The present disclosure relates to the technical field of liquid level measurement, in particular to a method for determining a reflector, a system for determining a reflector, a reflector, a vertical tank external measuring liquid level meter and a mounting method thereof.
The design process of the reflecting surface in the existing external measurement liquid level meter is as follows: each level of the N-level reflecting surface is designed by using a geometric construction calculation method, the positions of the boundary points of the reflecting surfaces at all levels are calculated step by step, and then the reflecting surfaces are designed according to the positions of the boundary points of the N-level reflecting surfaces. The reflecting surface can reflect the ray emitted by the ultrasonic measuring head in any direction to any specified direction, and has a wide range of applications. However, in the design process of the reflecting surface, there is no specific calculation formula, and the work is complicated and heavy.
The present disclosure aims to provide a determining method, a system, a reflector, a vertical tank external measurement liquid level meter and a mounting method thereof, and the reflector is designed on the basis that the positions of boundary points of reflecting surfaces at all levels do not need to be calculated step by step, so as to reduce the calculation workload and improve the working efficiency.
In order to achieve the above purpose, the present disclosure provides the following scheme.
In a first aspect, the present disclosure provides a determining method for determining a reflector for reflecting an ultrasonic signal emitted by an ultrasonic emission source, wherein the determining method includes:
In a second aspect, the present disclosure provides a determining system for determining a reflector for reflecting an ultrasonic signal emitted by an ultrasonic emission source, wherein the determining system includes:
In a third aspect, the present disclosure provides a reflector determined by the reflector determining method as described in the first aspect, wherein the reflector is used for reflecting an ultrasonic signal emitted by an ultrasonic emission source;
In a fourth aspect, the present disclosure provides a vertical tank external measurement liquid level meter, including a liquid level determining module, an ultrasonic signal source locator, and the reflector as described in the third aspect;
In a fifth aspect, the present disclosure provides a mounting method, wherein the mounting method is used for mounting the vertical tank external measurement liquid level meter as described in the fourth aspect, including:
According to the specific embodiment provided by the present disclosure, the present disclosure discloses the following technical effects.
In the present disclosure, a parabolic function is used to design a reflector of a vertical tank external measurement liquid level meter. When the vertical tank external measurement liquid level meter works, an ultrasonic transmitting probe thereof is mounted on an outer wall of the measured vertical tank, and an ultrasonic signal emitted by the ultrasonic transmitting probe penetrates through a side wall of the vertical tank and generates an ultrasonic emission source at an inner wall of the vertical tank; a position point of the ultrasonic emission source is also a focus of the reflector; an ultrasonic signal emitted by the ultrasonic emission source is emitted to the reflector, is reflected by the reflector, is emitted in parallel to a preset direction, is returned to the position of the ultrasonic emission source according to the original path after passing through the liquid level of the measured vertical tank, penetrates through the side wall of the vertical tank and is received by a measuring head of the external measurement liquid level meter mounted outside the side wall of the vertical tank; the external measurement liquid level meter determines, according to the emitted ultrasonic signal and the received ultrasonic signal, the liquid level position of the measured vertical tank. Obviously, the reflector provided by the present disclosure can meet the requirement that the rays emitted from the focus to any direction in front are emitted parallel to the preset direction after being reflected by the reflector without calculating the positions of boundary points of reflecting surfaces at all levels step by step, thus achieving the purpose of reducing the calculation workload and improving the working efficiency.
In order to explain the technical scheme of the embodiments of the present disclosure or the prior art more clearly, the drawings needed in the embodiments will be briefly introduced hereinafter. Obviously, the drawings in the following description are some embodiments of the present disclosure, and other drawings can be obtained according to these drawings without creative labor for those skilled in the art.
The technical schemes in the embodiments of the present disclosure will be clearly and completely described with reference to the drawings in the embodiments of the present disclosure hereinafter. Obviously, the described embodiments are only some embodiments of the present disclosure, rather than all of the embodiments. Based on the embodiment of the present disclosure, all other embodiments obtained by those skilled in the art without creative labor belong to the scope of protection of the present disclosure.
The present disclosure aims to provide a determining method, a system, a reflector, a vertical tank external measurement liquid level meter and a mounting method thereof, and the reflector is designed on the basis that the positions of boundary points of reflecting surfaces at all levels do not need to be calculated step by step, so as to reduce the calculation workload and improve the working efficiency.
In order to make the above objectives, features and advantages of the present disclosure more obvious and understandable, the present disclosure will be further described in detail hereinafter in conjunction with the attached drawings and specific embodiments.
In order to make the vertical tank external measurement liquid level meter conveniently measure the liquid level of the vertical tank from the outside of the side wall of the vertical tank, the present disclosure provides a reflector as shown in
As shown in
The reflector is a parabolic reflector; a center point of the parabolic reflector is the coordinate origin O, a focus of the parabolic reflector is the position point T, and the focal length of the parabolic reflector is the focal length P.
The coordinate of the center point of the reflector on the third right-handed rectangular coordinate system OXYZ is the coordinate origin O (0, 0, 0); the coordinate of the center point of the reflector on the second right-handed rectangular coordinate system TXPYPZP is (P,0,0), and the coordinate of the center point of the reflector on the first right-handed rectangular coordinate system O1X1Y1Z1 is (P,P/2,0).
The equations of paraboloids in the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1, the second right-handed three-dimensional rectangular coordinate system TXPYPZP and the third right-handed three-dimensional rectangular coordinate system OXYZ are used to form a data table (x,y,z) of paraboloids, and a parabolic reflector is manufactured according to the data table (x,y,z) of paraboloids.
The position point T is at a positive value of an O1Y1 coordinate axis of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1, and a length of a line segment O1T is equal to half of the focal length P; the position point T is a coordinate origin of the second right-handed three-dimensional rectangular coordinate system TXPYPZP, the second right-handed three-dimensional rectangular coordinate system TXPYPZP is obtained by translating the length of the line segment O1T in a direction of the positive value of the O1Y1 coordinate axis of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1; a coordinate origin O of the third right-handed three-dimensional rectangular coordinate system OXYZ is at a positive value of the coordinate axis TXp of the second right-handed three-dimensional rectangular coordinate system TXPYPZP, and the coordinate origin O of the third right-handed three-dimensional rectangular coordinate system OXYZ is the other end point of the reference line segment; the length of the line segment TO is equal to the focal length P, the third right-handed three-dimensional rectangular coordinate system OXYZ is obtained by translating the length of the line segment TO in the direction of the positive value of the coordinate axis TXp of the second right-handed three-dimensional rectangular coordinate system TXPYPZP; and the position point T is located at a negative value of the OX axis of the third right-handed three-dimensional rectangular coordinate system OXYZ.
According to the position point T and the focal length P, determining a basic cross section of the reflector on a O1X1Y1 coordinate plane of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1 is determined; wherein the basic cross section is a basic parabola, the focal length of the basic parabola is the focal length P; the focus of the basic parabola is the position point T; and the basic parabola rotates with the O1Y1 coordinate axis as the rotation axis to form a paraboloid.
The equation of the basic parabola on the O1X1Y1 coordinate plane of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1 is x12=2Py1; where x1 is an X1 coordinate of the O1X1Y1 coordinate plane, and y1 is the Y1 coordinate of the O1X1Y1 coordinate plane.
The parabolic equation is in the form of x12+z12=2Py1 on the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1; wherein x1 is the coordinate on the coordinate axis O1X1 of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1, y1 is the coordinate on the O1Y1 coordinate axis of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1, and z1 is the coordinate on the O1Z1 coordinate axis of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1.
The parabolic equation is in the form of xp2+zp2=2P(yp+P/2) in the second right-handed three-dimensional rectangular coordinate system TXPYPZP; wherein xp is the coordinate on the coordinate axis TXp of the second right-handed three-dimensional rectangular coordinate system TXPYPZP, yp is the coordinate on the TYp coordinate axis of the second right-handed three-dimensional rectangular coordinate system TXPYPZP, and zp is the coordinate on the TZp coordinate axis of the second right-handed three-dimensional rectangular coordinate system TXPYPZP.
The parabolic equation is in the form of (x+P)2+z2=2Py+P2 in the third right-handed three-dimensional rectangular coordinate system OXYZ; wherein x is the coordinate on the OX coordinate axis of the third right-handed three-dimensional rectangular coordinate system OXYZ, y is the coordinate on the OY coordinate axis of the third right-handed three-dimensional rectangular coordinate system OXYZ, and z is the coordinate on the OZ coordinate axis of the third right-handed three-dimensional rectangular coordinate system OXYZ.
The equation of the first parabola is xp2=2Pyp+P2; on the first cross section, a pitch angle of the ultrasonic emission source emitted from the coordinate origin T on the TXpYp coordinate plane of the second right-handed three-dimensional rectangular coordinate system TXPYPZP to any point (xp,yp) on the first parabola of the reflecting surface of the parabolic reflector is θ=art (yp/xp); wherein xp is a TXp coordinate value of a projection point (xp,yp) on the first parabola, yp is a TYp coordinate value of the projection point (xp,yp) on the first parabola; the range of the pitch angle is the range of a radiation angle of the ultrasonic signal emitted by the ultrasonic emission source on the TXpYp coordinate plane.
The equation of the arc is xp2+zp2=P2; a horizontal angle of the ultrasonic emission source from the coordinate origin T of the second right-handed three-dimensional rectangular coordinate system TXPYPZP to any point (xp,zp) on the arc of the reflecting surface of the parabolic reflector is θ=art(zp/xp); wherein xp is a TXp coordinate value of the projection point (xp,zp) that the ultrasonic signal emitted from the position point T emits on the arc of the TXpZp coordinate plane, zp is a TZp coordinate value of the projection point (xp,zp) that the ultrasonic signal emitted from the position point T emits on the arc of the TXpZp coordinate plane; the range of the horizontal angle is the range of the radiation angle of the ultrasonic signal emitted by the ultrasonic emission source on the TXpZp coordinate plane; the equation of the second parabola is z2=2Py, and the second parabola is on the OYZ coordinate plane of the third right-handed three-dimensional rectangular coordinate system OXYZ.
The reflector is made of materials such as steel and brass whose acoustic impedance is much greater than that of the measured liquid. For example, the acoustic impedance of liquid is 1, the acoustic impedance of steel is 45, and the acoustic reflectivity in liquid is 1−1/45=97.8%. In order to prevent the interference resulted from the reflected wave on the front of the reflector and the reflected wave on the back of the reflector, the reflector is made into a thin plate with a thickness of 0.5˜1 mm, or a non-plate member whose back is not parallel to the front. For the convenience of subsequent mounting, a locating hole O with a diameter of Φ0.3˜Φ0.5 is provided at the center of the reflector, that is, a center hole. A semicircular groove N with a diameter of Φ0.5˜Φ2 is provided at the highest point of the reflector, that is, at the highest point (XN,YN,0) of the cross section of the XOY coordinate plane of the third right-handed three-dimensional rectangular coordinate system OXYZ of the reflector.
The third right-handed three-dimensional rectangular coordinate system OXYZ is constructed based on the focal length P and the center point of the reflector, wherein the focus is located at the negative value of the OX axis of the third right-handed three-dimensional rectangular coordinate system OXYZ.
In this embodiment, the parabolic function is used to design the reflector without calculating the positions of boundary points of reflecting surfaces at all levels step by step, so as to reduce the calculation workload, improve the working efficiency, and popularize and apply the parabolic reflector easily.
Referring to
The ultrasonic signal source locator includes an ultrasonic transmitting probe, an ultrasonic transmitting circuit connected with the ultrasonic transmitting probe, an ultrasonic receiving probe, an ultrasonic receiving circuit connected with the ultrasonic receiving probe and an ultrasonic intensity indicator; wherein the ultrasonic transmitting probe emits ultrasonic waves to a vertical tank wall from the outside of the vertical tank, and the ultrasonic receiving probe receives ultrasonic signals from the inside of the vertical tank wall, uses the intensity indication displayed by the ultrasonic intensity indicator to find the position of the received strongest ultrasonic signals, and determines a position point T of an ultrasonic transmitting source formed on the inside of the vertical tank wall after the ultrasonic waves emitted by the ultrasonic transmitting probe from the outside of the vertical tank wall pass through the vertical tank wall; the liquid level determining module consists of an external measurement liquid level meter; and the external measurement liquid level meter is configured to measure a liquid level height in the vertical tank from the outside of the vertical tank.
On the basis of Embodiment 2, the external measurement liquid level meter further includes a supporting part. The supporting part is used for mounting the reflector in the measured vertical tank.
The supporting part described in this embodiment can fix the reflector in any way, which can be said to be infinite. For example, the supporting part uses four supporting rods, and for example, the supporting part is fixed on the side wall of the vertical tank.
In one example, as shown in
The focus is located at the negative value of the OX axis of the third right-handed three-dimensional rectangular coordinate system OXYZ. In addition, the third right-handed three-dimensional rectangular coordinate system OXYZ further includes an OY axis and an OZ axis.
The platform 2 is a platform made of a metal sheet, and the reflector 1 is fixed on the platform.
The bc arc edge of the platform 2 near the side wall of the vertical tank coincides with the lower end of the reflector 1, where point A(XA,YA,0) is the lower end point of the parabola of the cross section between the reflector and the OXY coordinate plane of the third right-handed three-dimensional rectangular coordinate system OXYZ. The end of the platform 2 far away from the side wall of the vertical tank is located at the point M(XM,0,0) on the third right-handed rectangular coordinate system OXYZ. A semicircular groove M with a diameter of Φ0.5˜Φ1 is provided at the point M(XM,0,0) of the platform. The platform 2 is equipped with a level meter in the direction of the OX coordinate axis and a level meter in the direction of the OZ coordinate axis. The purpose of mounting these two level meters is to mount the platform 2 parallel to the OXZ coordinate plane.
Further, the supporting part further at least includes three tubular supporting rods 3 with adjustable lengths and fastened by screws, namely a first supporting rod a, a second supporting rod b and a third supporting rod c; the first supporting rod a, the second supporting rod b and the third supporting rod c are connected and fixed with each other through a transverse connecting rod.
An upper end of the first supporting rod passes through the vicinity of a semicircular groove M of the supporting part and the vicinity of a semicircular groove N of the reflector in sequence; the second supporting rod and the third supporting rod are located at both sides of the first supporting rod, respectively; an upper end of the second supporting rod and an upper end of the third supporting rod are both fixed on the supporting part (or points b and c of the platform 2 as shown in
A highest point (XN,YN,0) of the reflector 1 on the OXY coordinate plane of the third right-handed three-dimensional rectangular coordinate system OXYZ is the semicircular groove N; the semicircular groove M is on the symmetrical center line of the platform, and the coordinate of the semicircular groove M in the third right-handed three-dimensional rectangular coordinate system OXYZ is (XN,0,0).
A lower end of the first supporting rod a, a lower end of the second supporting rod b and a lower end of the third supporting rod c are all fixed at the bottom of the measured vertical tank during operation.
In another example: for the working condition that the reflector cannot be mounted at the bottom of the tank, for example, 1, when the reflector cannot be mounted at the bottom of the measured vertical tank; 2, when the vertical tank external measurement liquid level meter is used in a sausage-shaped tank, there are other devices in the tank for sheltering or the radian of the oval tank bottom is large, that is, the reflector cannot be mounted at the bottom of the vertical tank. At this time, the supporting rod of the steering gear should be fixed on the side wall of the vertical tank.
As shown in
Because the steering gear needs to be mounted on the inner side wall of the measured vertical tank by welding, the necessary condition for mounting the steering gear is that people can enter the tank and fire.
The mounting position of the steering gear is selected as follows: a low position in the tank for easy operation, but it is not allowed to enter the liquid residue sediment layer accumulated at the bottom of the tank to prevent the sediment from blocking the ultrasonic signal propagation, and avoid upper structural parts to prevent the transmission of ultrasonic waves between the steering gear and the liquid level from being obstructed.
In addition, the steering gear can be horizontally mounted on the inner side wall of the measured vertical tank, and its physical diagram is shown in
On the basis of Embodiment 3, this embodiment provides a mounting method.
As shown in
In Step 602, the ultrasonic signal source locator includes an ultrasonic transmitting circuit, an ultrasonic transmitting probe, an ultrasonic receiving circuit, an ultrasonic receiving probe and an ultrasonic intensity indicator connected with the ultrasonic receiving probe.
Step 602 specifically includes:
Referring to
When implementing Step a, the adsorption end is fixed on the magnetic base perpendicular to the inner wall of the vertical tank, and the position where the magnetic base is located is the position point of the ultrasonic emission source.
In Step 604, according to the placement point of the center point of the reflector 1, the reflector is mounted, and the reflector is moved so that the tip end of the focal length scale is aligned with and enters the center point of the reflector. Using the characteristic that the length of the focal length scale is a fixed focal length P, the tip end of the focal length scale is aligned with and enters the central point of the reflector (that is, the central hole O), so that the precise position positioning of the central point O of the reflector on the coordinate axis TXP is simply realized.
Therefore, in Step 604, mounting the reflector 1 according to the placement point specifically includes:
For a vertical tank with a diameter greater than 4 meters, for example, 15 meters, in order to ensure that there is no support structure for supporting the floating tank top and blocking the ultrasonic signal propagation between the upward side of the reflector and the top of the liquid level floating tank, it is necessary to increase the distance between the reflector and the side wall of the vertical tank, for example, 1000 mm or more. At this time, the focal length P should be selected to be relatively large, for example, 1000 mm or more. At this time, it is necessary to use a focal length scale of 1000 mm or longer, so that it is difficult to be operated and kept in a horizontal straight line. In this case, a laser ranging calibrator can be used. The magnetic base of the laser ranging calibrator is fixed at the position point of the ultrasonic emission source. The positions of the reflector and the platform are adjusted so that the laser emitted by the laser ranging calibrator is emitted at the O point of the reflector, and the displayed distance is equal to the focal length P. Thereafter, the pitch angle and the horizontal angle of the reflector and the platform are adjusted, so that the pitch angle θ of the reflector is 0 degrees and the horizontal angle φ is 0 degrees, and then the two mutually perpendicular level meters on the supporting part are horizontal.
Step 2 further includes:
The specific process of adjusting the position of the reflector using the scanning function of the laser ranging calibrator is as follows:
In Step 2, another simple method to adjust the mounting angle of the steering gear to make the pitch angle and the horizontal angle of the reflector equal to 0 degrees is to hang the heavy hammer line on the semicircular groove N at the highest position of the reflector with a hook at one end of the heavy hammer line 5, so that the heavy hammer can hang freely. The pitch angle θ of the reflector in the TXY coordinate plane of the third right-handed three-dimensional rectangular coordinate system OXYZ and the horizontal angle φ in the TXZ coordinate plane of the third right-handed three-dimensional rectangular coordinate system OXYZ are adjusted, so that the heavy hammer line 5 enters the semicircular groove M of the platform. The heavy hammer line 5 is not in contact with the edge of the semicircular groove M. The pitch angle and the horizontal angle of the reflector are adjusted, so that the two mutually perpendicular level meters on the supporting part are horizontal, and the accurate angle positioning of the reflecting surface platform is simply completed.
The third right-handed three-dimensional rectangular coordinate system OXYZ is constructed based on the focal length P and the center point of the reflector. The highest point (XN,YN,0) of the reflector on the OXY coordinate plane of the third right-handed three-dimensional rectangular coordinate system OXYZ is the semicircular groove N; and the coordinate of the semicircular groove M in the third right-handed three-dimensional rectangular coordinate system OXYZ is (XN,0,0).
In this embodiment, it is also necessary to finely adjust the mounting position of the reflector by using the heavy hammer line 5 and a power-assisted fixer.
One end of the heavy hammer line 5 is fixed with a hook, and the other end of the heavy hammer line 5 is hung with a heavy hammer. The power-assisted fixer is formed in such a manner that two ends are equipped with a neodymium magnet respectively and the two ends are connected by rubber bands.
Specifically, the hook is hung in the semicircular groove N of the reflector. When the heavy hammer line is hung freely and statically, the heavy hammer is embedded in the semicircular groove M of the platform 2 and is not contact with the wall of the semicircular groove M, so as to quickly and accurately determine the accurate angles in three directions when the reflector is mounted.
That is, after mounting the reflector 1 according to the placement point, the method further includes:
The third right-handed three-dimensional rectangular coordinate system OXYZ is constructed based on the focal length P and the center point of the reflector, and the highest point (XN,YN,0) of the reflector on the XOY coordinate plane of the third right-handed three-dimensional rectangular coordinate system OXYZ is the semicircular groove N; and the coordinate of the semicircular groove M in the third right-handed three-dimensional rectangular coordinate system OXYZ is (XN,0,0).
In order to facilitate the mounting, the power-assisted fixer can be used, which consists of two neodymium magnet blocks and a rubber band connecting the two magnets. During mounting, a neodymium magnet of the power-assisted fixer is sucked at point A of the platform 2, and a neodymium magnet at the other end thereof is sucked at the lower part of the focus T inside the tank wall. The steering gear is tensioned and temporarily fixed to the tank wall with the help of the tension of the rubber band, which is convenient for adjustment and position calibration.
After the reflector is mounted and calibrated, the points a, b, c and d of the reflector 1 are fixed on the tank wall by welding, bonding or magnetic attraction. The first supporting rod a, the second supporting rod b and the third supporting rod c are fixed. The focal length scale 4, the heavy hammer line 5, the power-assisted fixer and the plane reflecting plate 6 are dismantled. The plane reflecting plate 6 mounted on the floating roof in the floating roof tank will not be dismantled after mounting the reflector of the steering gear.
Because the tank wall where the probe is mounted is not guaranteed to be exactly perpendicular to the horizontal plane, the focal length scale vertically adsorbed on the side wall is not guaranteed to be exactly horizontal, nor is it guaranteed to be exactly perpendicular to the side wall of the vertical tank. However, as long as the distance between the center point O of the reflector and the ultrasonic emission source T on the inner side wall of the vertical tank is guaranteed to be exactly equal to the focal length P by using the focal length scale 4 or the laser ranging scanner, the level meters vertically mounted on the platform 2 of the steering gear are horizontal, and then the angle of the reflector and the shape of the reflecting surface are finely adjusted by using the laser ranging scanner, so that the laser emitted from the laser ranging scanner can be reflected upwards to the horizontally mounted plane reflecting plate 6 through the reflector 1. The shape of the light spot reflected back to the ultrasonic emission source T through the reflector 1 is a small dot, so that the pitch angle error and the horizontal angle error of the focal length scale do not affect the reflector 1 to accurately reflect and focus the ultrasonic waves from all directions back to the ultrasonic emission source.
When the external measurement liquid level meter works, an ultrasonic probe thereof is mounted on an outer wall of the measured vertical tank, and the ultrasonic probe generates an ultrasonic emission source at an inner wall of the measured vertical tank; a position point of the ultrasonic emission source is also a focus of the reflector; an ultrasonic signal emitted by the ultrasonic emission source is emitted to the reflector, is reflected by the reflector, is emitted in parallel to a preset direction, returns according to the original path after passing through the liquid level of the measured vertical tank, and is received by the external measurement liquid level meter; the external measurement liquid level meter determines, according to the ultrasonic signal emitted by the ultrasonic probe and the ultrasonic signal received by the ultrasonic probe, the liquid level position of the measured vertical tank. Obviously, the reflector provided by the present disclosure can meet the requirement that the rays emitted from the focus to any direction in front are emitted parallel to the preset direction after being reflected by the reflector without calculating the positions of boundary points of reflecting surfaces at all levels step by step, thus achieving the purpose of reducing the calculation workload and improving the working efficiency.
Referring to
The focal length P is artificially selected according to the diameter D of the measured vertical tank, and the principle of selection is that the focal length P is less than or equal to D/2.
For example, the horizontal cross section in the vertical tank where the reference line segment is located is the standard plane of the measured vertical tank; and the focal length P is less than or equal to the radius of the standard plane.
For another example, when the method is used to measure the depth of the oil level in an oil well from the wellhead, D=200 mm, and the focal length P=d/2=100 mm is selected.
For another example, when measuring the depth from the water surface of a deep well to the wellhead, when the diameter of the well is D=400 mm, the focal length P=D/2=200 mm is selected.
In addition, when the diameter D of the measured target vertical tank is very large, such as a vertical liquid storage tank, and the diameter D is between 500 mm and 50 m, the principle of determining the focal length P is that there are no structures, such as pipes and beams, that blocks the ultrasonic signal propagation between the upward side of the reflecting surface and the liquid level or the floating roof floating on the liquid level, and ultrasonic waves are not allowed to be emitted on the circular sealing hose at the edge of the floating roof disc. The structural parts in the vertical tank with a large diameter are relatively large. The focal length P of the paraboloid of the selected reflector should be larger if the reflecting surface needs to be farther away from the side wall. For the vertical tank with a diameter of more than 4 meters, the focal length P can be about 1000 mm. When the reflector is larger than the manhole with a diameter of 600 mm in the vertical tank, it is necessary to split the reflector into several parts, which are then sent into the vertical tank through the manhole and then are assembled into a reflector accurately.
The position point T is at a positive value of an O1Y1 coordinate axis of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1, and a length of a line segment O1T (one endpoint is the origin of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1, and the other endpoint is the position point T) is equal to half of the focal length P; the position point T is a coordinate origin of the second right-handed three-dimensional rectangular coordinate system TXPYPZP, the second right-handed three-dimensional rectangular coordinate system TXPYPZP is obtained by translating the length of the line segment O1T in a direction of the positive value of the O1Y1 coordinate axis of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1; the TYP coordinate axis of the second right-handed three-dimensional rectangular coordinate system TXPYPZP coincides with the O1Y1 coordinate axis of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1, the coordinate axis TXp of the second right-handed three-dimensional rectangular coordinate system TXPYPZP is parallel to the coordinate axis O1X1 of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1, and the TZP coordinate axis of the second right-handed three-dimensional rectangular coordinate system TXPYPZP coincides with the O1Z1 coordinate axis of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1.
The coordinate origin O of the third right-handed three-dimensional rectangular coordinate system OXYZ is at a positive value of the coordinate axis TXp of the second right-handed three-dimensional rectangular coordinate system TXPYPZP, and the coordinate origin O of the third right-handed three-dimensional rectangular coordinate system OXYZ is the other end point of the reference line segment; the length of the line segment TO is equal to the focal length P, the third right-handed three-dimensional rectangular coordinate system OXYZ is obtained by translating the length of the line segment TO in the direction of the positive value of the coordinate axis TXp of the second right-handed three-dimensional rectangular coordinate system TXPYPZP; and the position point T is located at a negative value of the OX axis of the third right-handed three-dimensional rectangular coordinate system OXYZ; the OX coordinate axis of the third right-handed three-dimensional rectangular coordinate system OXYZ coincides with the coordinate axis TXp of the second right-handed three-dimensional rectangular coordinate system TXPYPZP; the OY coordinate axis of the third right-handed three-dimensional rectangular coordinate system OXYZ is parallel to the TYP coordinate axis of the second right-handed three-dimensional rectangular coordinate system TXPYPZP, and the OZ coordinate axis of the third right-handed three-dimensional rectangular coordinate system oxy is parallel to the TZP coordinate axis of the second right-handed three-dimensional rectangular coordinate system TXPYPZP.
The edge shape of the reflector surface can be arbitrarily selected according to the specific situation, and it is not unique. For example, in order to send the reflector into the vertical tank through a manhole (that is, a circular hole with a sealed cover and a diameter of less than 600 mm reserved on the side wall of the vertical tank for construction workers to enter the interior of the vertical tank) for mounting, the reflector needs to be made into a strip with a width less than 600 mm. For another example, in order to reduce the cost of the mold for processing the reflecting surface, the reflecting surface can be processed into an ellipse to reduce the mold area. As shown in
Taking
In this embodiment, the reflector designed by using the parabolic function method can achieve the purpose of reflecting all the rays emitted from the focus in any direction in front to the parallel direction, which significantly reduces the design and calculation workload and improves the efficiency.
In one example, the parabolic equation of the basic cross section on the O1X1Y1 coordinate plane of the first coordinate system O1X1Y1Z1 is x12=2Py1, wherein x1 is the X1 coordinate of the coordinate plane O1X1Y1, and y1 is the Y1 coordinate of the coordinate plane O1X1Y1. The parabola of the basic cross section rotates with the O1Y1 coordinate axis as the rotation axis to form a paraboloid; and the angle range in which the paraboloid rotates along the O1Y1 coordinate axis is the horizontal angle range.
The parabolic equation of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1 is x12+z12=2Py1; wherein x1 is the coordinate on the coordinate axis O1X1 of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1, y1 is the coordinate on the O1Y1 coordinate axis of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1, and z1 is the coordinate on the O1Z1 coordinate axis of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1; and the paraboloid passes through the coordinate origin (0, 0, 0) of the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1.
According to the relationship between the first right-handed three-dimensional rectangular coordinate system O1X1Y1Z1 and the second right-handed three-dimensional rectangular coordinate system TXPYPZP, x1=xp, y1=yp+P/2 and z1=zp. The paraboloid equation of the first right-handed three-dimensional rectangular coordinate system is in the form of xp2+zp2=2P(yp+P/2) in the second right-handed three-dimensional rectangular coordinate system TXPYPZP.
The paraboloid passes through point (P,0,0), point (−P,0,0), point (0,−P/2,0), point (0,0,P) and point (0,0,−P) of the second right-handed three-dimensional rectangular coordinate system TXPYPZP. The parabolic equation of the cross section of the reflector parabola on the TXPYP coordinate plane of the second right-handed rectangular coordinate system TXPYPZP is xp2=2P(yp+P/2).
According to the relationship between the second right-handed three-dimensional rectangular coordinate system TXPYPZP and the third right-handed three-dimensional rectangular coordinate system OXYZ, xp=x+P, yp=y, zp=z. The paraboloid equation of the second right-handed three-dimensional rectangular coordinate system TXPYPZP is in the form of (x+P)2+z2=2P(y+P/2) in the third right-handed three-dimensional rectangular coordinate system OXYZ. The paraboloid passes through the origin (0, 0, 0) of the third right-handed three-dimensional rectangular coordinate system.
The parabolic equation of the first cross section of the reflector paraboloid on the OXY coordinate plane of the third right-handed rectangular coordinate system OXYZ is (x+P)2=2P(y+P/2), from which the first parabola function is y=(x+P)2/(2P)−P/2. Based on this, a parabola of the first cross section of the reflector on the coordinate plane OXY of the third right-handed rectangular coordinate system OXYZ can be drawn, as shown in
According to the parabolic equation in the third right-handed rectangular coordinate system OXYZ, when y=0, the equation (x+P)2+z2=P2 of the reflector on the second cross section of the coordinate plane OXZ is obtained. This is an arc with T as the center and P as the radius. The upper and lower edges of the reflector are concentric arcs with T as the center.
According to the parabolic equation of the reflector in the third right-handed rectangular coordinate system OXYZ, it can be concluded that the parabolic function in the third right-handed rectangular coordinate system is y=((x+P)2+z2)/(2P)−P/2.
The paraboloid passes through the origin (0, 0, 0) of the third right-handed rectangular coordinate system. According to the paraboloid function in the third right-handed rectangular coordinate system, y value corresponding to each group of (x,z) values is calculated. A paraboloid data table is listed. A paraboloid reflector processing die is processed according to the data table to manufacture the paraboloid reflector.
The range of the pitch angle is the range of the radiation angle θ of the ultrasonic signal emitted by the ultrasonic emission source from the position point T in the TXp direction on the TXpYp coordinate plane, and the pitch angle θ=art(yp/xp), as shown in
Based on this, taking the focal length P=150 mm as an example, the data table of the first parabola of the paraboloid reflecting surface in Table 1 can be calculated in unit of mm.
The range of the pitch angle and the range of the horizontal angle are both determined according to actual conditions and work requirements; there is no structure between the parabolic reflector and the liquid level of a measured vertical tank to block the ultrasonic signal propagation; and the focal length P is less than or equal to the radius of the measured vertical tank.
Preferably, the range of the pitch angle and the range of the horizontal angle are both determined according to actual conditions and work requirements; there is no structure between the parabolic reflector and the liquid level of a measured vertical tank to block the ultrasonic signal propagation; and the focal length P is less than or equal to the radius of the measured vertical tank.
The range of the pitch angle θ in this embodiment is about −82°˜61°; the range of the horizontal angle is about −80°˜80°. The larger the range of the pitch angle θ and the horizontal angle φ, the more ultrasonic signals emitted by the ultrasonic emission source covered by the reflector, the stronger the reflected wave of the liquid level received by the ultrasonic probe, the more accurate the liquid level measured by the external measurement liquid level meter, the greater the liquid viscosity that can be measured, and the wider the application range.
When the pitch angle θ is close to 90°, the height value of the reflector is close to ∞, which cannot be realized. When the maximum value is 61°, enough ultrasonic signals emitted upward are covered. The negative value of the pitch angle θ has a maximum value of −82°, enough ultrasonic signals emitted downward are covered. When the horizontal angle φ has a value of −80° or 80°, the reflector approaches the tank wall in the horizontal direction, and the reflector can be fixed on the tank wall through the connector.
Further, the method provided by this embodiment further includes: if the tank wall at the probe mounted in the measured vertical tank is in an inclined state, adjusting and selecting an appropriate part of the paraboloid as the reflecting surface of the paraboloid reflector, and finally determining the reflector required for measuring the measured vertical tank, specifically including:
For example, in the third right-handed three-dimensional rectangular coordinate system OXYZ,
Referring to
For the problem of measuring the liquid level of the vertical tank by using a parabolic focusing steering gear with an external measurement liquid level meter, because the measured liquid level is horizontal, the specified direction A that requires the ultrasonic wave to be emitted after being reflected by the steering gear is vertically upward toward the horizontal liquid level. Therefore, the reference line segment is a horizontal straight line segment perpendicular to the specified direction A. Therefore, the coordinate axis O1X1 of the established first right-handed rectangular coordinate system O1X1Y1Z1 is parallel to the reference line segment, and the direction of the coordinate axis O1X1 is rightward.
The specified direction A that requires the ultrasonic wave to be reflected by the steering gear is any direction, and the reference line segment is a straight line segment perpendicular to the specified direction A. The coordinate axis O1X1 of the first right-handed rectangular coordinate system O1X1Y1Z1 is parallel to the reference line segment, and the direction of the coordinate axis O1X1 is the same as the ultrasonic emission direction.
The parabolic equation of the reflector expressed by the three-dimensional right-handed rectangular coordinate system used in the present disclosure can also be transformed into a form of a three-dimensional right-handed polar coordinate system through ordinary coordinate transformation.
According to the present disclosure, the reflector is calculated and determined by using the paraboloid function under the narrowed application range that the reflection directions are parallel, so that the reflecting surface data with any precision requirement can be easily calculated, the man-hour of drawing to verify the correctness of the calculated number is saved, the design and calculation workload is reduced, the design time is shortened, the production efficiency is improved, the purpose of measuring the liquid level of the vertical tank from the side wall by using an external measurement liquid level meter is effectively realized, and the method is more practical and easier to be widely applied.
In this specification, various embodiments are described in a progressive way. The differences between each embodiment and other embodiments are highlighted, and the same and similar parts of various embodiments can be referred to each other. In this specification, specific examples are used to explain the principle and implementation of the present disclosure. The description of the above embodiments is only used to help understand the method of the present disclosure and its core idea. At the same time, according to the idea of the present disclosure, there will be changes in the specific implementation and application scope for those skilled in the art. In summary, the contents of this specification should not be construed as limiting the present disclosure.
Number | Date | Country | Kind |
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202210413543.0 | Apr 2022 | CN | national |
This patent application is a national stage application of International Patent Application No. PCT/CN2022/108766, filed on Jul. 29, 2022, which claims the benefit of and priority to Chinese Patent Application No. 202210413543.0, filed in the Chinese Patent Office on Apr. 14, 2022, each of which is hereby incorporated by reference herein in its.
Filing Document | Filing Date | Country | Kind |
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PCT/CN2022/108766 | 7/29/2022 | WO |