Patent Abstract:
A method for evacuating a chamber employs a pump arrangement composed of a booster pump and of a downstream forepump is connected to the chamber. The booster pump is accelerated, gas from the chamber is introduced into the booster pump, such that from the booster pump there is temporarily extracted an excess power which exceeds the power provided by the drive of the booster pump. The gas is discharged through a bypass valve while the outlet pressure of the booster pump lies above a predefined threshold value, and the gas is directed to the forepump when the outlet pressure of the booster pump has fallen below the threshold value. The gas supplied by the booster pump is compressed by means of the forepump.

Full Description:
BACKGROUND 
       [0001]    The invention relates to a method and a pump arrangement for evacuating a chamber. The pump arrangement, which is connected to the chamber, comprises a booster pump and a downstream forepump. 
         [0002]    In many technical applications, it is nowadays required for a chamber to be evacuated to a predefined vacuum within a short time. One example is lock chambers through which products are introduced into a vacuum chamber. The products may be, for example, mass-produced articles such as solar cells, displays etc. for which individual manufacturing steps are carried out in the vacuum chamber. It is sought for such products to be introduced into the vacuum chamber with ever shorter cycle times. It is not uncommon for lock chambers with a volume of a few hundred liters to have to be evacuated to a pressure of less than 10 −2  mbar in considerably less than 10 seconds. 
         [0003]    For the evacuation of such lock chambers, use is normally made of pump arrangements composed of two series-connected pumps, wherein the first pump is normally referred to as booster pump, and the downstream pump is normally referred to as forepump. The series connection of two pumps is expedient because, according to the ideal gas law (pressure*volume=constant; assuming constant temperature), the forepump can be designed for a significantly smaller volume flow than the booster pump. 
         [0004]    If, however, a lock chamber is to be evacuated proceeding from atmospheric pressure within a very short time, the booster pump initially delivers a large volume flow at high pressure, with the result that a large volume flow arrives at the outlet of the booster pump. Forepumps that can handle such a large volume flow are cumbersome and expensive. 
       SUMMARY 
       [0005]    The invention is based on the object of providing a method and a pump arrangement which permit the fast evacuation of a chamber with reduced outlay in terms of apparatus. Taking the stated prior art as a starting point, the object is achieved by means of the features of the independent claims. The subclaims relate to advantageous embodiments. 
         [0006]    In the method according to the invention, the booster pump is initially accelerated. Gas from the chamber to be evacuated is then introduced into the booster pump, such that from the booster pump there is temporarily extracted an excess power which exceeds the power provided by the drive of the booster pump. The gas that is delivered to the outlet of the booster pump is discharged through a bypass valve for as long as the outlet pressure in the booster pump lies above a predefined threshold value. The gas is conducted onward to the forepump when the outlet pressure of the booster pump has fallen below the threshold value. The gas supplied by the booster pump is compressed by means of the forepump. 
         [0007]    A few expressions will firstly be explained. The expressions “booster pump” and “forepump” illustrate the sequence of the pumps in the pump arrangement. Said expressions do not yield a limitation with regard to the configuration of the pump. 
         [0008]    The invention has recognized that, as a result of the acceleration of the booster pump and the subsequent extraction of the excess power, it is possible for the gas from the chamber to be delivered to the outlet of the booster pump at such a high pressure that the gas can be discharged directly, bypassing the forepump. Only when the evacuation process has progressed to such an extent that the booster pump is no longer capable of compressing the gas to the corresponding pressure is the forepump additionally used for the further compression. By means of the invention, it is possible for the forepump to be designed not only for a smaller volume flow but also for a small mass flow than the booster pump. 
         [0009]    In general, atmospheric pressure prevails at the outlet of the bypass valve. In this case, the threshold value corresponds to the atmospheric rusher. The gas thus emerges through the bypass valve for as long as the outlet pressure of the booster pump lies above atmospheric pressure. At its peak, the outlet pressure of the booster pump may be at least 1 bar, preferably at least 2 bar, more preferably at least 3 bar above atmospheric pressure. The gas compressed by means of the forepump may likewise be discharged at atmospheric pressure to the environment. 
         [0010]    At the start of the evacuation process, atmospheric pressure generally prevails in the chamber, such that the evacuation process begins at atmospheric pressure. Before the beginning of the evacuation process, the inlet of the booster pump may be closed, such that no gas from the chamber can enter into the booster pump. The evacuation process then begins at the time at which gas is introduced into the booster pump. 
         [0011]    In order to be able, at the beginning of the evacuation process, to deliver a large volume flow at high pressure (for example atmospheric pressure), the booster pump must provide a high compression power. The high compression power is provided by virtue of the fact that, during the evacuation process, there is temporarily extracted from the booster pump more compression power than is provided by the drive of the booster pump. The excess power that exceeds the drive power is extracted from the kinetic energy of the booster pump. The booster pump is thus braked, and the rotational speed of the pump decreases. 
         [0012]    Within the context of the invention, the power extracted in the booster pump may be considerably higher than the drive power. It is for example possible that, at its peak, the excess power is more than 50%, preferably more than 100%, more preferably more than 200%, of the drive power. In the case of an excess power of 100%, the compression power is twice as great as the drive power. 
         [0013]    It may also be provided that the excess power is extracted not only instantaneously but rather over a certain time period. If the evacuation process begins at the time at which the pressure in the chamber falls below the outlet pressure, and ends at the time at which the final pressure in the chamber is reached, the time period during which excess power is extracted may extend for example over 10%, preferably over 20%, more preferably over 50% of the evacuation process. The rotational speed of the booster pump may, as a result of the extraction of the excess power, be reduced by at least 5%, preferably at least 10%, more preferably at least 25%. 
         [0014]    In order that it is possible for excess power to be extracted from the pump to such an extent, the pump must, before the beginning of the evacuation process, be placed into a state in which a correspondingly large amount of kinetic energy is available. The pump is thus accelerated before the beginning of the evacuation process. 
         [0015]    To be able to provide adequate kinetic energy, the rotational speed of the booster pump at the start of the evacuation process is preferably higher than 8000 rpm, more preferably higher than 10,000 rpm, more preferably higher than 12,000 rpm. The diameter of the parts that are in rotation is preferably greater than 5 cm, more preferably greater than 10 cm, more preferably greater than 20 cm. 
         [0016]    If the gas from the chamber is introduced into the booster pump at substantially atmospheric pressure, the booster pump is subjected to an abrupt load. Some pump types which have hitherto been used as booster pumps, such as for example Roots pumps, are generally less suitable for accommodating such abrupt loads. In one advantageous embodiment, as a booster pump, use is made of a screw-type pump, the preferred configuration of which is explained in more detail below. The forepump may for example be a conventional liquid-ring vacuum pump. 
         [0017]    With the method according to the invention, it is possible for a chamber with the volume of more than 100 L to be evacuated from atmospheric pressure to a pressure of less than 10 −2  mbar in less than five seconds. This possibility is of particular interest within the context of lock applications where a lock chamber of said order of magnitude must be repeatedly evacuated with a short cycle time. Atmospheric pressure prevails at the inlet of the lock chamber, which means that atmospheric pressure is also assumed in the lock chamber when the inlet is opened in order to introduce a component into the lock chamber. The outlet of the lock chamber is adjoined by a vacuum chamber in which the pressure is for example 10 −2  mbar. The lock chamber must thus be evacuated to said pressure before the outlet can be opened in order to transfer the component into the vacuum chamber. 
         [0018]    If the cycle time of the lock is for example 10 seconds, then the time period in which excess power is extracted from the booster pump may be for example one second, while the rest of the cycle time is utilized to accelerate the booster pump to the starting rotational speed again. In more general terms, the time period of the extraction of excess power is preferably at least 5%, more preferably at least 10% of the cycle time. During at least 30%, preferably at least 50%, more preferably at least 70% of the cycle time, the power extracted from the booster pump is lower than the drive power, such that the booster pump is accelerated. 
         [0019]    The invention also relates to a pump arrangement. The pump arrangement comprises a booster pump and a forepump, wherein the outlet of the booster pump is connected to the inlet of the forepump. Between the booster pump and the forepump, there is arranged a bypass valve by means of which gas delivered by means of the booster pump can be discharged while bypassing the forepump. The pump arrangement also comprises a control unit which is configured so as to output a control signal if the rotational speed of the booster pump lies above a predefined rotational speed threshold value. The rotational speed threshold value is such that, after the respective rotational speed is exceeded, the booster pump is ready for the extraction of excess power. Such a pump arrangement is suitable for evacuating a chamber in a short time in accordance with the method according to the invention. 
         [0020]    The control signal may be transmitted to a controller of the chamber to be evacuated, in order to indicate that the booster pump is ready for the next evacuation process. The controller of the chamber may thereupon open the inlet of the booster pump via which the booster pump is connected to the chamber. The gas from the chamber then enters into the booster pump, and the chamber is quickly evacuated. As the gas enters the booster pump, the load increases abruptly, such that the rotational speed of the booster pump decreases. 
         [0021]    The control unit of the booster pump may furthermore be configured to accelerate the booster pump before the beginning of the evacuation process such that the rotational speed threshold value is exceeded. To provide an adequate amount of kinetic energy for the extraction of the excess power, the rotational speed threshold value preferably lies above the delivery rotational speed of the booster pump. The delivery rotational speed denotes the rotational speed which is assumed as a steady state when the induction pressure is 100 mbar. The drive power corresponds, at the delivery rotational speed, to the pump power, which means that the rotational speed of the booster pump remains constant. The rotational speed threshold value may be higher, by 10%, preferably by 30%, more preferably by 50%, than the delivery rotational speed. In absolute numbers, the rotational speed threshold value may for example be at least 8000 rpm, preferably at least 10,000 rpm, more preferably at least 12,000 rpm. Normally, booster pumps used for an application within the context of the invention are operated at considerably lower rotational speeds. A rotational speed of 6000 rpm is generally not exceeded during the operation of such booster pumps. In the case of the method according to the invention, too, the booster pump can be accelerated beyond the delivery rotational speed. 
         [0022]    The arrangement according to the invention may furthermore encompass the chamber to be evacuated. The control unit of the arrangement may for this purpose be designed to open the inlet of the pump, via which the booster pump is connected to the chamber, after the rotational speed threshold value has been exceeded. Furthermore, the control unit may be configured to keep the inlet closed while the booster pump is accelerated. 
         [0023]    In one advantageous embodiment, as a booster pump, use is made of a screw-type pump in which the screws of two threads engage with one another in such a way that the gas is conveyed from a suction side to a pressure side between the thread turns. To be able to withstand the stated high rotational speeds, the screws preferably have in each case two threads, such that the forces that arise in the longitudinal direction of the screws cancel one another out. The threads of the screws are preferably of double-start configuration. Here, in a radial direction, point-symmetry of the screws may exist such that the screws are imaged into themselves by a rotation of 180° about the longitudinal axis. The diameter of the screws is preferably greater than 10 cm, more preferably greater than 15 cm, more preferably greater than 20 cm, such that the screws, as a whole, have approximately the above-stated dimensions. 
         [0024]    In order that the screw-type pump can accommodate the large volume flow required in the case of booster pumps, the inlet opening is preferably larger than 60%, more preferably larger than 80%, more preferably larger than 100% of the cross-sectional area of a screw. To keep leakage losses low, it is provided that, close to the pressure side, the radial spacing between the housing of the pump and the thread of the screw is as small as possible (radial minimum spacing), for example less than 0.2 mm, preferably less than 0.1 mm. 
         [0025]    In the inlet region, that is to say in particular in that housing portion in which the inlet opening is formed, a suction gap may exist between the thread of the screw and the housing in order to permit a large volume flow into the working chambers of the pumps. The radial diameter of the suction gap is larger, preferably by a factor of 50, more preferably by a factor of 100, more preferably by a factor of 200, than the radial minimum spacing. The suction gap may extend for example of a circumferential angle of at least 15°, preferably at least 30° of the housing. In the longitudinal direction, the suction may extend over at least 20%, preferably at least 30%, more preferably at least 40% of the length of a thread of the screw. The length of the suction gap preferably corresponds to the length of a 360° turn of the thread in said region. The thread thus has a very large pitch in the inlet region. The first 360° turn may extend for example over at least 20%, preferably at least 30%, more preferably at least 40% of the length of the thread. Overall, each thread turn of the double-start thread preferably comprises at least three, more preferably at least four complete 360° turns. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0026]    The invention will be described by way of example below with reference to the appended drawings on the basis of advantageous embodiments. In the drawings: 
           [0027]      FIG. 1  shows a pump arrangement according to the invention which is connected to a lock chamber; 
           [0028]      FIG. 2  shows a perspective, partially cut-away illustration of a screw-type pump suitable for the arrangement according to the invention; 
           [0029]      FIG. 3  shows a detail of the pump from  FIG. 1  in an enlarged illustration; 
           [0030]      FIG. 4  shows the view from  FIG. 3  in another state of the pump; 
           [0031]      FIG. 5  shows a schematic cross-sectional view of a screw-type pump suitable for the arrangement according to the invention, along an axis of a screw; and 
           [0032]      FIGS. 6A and 6B  show sections along the lines A-A and B-B in  FIG. 5 . 
       
    
    
     DETAILED DESCRIPTION 
       [0033]    In a vacuum chamber  40  shown in  FIG. 1 , certain method steps are performed on a product  41 . The product  41 , which is illustrated in simplified block form, may be for example a multiplicity of semiconductor components such as for example solar cells or displays. The method step may be a coating process. For the method step, it is necessary for the pressure in the vacuum chamber  40  to be below 0.5 mbar. To keep the vacuum chamber at said pressure, a vacuum pump (not illustrated in  FIG. 1 ) is connected to the vacuum chamber  40 . 
         [0034]    The vacuum chamber  40  is adjoined by a lock with a lock chamber  42  through which the product  41  is introduced into the vacuum chamber. The lock chamber  42  has an inlet opening and an outlet opening which are provided with sliding doors  43 ,  44 . The sliding doors  43 ,  44  are controlled by a controller  50  such that they are not both simultaneously open at any time. When the sliding door  43  is open, atmospheric pressure prevails in the lock chamber  42 . The lock has a volume of for example 200 l. 
         [0035]    When the sliding door  43  is open, the product  41  can be introduced into the lock chamber  42  by means of conveyor belts  45 . After the sliding door  43  has subsequently been closed again, the lock chamber  42  is evacuated by means of a pump arrangement connected to the lock chamber  42 , such that the pressure in the lock chamber  42  corresponds to the pressure of less than 0.5 mbar prevailing in the vacuum chamber  40 . After the completion of the evacuation process, the sliding door  44  is opened, and the product  41  is introduced into the vacuum chamber  40  by means of the conveyor belts  45 . The sliding door  44  is subsequently closed again, the lock chamber  42  is brought to atmospheric pressure, and the sliding door  43  is opened. A cycle in the lock is thus completed. The cycle time of the cycle is approximately 10 seconds. 
         [0036]    For the evacuation process itself, by means of which the pressure in the lock chamber is reduced from atmospheric pressure to a final pressure of less than 0.5 mbar, a time period is available which is considerably shorter than the cycle time. The evacuation process may extend for example over a time period of five seconds. 
         [0037]    To be able to evacuate a lock of this volume in such a short time, a powerful pump arrangement is required which in particular has a high suction capacity across the entire pressure range between atmospheric pressure and final pressure. This is provided by the pump arrangement according to the invention, in which, as per  FIG. 1 , a screw-type pump as a booster pump  46  and a liquid-ring vacuum pump as a forepump  47  are connected in series. The liquid-ring vacuum pump is of conventional configuration, such that a detailed description is not necessary. 
         [0038]    To start the evacuation process, the booster pump  46  is initially accelerated to a rotational speed considerably higher than the delivery rotational speed. A valve  48  arranged between the booster pump  46  and the lock chamber  42  is closed, such that no gas from the lock chamber  42  can enter into the inlet of the booster pump  46 . The booster pump  46  is thus not under load, such that a relatively low drive power is sufficient to accelerate the booster pump  46 . 
         [0039]    When the booster pump  46  has been accelerated to such an extent that a predefined rotational speed threshold value is exceeded, a control unit  16  of the booster pump  46  transmits a control signal to the controller  50  of the lock chamber. The controller  50  is thus provided with the information that the booster pump  46  is ready for the next evacuation process. When the lock chamber  42  is also ready for the next evacuation process, the controller  50  can open the valve  48  such that the booster pump  46  can induct air from the lock chamber  42 . The air is delivered, and in the process compressed, by the booster pump  46  such that a pressure considerably higher than atmospheric pressure prevails at the outlet of the booster pump  46 . At its peak, a pressure of 3 bar above atmospheric pressure may for example prevail at the outlet of the booster pump  46 . 
         [0040]    Between the forepump  47  and the booster pump  46  there is arranged a bypass valve  49 , at the outlet of which atmospheric pressure prevails. The bypass valve  49  is configured as an overpressure valve, such that the compressed gas from the outlet of the booster pump  46  automatically exits via the bypass valve  49  for as long as the pressure at the outlet of the booster pump  46  lies above atmospheric pressure. If the pressure at the outlet of the booster pump  46  falls below atmospheric pressure, the bypass valve  49  closes. The gas is then taken on by the forepump  47  and compressed further such that said gas can be discharged at atmospheric pressure to the environment. 
         [0041]    The closer the pressure in the lock chamber  42  comes to the final pressure, the lower the pressure between the booster pump  46  and the forepump  47  also becomes. The forepump  47  is configured such that it can compress the gas from said pressure to atmospheric pressure. 
         [0042]    During such an evacuation process, the booster pump  46  is subjected to particularly high loads. When the valve  48  is opened, the air flow entering the booster pump  46  generates an abrupt load. Furthermore, as a result of the entry of a large volume flow at atmospheric pressure, a high compression power is demanded of the booster pump  46 . Said compression power exceeds the drive power of the booster pump  46 , which means that an excess power is extracted from the booster pump  46 . The excess power is gained from the kinetic rotational energy of the booster pump  46 , which means that the rotational speed of the booster pump  46  decreases in said phase. 
         [0043]    To be able to provide adequate kinetic rotational energy, the booster pump  46  is accelerated to a high rotational speed of higher than 10,000 rpm before the beginning of the evacuation process. As a result of the extraction of the excess power, the rotational speed decreases within one second to 9000 rpm. The remaining cycle time is utilized to accelerate the booster pump  46  to the original rotational speed again. In this phase, the drive power is consequently higher than the compression power extracted from the booster pump  46 . 
         [0044]    The booster pump  46  which firstly withstands the loads at the beginning of the evacuation process and which secondly has the required suction capability across the entire pressure range is described below. 
         [0045]    The screw-type pump which is suitable as a booster pump comprises, as per  FIG. 2 , two screws  14  which are accommodated in a pump housing  15 . Owing to the pump housing  15  not being illustrated in its entirety, one of the screws  14  is visible over the entire length, whereas the other screw  14  is largely hidden by the pump housing  15 . The two screws  14  engage with one another, which means that the thread projections of one screw  14  engage into the depression between two thread projections of the other screw  14 . 
         [0046]    The pump comprises a control and drive unit  16  in which, for each of the screws  14 , there is arranged an electronically controlled drive motor  17 . The electronic controller of the drive motors  17  is set up such that the two screws  14  run entirely synchronously with respect one another, without the thread projections of the screws  14  making contact. For additional security against damage to the screws  14 , the two screws  14  are in each case equipped with a gearwheel  18 . The gearwheels  18  mesh with one another and generate positive coupling of the two screws  14  in the event of failure of the electronic synchronization of the screws  14 . 
         [0047]    Each screw  14  is equipped with two threads  19 , such that the pump has a total of four threads  19 . The threads  19  extend in each case from a suction side  20  in the centre of the screw  14  to a pressure side  21  at the outer ends of the screw  14 . The two threads of a screw  14  are oriented in opposite directions such that they work from the suction side  20  toward the pressure side  21 . 
         [0048]    Each of the threads  19  comprises a first thread turn  22  and a second thread turn  23 . The threads  19  are thus of double-start form in the sense that the thread turns  22 ,  23  are interlaced with one another such that they together form a double-helix-like form. The two thread turns  22 ,  23  are formed such that the threads  19  are symmetrical in a radial direction. The screw  14  furthermore has symmetry in a longitudinal direction when the screw  14  is viewed from the pressure side of the first thread  19  to the pressure side of the second thread  19 . 
         [0049]    The threads  19  are configured such that a larger volume is enclosed between two adjacent thread projections in the region of the suction side  20  than in the region of the pressure side  21 . The volume of the working chambers, which corresponds to the volume enclosed between the thread projections, thus decreases from the suction side to the pressure side, such that gas contained in the working chamber is compressed on the path from the suction side to the pressure side. 
         [0050]    The housing  15  of the pump is provided with an inlet opening  24  which is arranged so as to provide access to the suction side  20  of all four threads  19 . To permit a large volume flow into the pump, the inlet opening  24  has a large cross section. In the exemplary embodiment, the cross-sectional area of the inlet opening  24  is larger than the circular contour spanned by a screw  14 . 
         [0051]    To further improve the volume flow into the working chambers, there is formed on the housing  15  of the pump a suction gap  25  which adjoins the inlet opening  24  and which follows the contour of the screw  14  in the circumferential direction. In the longitudinal direction, the suction gap  25  extends over approximately half of the length of the thread  19  between the suction side  20  and the pressure side  21 . In the circumferential direction, the dimensioning of the suction gap  25  varies with the inlet opening; the further the inlet opening  24  extends to the side at the respective point, the shorter is the extent of the suction gap  25  in the circumferential direction at said point. At the widest point of the inlet opening  24 , the suction gap  25  extends over a circumferential angle of approximately 45°. In the region which the inlet opening  24  no longer covers the suction gap  25 , the suction gap  24  extends over a circumferential angle of approximately 120°. The dimension of the suction gap  25  in the radial direction corresponds to the spacing between the pump housing  15  and the contour of the screw  14  in said region. Said spacing lies in the range of approximately 10 mm. 
         [0052]    As a result of the suction gap, the gas is no longer restricted to entering the working chambers in a radial direction, and instead the gas can also move into the working chamber across a thread projection and through the suction gap. The volume flow into the working chambers is further increased in this way. 
         [0053]    A further contribution to the increase of the volume flow into the working chamber is achieved by virtue of the fact that there is a spacing between the suction side  20  of the first thread  19  of a screw  14  and the suction side  20  of the second thread  19  of the screw  14 . In this way, in the centre of the screw  14 , a space is left free through which the gas can also enter into the working chamber in a radial direction. 
         [0054]    The region in which the suction gap  25  extends (=first housing portion  26 ) serves for the filling of the working chambers. In the adjoining second housing portion  27 , the spacing between the housing and the contour of the screw  14  is as small as is technically possible (radial minimum spacing). The compression takes place in the second housing portion, and a leakage flow from one working chamber into the next working chamber is undesirable. 
         [0055]    A transition edge  28  is formed at the transition from the first housing portion  26  to the second housing portion  27 . The transition edge  28  extends in a circumferential direction over the entire section  25  and defines the transition from the suction gap  25  to the second housing portion  27 , in which the radial minimum spacing exists between the housing  15  and screw  14 . 
         [0056]    The compression begins when the working chamber has passed into the second housing portion, that is to say when the thread projection which delimits the working chamber toward the suction side has formed a closure with the transition edge  28 . The transition edge  28  is arranged such that the formation of a closure between the thread projection and the transition edge  28  takes place at a time at which the working chamber still has its maximum volume. 
         [0057]    As viewed in the circumferential direction, the transition edge  28  encloses with the transverse direction an angle smaller than the gradient of the thread projection which forms a closure with the transition edge  28 . It is achieved in this way that the formation of a closure between the thread projection and the transition edge  28  does not take place abruptly but rather extends over a short time period. The operating noise of the pump is reduced in this way. 
         [0058]    The actual volume compression takes place in a short portion of the thread directly after the closure of the working chamber. The adjoining further turns of the thread served for sealing and also effect a thermodynamic compression. 
         [0059]    On the pressure side  21  of the thread  19 , the gas is discharged from the working chamber. Through a bore  29  in the pump housing  15 , the compressed gas from the pressure sides  21  situated at the outside are brought together to a central outlet opening. The outlet opening (not visible in the figures) is arranged opposite the inlet opening  24 . As shown in  FIGS. 2 ,  3  and  5 , the bore  29  is integrated into the pump housing  15  and extends between the two screws  14 , wherein the line  29  is arranged partially within a tangential plane  35  resting on the two screws  14 .

Technology Classification (CPC): 5