This disclosure concerns a rotating part associated with a hydraulic machine, a hydraulic machine and an installation for converting energy having such a machine.
In the area of the conversion of hydraulic energy into mechanical or electric energy, using a hydraulic machine such as a turbine, pump or Francis-type turbo-pump is known. In turbine mode, the hydraulic machine rotatingly drives a shaft thus transforming hydraulic energy into mechanical energy. The conversion of energy is realized by a wheel which forms a rotating part and includes runners which can be distributed around the axis of rotation of the wheel. The runners extend between a first edge and a second edge which are respectively, during operation, a leading edge and a trailing edge for the flow of water.
One of the challenges persisting in a Francis turbine is the research into the best quality of flow possible downstream of the rotating part. For example, it is important to be able to master the distribution of velocities of the flow leaving the wheel, to avoid cavitation phenomena or also to preserve the stability of the flow, that is to say to avoid the formation of turbulences or vortices.
To do this, a wheel with non-movable runners can have an optimum operating flow rate for which the direction of the water leaving the trailing edge of the runners is relatively parallel to the axis of rotation of the wheel with a relatively uniform distribution of output velocity. In such a configuration, the direction of the water leaving the trailing edge can have a limited rotational component, and the nature of the flow allows harmful phenomena such a vortex to be avoided within the intake duct.
On the other hand, for a flow rate that is different from the optimum operating flow rate, the rotation of the wheel causes the water, leaving the trailing edge, to have a direction which is deflected with respect to the axis of rotation of the wheel and at the same time there is deterioration in the uniformity of the output velocities. Thus, the flow leaving the wheel is of a lesser quality and is even more likely to give rise to an increase in losses, vortices and instabilities.
Similar issues arise with other types of turbines, notably for propeller-type turbines.
In order to address this issue, it is known to use controlled mechanisms to displace the runners of the Kaplan, Bulbe or Deriaz turbines according to the turbine flow rate so as to maintain a good quality of flow downstream of the wheel. However, such mechanisms increase the end cost of the turbine and their use is limited to restricted heights of head applied to turbines.
A rotating part of a hydraulic machine is disclosed which, when it is traversed by a flow of water, rotates around an axis of rotation and which comprises: runners which are distributed around the axis of rotation and each extend between a leading edge and a trailing edge, wherein each runner includes: a first part which defines its leading edge; and a second part which is attached to the first part and defines its trailing edge at least in part, the second part being elastically deformable or displaceable in a reversible manner with respect to the first part, under the action of the flow of water, said second part defining, when the machine operates, the direction of flow of water downstream of the runner.
Features of the invention will be better understood and other advantages of the same will appear more clearly in light of the description which will follow regarding embodiments of a rotating part which is associated with a hydraulic machine, given by way of example and referring to the accompanying drawings in which:
The present disclosure proposes a hydraulic machine which allows the quality of the flow leaving the wheel to be improved over a wider range of flow rates.
To this end, the rotating part of a hydraulic machine is disclosed which, when it is traversed by a flow of water, rotates around an axis of rotation and which includes runners which can be distributed around the axis of rotation and each extend between a leading edge and a trailing edge. According to the exemplary embodiment, each runner of the rotating part includes a first part which defines its leading edge and a second part which is attached to the first part and defines its trailing edge at least in part, whilst the second part is elastically deformable or displaceable in a reversible manner with respect to the first part, under the action of the flow of water, the second part defining, when the machine operates, the direction of the flow of water downstream of the runner.
The runners can be deformed according to the flow rate of incoming water, in order to direct the water leaving the trailing edge along an adapted direction which optimizes the quality of the flow leaving the wheel.
According to advantageous but not obligatory aspects, a rotating part associated with a hydraulic machine can incorporate one or several of the following characteristics, taken in all combinations that can be technically admissible:
A hydraulic machine is also disclosed which includes a rotating part as defined previously.
An installation is also disclosed for converting hydraulic energy into electric energy or mechanical energy which includes a hydraulic machine such as defined previously.
The profile of the runners 208 shown in dotted lines can be seen in
The runners 208 of the wheel 202 can be formed in two parts. A first part 208A defines the leading edge 2080 of each runner and a second part 208B defines its trailing edge 2082 and is attached to the first part 208A. As can be better seen in
In a known manner, in a rotating datum-point linked to the wheel, the water flows tangentially to the lower surface 2084′ and to the upper surface 2086′, along the profile of the runner. More precisely, a chord 2088′ is defined as a line that is equidistant from the lower surface 2084′ and from the upper surface 2086′. The chord 2088′ goes through the leading edge 2080′ and through the trailing edge 2082′. Thus, the upper edge 2086′ and the lower edge 2082′ converge on the chord 2088′. In the first instance, the chord 2088′, in its extension of the trailing edge 2082, defines the direction D208′ of flow of the water leaving the runner 208. A velocity vector {right arrow over (V′2)} is defined which shows the velocity of the water in a relative datum-point linked to the wheel and which is obtained for a flow having an optimum operating flow rate. The vector {right arrow over (V′2)} extends along the direction of flow D208′.
In an absolute datum-point, that is to say which does not rotate at the same time as the wheel, the water further includes a rotational component {right arrow over (U)} that is created by the rotation of the wheel. In the configuration of an optimum operating flow rate, the sum of the vector {right arrow over (V′2)} and of the vector U gives a vector {right arrow over (C′2)} which is principally output, that is to say which is oriented parallel to an axis Z202′ of rotation of the wheel, and is directed downward, in the direction of the intake duct 26. The result comes from the fact that the velocity {right arrow over (V′2)} leaving the runner 208 can have a rotational component {right arrow over (U)}′2 which is directly opposed to the velocity {right arrow over (U)} of rotation of the wheel. Thus, the water circulating between the runners 208′ falls vertically directly into the intake duct 26. The risk of a vortex appearing is therefore limited and the flow leaving the wheel is more stable.
On the other hand, for a flow rate that is different from the optimum operating flow rate, for example, equal to half the optimum operating flow rate, the tangential velocity leaving the runner, called {right arrow over (V′1)}, is two times less than the velocity obtained for an optimum operating flow rate. As a result, when the velocity vector {right arrow over (V′1)} is added to the velocity vector {right arrow over (U)} which is linked to the rotation of the wheel, the result is a velocity vector {right arrow over (C′1)} which is not parallel to the axis of rotation Z202′ of the wheel. In fact, the velocity {right arrow over (V′1)} can have a rotational component {right arrow over (U′1)} which is not large enough to compensate for the velocity {right arrow over (U)} of ration of the wheel. Thus, the fluid, leaving the runners 208′ of the wheel, is made to rotate around the axis of rotation Z202′. The rotation can bring about the appearance of vortices, increase turbine losses and damage the overall quality of the flow leaving the wheel.
Following the description details of the operating of one single runner 208 of the wheel 202 according to exemplary embodiments, are given as this can be transposed to the other runners of the wheel 202. The runner, which is shown on its own in
For the clarity of the drawing, the chord 2088 is only shown in the third configuration in
When the turbine 20 is fed, the second part 208B is deformed elastically following a rotational movement with respect to the first part 208A. The movement is shown in
When the flow rate reduces, the part 208B of the runner 208 is displaced as a result of the effect of the material making up the part 208B elastically recovering its shape in the direction opposite the arrow F1. There is therefore reversible deformation. For example, if the wish is to operate the turbine at a flow rate that is two times less than the optimum operating flow rate, the second part 208B of the runner 208 goes from the third to the second configuration. This is the to be a passive system as the form of the runner adapts automatically according to the feed flow rate of the turbine 20 without any outside intervention. When the operating of the turbine is stopped, the second part 208B returns into its first position. The first position is therefore a predetermined position of the runner 208 when the turbine is not operating.
Only three configurations can be shown in
Furthermore, the second part 208B of the runner is deformed such that the rotational component, that is to say the component which is ortho-radial to the axis of rotation Z202 of the wheel 202, of the tangential velocity of the flow S′ opposes the velocity of rotation of the wheel overall.
The velocity of the flow for the second configuration in a datum-point linked to the wheel is noted as {right arrow over (V1)}. The velocity vector {right arrow over (V1)} is overall tangential to the profile of the runner at the trailing edge 2082 and is oriented along the direction of flow 208 defined by the rectilinear extension of the chord 2088. The second part 208B of the runner can have a different position compared to the runner 208′ of a wheel of the prior art, the vector {right arrow over (V1)} is therefore oriented differently compared to the vector {right arrow over (V′1)}. The extension of the chord 2088 downstream of the trailing edge when the runner is in its second position defines the direction D2081 which is different from the direction D208′. In fact, the vector {right arrow over (V1)} includes a vertical component {right arrow over (C1)} parallel to the axis of rotation Z202 and a rotational component {right arrow over (U1)} which is ortho-radial to the axis Z202. In the configuration, the component {right arrow over (U1)} is directly opposite to the velocity vector {right arrow over (U)} of rotation of the wheel 202. Thus, in a fixed datum-point, the sum of the vector {right arrow over (V1)} and the vector {right arrow over (U)} directly gives the vector {right arrow over (C1)} which is principally output.
Regarding the third configuration, the velocity of the water leaving the runner 208 in a movable datum-point linked to the wheel is noted as {right arrow over (V2)}. The velocity is oriented along the direction of flow D2082 defined by the rectilinear extension of the chord 2088. The direction D2082 is analogous to the direction D208′ for the runner 208′ in
Thus, the elastic deformation of the second part 208B of the runner 208 allows a flow to be obtained with a principally output direction when leaving the runners 208, for various operating points of the turbine. This allows a good quality of flow leaving the wheel 202 to be preserved.
The deformation of the second part 208B of the runner 208 is facilitated by the fact that the material making up the second part 208B can have a modulus of elasticity which is about twenty times less than that of the material making up the first part 208A. More precisely, the material of the second part 208B of the runner 208 can have a modulus of elasticity of between 0.5 GPa and 200 GPa inclusive, notably equal to 10 GPa, whilst the part 208A is in metal, notably steel.
When the operating flow of the turbine is reduced or when the turbine stops operating, the corner 2083 relaxes in order to recover its initial form and therefore pushes the second part 208B in a direction opposite to the arrow F2 in
A third embodiment is shown in
In another exemplary embodiment that is not shown, the second part 208B is formed by a number of elements that is different to three.
In another exemplary embodiment that is not shown, the elements 208B1, 208B2 and 208B3 can be articulated on the first part 208A independently of one another.
As a variant, the second part 208B can define the totality of the trailing edge 2082, whilst having a variable length L208B.
In the example shown, the covering 208B1 surrounds the rigid core 208B2. In another exemplary embodiment, the covering 208B1 is arranged solely in the top part or in the bottom part of the rigid core 208B2.
According to another variant, the core 208B2 is fixed to the first part 208A by soldering.
As can be seen in
In an analogous manner to the five first embodiments, the second part 208B of the runner 208 is elastically deformable so as to adapt the best to the operating point of the turbine. The advantage of using a composite material for the shell of the second part 208B is that it bestows it with good mechanical strength.
In another exemplary embodiment that is not shown specific to the sixth embodiment, the arrangement and the number of layers within the shell can be different.
In another exemplary embodiment not shown that is applicable to the six first embodiments, the second part 208B of the runners 208 is fixed to the crown 2022 and/or to the band 2020.
The runners 208 of the propeller turbine can be realized in two parts. A first part 208A defines the leading edge 2080 of each runner when seen through the flow E and is integral with the hub 205. A second part 208B defines the trailing edge 2082 of each runner when seen through the flow E. The part 208B is attached to the first part 208A but is not integral with the hub 205. The second part 208B is realized in an elastically deformable material. Thus, as the flow E passes, the second part 208B of the runners 208 is deformed in order to define the direction of the flow E of water downstream of the runner 208. More precisely, the deformation of the second part 208B of the runner 208 allows the water, leaving the runner 208, to be directed along a direction parallel to the axis Z204 of rotation of the hub 205 and of the shaft 204. This is also called an output direction. The flow leaving the runners or the blades 208 is therefore stable.
In a variant that is not shown that is applicable to the seventh embodiment, the second part 208B of the runner 208 is not integral with the hub 205.
In a variant that is not shown of the embodiment in
According to another variant that is not shown of the embodiment in
In a variant that is not shown that is applicable to the first, third, fourth and sixth embodiments, the first part 208A and the second part 208B can be glued or screw-connected together.
In a variant is not shown, the axis of rotation Z202 of the wheel is horizontal.
Exemplary embodiments are also applicable to Bulbe-type, Kaplan-type or Deriaz-type turbines.
The variants and embodiments above can be combine to give new embodiments as well.
Thus, it will be appreciated by those skilled in the art that the present invention can be embodied in other specific forms without departing from the spirit or essential characteristics thereof. The presently disclosed embodiments are therefore considered in all respects to be illustrative and not restricted. The scope of the invention is indicated by the appended claims rather than the foregoing description and all changes that come within the meaning and range and equivalence thereof are intended to be embraced therein.
Number | Date | Country | Kind |
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13 54771 | May 2013 | FR | national |
This application claims priority as a continuation application under 35 U.S.C. § 120 to PCT/EP2014/060207 filed as an International Application on May 19, 2014 designating the U.S., and which claims priority to French Application 1354771 in France on May 27, 2013. The entire contents of these applications are hereby incorporated by reference in their entireties.
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Number | Date | Country | |
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20160076508 A1 | Mar 2016 | US |
Number | Date | Country | |
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Parent | PCT/EP2014/060207 | May 2014 | US |
Child | 14952274 | US |