U.S. patent number 3,840,051 [Application Number 05/388,261] was granted by the patent office on 1974-10-08 for straightener.
This patent grant is currently assigned to Mitsubishi Jukogyo Kabushiki Kaisha. Invention is credited to Koichiro Akashi, Kenichi Koga, Hisao Watanabe.
United States Patent |
3,840,051 |
Akashi , et al. |
October 8, 1974 |
STRAIGHTENER
Abstract
A perforated-plate type straightener adapted to be fitted in a
cylindrical pipe across the passage of a fluid flowing through the
pipe, comprising a perforated plate having a plurality of round
holes which are the same in diameter and so provided that the
distances between the adjacent holes are short in the axial center
of the pipe and are gradually longer near the surrounding wall.
Inventors: |
Akashi; Koichiro (Nagaski,
JA), Watanabe; Hisao (Nagaski, JA), Koga;
Kenichi (Nagaski, JA) |
Assignee: |
Mitsubishi Jukogyo Kabushiki
Kaisha (Tokyo, JA)
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Family
ID: |
27280225 |
Appl.
No.: |
05/388,261 |
Filed: |
August 14, 1973 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
Issue Date |
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230403 |
Feb 29, 1972 |
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Foreign Application Priority Data
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Mar 11, 1971 [JA] |
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46-13385 |
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Current U.S.
Class: |
138/37; 428/131;
428/596; 73/861.52; 376/352 |
Current CPC
Class: |
G01F
1/40 (20130101); F15D 1/025 (20130101); F16L
55/02763 (20130101); Y10T 428/12361 (20150115); Y10T
428/24273 (20150115) |
Current International
Class: |
G01F
1/40 (20060101); F16L 55/027 (20060101); F16L
55/02 (20060101); G01F 1/34 (20060101); F15D
1/00 (20060101); F16d 001/00 () |
Field of
Search: |
;138/39,40,44,37,41
;73/198,25L,211 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Ruehl; Charles A.
Attorney, Agent or Firm: Toren and McGeady
Parent Case Text
This is a continuation of application Ser. No. 230,403 filed Feb.
29, 1972, now abandoned.
Claims
What is claimed is:
1. In apparatus for forming a turbulent-flow velocity distribution
within a cylindrical pipe having fluid flowing therethrough, said
apparatus including a perforated plate mounted within said pipe to
extend transversely across the path of fluid flowing through said
pipe, the improvement comprising, in combination:
means defining a plurality of cylindrical flow conduits extending
through said plate in the direction of said fluid flow,
said conduits being of substantially equivalent diameter and
disposed in said plate with the spacing between adjacent conduits
increasing progressively from the inner radial portion of said
plate to the outer radial portion thereof; and
means defining the upstream ends of said conduits with a beveled
configuration extending from a wider diameter to a smaller diameter
taken in the direction of fluid flow;
said conduits extending downstream from said beveled configuration
over the major portion of their lengths with a generally uniform
diameter throughout, said uniform diameter being generally
coincident with said smaller diameter of said beveled
configuration.
2. Apparatus according to claim 1, wherein said perforated plate
comprises a thickness dimension taken in the direction of fluid
flow through said pipe, with the ratio between said thickness
dimension and said uniform diameter being within the range between
1 and 3.
3. Apparatus according to claim 1, wherein said beveled
configuration is in the form of frusto-conical surface.
Description
This invention relates to a straightener for use in the measurement
of the flow rate of a single phase fluid, either gas or liquid,
flowing through a pipe which is cylindrical.
Conventional straightening devices for this purpose are available
in a variety of types, such as shown in FIGS. 1 to 5. Referring to
the figures, the devices consist of a perforated plate 02, grid 03,
wire gauge 04, perforated plate 05 plus a downstream grid 06, or
wire gauge 07 plus a downstream grid 08, fitted in a pipe 01. The
straighten either an upstream channeling or swirling flow or the
both to ensure uniform flow velocity distribution. However, they
fail to bring a trubulent-flow velocity distribution which is
necessary for the measurement with a throttling flowmeter. If a
proper turbulent-flow velocity distribution is to be obtained with
the use of such a straightener, there is no alternative but to
employ an extended straight length and take advantage of the extra
friction of the fluid with the inner wall surface of the pipe.
In an effort to eliminate the foregoing disadvantage, it has been
proposed to install, as shown in FIG. 6, an assembly 09 consisting
of a grid 010 and a perforated plate 011 adjoining to the upstream
face of the grid in a cylindrical pipe, the holes of the perforated
plate 011 being gradually made larger in diameter toward the center
and smaller toward the periphery. As compared with the
straighteners of FIGS. 1 through 5, the device of the construction
described immediately above permits the use of a relatively short
straight pipe portion to obtain the necessary turbulent-flow
velocity distribution. Nevertheless, the device has following
drawbacks.
1. A straight pipe portion having a length about 10 times the
diameter of the pipe must be provided downstream of the
straightener.
2. The pressure loss is great.
3. The manufacturing cost is high.
Thus, none of the known straighteners has proved quite satisfactory
as means for creating a turbulent-flow velocity distribution. In
view of this and on the following additional grounds, the
introduction of a straightener which can give a turbulent-flow
velocity distribution with a short straight length of a pipe has
been ardently called for.
A. The recent industrial tendency toward introduction of
larger-capacity plants and machinery has made it no longer easy to
maintain large length-to-diameter ratios for the straight lengths
upstream of throttling flowmeters for the measurement of fluid flow
in pipelines. On the other hand, the industry is demanding more and
more enhanced accuracy of measurement and is urgently looking for
the straighteners which can attain such accuracy with the shortest
possible straight lengths.
B. When a throttling flowmeter which has been calibrated is to be
used in actual measurement of fluid flow, there is a possibility of
errors due to the lack of hydrodynamic similarity if the measuring
conditions differ from those at the time of calibration because of
the influence of any obstacle which may exist in the pipeline, such
as a bend upstream of the primary element of the flowmeter. It has
been confirmed that, particularly when the Reynolds number is high,
a throttling flowmeter will give an unusual value of flow
coefficient under the influence of an ununiform upstream flow. For
this reason it is most essential to install a straightener which is
capable of highly efficiently counteracting the effect of such
upstream obstacle as a branch pipe, bend, or valve between the
primary element of the flowmeter and the particular obstacle.
c. It is clear from a number of experiments so far conducted as
well as from the literature that the flow velocity distribution
upstream of a throttling flowmeter can materially affect the
accuracy of the measurement. This means that a straightener capable
of effectively attaining a turbulent-flow velocity distribution is
of absolute necessity.
d. Conventional straighteners can uniformalize the flow velocity
distribution but are unable to give a turbulent-flow velocity
distribution. Where the latter is to be attained a long straight
length must be used.
It is therefore a fundamental object of this invention to provide a
straightener which can settle all of the problems above
enumerated.
Another object of the invention is to provide a highly efficient
straightener capable of meeting the requirements immediately above
noted.
The present invention, perfected to realize the foregoing objects,
resides in a straightener characterized by the use of a perforated
plate in which holes of the same diameter are scattered densely in
the central portion and thinly in the peripheral portion.
These and other objects, advantages and features of the present
invention will be better understood from the following detailed
description taken in conjunction with the accompanying drawings
showing preferred embodiments thereof.
In the drawings:
FIGS. 1 to 6 show conventional straighteners as fitted in a
cylindrical pipe 01; FIG. 1 being a front view of a perforated
plate 02, FIG. 2 a front view of a grid 03; FIG. 3 a front view of
a wire gauze 04; FIG. 4 a longitudinal sectional view of a
cylindrical pipe 01 wherein are installed a perforated plate 05 and
a grid 06 downstream of the plate; FIG. 5 a longitudinal sectional
view of a cylindrical pipe 01 wherein are installed a wire gauze 07
and a downstream grid 08; and FIG. 6 a perspective view of a
straightener 09 which combines a grid 010 and a perforated plate
011 attached to the upstream face of the grid;
FIG. 7 is a front view of a straightener embodying the invention as
fitted in a cylindrical pipe 1;
FIG. 8 is a sectional view taken on the line VIII -- VIII of FIG.
7;
FIG. 9 is a view illustrating the changes of velocity distribution
within a pipe 01 equipped with a known perforated-plate type
straightener 012 shown in FIG. 1 (pipe size 205 mm, plate thickness
14 mm, hole diameter 7 mm, and area ratio 0.5);
FIG. 10 is a view illustrating the changes of velocity distribution
within a pipe 1 equipped with the straightener 2 according to the
present invention;
FIG. 11 is a view comparing the results of experiments with a
conventional straightener of FIG. 6 and the straightener of the
invention shown in FIGS. 7 and 8;
FIG. 12 is a graph comparing the results of experiments on the
necessary straight lengths for different straighteners;
FIG. 13 is a graph illustrating the results of experiments on the
straightening effects achieved by straighteners of different sizes
according to the invention;
FIG. 14 is a plan view of the perforated plate of the straightener
09 shown in FIG. 6;
FIG. 15 is a plan view of a quadrant of the perforated plate of the
straightener according to the present invention; and
FIG. 16 is a sectional view of the quadrant.
Throughout FIGS. 7, 8 and 15 showing embodiments of the present
invention, the hole diameter d of the plurality of holes 3 formed
in the perforated plates 2 are the same. The distances l between
adjacent holes 3 are gradually increased from the center of the
cylindrical pipe 1 toward its surrounding wall. In other words, the
number of holes 3 per unit area of the plate becomes larger towards
the diametral center of the pipe and smaller towards the periphery.
The upstream ends or inlets of the holes 3 are beveled. Also, the
holes are so made that the ratio of the plate thickness t to the
hole diameter d, or t/d, is within the range of 1.0 to 3.0.
Next, the functions of the straightener according to this invention
will be described hereunder with reference to FIGS. 9 and 10 and in
comparison with the functions of conventional devices. In FIG. 9
are shown the changes of velocity distribution which are caused in
a cylindrical pipe 01 by a conventional straightener 012. A fluid
whose velocity distribution A is made ununiform by an obstacle not
shown which is located upstream of the straightener 012 flows
through the straightener 012 to attain a velocity distribution B
which is an almost uniform flow. As the fluid proceeds through the
straight length, a velocity distribution C is obtained, and
downstream of it or at a distance of about 10 D (ten times the
diameter of the pipe) from the straightener, a turbulent-flow
velocity distribution E is obtained. It means that a measuring
instrument, e.g., a throttling flowmeter 014, must be installed
further downstream.
FIG. 10 shows the changes of velocity distribution in a cylindrical
pipe 1 with a straightener 2 of the present invention. A fluid with
a velocity distribution A made uneven by an obstacle not shown
upstream of the straightener 2 then obtains a turbulent-flow
velocity distribution F after passage through a short straight
length following the straightener 2.
The straightener according to the present invention thus has the
following advantages:
i. The straight length upstream of a throttling flowmeter can be
extremely shortened.
ii. Swirl of the fluid can be reduced to almost zero.
iii. Pressure loss is negligible.
iv. Because the diameters of the holes in the perforated plate are
the same, the straightener can be manufactured at low cost.
v. Fluid flow measurement is possible with a high degree of
accuracy.
The velocity distribution characteristic, straight length
requirements, and attenuation of swirling flow by the straightener
according to this invention will be discussed hereunder in
connection with the results of experiments diagrammatically
represented or charted in FIGS. 11 to 13.
I. velocity distribution characteristic (Refer to FIG. 11.)
1. first, devices of three different sizes E, F and G as given in
Table 1 were made of perforated plates as perspectively shown in
FIG. 6 and having a plane as in FIG. 14.
Table 1 ______________________________________ No. E F G
______________________________________ d/D d/D d/D I 0.141 0.151
0.131 II 0.139 0.149 0.129 III 0.110 0.118 0.102 IV 0.139 0.149
0.129 V 0.136 0.146 0.126 VI 0.077 0.083 0.072 VII 0.110 0.118
0.102 VIII 0.077 0.083 0.072 ______________________________________
Notes: d = diameter of hole D = I.D. of pipe = 205 mm Thickness of
perforated plate = 0.02 D Thickness of grid plate = 0.005 D Depth
of grid plate = 1.0 D
2. next, using perforated plates having a plane as shown in FIGS.
15 and 16, devices H, I and J with dimensions as given in Table 2
were formed.
Table 2 ______________________________________ No. H I J
______________________________________ x y x y x y I 0 0 0 0 0 12.0
II 0 28.5 0 29.0 12.0 38.0 III 0 57.0 0 58.0 0 63.0 IV 0 85.0 0
87.0 0 90.0 V 25.0 14.5 25.5 14.5 24.0 12.0 VI 26.5 46.0 26.0 44.5
35.0 35.0 VII 32.0 78.0 30.0 78.0 24.0 69.5 VIII 50.0 0 51.0 0 48.0
12.0 IX 50.0 28.5 51.0 29.0 56.0 48.0 X 59.0 59.0 55.5 60.0 50.0
74.0 XI 81.0 0 82.0 0 72.0 16.5 XII 79.0 31.0 80.0 33.0 79.5 40.5
Hole 26.5 28.0 20.0 dia. ______________________________________
Notes: Unit = mm Perforated plate dia. R = 102.55 mm
3. The conventional device E and the device H of the invention,
both adjusted in size to 200 mm in diameter, were fitted in
straight pipes 1 having a inside diameter of 200 mm, and a bend was
connected upstream to each pipe, and then the flow velocity
distributions in the pipes were determined. The data thus obtained
are diagrammatically represented in FIG. 11. At a point 1 D (a
distance equal to the pipe diameter D) upstream of each
straightener, the flow velocity distribution was irregular as
represented by a curve A. At a point 1.5 D downstream of the
straightener, the distribution was changed as represented by the
curve B in the case of a conventional straightener of FIG. 6 or by
the curve B in the case of the device of the invention shown in
FIGS. 15 and 16. In either case the resulting curve was
substantially symmetrical with the center axis of the pipe.
Nevertheless, as will be obvious from those figures, the
conventional straightener gave a distribution much different from
the turbulentflow velocity distribution which is required for a
throttling flowmeter, whereas the straightener of the invention
produced a substantially perfect turbulentflow velocity
distribution. When the pressure loss involved was determined, the
loss with the straightener of the invention was several ten percent
less than that with the conventional device.
Ii. straight length characteristic (Refer to FIG. 12.)
In FIG. 12 which records the results of experiments on straight
length requirements, the numbers on the abscissa indicate the
diameter ratio of the orifice 14. Plotted as ordinate is the ratio
of straight length L to pipe diameter D which is required for
confining the error due to the effect of conditions upstream of the
orifice within the tolerance value of 0.5 per cent as specified in
the ISO Recommendation R541.
The curve drawn with an alternate long and short dash line in FIG.
12 indicates the straight length required upstream of an orifice,
where no straightening device is employed, in accordance with the
ISO Recommendation. The broken-line curves represent the results
with the conventional straighteners having the contours as
illustrated in FIGS. 6 and 14 and having the dimensions of E, F and
G in Table 1. The solid-line curves represent the results with the
straighteners according to this invention which have the contours
as shown in FIGS. 15 and 16 and the dimensions of H, I and J as
given in Table 2. In each experiment the test pipe was fitted with
two 90.degree. bends in different planes upstream of the
flowmeter.
It will be appreciated from the graph that the straightener
according to the present invention makes it possible to use by far
the shorter straight length upstream of the flowmeter than the
lengths usually required by the conventional devices.
Iii. swirling-flow attenuation characteristic (Refer to FIG.
13.)
Using straighteners according to the invention with varied ratios
of the thickness t of its perforated plate 2 to the hole diameter d
and supplying a swirling flow at a certain angle of swirl to the
upstream of each test straightener, the angle of swirl downstream
of the device was determined. The results are given in FIG. 13. The
angles were determined at points 1 D upstream and 1.5 D downstream
of each test straightener. The curves H, I and J correspond to the
columns H, I and J of Table 2.
As can be seen from the graph, the straightener of the present
invention kills almost all of the swirl and gives out practically
no swirl immediately downstream thereof provided that the ratio of
its plate thickness to the hole diameter, t/d, is 1.0 or upwards.
If the t/d is less than 1.0, the straightening effect will be
limited with little attenuation of the swirling flow. With a t/d in
excess of 3.0, the swirling flow will not be materially reduced and
the accuracy of fluid flow measurement will remain practically
unimproved. In addition, the thick perforated plate will be costly
and inconvenient to handle.
The straightener according to the present invention has the
following advantages:
A. High precision measurement of fluid flow with a throttling
flowmeter is made possible.
B. On the basis of computation of the flow velocity at one point
within a pipeline (e.g., without traversing with a pilot tube), the
fluid flow can be measured.
C. Fluid flow can be measured with noncontact currentmeters and
flowmeters (e.g., ultrasonic currentmeter and electromagnetic
flowmeter).
The straightener of the present invention is useful for the
measurement of fluid flow particularly in such largediameter
pipelines of large machines and plants which cannot be provided
with adequate straight lengths for foreflow up to the points of
measurement.
* * * * *