 2 is preferably 1 mm, more preferably
2 mm, and still more preferably 3 mm. Meanwhile, the upper limit of the average width
Z
1 is preferably 20 mm, more preferably 18 mm, and still more preferably 16 mm. If the
average width Z
1 is less than the lower limit, agitation of a vapor of a working medium may be insufficient,
resulting in failure to accelerate condensation of the working medium. Conversely,
if the average width Z
1 is greater than the upper limit, a condensate may be retained in the first regions
2, resulting in inefficient discharge of the condensate. It is to be noted that "average
width" refers to an average value of widths at five arbitrarily selected points in
one object.
(First ridges)
[0019] In the first regions 2, the plurality of the first ridges 21 is provided such that
the first ridges 21 are substantially parallel to each other and at substantially
equal intervals. The first ridges 21 are long, thin, rod-shaped ridges in plan view,
and each has such a length that both ends reach both side portions of the first region
2, which is strip-shaped. It is to be noted that, although the first ridges 21 in
FIG. 1 are substantially rectangular, the first ridges 21 only need to be formed so
that two long sides are substantially parallel to each other in plan view; both ends
may be curved, for example. Further, a method for forming ridges on the surface of
the metal base plate material 1 is not particularly limited, but for example, a method
in which protrusions/recessions are transferred during rolling, and the like are employed.
[0020] The angle of intersection θ
1 of the first ridges 21 with the longitudinal direction of the first regions 2 is
set to an acute angle to curb slowdown of a downward flow of the condensate. The lower
limit of the angle of intersection θ
1 is preferably 10°, more preferably 12°, and still more preferably 13°. Meanwhile,
the upper limit of the angle of intersection θ
1 is preferably 25°, more preferably 22°, and still more preferably 20°. If the angle
of intersection θ
1 is less than the lower limit, the condensate may fail to be properly guided along
sides of the first ridges 21. Conversely, if the angle of intersection θ
1 is greater than the upper limit, the condensate may be retained in the first regions
2 and inefficiently discharged. It is to be noted that "angle of intersection" refers
to an acute angle of two angles formed when two straight lines cross each other.
[0021] The lower limit of an average width a
1 in a crosswise direction of the first ridges 21 is preferably 0.10 mm, more preferably
0.11 mm, and still more preferably 0.12 mm. Meanwhile, the upper limit of the average
width a
1 is preferably 1.0 mm, more preferably 0.8 mm, and still more preferably 0.6 mm. If
the average width a
1 is less than the lower limit, strength of the first ridges 21 may be insufficient.
Conversely, if the average width a
1 is greater than the upper limit, the condensate may flow down on top surfaces of
the first ridges 21, resulting in failure to properly guide the condensate along the
sides of the first ridges 21.
[0022] The lower limit of an average distance b
1 between two of the first ridges 21 is preferably 0.1 mm, more preferably 0.2 mm,
and still more preferably 0.3 mm. Meanwhile, the upper limit of the average distance
b
1 is preferably 1.0 mm, more preferably 0.9 mm, and still more preferably 0.8 mm. If
the average distance b
1 is less than the lower limit, the condensate may spill over the top surfaces of the
first ridges 21, resulting in failure to properly guide the condensate along the sides
of the first ridges 21. Conversely, if the average distance b
1 is greater than the upper limit, the condensate may be retained between the first
ridges 21 and inefficiently discharged. It is to be noted that "average distance"
is an average of distances in the crosswise direction of the ridges, and refers to
an average value of five arbitrarily selected five between two ridges.
[0023] The lower limit of an average height h of the first ridges 21 with respect to the
surface of the metal base plate material 1 is preferably 0.02 mm, more preferably
0.03 mm, and still more preferably 0.04 mm. Meanwhile, the upper limit of the average
height h is preferably 0.10 mm, more preferably 0.09 mm, and still more preferably
0.08 mm. If the average height h is less than the lower limit, agitation of the vapor
of the working medium may be insufficient, resulting in failure to accelerate condensation
of the working medium. Conversely, if the average height h is greater than the upper
limit, processing cost may increase.
Second regions
[0024] Like the first regions 2, the second regions 3 are strip-shaped regions provided
on the surface of the metal base plate material 1. The plurality of the second regions
3 is provided such that the second regions 3 are substantially parallel to each other.
Each of the second regions 3 has a plurality of second ridges 31 arranged substantially
parallel to each other and at substantially equal intervals, and at an angle θ
2 to face the plurality of the first ridges 21 in a crosswise direction.
[0025] The lower limit of an average width Z
2 in the crosswise direction of the second regions 3 is preferably 1 mm, more preferably
2 mm, and still more preferably 3 mm. Meanwhile, the upper limit of the average width
Z
2 is preferably 20 mm, more preferably 18 mm, and still more preferably 16 mm. If the
average width Z
2 is less than the lower limit, agitation of the vapor of the working medium may be
insufficient, resulting in failure to accelerate condensation of the working medium.
Conversely, if the average width Z
2 is greater than the upper limit, the condensate may be retained in the second regions
3, resulting in inefficient discharge of the condensate.
(Second ridges)
[0026] In the second regions 3, the plurality of the second ridges 31 is provided such that
the second ridges 31 are substantially parallel to each other and at substantially
equal intervals. Similarly to the first ridges 21, the second ridges 31 are long,
thin, rod-shaped ridges in plan view, and each has such a length that both ends reach
both side portions of the second region 3, which is strip-shaped. Although in FIG.
1, a shape of the second ridges 31 is a substantially rectangular shape similar to
that of the first ridges 21, the second ridges 31 only need to be formed so that two
long sides are substantially parallel to each other in plan view, similarly to the
first ridges 21. In addition, in light of a balance of amounts of downward flow of
the condensate, it is preferable that the shape of the second ridges 31 are similar
to the first ridges 21 in plan view and that a height of the second ridges 31 with
respect to the surface of the metal base plate material 1 is equal to the height h
of the first ridges 21 with respect to the surface of the metal base plate material
1 as shown in FIG. 2.
[0027] The second ridges 31 are angled to face the first ridges 21 in the crosswise direction;
therefore, when one orientation of the longitudinal directions of the first regions
2 and the second regions 3 is defined as a downstream direction, first ends 21a on
a downstream side of the plurality of the first ridges 21 and second ends 31a on a
downstream side of the plurality of the second ridges 31 are adjacent to each other
with gap regions 4 interposed therebetween.
[0028] An angle of intersection θ
2 of the second ridges 31 with the longitudinal direction of the second regions 3 is
set to an acute angle to curb the slowdown of the downward flow of the condensate.
The lower limit of the angle of intersection θ
2 is preferably 10°, more preferably 12°, and still more preferably 13°. Meanwhile,
the upper limit of the angle of intersection θ
2 is preferably 25°, more preferably 22°, and still more preferably 20°. If the angle
of intersection θ
2 is less than the lower limit, the condensate may fail to be properly guided along
sides of the second ridges 31. Conversely, if the angle of intersection θ
2 is greater than the upper limit, the condensate may be retained in the second regions
3 and inefficiently discharged. It is to be noted that in light of the balance of
the amounts of downward flow of the condensate, an absolute value of the angle of
intersection θ
1 is preferably equal to that of the angle of intersection θ
2.
[0029] The lower limit of an average width a
2 in the crosswise direction of the second ridges 31 is preferably 0.10 mm, more preferably
0.11 mm, and still more preferably 0.12 mm. Meanwhile, the upper limit of the average
width a
2 is preferably 1.0 mm, more preferably 0.8 mm, and still more preferably 0.6 mm. If
the average width a
2 is less than the lower limit, the strength of the second ridges 31 may be insufficient.
Conversely, if the average width a
2 is greater than the upper limit, the condensate may flow down on top surfaces of
the second ridges 31, resulting in failure to properly guide the condensate along
the sides of the second ridges 31. It is to be noted that in light of the balance
of the amounts of downward flow of the condensate, the average width a
1 is preferably equal to the average width a
2.
[0030] The lower limit of an average distance b
2 between two of the second ridges 31 is preferably 0.1 mm, more preferably 0.2 mm,
and still more preferably 0.3 mm. Meanwhile, the upper limit of the average distance
b
2 is preferably 1.0 mm, more preferably 0.9 mm, and still more preferably 0.8 mm. If
the average distance b
2 is less than the lower limit, the condensate may spill over the top surfaces of the
second ridges 31, resulting in failure to properly guide the condensate along the
sides of the second ridges 31. Conversely, if the average distance b
2 is greater than the upper limit, the condensate may be retained between the second
ridges 31 and inefficiently discharged. It is to be noted that in light of the balance
of the amounts of downward flow of the condensate, the average distance b
1 is preferably equal to the average distance b
2.
[0031] When one orientation of the longitudinal directions of the first regions 2 and the
second regions 3 is defined as the downstream direction, the first ends 21a on the
downstream side of the plurality of the first ridges 21 and the second ends 31a on
the downstream side of the plurality of the second ridges 31 are positioned differently
from each other in the longitudinal directions as shown in FIG. 1. An amount of positional
difference longitudinally between the first ends 21a and the second ends 31a includes
an amount of positional difference W
1 in a case where the first end 21a is on the downstream side with respect to the second
end 31a and an amount of positional difference W
2 in a case where the first end 21a is on the upstream side with respect to the second
end 31a. In light of the balance of the amounts of downward flow of the condensate,
the amount of positional difference W
1 is preferably equal to the amount of positional difference W
2; however, there is no particular limitation, and the amount of positional difference
W
1 may be different from the amount of positional difference W
2. It is to be noted that "an end on the downstream side of ridges" refers to a downstream
terminal on an upstream long side of the ridge.
[0032] The lower limit of the amount of positional difference W
1 longitudinally between the first end 21a and the second end 31a is preferably 0.1
mm, more preferably 0.6 mm, and still more preferably 1.0 mm. Meanwhile, the upper
limit of the amount of positional difference W1 is preferably 5.8 mm, more preferably
4.5 mm, and still more preferably 3.5 mm. If the amount of positional difference W
1 is less than the lower limit, concentration of the condensate on spaces between the
first ends 21a and the second ends 31a may fail to be reduced and the condensate may
be improperly dispersed. Conversely, if the amount of positional difference W
1 exceeds the upper limit, the condensate may fail to be properly guided along the
first ridges 21 and the second ridges 31. It is to be noted that the upper limit and
the lower limit of the amount of positional difference W
2 is similar to that of W
1.
Gap Regions
[0033] The first regions 2 are separated from the second regions 3 adjacent thereto by the
gap regions 4 therebetween, respectively, at substantially equal intervals. The gap
regions 4 are strip-shaped regions parallel to the longitudinal directions of the
first regions 2 and the second regions 3, and the first regions 2 and the second regions
3 are arranged parallel to each other with the gap regions 4 interposed therebetween.
Protrusions/recessions such as ridges and the like are not formed in the gap regions
4, and most of the condensate flows down the gap regions 4 in a zigzag manner.
[0034] The lower limit of an average distance X between the first regions 2 and the second
regions 3 is preferably 0.2 mm, more preferably 0.3 mm, and still more preferably
0.4 mm. Meanwhile, the upper limit of the average distance X is preferably 4.0 mm,
more preferably 3.5 mm, and still more preferably 3.0 mm. If the average distance
X is less than the lower limit, the condensate may be inefficiently discharged. Conversely,
if the average distance X is greater than the upper limit, the condensate may fail
to be properly guided along the first ridges 21 and the second ridges 31.
(Advantages)
[0035] Since the metal base plate material 1 has the gap regions 4 between the first regions
2 and the second regions 3 and ends (the first ends 21a and the second ends 31a) of
two kinds of ridges (the first ridges 21 and the second ridges 31) are arranged to
be positioned differently from each other in the longitudinal directions of the first
regions 2 and the second regions 3, the concentration of the condensate on the spaces
between the ends of the two kinds of ridges can be reduced, and the condensate can
be properly dispersed. Moreover, in the metal base plate material 1, since the two
kinds of ridges are arranged such that the angles of intersection with the longitudinal
directions of the first regions 2 and the second regions 3 is greater than or equal
to 10° and less than or equal to 25°, the slowdown of the downward flow of the condensate
can be curbed, enabling efficient discharge of the condensate.
[0036] Furthermore, in the metal base plate material 1, the average distance b
1 between the first ridges 21, the average distance b
2 between the second ridges 31, and the average distance X between the first regions
2 and the second regions 3 are properly adjusted, enabling efficient discharge of
the condensate.
[0037] Furthermore, in the metal base plate material 1, the amount of positional difference
W
1 and W
2 longitudinally between the first ends 21a and the second ends 31a is properly adjusted,
enabling the condensate to be properly dispersed.
[OTHER EMBODIMENTS]
[0038] The metal base plate material for a heat exchange plate of the present invention
is not limited to the above embodiment.
[0039] In the above embodiment, the metal base plate material 1 having the gap regions 4
between the first regions 2 and the second regions 3 has been described. However,
it is only necessary that the gap regions 4 are provided between the first ends 21a
and the second ends 31a; it is not necessary that the gap regions 4 be provided between
ends on the upstream side of the first ridges 21 and ends on the upstream side of
the second ridges 31.
EXAMPLES
[0040] Hereinafter, the present invention will be described in detail by way of Examples;
however, the Examples are not construed as limiting the present invention.
[0041] As a test of condensation heat transfer performance, overall heat transfer coefficients
were evaluated by using metal base plate materials No. 1 to No. 4. Hydrofluorocarbon
(R134a) was used as a working medium to be in contact with surfaces of the metal base
plate materials, and cold water was used as a refrigerant to be in contact with rear
surfaces of the metal base plate materials to condense the working medium. The working
medium, whose inflow temperature was set to 30°C with a heater, was made to flow onto
the surfaces of the metal base plate materials at a pressure of 0.68 MPa. Cold water
was brought to an inflow temperature of 20°C and made to flow onto the rear surfaces
of the metal base plate materials at a flow rate of 3 L/min. Further, a heat transfer
area of the metal base plate materials was 17,500 mm
2, and a depth W was 2 mm. The overall heat transfer coefficients were calculated using
the temperature at which the cold water flowed onto the rear surfaces of the metal
base plate materials, the temperature at which the cold water flowed out from the
rear surfaces of the metal base plate materials, the heat transfer area of the metal
base plate materials, and the difference between the inflow temperature of the working
medium and the inflow temperature of the cold water.
[0042] The surfaces of the metal base plate materials, which were to be in contact with
the working medium, are as follows. It is to be noted that the metal base plate materials
No. 1 and No. 2 are the metal base plate material 1 of the above embodiment, and the
metal base plate material No. 3 is the metal base plate material 1 of the above embodiment
wherein the angle of intersection θ of the ridges with the longitudinal directions
of regions in which the ridges are provided, and the amount of positional difference
W longitudinally between the ends of the ridges are outside ranges of the embodiment.
Further, the metal base plate material No. 4 is a flat plate material wherein a surface
has no ridge. It is to be noted that the first ridges and the second ridges of the
metal base plate materials No. 1 to No. 3 are identical in shape.
Metal base plate material No. 1
[0043] Height h of the ridges: 0.05 mm; width a in the crosswise directions of the ridges:
0.125 mm; distance b between the ridges: 0.6 mm; angle of intersection θ of the ridges
with the longitudinal directions of the regions in which the ridges are provided:
15°; distance X between the regions in which the ridges are provided: 0.98 mm; width
Z in the crosswise directions of the regions in which the ridges are provided: 4.88
mm; amount of positional difference W longitudinally between the ends of the ridges:
1.4 mm
Metal base plate material No. 2
[0044] Height h of the ridges: 0.05 mm; width a in the crosswise directions of the ridges:
0.125 mm; distance b between the ridges: 0.6 mm; angle of intersection θ of the ridges
with the longitudinal directions of the regions in which the ridges are provided:
15°; distance X between the regions in which the ridges are provided: 0.49 mm; width
Z in the crosswise directions of the regions in which the ridges are provided: 2.44
mm; amount of positional difference W longitudinally between the ends of the ridges:
1.4 mm
Metal base plate material No. 3
[0045] Height h of the ridges: 0.05 mm; width a in the crosswise directions of the ridges:
0.125 mm; distance b between the ridges: 0.6 mm; angle of intersection θ of the ridges
with the longitudinal directions of the regions in which the ridges are provided:
45°; distance X between the regions in which the ridges are provided: 4 mm; width
Z in the crosswise directions of the regions in which the ridges are provided: 20
mm; amount of positional difference W longitudinally between the ends of the ridges:
0 mm
[0046] The test results are as follows: the overall heat transfer coefficient of the metal
base plate material No. 1 was 3,592 W/m
2K, the overall heat transfer coefficient of the metal base plate material No. 2 was
3,436 W/m
2K, the overall heat transfer coefficient of the metal base plate material No. 3 was
2,518 W/m
2K, and the overall heat transfer coefficient of the metal base plate material No.
4 was 2,305 W/m
2K, confirming that the metal base plate materials No. 1 and No. 2 showed high overall
heat transfer coefficients. Thus, it can be concluded that the overall heat transfer
coefficient of a metal base plate material is improved by properly arranging ridges
on a surface of the metal base plate material as in the metal base plate materials
No. 1 and No. 2.
[0047] The metal base plate material for a heat exchange plate of the present invention
can properly disperse a condensate of a working medium and efficiently discharge the
condensate.
[Explanation of the Reference Symbols]
[0048]
- 1
- Metal base plate material
- 2
- First region
- 3
- Second region
- 4
- Gap region
- 21
- First ridge
- 21a
- First end
- 31
- Second ridge
- 31a
- Second end