Vortex flow meter

Abstract: A vortex flow meter capable of operating with minimum piping effect is disclosed. A stream-lined protrusion , extending toward the upstream side is disposed at the upstream surface 2 of a vortex generator joined to the inner wall 1 of a flow pipe in order to remove thereat horseshoe vortexes produced in front of the vortex generator. Therefore, the possible affection of horseshoe vortexes, that may considerably depends upon the piping conditions, can be eliminated.

Description: BACKGROUND OF THE INVENTION The present invention relates to a vortex flow meter according to the preamble of claim 1 and, more particularly, to a vortex flow meter which is constructed and operated with a minimum amount of error as regards its instrumental function even when there is a change in the velocity of the flow's distribution due to the configuration of the flow's piping. An inferential type of flow meter is an instrument for determining the quantity of fluid or the velocity of the fluid's flow by measuring the physical quantity of the fluid produced in relation to the fluid's flow. To assure a certain relationship between the fluid's flow and the corresponding physical quantity of the fluid it is necessary to keep a constant state of the fluid's flow to be measured. For this reason, in order to attain the required accuracy of the inferential type of flow meter, it is necessary to provide a flow-rectifying device at the upstream side in the flow pipe wherein the flow meter is installed. Constructions of flow-rectifying devices and piping conditions for orifice and turbine flow meters are defined by the international standard and the national standard. It is well known that a vortex flow meter is related to an inferential type of flow meter which utilize a number of Karman's vortexes produced by a vortex generator installed in a flow pipe and which is substantially proportional to the flow rate of the fluid within a certain range of Reynolds number. This proportional constant is called the Strouhal number. In an ideal vortex flow meter, the Strouhal number can be kept at a constant value even when the Reynolds number varies. In other words, the ideal vortex flow meter has a constant characteristic (Strouhal number) in a wide range of the fluid's flow and is least affected by the physical properties of a fluid and the conditions of the piping. However, any practical vortex flow meter has a Strouhal number depending on a Reynolds number and its characteristic may be affected by the piping's conditions. A conventional vortex flow meter has a simple construction where a vortex generator is disposed at a right angle to the axis of the fluid's flow inside a cylindrical body. Many proposals for the shape and quantity of the vortex generators and the internal construction of the vortex flow meter have been made to keep the Strouhal number of the flow meters at a constant value against the Reynolds number. For example, one of the proposals was the improvement of the ratio d/D (width "d" of a vortex generator in perpendicular direction to the fluid's flow and an inside diameter "D" of the body) and a vortex detecting position. Especially, most available vortex flow meters have a ratio d/D being nearly equal to 0.28 in order to aim at obtaining the characteristic satisfying the stable two-dimensional conditions of the ideal Karman's vortex street. However, any practical vortex flow meter does not detect Karman's vortexes produced by a two-dimensional flow but rather those produced by a three-dimensional flow. Consequently, the characteristic of the vortex flow meter varies depending upon a change in the three-dimensional flow. For example, a bent pipe (including an elbow portion), reducer, diffuser, valve, branch pipe and collector may produce a rotational flow and deflect the flow of the fluid which in turn causes a change in the instrumental error of the vortex flow meter. A flow rectifier is provided to eliminate the above-mentioned irregularity of flow. Components of the rotational flow and the deflected flow may still remain in the flow of the fluid passing through the vortex flow meter, which affects the flow meter's instrumental error. A vortex flow meter according to the preamble of claim 1 is known from WO-A-8502970, EP-A-010764 and GB-A-293997, respectively. These known flow meters comprise a flow pipe, a vortex generator and a detection element downstream from the vortex flow meter for detecting a quantity of vortexes generated per unit of time from the vortex generator. In the vortex flow meter known from EP-A-0107641, a sensor body which also serves as a vortex shedding bluff body has a rod-like shape with opposing side and end walls, and piezo-electric disks, as pressure sensors, are provided in the side wall. At one end, the sensor body comprises an enlarged generally cylindrical portion which is disposed within an opening in the flow pipe when the sensor body is mounted within the flow meter. The bottom surface of the cylindrical portion is concave, so as to blend with the contour of the inner wall of the flow pipe. It is the object of the present invention to provide a vortex flow meter according to the preamble of claim 1 which prevents the generation of horseshoe vortexes. This object is solved by either solution according to claims 1, 2 and 3. The present invention provides a vortex flow meter which is reliable in measuring and capable of operating with a minimum amount of instrumental error possibly caused by the configuration of the flow pipe wherein it is installed. The present invention provides a vortex flow meter capable of operating with a minimum effect on the piping by eliminating the possibility of producing horseshoe vortexes around the upstream portion of a vortex generator. Furthermore, the present invention provides a vortex flow meter comprising a vortex generator joined to the inner wall of a flow pipe having a protrusion which is formed at the upstream surface of the vortex generator, fronting the fluid's flow and extending toward the upstream side along the inner wall of the flow pipe. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a partial view for explaining horseshoe vortexes. FIGS. 2a. 2b are views for explaining an example of a construction of a vortex flow meter embodied in the present invention. FIG. 3 is a view for explaining a vortex flow meter embodied in the present invention. FIG. 4 is a partially cutaway perspective view for explaining another embodiment of a vortex flow meter according to the present invention. FIG. 5 is a partially cutaway perspective view for explaining a further embodiment of a vortex flow meter, according to the present invention. FIG. 6 is a partially cutaway perspective view for explaining still another embodiment of a vortex flow meter, according to the present invention. FIG. 7 is a graph showing an example of an instrumental error characteristic of a vortex flow meter, according to the present invention. FIG. 8 is a graph showing an example of a piping effect characteristic of a vortex flow meter, according to the present invention. DETAILED DESCRIPTION OF THE INVENTION First, the operating principal of a vortex flow meter, according to the present invention is described as follows: Conventionally, a vortex flow meter is intended to detect vortexes produced by a vortex generator in a fluid passing therethrough. In a practical vortex flow meter, Karman's vortexes and horseshoe vortexes are produced which interfere with each other and thereby interfered with vortexes are detected. The horseshoe vortexes may be produced archwise in front of a vortex generator in a boundary layer along the inner wall of a flow pipe and are divided into two vortex tubes moving along both sides of the vortex generator. These vortex tubes can interfere with Karman's vortex tubes leaving from the sides of the vortex generator. Fig. 1 is a partially cutaway perspective view for explaining a horseshoe vortex. The numeral 10 designates the inner wall of a flow pipe and the numeral 11 designates vortex generator. In Fig. 1, the vortex generator 11 has a section in the form of an isosceles triangle with the base facing the fluid's flow and a flow pipe which has a flat inner wall 10. The vortex generator 11 is installed on the inner wall 10 of the flow pipe at a right angle to the direction of the fluid's flow, indicated by an arrow. The fluid's flow pressure applied on the vortex generator 11 is distributed in such a way that the pressure of the main flow, along an upstream surface 11a of the vortex generator 11, is high at the center axis O-O of a curve P A and decreases in the direction toward both sides of the vortex generator 11. The fluid's flow has a velocity V L decreasing as it approaches the boundary with the inner wall 10 of the flow pipe as shown in Fig. 1. The pressure is also reduced as the velocity decreases. Consequently, the pressure P A , applied by the main flow, decreases in the direction from the upstream surface 11a of the vortex generator 11 to the pipe's wall 10 whereon the pressure P F , decreases in the direction toward the upstream side. This results in that a boundary layer of fluid flow is divided to form horseshoe vortexes H V . Since these horseshoe vortexes H V depend upon the velocity of the flow velocity of a fluid along the upstream surface of the vortex generator 11, they may vary in size and symmetry if the main flow includes deflected flow and a rotational flow and, therefore, the effect of the horseshoe vortexes interfering with a street of karman's vortexes (not shown), produced by the vortex generator 11, can also change. The change in the interference effect may cause a change in the instrumental error of the vortex flow meter, i.e., a change in the Strouhal number. The visualization of the horseshoe vortexes is described in the printed material "A flow visualization around a protrusion in a parallel channel" ("Flow visualization", Vol. 6 No. 22, 1986-7). This paper reports that when a cubic body , whose height is substantially equal to the thickness of a boundary layer of water flowing therealong, is installed in a water bath, horseshoe vortexes may be produced around the cubic body but they also may disappear if the cubic body is elongated by tapering in the flows direction. Figs. 2(a) and 2(b) are views for explaining an example of the construction of a vortex flow meter embodied the present invention: Fig. 2(a) is a front view of the vortex flow meter being viewed from the flow's direction and Fig. 2(b) is a section taken along line B-B of Fig. 2(a). Numerals 1, 2 and 3 denote a flow pipe, a vortex generator and protrusion respectively. In Figs. 2(a) and 2(b), the vortex generator 2 has a uniform section in the form of an isosceles triangle with its base directed to the upstream side of the flow pipe for fluid flowing in the direction shown by an arrow and it is installed on the diametrical axis of the cylindrical section of the flow pipe 1 in such a way that its upstream surface is disposed at a right angle to the fluid's flow in the flow pipe 1. Stream-lined protrusions 3, extending in the upstream direction, are provided at both joints of the upstream (front) surface 2a of the vortex generator 2. The height H of each protrusion 3 at the upstream surface 2a of the vortex generator 2 is desirable to substantially equal the thickness of boundary layer of the fluid flowing at a low flow rate so that H≦1/6 D (D: diameter of a flow pipe) and the length of the protrusion on the inner wall of the pipe in the direction of the fluid's flow may be within the range of H to 3H. The stream-lined protrusions 3 may be formed integrally with the vortex generator in order to be secured to the inner wall 1a of the flow pipe 1 or separately to be secured to the upstream surface of the vortex generator 2. While the above-mentioned vortex generator 2 has a section in the form of an isosceles triangle with its base directed to the upstream side, it may be made in a shape of trapezoidal form, a circular one or any other form. Thus formed protrusions 3 are effective to eliminate the possibility of producing horseshoe vortexes in front of a vortex generator 2. Namely, the fluid flowing along the inner wall 1a of the flow pipe 1 moves over the protrusions 3 and reaches the upstream surface 2a of the vortex generator 2. This flow reduces the pressure P F against the inner wall of the flow pipe as shown in Fig. 1 and thereby prevents horseshoe vortexes. Fig. 3 is a partially cutaway perspective view for explaining a vortex flow meter embodied in the present invention. A protrusion 3 faces an upstream surface 2a of a vortex generator at its circular, arched surface that has a chord being a straight line joining the both side edges A and B of a vortex generator 2 with the inner wall 1a of a flow pipe. The height H of the arch of the protrusion above the inner wall 1a of the flow pipe may be gradually reduced in the direction toward a given position on the upstream-side inner wall of the flow pipe. The whole protrusion is made in the form of a wedge. As regards the the length of the protrusion 3 in the direction of the fluid's flow, along the inner wall 1a of the flow pipe, it it is preferable to keep it within the range of H to 3H. Fig. 4 is a partially cutaway perspective view for explaining another embodiment of a vortex flow meter according to the present invention. In the shown case, protrusion 3 is a flat circular, arched plate of the thickness H that has a chord defined between both sides A and B, of a vortex generator 2. Fig. 5 is a partially cutaway perspective view for explaining a further embodiment of a vortex flow meter according to the present invention, wherein protrusion 3 is a quadrangular pyramid having an isosceles triangle as its base, described by line segments joining both side edges A and B, of a vortex generator 2 and a vertex C of the height H at the center portion thereof. Fig. 6 is a partially cutaway perspective view for explaining still another embodiment of a vortex flow meter according to the present invention. In the shown embodiment, a protrusion 3 is made in the form of an arrowhead that has a triangular base defined by curved line sides "m" and "n" with an apex C of a height H at the center of a chord between both side edges A and B, of a vortex generator 2. The height H of the apex C of the triangle is gradually reduced in the direction of the inner wall of a flow pipe. Fig. 7 is a graph showing an example of an instrumental error characteristic of a vortex flow meter according to the present invention. The graph indicates a Reynolds number (Re. No.) on the axis of abscissas and a flow coefficient (K-factor, liter per pulse) on the axis of the ordinates. A vortex generator 2 is provided with protrusions 3 in the form of a flat circular arched plate as shown in Fig. 4. The thickness (H) of each protrusion is 7 millimeters. The vortex generator 2 has a length of (D) = 151 millimeters and a width of (W) = 42 millimeters. The conditions of the pipes are as follows: The length of the upstream straight pipe is equal to 100D and the testing fluid is water. Curve A shows an instrumental error of a vortex flow meter according to the present invention and curve B shows an instrumental error of a conventional vortex flow meter which has a vortex generator with no protrusion 3. The curve B indicates that the K-factor increases in a range of low values of the Reynolds number and there is a deviation of about 1% at the Reynolds number = 2∼ 9×10 5 . On the contrary, as is apparent from the curve A, the vortex flow meter according to the present invention, has an improved deviation of about 0.15% of the substantially same range as the Reynolds number. Fig. 8 shows an example of a piping effect characteristic of a vortex flow meter according to the present invention. The graph indicates the length D of a straight pipe from the vortex flow meter to a double planes elbow (doubly bent at 90° out of a plane) on the axis of abscissas and an instrumental error (E) on the axis of ordinates. It shows how the length D of the straight pipe, between the cubic double elbow and a vortex generator, provided with protrusions, exerts an effect on the instrumental error (E) of the vortex flow meter. The test fluid is kerosene. Curves A and B indicate an instrumental error at the Reynolds number of 3×10 5 and 7×10 5 respectively. The piping, having a cubic double elbow may be considered to be in its worst condition wherein the fluid's flow may include a complicated rotational flow and a deflected flow. The vortex flow meter, according to the present invention can hardly be affected by piping of the length 10D of the upstream straight pipe. The curves A and B indicate that the instrumental error of the flow meter with a straight pipe length of 30D is almost eliminated even when the Reynolds number varies. As is apparent from the foregoing, according to the present invention, it is possible to provide a vortex flow meter capable of operating with a minimum effect on the piping in its accuracy of measurement and wherein protrusions extending toward the upstream side along the inner wall of a flow pipe, are provided, one at the joining portions of the upstream surface of a vortex generator to the inner wall of the flow pipe to eliminate the possibility of producing horseshoe vortexes around the upstream portion of the vortex generator, i.e., a mutual interference of the horseshoe and Karman vortexes, which may considerably vary in dependence upon the piping effect and affect an instrumental error in the vortex flow meter.

Claims: A vortex flow meter comprising a flow pipe (1) and a vortex generator (2) exposed at a right angle to the fluid's flow along the flow pipe (1) for determining flow rate of the fluid from a quantity of vortices generated per unit of time from the vortex generator, characterized in that the vortex generator (2) joined to the inner wall of the flow pipe has a protrusion (3) which is formed at the upstream surface (2a) of the vortex generator fronting and exposed to the fluid's flow and extending toward the upstream side along the inner wall (1a) of the flow pipe (1), wherein said protrusion (3) has a shape of a wedge, one end of which joining to the upstream surface (2a) of the vortex generator (2) extends between two sides of the vortex generator (2), and the wedge has two opposing surfaces, one of which faces the inner wall (1a) of the flow pipe (1) and the other is cylindrically rounded and inclined such that the height of the wedge above the inner wall (la) of the flow pipe (1) gradually decreases in the upstream direction. A vortex flow meter comprising a flow pipe (1) and a vortex generator (2) exposed at a right angle to the fluid's flow along the flow pipe (1) for determining flow rate of the fluid from a quantity of vortices generated per unit of time from the vortex generator, characterized in that the vortex generator (2) joined to the inner wall of the flow pipe has a protrusion (3) which is formed at the upstream surface (2a) of the vortex generator fronting and exposed to the fluid's flow and extending toward the upstream side along the inner wall (1a) of the flow pipe (1), wherein said protrusion (3) has a shape of a minor segment of a plate-like cylinder sectioned in a plane parallel to its axis, wherein the sectional area of the segment joining to the upstream surface (2a) of the vortex generator (2) extends between both sides of the vortex generator (2). A vortex flow meter comprising a flow pipe (1) and a vortex generator (2) exposed at a right angle to the fluid's flow along the flow pipe (1) for determining flow rate of the fluid from a quantity of vortices generated per unit of time from the vortex generator, characterized in that the vortex generator (2) joined to the inner wall of the flow pipe has a protrusion (3) which is formed at the upstream surface (2a) of the vortex generator fronting and exposed to the fluid's flow and extending toward the upstream side along the inner wall (1a) of the flow pipe (1), wherein said protrusion (3) is a tapered body having three edges converging in the upstream direction into one point, wherein two of said edges originate from opposing side points (A, B) on the vortex generator and one edge originates from a point (C) on a center line of the upstream surface (2a) between said two side points and is inclined such that the height of the protrusion (3) above the inner wall (la) of the flow pipe (1) gradually decreases in the upstream direction. A vortex flow meter according to claims 1, 2 or 3, wherein the protrusion (3) has the height of H on the upstream surface of the vortex generator (2) and a length of 3H in the upstream direction. A vortex flow meter according to claim 3 wherein said edges are curved such that said tapered body is formed in a manner similar to an arrowhead (3).

Inventors: MATSUBARA NAOKI, MISUMI MASAO, NAKAO YUICHI, MATSUBARA, NAOKI, MISUMI, MASAO, NAKAO, YUICHI, Matsubara, Naoki, c/o Oval Corporation, Misumi, Masao, c/o Oval Corporation, Nakao, Yuichi, c/o Oval Corporation
Applicants: OVAL CORP, OVAL CORPORATION
Application year: 1993
Main classification: G01F1
IPC codes: G01F1, G01F15