This invention relates to valves resistant to erosion for the fluid carrying solid particles or liquid drops, and more particularly to a closure element in the valves.
It is frequently needed to use a valve assembly to control flow of the fluid in the pipelines which incorporates the solid particles or liquid drops. Upstream surface of the closure element in a prior art valve will be damaged by impingement of such fluid for a short period of time during rotational or linear sliding motion between open and closed positions, so that the closure element loses the sealing capability engaged with upstream seat ring after the valve is closed and the valve begins to leak. And then they will still attack leaking paths formed on the upstream sealing surface of the closure element much stronger in fully closed position and cause them into heavy leaking openings rapidly, the valve has to be removed from the pipelines.
Valve manufacturers have being devoted themselves to improving surface hardness of the closure element made of metallic materials or employed the closure element made of or coated with high hardness ceramics in the prior art valve, in order to enhance its capacity of erosion resistant. It is effective only that hardened surface hardness of the metallic closure element is higher than the hardness of the solid particles, or disadvantage of micro fracture characteristic occurred easily in the ceramics has to be overcome after they are impacted by the solid particles or liquid drops carried in the fluid. The means improving surface hardness of the closure element will greatly increase material cost, expense of hardening process and processing charge machining hardened surface, and is neither a sole nor an universal choice solving erosion resistant.
The magnitude of the impact angles included between the particle flow directions in the fluid and the eroded surface of the different places on surface of the valve closure element, is various during a valve opening or closing operation, and different kinds of materials have their own impact angles at which it is high resistance to erosion, so that it is rather difficult to find out a material for the closure element which can resist the erosion at various impact angles simultaneously.
Additionally, the erosion loss of material is affected by shape, size, hardness and brittleness of the solid particles, as well as velocity and concentration of the particle flow. The solid particle erosion impinged on the surface of materials can be avoided only that the particles are flowing at a very slow velocity, but this way would not be adopted generally, because it will decrease the fluid conveying efficiency.
Surfaces of the ball closure element both in V-port ball valve and in semi-spherical ball valve have a regular curvature, because they are a segmental spheroid with a V-notch flowway or one portion of an entire spheroid respectively, and additionally, the closure element of a plug valve is a truncated cone or a cylinder and its surface also has a regular curvature. Although all of the closure elements are not an entire spheroid and have not a cylindrical flowway there through, they have a similar sealing principle and configuration to the ball valve, and rotate about an axis of their stems between fully open and fully closed positions; therefore the ball valve will be taken as representative of them.
The ball valve and gate valve are described and cited in their illustrations respectively hereinafter.
A pair of annular seat rings 14 are received within recesses 15 and 16 of the left-hand housing section 2 and the right-hand housing section 3 surrounding passageways 13 respectively, and are defined between the valve housing 1 and the ball closure element 17, and have the same inner diameter as the port of the passageways 13 of the housing sections 2 or 3 adjacent to it generally.
The ball closure element 17 is mounted between the two seat rings 14, and has a cylindrical flowway 18 extending there through which axis passes through the center of the ball closure element 17 and is normal to the axis of the stem 19. The flowway 18 of the ball closure element 17 is aligned with the passageways 13 of the housing sections 2 and 3, and permits the fluid to flow through smoothly when the valve 1 is in fully open position as shown in
An imaginary annular spherical surface surrounding the flowway 18a plotted in dotted line, which inner diameter is the same as the upstream seat ring 14, the radial width is equal to the initial stroke length 20 and center of the circle is the point P intersected by the axis 30 of flowway 18a and the upstream surface 22 of the ball closure element 17 in fully closed position, could be constructed on the upstream surface 22 of the ball closure element 17. This annular spherical surface is the sealing surface of the ball closure element 17 engaged with the sealing surface 21 of the upstream seat ring 14 in fully closed position. The point B is located at periphery of the imaginary annular spherical surface.
A lot of tests demonstrated that the needed radial width of the sealing surface of a seat ring depends on leakage classes of a valve, the maximum pressure differential across the valve when it is closed, fluid categories and nature, material of the sealing surface and the coefficients related to the material of the sealing surface. The annular spherical surface of the ball closure element and the sealing surface of the seat ring are a pair of matched sealing surfaces, so the radial width of the annular spherical surface has to be equal to, or just a bit longer than the one of the sealing surface of the seat ring after the radial width of the sealing surface of the seat ring has been determined according to the prior art mentioned above, in order to ensure that an effective sealing between the ball closure element and the seat ring can be achieved. That is to say, the initial stroke length of the ball closure element is the same as the radial width of the seat ring at least.
The initial stroke length of a ball closure element relates to its diameter closely, overlong initial stroke length will not only lengthen the diameter of a ball closure element unduly, and cause cost of production to be raised further, but also increase the actuated torque of the valve, therefore the valve manufacturers always select a diameter for a ball closure element having an initial stroke length just equal to the radial width of sealing surface of the seat ring in fact for meeting the sealing requirement of the valve in a prior art.
The points A and C are two intersections intersected by the flowway 18a, the upstream surface 22 of the ball closure element 17 and the plane through the center ◯ of the ball closure element 17 and normal to the axis of the stem 19 (not shown). The angle included between two radiuses linked such two points and the center ◯ of the ball closure element 17 respectively, is the flowway angle β of the ball closure element 17. The circular arc length between the points A and C facing the flowway angle β is a flowway stroke length of the ball closure element opposite to the inner port diameter of the passageways 13.
As shown in
The point B, which is in the position disengaged with the seat ring finally when opening the valve or the position blocking the passageway at last when closing the valve on the surface of the ball closure element, on the periphery of the annular spherical surface is beside the opening of the ball valve. The area around the point B is exposed to the fluid flowing in upstream passageway for the longest time and eroded at the highest velocity relatively during opening or closing operation. A velocity of the fluid flowing across the point A on the inside edge of the annular spherical surface is higher and time is longer too as it is near the point B for reasons of the narrow initial stroke length. On the other hand, a velocity flowing across the area away from the point B will be much lower, and the time also much shorter than the point B. Whenever the fluid carries the solid particles or liquid drops, the annular spherical surface around the point B will be eroded the most severely because of the highest velocity and the longest time. The damaged annular spherical surface keeps effective engaging with the sealing surface of the seat ring no longer and the valve becomes a much more severe leakage after staying in fully closed position for a short time.
The point B enters into the passageway 13 and the fluid starts to flow through the valve after the ball closure element 17 is turned through the initial stroke length from fully closed position counterclockwise. Provided 1o that the angle θ is smaller than the angle β, some area of not only the exterior but the interior annular spherical surface is exposed to the fluid flowing in the upstream passageway 13, both of the annular spherical surfaces will be eroded severely whenever the fluid carries the solid particles or liquid drops. Differing from the prior art valve, the area around the point B eroded the easiest has not been on the outside edge of the interior annular spherical surface engaged with the sealing surface of seat ring 14 in fully closed position now, but on the periphery of the exterior annular spherical surface not engaged with the sealing surface of seat ring 14 in fully closed position, as a result, the exterior annular spherical surface bears the most severe erosion that should be borne by the interior annular spherical surface, and protects the interior one from much erosion, and it causes the eroded area, time and velocity for the interior annular spherical surface exposed to the fluid flowing in the upstream passageway 13 to be less and slower than the prior art ball valve. The bigger the θ is, the shorter the time is, the less the area is, the slower the velocity that the fluid flows across the area is, so the less the suffered erosion is. Provided that the angle θ is equal to or larger than the angle β, only some area on the exterior annular spherical surface exposed to the upstream passageway 13 will be eroded by the flowing fluid now, any area on the interior annular spherical surface relating to angle γ just leaves or has been moved out of the passageway 13 and would not be eroded. Consequentially the time, area and velocity eroded by the flowing fluid on the interior annular spherical surface depend on the length of the lengthened initial stroke mainly.
In reverse, when the ball closure element 17 starts to be turned from fully open position toward closed direction clockwise, and the area around the point B on the exterior annular spherical surface enters into the valve lo upstream passageway 13 firstly and is eroded by the flowing fluid immediately.
Provided that the angle θ is larger than or equal to the angle β, any area on the inner annular spherical surface has not entered into the passageway 13 yet or just wants to do it when the upstream surface 22 of the ball closure element 17 is rotated to the position where the point B touches the sealing surface 21 of the seat ring 14 and the flow starts to be blocked, so the erosion of the inner annular spherical surface would not take place. During the period of time to keep rotating the ball closure element 17 until it arrives in fully closed position, the inner annular spherical surface entered into the upstream passageway 13 would not be also eroded naturally because the fluid has been blocked by the exterior annular spherical surface and cannot flow.
Provided that the angle θ is smaller than the angle β, some area on the interior annular spherical surface also enters into the passageway 13 following the exterior annular spherical surface and is eroded by the flowing fluid before the point B touches the seat ring 14 and the passageway 13 has been blocked, but the position eroded firstly and severely is still the area around the point B on the exterior annular spherical surface, so that the interior annular spherical surface gets protected by the exterior annular spherical surface to some extent, and it causes the eroded time, area and velocity for the interior annular spherical surface exposed to the fluid flowing in the upstream passageway 13 to be less than the prior art ball valve, until the upstream passageway 13 is blocked by the upstream surface 22 of the ball closure element 17 completely. The factors affecting the extent of the erosion of the interior spherical surface are the same as the description of opening the valve above, and also depend on the magnitude of the angle θ lo or the initial stroke length.
The inner annular spherical surface entered into the passageway 13 would not be eroded yet even through the area around the point B on the exterior annular spherical surface has been damaged somewhat and cannot engage with the sealing surface of the seat ring perfectly after many times of opening and closing operation. The slight leakage between them only lasts a short period of time in which the damaged exterior annular spherical surface is brought into touch with the sealing surface of the seat ring 14, and the velocity of the fluid leaking across the leakage paths is slow, therefore it is not enough to constitute an erosive threat to any area on the interior spherical surface which has entered into the upstream passageway 13. The reason is that the velocity flowing across any area on the inner annular spherical surface should be much lower than the area around point B as it is at a distance from the damaged surface on the exterior annular spherical surface,
The position eroded the most severely on the upstream surface 22 of the ball closure element 17 is the area around point B on the periphery of the exterior annular spherical surface, and a degree of the erosion tapers off from the point B on the exterior annular spherical surface towards the interior annular spherical surface along the upstream surface 22 of the ball closure element 17. Therefore the longer the diameter of a ball closure element is, the longer its initial stroke length is, and the longer the circular arc length facing the angle θ in the initial stroke length is also, the better the interior annular spherical surface will get protected by the exterior annular spherical surface, and the ball closure element becomes much erosion resistant.
A planar radial end face of the annular seat rings 23 establishes sliding engagement with the planar sealing surface of the gate closure element 26. The other rear radial end face is abutted on a shoulder 30 in the annular recesses 29. The valve housing 27 is provided with either wafer or flanges at each end thereof as traditional ways for connected to a pipeline.
A length at the bottom of the upstream surface of the gate closure element 26 from the end edge 25 along the axis of the stem 28 upwards, which is equal to the radial width of the sealing surface of the seat ring 23 normally, is an initial stroke length of the gate closure element 26. Another length being equal to the inner bore diameter of the seat ring 23 on the initial stroke length along the axis of the stem 28 upwards is a flowway stroke length of the gate closure element 26. A length of gate closure element 26 of the prior art gate valve along the axis of the stem 28 is equal to or a little longer than the sum of the radial width of the sealing surface of the seat ring 23 and the inner diameter of the seat ring 23, excluding the length for connecting the stem 28 with the gate closure element 26, after the inner diameter of the passageway 24 has been determined as the description of the ball valve in
For the same reason as the ball valve described above, an overlong gate closure element can also increase a weight and production cost of the valve, thereby the length of a gate closure element of a prior art gate valve along the axis of a stem is exactly the sum of the radial width of the sealing surface and the inner diameter of the seat ring.
It has the same situation during closing the valve also. The area around the middle point B of the end edge 25 starts to be eroded by the flowing fluid as long as it enters into the passageway 24. The area exposed to the passageway 24 gets larger and larger with the valve being closed further, all of the area will be eroded, but the area around the middle point B will be eroded the longest and the velocity of the fluid flowing there through is the highest, so that it suffers the most severe erosion. The fluid stops flowing and the erosion ends after the middle point B of the end edge 25 has slid across the flowway stroke DN and touches the sealing surface of the seat ring 23. The valve arrives in fully closed position after the gate closure element 26 is pushed downwards further and has slid across an initial stroke h (being equal to the radial width b of sealing surface of the seat ring 23) again.
The upstream sealing surface around the middle point B of the end edge 25 of the gate closure element 26 has been severely eroded by the solid particles or the liquid drops incorporated in the fluid repeatedly after many cycles of operating the valve, and the length of its sealing surface engaged with the seat ring 23 has been shortened, the sealing capability between them fails in fully closed position, the valve starts leaking uninterruptedly. The solid particles or the liquid drops will attack and expand the leakage paths rapidly within a relatively short period of time when the gate closure element stays in fully closed position, and cause the valve to be damaged severely.
The longer the initial stroke length H of the gate closure element 26a is lengthened after determined the size of the valve, the wider the width of rectangular area of the lower portion is, the better the surface of the rectangular area of the upper portion engaged with the sealing surface of the seat ring in fully closed position will be protected, so that the gate closure element 26a can get longer life.
The middle point B of end edge 25 in lower portion of the lengthened gate closure element 26a starts to be disengaged with the sealing surface of the seat ring 23 and the fluid flows through the passageway 24, as long as that it enters into the passageway 24 during opening the valve (lifting the stem 28 upwards). The upper and lower portions are both eroded by the fluid, provided that the width L of the rectangular area of the lower portion is shorter than the flowway stroke DN of the valve (being equal to the inner bore diameter of the seat ring 23) during operating the valve, but the lower portion shall be eroded more severely than the upper portion because it is near the point B, so the upper portion can be protected by the lower portion in part. The upper portion is protected by the lower portion completely and will not be eroded by the fluid at all, provided that the width L of the rectangular area of the lower portion is equal or longer than the flowway stroke length DN. The reason is that any area of the upper portion has left or just wants to leave the passageway 24 when the middle point B of end edge 25 enters into the passageway 24.
The principle of closing operation related to the gate closure element of the present invention will not be described, since it is the reverse of the opening valve described above and similar to the description for the ball valve too.
Although the present invention was described in terms of specific embodiments, it is obvious to a person skilled in the art that various alterations and additions are possible without departing from the spirit of the invention which is set out in the appended claims, therefore the extent disclosed in the embodiments above is only for purpose of illustration and not intended to be limited by this description. The art of the present invention valve closure elements are also applicable to full bore ball valve, reduced bore ball valve, V-port ball valve, semi-spherical ball valve, floating ball valve, trunnion ball valve, plug valve, parallel-slide gate valve, knife gate valve and sliding gate valve, etc.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/CN2005/001650 | 10/8/2005 | WO | 00 | 4/8/2008 |