# Patent

## Title
Detecting the clogging of a fluid filter

## Abstract

A method of detecting clogging of a fluid filter is disclosed. The method includes measuring, at successive sampling instants, the pressure difference ΔP from upstream to downstream across the filter, calculating the first time derivative {ΔP}′ of the pressure difference ΔP at different instants, and then sending a clogging signal SC representative of the filter being clogged when the first derivative {ΔP}′ is equal to zero.

## Background
CROSS-REFERENCE TO RELATED APPLICATIONS
This application is a division of U.S. application Ser. No. 12/364,754 filed Feb. 3, 2009, the entire contents of which is incorporated herein by reference. U.S. application Ser. No. 12/364,754 claims the benefit of priority from prior French Application No. 08 50744 filed Feb. 6, 2008.


FIELD OF THE INVENTION
The present invention relates to the field of fluid filters.
More particularly, the invention relates to a method and a device for detecting the clogging of a fluid filter.
BACKGROUND OF THE INVENTION
A fluid circuit is generally fitted with a filter that serves to filter the fluid, i.e. to remove impurities and residues therefrom that might otherwise damage the equipment in which the fluid flows. By way of example the fluid may be a lubricant such as oil, or it may be a fuel.
In use, by recovering such impurities and residues, the filter clogs up progressively, and ends up preventing fluid from passing through the filter. In order to avoid that situation, the branch of the fluid circuit having the filter mounted therein includes a bypass circuit in parallel. This configuration is shown in FIG. 1, which shows the state of the art. In the description below, the terms “upstream” and “downstream” are defined relative to the normal flow direction of the fluid in the circuit. The filter 20 is mounted in a main branch 10 of a fluid circuit. Upstream from the filter, the main branch 10 splits into two branches, a first branch 12 extending the main branch 10 and having the filter 20 mounted therein, and a second branch 14 having a check valve device 40 mounted therein (a “bypass” device). Downstream from the bypass device 40, the second branch 14 rejoins the first branch 12 downstream from the filter 20 so as to reform the main branch 10, such that the bypass device 40 is mounted in parallel with the filter 20. Consequently, the fluid pressure upstream from the bypass device 40 is substantially equal to the pressure P upstream from the filter 20. In FIG. 1, the fluid flows from left to right, as represented by arrow F.
When the filter is not clogged with impurities, i.e. at the beginning of its operation, the pressure Pf immediately downstream from the filter 20 (in the first branch 12) is substantially equal to the pressure P upstream from the filter 20. Similarly, the pressure Pdc immediately downstream from the bypass device 40 (in the second branch 14) is substantially equal to the pressure P upstream from the bypass device 40. All of the fluid flows in the branch 12, and the fluid in the upstream portion of the branch 14 is blocked by the bypass device 40. This bypass device 40 behaves like a valve that allows fluid to pass only when the pressure difference ΔP=P−Pdc from upstream to downstream across the bypass device 40 is greater than a critical value ΔPC. Such a bypass device 40 is known in the prior art. For example it may be a device comprising a ball valve, operating in the manner recalled briefly above.
A device with a ball valve comprises a container containing a ball and a spring. When the ball valve device is in its closed position, the ball is urged by the spring to block the upstream end of the container and thereby prevents the fluid in the portion of the branch situated upstream from the container from penetrating therein. When the pressure of the fluid upstream from the container increases relative to the pressure of the fluid downstream from the container, the force exerted by said fluid by the ball, and thus against the spring, increases in proportion. At a certain critical value ΔPC for the pressure difference between upstream and downstream of the ball valve device, the reaction force from the spring is exactly counterbalanced by the force generated by the pressure ΔPC on the ball. When this pressure exceeds the critical value ΔPC, the ball is pushed downstream and thus allows the fluid to pass through the ball valve device, which is then in its open position.
It will be understood that as the filter 20 becomes clogged as a result of impurities accumulating thereon, the upstream to downstream pressure difference ΔP=P−Pf across the filter 20 increases. The pressure difference across the bypass device 40 also increases since this difference is substantially equal to the pressure difference across the filter, since the first branch 12 including the filter 20 and the second branch 14 including the bypass device are in parallel. The bypass device 40 is calibrated in such a manner as to switch to its open position when the filter 20 becomes completely clogged. Thus, the critical value ΔPC is referred to as the clogging value (or the “clogging pressure difference”).
Once the filter 20 is completely clogged, the fluid thus passes via the second branch 14 of the circuit, through the bypass device 40, and is therefore no longer filtered. The fluid therefore continues to reach the downstream mechanism for which it is intended (e.g. an engine if the fluid is a fuel, a ball bearing or any other moving part if the fluid is an oil), but it does so filled with impurities. The impurities run the risk of damaging the mechanism, and in practice it is therefore essential to replace the filter 20 before it becomes completely clogged.
That is why the filter 20 is used in association with a pressure detector that informs the user (e.g. the pilot) that the filter 20 is about to become clogged and needs to be replaced quickly. FIG. 1, showing the prior art, shows one such detector 60. The detector 60 is mounted in a third branch 16 that is connected to the first branch 12 on either side of the filter 20. The detector 60 is a device that is known in the prior art (e.g. it is of the pressure contact type) and its structure is not described in detail here. It operates on the following principle: when the pressure difference ΔPm across the detector 60 reaches a threshold value ΔPS′ the pressure contact sends a signal (typically an electrical signal) to the user to inform the user that the pressure difference ΔPm across the detector 60 has crossed the threshold value ΔPS. The threshold value ΔPS is selected to be less than the clogging critical value ΔPC (e.g. 90% of said critical value). Thus, when the signal coming from the detector 60 is received by the user, the user knows that the filter 20 needs to be replaced soon, and sufficient time remains for the replacement to take place before the filter 20 becomes completely clogged. This information is passed on to the maintenance crew who perform the change in good time during a subsequent maintenance operation.
When the filter 20 is still not completely clogged, merely replacing the filter suffices prior to putting the circuit back into operation. However, it can happen that the maintenance crew performs this maintenance operation late, possibly after the filter 20 has become completely clogged. Under such circumstances, the filter 20 will have been bypassed and fluid will have continued to flow in the circuit, taking impurities through the bypass device 40 into the entire circuit downstream from the filter 20. Under such circumstances, it is essential for the circuit to be inspected exhaustively and cleaned, which operations are much more burdensome than replacing a filter. When the maintenance crew are performing a maintenance operation, it is therefore necessary for them to know whether or not the filter has already become clogged and has been bypassed.
That is why the portion of the second branch 14 that is situated downstream from the bypass device 40 is provided with a visual indicator 70 (see FIG. 1) that shows whether the fluid has flowed in the downstream portion of the second branch 14, i.e. whether the fluid has passed through the bypass device 40. The visual indicator 70 reveals such passage of fluid when the bypass device 40 is inspected visually. The visual indicator 70 may, for example, be a pop-up type indicator, i.e. it has a tongue that is initially contained inside the visual indicator 70 (the tongue is therefore not visible from the outside). Such a visual indicator 70 is known in the prior art and its operation is not described in detail herein. When the fluid passes through the portion of the second branch 14 that is situated downstream from the bypass device 40 and where the visual indicator 70 is located, the visual indicator 70 causes the tongue to move so that it can be seen by the maintenance crew. Thus on looking at the bypass device 40 (and its visual indicator 70), the crew can tell immediately whether the filter 20 has become clogged and whether or not it has been bypassed.
That clogging detection system associated with the filter 20 nevertheless presents the drawback that it is necessary to inspect the visual indicator 70 in order to know whether the filter has become completely clogged or has been clogged only partially.
OBJECT AND SUMMARY OF THE INVENTION
The invention seeks to propose a method of detecting the clogging of a filter that makes it possible to eliminate the need to use the visual indicator and to inspect it when performing a maintenance operation.
This object is achieved by the fact that the method of detecting clogging of the filter comprises measuring, at successive sampling instants, the pressure difference ΔP from upstream to downstream across the filter, then calculating at different instants the first time derivative {ΔP}′ of the pressure difference ΔP, and then sending a clogging signal SC representative of the filter being clogged when the first derivative {ΔP}′ is equal to zero.
By means of these provisions, the user (e.g. the pilot of the airplane if the filter is in a circuit of a turbojet) and the maintenance crew are informed that the filter is clogged. When the filter is completely clogged, the pressure difference ΔP across the filter becomes constant and remains constant. The first derivative {ΔP}′ of the pressure difference ΔP then becomes zero and the clogging signal SC is sent.
Advantageously, prior to sending the clogging signal SC, the method includes sending a threshold signal SS when the pressure difference ΔP exceeds a threshold value ΔPS less than the pressure difference ΔPC corresponding to the filter being clogged.
Thus, a single sensor is used for detecting both crossing the threshold value ΔPS and crossing the clogging value ΔPC that indicates that the filter is completely clogged, instead of using a detector and a visual indicator. This reduces costs both on purchase, and during maintenance of the filter, as explained above. The user and the maintenance crew are informed both of the fact that the filter is partially clogged beyond a level corresponding to the threshold value, and that the fact the filter is or is not completely clogged, without it being necessary to inspect the visual indicator.
The invention also provides a detector device for detecting clogging of a fluid filter, the device being mounted on a circuit for said fluid.
According to the invention, the detector device comprises: a sensor connected to the circuit upstream and downstream from the filter, and suitable for measuring, at successive sampling instants, the upstream to downstream pressure difference ΔP across the filter; and a processor suitable for calculating at different instants the first time derivative {ΔP}′ of the pressure difference ΔP, and suitable for sending a clogging signal SC representative of clogging of the filter when the first derivative {ΔP}′ is equal to zero.
Advantageously, prior to sending the clogging signal SC, the processor is suitable for sending a threshold signal SS when the pressure difference ΔP exceeds a threshold value ΔPS less than the clogging pressure difference ΔPC corresponding to the filter being clogged.



BRIEF DESCRIPTION OF THE DRAWINGS
The invention can be better understood and its advantages appear more clearly on reading the following detailed description of an embodiment given by way of non-limiting example. The description refers to the accompanying drawings, in which:
FIG. 1 is a diagram of a prior art filter and method for detecting clogging of the filter;
FIG. 2 is a diagram of a filter of the invention and of the method of the invention for detecting clogging of the filter; and
FIG. 3 is a graph showing the variation over time in the pressure difference ΔP across the filter, the variation in the first derivative of said pressure difference ΔP, and the variation in the second derivative of said pressure difference ΔP.



MORE DETAILED DESCRIPTION
FIG. 2 shows a filter 20 mounted in a main branch 10 of a fluid circuit. By way of example, the filter 20 may be mounted in a fluid circuit of a turbomachine. The fluid may be constituted, for example, by a lubricant such as oil, or by a fuel. Upstream from the filter 20, the main branch 10 splits into two branches, a first branch 12 that extends the main branch 10 and that has the filter 20 mounted therein, and a second branch 14 that has a bypass device 40 mounted therein. Downstream from the bypass device 40, the second branch 14 rejoins the first branch 12 downstream from the filter 20 so as to reform the main branch 10, so that the bypass device 40 is mounted in parallel with the filter 20. In FIG. 2, the fluid flows from left to right as represented by the arrow F.
A sensor 160 is connected to the first branch 12 containing the filter 20, on either side of the filter 20. Thus, a third branch 16 of the fluid circuit connects the first branch 12 upstream from the filter 20 to the second branch 12 downstream from the filter 20 via the sensor 160, which is mounted in said third branch 16. The connection of the third branch 16 upstream from the filter 20 is thus located downstream from the connection of the second branch 14 that is upstream from the filter 20, and the connection of the third branch 16 downstream from the filter 20 is thus located upstream from the connection of the second branch 14 that is downstream from the filter 20. It would also be possible to connect the third branch 16 to the main branch 10 upstream from the filter 20 and upstream from the location where the second branch 14 is connected to said main branch 10, and to connect the third branch 16 to the main branch 10 downstream from the filter 20 downstream from the location where the second branch 14 is connected to said main branch 10. Whatever the configuration, the first branch 12 including the filter 20 and the third branch 16 including the sensor 160 are in parallel, and the pressure difference across the ends of the sensor 160 is substantially equal to the pressure difference ΔP (head loss) across the ends of the filter 20. The solution shown in FIG. 2 (the third branch 16 in parallel with the first branch 12, i.e. closer to the ends of the filter 20) is preferable since the pressure difference measured by the sensor 160 is then closer to the pressure difference ΔP across the ends of the filter, given that the head loss due to the length of the branches in the circuit has no influence on the measurement. The sensor 160 is also connected to a processor 165 capable of processing a signal, typically an electrical signal. The sensor 160 is a device that is known in the prior art, as is the processor 165 associated therewith. Their structures are therefore are not described in detail below.
The sensor 160 is suitable for continuously measuring the pressure difference ΔP across the filter 20 in the third branch 16. Thus, the pressure difference ΔP is measured at successive time intervals, these instants at which the measurement is taken constituting sampling over time. Ideally, these intervals are substantially regular, and the instants at which the measurement is taken are sufficiently close together to reproduce reliably the variations over time in the pressure difference ΔP. This variation in the difference ΔP is shown in FIG. 3. The pressure difference ΔP increases continuously from zero up to a value ΔPC corresponding to the filter 20 being completely clogged and to the bypass device 40 opening and allowing fluid to pass therethrough in the second branch 14. Once the filter 20 has become clogged, the difference ΔP remains constant and equal to the clogging value ΔPC.
The sensor 160 sends a threshold signal SS (typically an electrical signal) to the user (e.g. the pilot) when the pressure difference ΔP across the sensor 160 (i.e. across the filter 20) reaches a threshold value ΔPS, i.e. at the instant tS in FIG. 3 (or the measurement instant immediately following tS). The threshold value ΔPS is selected to be less than the clogging value ΔPC, as shown in FIG. 3 (e.g. 90% of said critical value). Thus, when the signal coming from the sensor 160 is received by the user, the user knows that the filter 20 needs to be replaced soon. This information is forwarded to the ground crew who then perform this replacement in good time during a subsequent maintenance operation.
In addition, because the pressure difference ΔP is measured continuously by sampling, the processor 165 can make use of this continuous measurement for calculating, at least each sampling instant, or at a plurality of said instants, the derivative d/dt (ΔP) of the pressure difference ΔP relative to time (this derivative is the derivative of the measurement signal delivered by the sensor 160 to the processor 165, the measurement signal being proportional to the pressure difference ΔP). This first derivative is written {ΔP}′. Thus, the derivative




  
    d
    
      d
      ⁢
      
        
      
      ⁢
      t
    
  
  ⁢
  
    (
    
      Δ
      ⁢
      
        
      
      ⁢
      P
    
    )
  




is calculated at an arbitrary instant t1 (written





  
    
      
        d
        
          d
          ⁢
          
            
          
          ⁢
          t
        
      
      ⁢
      
        (
        
          Δ
          ⁢
          
            
          
          ⁢
          P
        
        )
      
    
    ]
  
  1




or {ΔP}′1) can be calculated, e.g. by using two measurements ΔP1 and ΔP2 of the pressure difference ΔP at the instant t1 and at the following instant t2 by applying the following formula:





  
    
      
        
          
            
              
                d
                
                  d
                  ⁢
                  
                    
                  
                  ⁢
                  t
                
              
              ⁢
              
                (
                
                  Δ
                  ⁢
                  
                    
                  
                  ⁢
                  P
                
                )
              
            
            ]
          
          1
        
        =
        
          
            
              Δ
              ⁢
              
                
              
              ⁢
              
                P
                2
              
            
            -
            
              Δ
              ⁢
              
                
              
              ⁢
              
                P
                1
              
            
          
          
            
              t
              2
            
            -
            
              t
              1
            
          
        
      
    
    
      
        (
        I
        )
      
    
  




The closer together the instants t1 and t2, the more accurate the calculation of the derivative. Ideally, the instants t1 and t2 are therefore selected to be two successive sampling instants. This therefore produces a continuous measurement of the derivative {ΔP}′ of the pressure difference across the filter 20.
When the filter 20 is completely clogged (i.e. at instant tc in FIG. 3), the pressure difference ΔP across the filter 20 becomes constant and remains constant (prior to the filter becoming clogged, the pressure difference increases over time, so its derivative is strictly positive). The derivative {ΔP}′ of the pressure difference then becomes zero, as shown in FIG. 3, which plots variation in the derivative {ΔP}′ as a function of time. When the derivative {ΔP}′ becomes zero (i.e. at a measurement instant equal to or immediately greater than tc), the processor 165 sends a clogging signal SC to the user who is then informed that the filter 20 has become completely clogged.
Thus, by using a single sensor (the sensor 160) and a processor 165, it is possible to inform the user (and thus the maintenance crew) that the filter 20 is clogged either partially or completely, without it being necessary to use a visual indicator on the bypass device 40.
The processor 165 may be incorporated in the sensor 160 or it may be separate therefrom. Under such circumstances, the processor 165 may be included in the engine monitoring unit (EMU) or in the airplane maintenance unit.
In order to confirm the fact that the filter is completely clogged, it is possible to configure the processor 165 so that the clogging signal SC is delivered only when the first derivative {ΔP}′ is equal to zero on at least two successive instants. The processor 165 could calculate a first derivative of zero in error, or the calculation could take place at the extremum of a fluctuation in the pressure difference ΔP (and thus give a first derivative that is zero). The probability of such an error occurring at two distinct instants is minimal, so it then becomes certain that the filter is completely clogged if the first derivative {ΔP}′ is equal to zero at two successive instants (e.g. at two successive sampling instants).
It is also possible to confirm the fact that the filter is completely clogged by calculating the second derivative




  
    
      d
      2
    
    
      d
      ⁢
      
        
      
      ⁢
      
        t
        2
      
    
  
  ⁢
  
    (
    
      Δ
      ⁢
      
        
      
      ⁢
      P
    
    )
  




of the pressure difference ΔP. When the first derivative is zero over a time interval of non-zero duration (and not just at a single point), the second derivative is zero over that interval. Thus, by using the processor 165 to calculate both the first derivative {ΔP}′ of the pressure difference ΔP at a given instant t1 and its second derivative (written {ΔP}′′) at said instant t1, it is possible to ensure that the pressure difference ΔP is constant over a time interval around the instant t1. In present circumstances, this means that the pressure difference ΔP is constant at all times greater than t1, and thus that the filter 20 is completely clogged. It can be seen in FIG. 3 that the second derivative of the pressure difference ΔP is zero at all times t greater than the instant tc when the filter becomes completely clogged. The second derivative {ΔP}′′ at an arbitrary instant t1 (written





  
    
      
        
          d
          2
        
        
          d
          ⁢
          
            
          
          ⁢
          
            t
            2
          
        
      
      ⁢
      
        (
        
          Δ
          ⁢
          
            
          
          ⁢
          P
        
        )
      
    
    ]
  
  1




or {ΔP}′1) can be calculated, e.g. by using two measurements ΔP1 and ΔP2 of the pressure difference at the instant t1 and at the following instant t2 (e.g. the sampling instant following the instant t1), and by applying the following formula together with formula (I):





  
    
      
        
          
            
              
                
                  d
                  2
                
                
                  d
                  ⁢
                  
                    
                  
                  ⁢
                  
                    t
                    2
                  
                
              
              ⁢
              
                (
                
                  Δ
                  ⁢
                  
                    
                  
                  ⁢
                  P
                
                )
              
            
            ]
          
          1
        
        =
        
          
            
              
                
                  
                    
                      
                        d
                        
                          d
                          ⁢
                          
                            
                          
                          ⁢
                          t
                        
                      
                      ⁢
                      
                        (
                        
                          Δ
                          ⁢
                          
                            
                          
                          ⁢
                          P
                        
                        )
                      
                    
                    ]
                  
                  2
                
                -
                
                  
                    d
                    
                      d
                      ⁢
                      
                        
                      
                      ⁢
                      t
                    
                  
                  ⁢
                  
                    (
                    
                      Δ
                      ⁢
                      
                        
                      
                      ⁢
                      P
                    
                    )
                  
                
              
              ]
            
            1
          
          
            
              t
              2
            
            -
            
              t
              1
            
          
        
      
    
    
      
        (
        II
        )
      
    
  




Thus, in order to confirm that the filter is completely clogged, it is possible to configure the processor 165 to calculate the second time derivative {ΔP}′′ of the pressure difference ΔP at different instants, and for the clogging signal SC to be sent to the user only when the second derivative {ΔP}′′ and the first derivative {ΔP}′ are equal to zero. This situation can only happen at instants that are later than the clogging instant tc, so it is certain that the filter is completely clogged.
Alternatively, given that when the first derivative is zero over a time interval of non-zero length, the derivative of order N (where N is greater than 2) is zero over said interval, and by calculating at a given instant t1, simultaneously the first derivative {ΔP}′ of the pressure difference ΔP and its Nth order derivative (written {ΔP}N), it is possible to ensure that the pressure difference ΔP is constant at any instant greater than t1, and thus that the filter 20 is completely clogged. Calculation of the Nth order derivative is trivial by iterating the formula (II).
The invention also provides a device for detecting clogging of the filter 20, the device comprising a sensor 160 and a processor 165 operating as stated above.

## Claims

1. A detector device for detecting clogging of a fluid filter, the detector device being mounted in a circuit for said fluid and comprising:
a sensor connected to said circuit both upstream and downstream from said filter and configured to measure, at successive sampling instants, a pressure difference ΔP across said filter;
a bypass device connected to said circuit upstream and downstream from said filter and allowing the fluid to pass only when the pressure difference across said bypass device is greater than a critical value ΔPC corresponding to the filter being clogged; and
a processor configured to calculate, at different instants, a first time derivative {ΔP}′ of said pressure difference ΔP, and configured to send a clogging signal SC representative of clogging of said filter when the first derivative {ΔP}′ is equal to zero.

2. A detector device according to claim 1, wherein, prior to sending said clogging signal SC, said processor is configured to send a threshold signal SS when said pressure difference ΔP exceeds a threshold value ΔPS less than the clogging pressure difference ΔPC that corresponds to said filter being clogged.

3. A detector device according to claim 1, wherein said processor is incorporated in said sensor.

4. A detector device according to claim 1, wherein said processor is configured to calculate, at different instants, a second time derivative {ΔP}′′ of said pressure difference ΔP, and is configured to send said clogging signal SC only when both said second derivative {ΔP}′′ and said first derivative {ΔP}′ are equal to zero.

5. An assembly comprising:
a fluid circuit; and
a detector device for detecting clogging of a fluid filter, the detector device being mounted in said fluid circuit, the detector device comprising:
a sensor connected to said circuit both upstream and downstream from said filter and configured to measure, at successive sampling instants, a pressure difference ΔP across said filter;
a bypass device connected to said fluid circuit upstream and downstream from said filter and allowing the fluid to pass only when the pressure difference across said bypass device is greater than a critical value ΔPC corresponding to the filter being clogged; and
a processor configured to calculate, at different instants, a first time derivative {ΔP}′ of said pressure difference ΔP, and configured to send a clogging signal SC representative of clogging of said filter when the first derivative {ΔP}′ is equal to zero.

6. A turbomachine comprising:
a fluid circuit provided with a filter; and
a detector device for detecting clogging of said filter, the detector device being mounted in said fluid circuit, the detector device comprising:
a sensor connected to said circuit both upstream and downstream from said filter and configured to measure, at successive sampling instants, a pressure difference ΔP across said filter;
a bypass device connected to said fluid circuit upstream and downstream from said filter and allowing the fluid to pass only when the pressure difference across said bypass device is greater than a critical value ΔPC corresponding to the filter being clogged; and
a processor configured to calculate, at different instants, a first time derivative {ΔP}′ of said pressure difference ΔP, and configured to send a clogging signal SC representative of clogging of said filter when the first derivative {ΔP}′ is equal to zero.