CONTROL DEVICE FOR CONTROLLING THE POWER SUPPLY TO AN OSCILLATING MOTOR FOR DRIVING A COMPRESSOR UNIT OF THE RESONANT-PISTON TYPE AND COMPRESSOR UNIT OF THE RESONANT-PISTON TYPE PROVIDED WITH SUCH A CONTROL DEVICE

Abstract: A control device (30) is disclosed for controlling the power supply to the coils (16A, 16B) of a drive motor (3) for a compressor unit of the resonant-piston type (1). The control device comprises a power-supply circuit (44) for energising the motor coils (16A, 16B) from a direct voltage source (45), means (46, 47, 48; 46, 60) for determining a measure (P, ), which indicate whether the power consumption of the motor as a function of the frequency of the energising current is at least approximately maximal, and means (40, 42, 43; 61, 42, 43) for adjusting the frequency of the energising current depending on the derived measure (P, ) to a value for which said measure (P, ) indicates that the power consumption of the motor (3) is maximal.

Description: The invention relates to a control device for controlling the power supply to an oscillating motor for driving a compressor unit of the resonant-piston type. United States Patent Specification No. 4,345,442 discloses a compressor unit in which the piston of a compressor of the resonant piston type is driven with an oscillating motion relative to the cylinder of the compressor by means of an oscillating motor constructed as a linear motor. The frequency of this oscillating motion is substanially constant and is substantially equal to the resonant frequency of the spring-mass system constituted by the compressor and the oscillating motor. In order to obtain this oscillation the oscillating motor is energised with an alternating current having a constant frequency substantially equal to this frequency. Since the resonant system is mainly driven in resonance the power required for reciprocating the piston is only low, enabling a motor with a lower driving power and hence smaller energising currents to be used. This has the advantage that the dimensions of the oscillating motor can be small, which is favourable for cost reasons. This is of particular importance in compressor systems for mass-manufactured products such as for example refrigerators and freezers. A known property of such compressors is that the resonant frequency varies continually as a result of changes in ambient parameters, such as for example temperature. This partly eliminates said advantage because the required driving power and energising current increase rapidly as the difference between the actual operating frequency and the optimum operating frequency, which corresponds substantially to the resonant frequency, increases. DE-A 2,457,999 discloses an oscillation motor which is energised with an alternating current with a frequency which is equal to the resonance frequency of the oscillation motor. In order to prevent that the frequency of the alternating current will differ from the resonance frequency in the event that the temperature changes, the frequency of the alternating current is controlled in dependence on the resistor value of NTC-resistor thermally coupled to the motor. Further in FR-A 1,068,560 it is described that the power of current supplied to an actuator of an oscillating system is a measure for finding the proper frequency of oscillation at the resonance circuit. It is an object of the invention to provide a control device by means of which a compressor unit of the resonant-piston type is always operated at an optimum oscillating frequency. According to the invention this object is achieved by a control device for controlling the power supply to an oscillating motor for driving a compressor unit of the resonant-piston type, comprising a circuit for supplying an alternating current from an electric power source to the oscillating motor, frequency control means for controlling the frequency of the alternating current to an optimal frequency value which substantially corresponds with the resonance frequency of the compressor unit, characterized in that the control device is provided with measurement means for determining the optimal frequency value during measurement cycles which are executed at regular intervals, which measurement means being provided with means for setting the frequency of the alternating current to a plurality of different values, means for determining a measure for the power absorbed by the oscillating motor for each of the different frequency settings, means for determining on basis of the power absorbed for the different frequency settings the frequency for which the absorbed power is maximal, and in that the control means are adapted to set the frequency in the interval following the measurement cycle to a value which substantially corresponds to the frequency determined during the previous measurement cycle. By means of the control device according to the invention the frequency of the alternating current is kept on a value, for which the power supplied to the compressor unit and thus the production of the compressor unit, e.g. the cold production in a refrigerator, is maximal. It is remarked that in general, owing to the damping in the motor-compressor unit, this optimal frequency is not equal to the resonance frequency of the motor-compressor system. It appears that the optimal frequency is somewhat higher than the resonance frequency. A suitable measure for inducting, whether the power supplied as a function of the frequency is maximal, is the power which is taken from the electric power source by the motor with a constant amplitude of the alternating current. The maximum of the power taken from the electric power source indicates the optimal frequency. Another suitable measure is the amplitude of the alternating current with a constant power consumption of the motor. In this case the minimum of the amplitude indicates the optimal frequency. The advantage of the two measures described before is that they can be determined without additional sensors located in the motor-compressor system. This is of particular importance for compressor units for refrigerating and freezing systems and/or heat pumps, where it is customary to accommodate the compressor together with the drive motor in a hermetically sealed vessel filled with refrigerant. The conditions obtaining in such vessels require the use of sensors which are specially adapted to these conditions. Moreover, when sensors are used this requires additional feed-throughs in the vessel wall for the passage of the signal wires connected to the sensors. A further embodiment is characterized in that the control device comprised comparator means for determining the difference between the instantaneous value of the measure for the power absorbed and the value of the power absorbed which corresponds with the optimal frequency determined in the previous measurement cycle, and initiation means for initiating a measurement cycle if the difference thus determined exceeds predetermined limits. This embodiment has the advantage that the number of measurement cycles can be minimised. In practice, it has been found that for stability reasons it is to be preferred to select the frequency of the alternating current to be slightly below the optimum frequency. A particularly suitable embodiment of the control device is therefore characterized in that the adaptation means are constructed to adjust the frequency of the alternating current to a frequency equal the optimum frequency minus a specific value. Another embodiment of the control device is characterized in that the control device comprises means for iteratively determining the optimum frequency. This embodiment has the advantage that the optimum frequency is determined in a limited number of iteration steps and hence in a comparatively short time. Embodiments of the invention and further advantages thereof will now be described in more detail, by way of example, with reference to Figures 1 to 9, of which Figure 1 shows a compressor unit of the resonant-piston type in which the control device in accordance with the invention may be used, Figure 2A and 2B represent the power consumption of the oscillating motor as a function of the frequency of the energising current, Figure 3 shows an embodiment of the control device in accordance with the invention; Figures 4, 5A, 5B and 6 are flow charts of the program performed by the embodiment shown in Figure 3, Figure 7 illustrates the relationship between the phase different between the energising current and energising voltage and the power consumption of the motor as a function of the frequency of the energising current. Figure 8 shows another embodiment of the control device, and Figure 9 is a detailed diagram of a power-supply circuit suitable for use in the control devices shown in Figures 3 and 8. Figure 1 shows a compressor unit 1 comprising a compressor 2 of the resonant-piston type and an oscillating motor 3 for driving the compressor 2. Such a compressor 2 and oscillating motor 3 are described comprehensively in the Applicant's European Patent A pplication EP 0,155,057 (PHN 10.965). This compressor 2 has a housing 4 which bounds a cylindrical cavity 5 in which the piston 6 is movable. At one end the cavity 5 is closed by a plate 7 in which a gas inlet valve 8 and a gas outlet valve 9 are mounted in a customary manner. The other end of the cavity 5 is closed by a plate 10, forming a variable-volume chamber with one end of the piston 6, which chamber contains an amount of gas. The variable-volume chamber forms a gas spring. The other closed end of the piston 6 constitutes one of the walls of a variable-volume chamber in which for example the refrigerant of a refrigerating system is compressed, the refrigerant being supplied and discharged via the valves 8 and 9. By means of a lever 11 the piston 6 is coupled to an armature 12 of the oscillating motor 3. The armature 12 is rotatably mounted on a motor shaft 13. The oscillating motor further comprises a stator 14 (14A, 14B) and a core 15 with two coils 16A and 16B arranged opposite one another. Two magnets 17 and 18 are arranged between the core 15 and the stator 14. At the end faces 19 of the coils 16 which are remote from each other circularly curved air gaps 20, 21, 22 and 23 are formed in which sliding elements 24 and 25 of the armature are movable. If in such an oscillating motor 3 the coils 16 are energised with an alternating current the magnetic field generated in the air gaps (20, 21, 22 23) by the magnets 18 and 19 and the coils 16 cause the sliding elements 24 and 25 of the armature to perform an oscillating motion in the circular air gaps 20, 21, 22 and 23 with a frequency corresponding to the frequency of the energising current through the coils 16. This oscillating motion of the armature 12 is transmitted to the piston 6 via the lever 11. For the spring-mass system constituted the compressor 2 and the oscillating motor 3 Figure 2A shows the power consumption P of the oscillating motor as a function of the frequency of a constant-amplitude energising current I. The power consumption P exhibits a maximum Popt at the frequency fopt. Since the amplitude of the current I is constant the loss in the motor is substantially constant for the given frequency range. The losses in the motor comprise copper and iron losses, which depend on the amplitude and frequency of the alternating current through the motor. Since the iron losses are substantially smaller than the copper losses and the copper loss is independent of the frequency the power delivered to the compressor by the motor is also maximal for the frequency fopt, which means that the amplitude of the reciprocating motion performed by the piston 6 is maximal. When the compressor 2 is used in a refrigerating system this also means that the maximum cold production is obtained for this frequency. If the oscillating motor 3 is energised with an alternating current having the optimum frequency fopt the current required for a specific cold production is always minimal which means that the dimensions of the motor can be particularly small and also that the losses in the motor are minimised. In practice it has been found that the relationship between the power consumption and the frequency depends strongly on ambient parameters such as for example the temperature in the compressor, with the result that the optimum frequency fopt changes constantly during operation. An embodiment of a control device 30 in accordance with the invention by means of which the optimum frequency is determined at regular intervals and subsequently the frequency of the energising motor is set to a specific optimum frequency fopt is shown in Figure 3. The control device 30 comprises a programmable control unit 40 of a customary type, comprising a central processing unit 31 (CPU), a ready-only memory 32 (ROM), a random-access memory 33 (RAM), analog-to-digital converter 34 and 35, and digital-to-analog converters 36 and 37. The memories 32 and 33 and the analog-to-digital converters 34 and 35 and the digital-to-analog converters are coupled to the central processing unit 31 in a customary manner via an address bus 38, a data bus 39 and control bus 41. The analog output of the digital-to-analog converter 36 is connected to the control input of a voltage-controlled oscillator 42 of a customary type, which generates a sinewave output signal of constant amplitude and a frequency which depends on the value of the voltage on the control input. The output signal of the oscillator 42 is applied to a first input of a multiplier 43, whilst a second input of the multiplier is connected to the analog output of the digital-to-analog converter 37. The output signal Ig of the multiplier 43, which represents the product of the output signals of the oscillator 42 and the digital-to-analog converters 37, is applied to a power-supply circuit 44 which is arranged between a direct-voltage source 45 and the motor coils 16. The power-supply circuit 44 is of a type which energises the coils 16 from a direct voltage source 45 with a current Is which is proportional to the instantaneous value of the signal Ig. The power-supply circuit 44 further comprises a measurement circuit for measuring the energising current and generating a measurement signal Im which is proportional to the measured energising current. The power-supply circuit 44 will be described in more detail with reference to Figure 9. The output terminals of the coils 16 are connected to the inverting and to the non-inverting input of a differential amplifier 46 for measuring the voltage across the motor. The differential amplifier 46 then generates a signal Um which is proportional to the voltage across the motor. The signal Um is applied to a first input of a multiplier 47 and the signal Im is applied to a second input of this multiplier 47, so that the output signal of the multiplier 47 is representative of the instantaneous electric power consumption of the motor 3. The output signal of the multiplier 47 is applied to a low-pass filter 48, so that the output signal Pin of the low-pass filter 48 is representative of the average power consumption of the motor 3. The signal Pin is applied to the input of an analog-to-digital converter 34. Further, a signal Tm is applied to the inverting input and a signal Tg to the non-inverting input of a differential amplifier 49. The signal Tm represents the temperature of the space to be cooled, measured by means of a sensor (not shown). The signal Tg represents the desired temperature. The output signal Tin of the differential amplifier, which is representative of the difference between Tm and Tg, is applied to the input of an analog-to-digital converter 35. The central processing unit 31 caries out of a program stored in the read-only member 32. While this program is carried out the optimum frequency of the energising current is determined at regular intervals. Each time that the optimum frequency has been determined the frequency of the energising current is adapted. A flow chart of such a program is illustrated in Figures 4, 5, and 6. Figure 4 shows the flow chart of the main program which is carried out constantly by the central processing unit 31. During the step S10 a subroutine Fopt is performed to determine the optimum frequency Fopt and the corresponding value of the power consumption Popt, and the frequency the energising current of the motor is adapted to the optimum frequency fopt thus determined. Subsequently, in the step S11 it is ascertained whether a flag FL has been set to the logic value "1". This flag indicates whether the desired value Iref of the amplitude of the energising current must be adapted. Should this be the case, the new value of Iref is applied to the digital-to-analog converter 37 during the step S12, which converter converts the digital value Iref into the signal Iout for adjusting the amplitude of the energising current via the multiplier 434. Moreover, the flag FL is reset to the logic value "0" during the step S12. After the step S12 has been performed the program proceeds with the step S10. However, if during the step S11 it has been found that the flag FL has not yet been set to the logic value "1", the step S11 is followed by the step S13. During the step S13 the digital value of Pin on the output of the analog-to-digital converter 34 is read by the central processing unit 31. This digital value of Pin, which represents the instantaneous power consumption of the motor 3, is compared with the optimum value Popt. Further, the absolute value ΔP of the difference between Popt and Pin is determined. Subsequently, during the step S14 it is ascertained whether the absolute value ΔP of the difference is smaller than a predetermined small value ε. If it is smaller, this means that the motor 3 is still energised with an alternating current whose frequency is near the optimum value Fopt. In that case the program proceeds with the step S14. However, if the value ΔP is larger than ε, this means that as a result of varying operating parameters, such as for example the temperature of the medium in the compressor 2, the frequency fopt of the energising current no longer corresponds to the actual optimum value. In that case the program proceeds with the step S10, after which the optimum frequency fopt is determined again during the subroutine Fopt. Figures 5A and 5B are flow charts of the subroutine Fopt. After the subroutine Fopt has been called the frequency of the energising current is first of all set to an initial value fo during the step S20. The central processing unit 31 then transfers a digital value Fo, which represents the initial value fo (see Figure 2A), to the digital-to-analog converter 36. The digital-to-analog converter 26 converts the digital value Fo into the signal Fr for adjusting the frequency of the alternating current via the voltage-controlled oscillator 42. Subsequently, during the step S21 a waiting time is observed to allow the resonant system to adjust to the new frequency. Subsequently, during the step S22 the power consumption values corresponding to the new frequency setting is read in via the analog-to-digital converter 34 and is stored in the random-access memory 33 as a variable P3. Moreover, the output signal Fr is incremented by a constant value ΔF, which corresponds to a frequency change Δf (see Figure 2A). As a result of this, the frequency of the energising current is set to a new value equal to fo+Δf. During the steps S23, S24, S25 and S26 the power consumption values at the frequencies fo+Δf and fo+2Δf are determined and stored as the variables P2 and P1 respectively. During S27 an estimate of the derivative Afg (+dp/df) for the last frequency setting is derived from the values of P1, P2, P3 and ΔF in accordance with the following relationship: During the step S28 it is ascertained whether the derivative Afg is smaller than zero. If it is not smaller, this means that each maximum of P is not yet reached. During the steps S29, S30 and S31 the frequency of the alternating voltage is then again incremented by the value Δf and a corresponding value of the power consumption is determined and stored in P1. Moreover, the values of P2 and P3, which represent the power-consumption values for the two preceding frequency settings are adapted. Subsequently, during the step S27 the derivative for the new frequency setting is determined. The program loop formed by the steps S27, S28, S29, S30 and S31 is repeated until the derivative Afg thus determined is smaller than zero. This indicates that the optimum frequency is situated between the last and penultimate frequency setting, indicated by the reference numerals 50 and 51 in Figure 2A. During the step S32 the value of Fr is then decremented by a value ΔF′ which is substantially smaller than the value ΔF, so that the frequency of the energising current is reduced by a small value Δf′ (see Figure 2B ). After a waiting step S33 the power consumption for the new frequency setting is determined in the step S34. Subsequently, during the step S35 it is ascertained whether the last power consumption value determined, represented by P2, is smaller than the penultimately determined power, represented by Pr. If it is not smaller, the program proceeds with the step S35. The program loop comprising the steps S32, S33, S34 and S35 is repeated until the last power consumption value determined is smaller than the power consumption determined pen ultimately. (The corresponding frequency f and the power consumption are represented by the circle 52 in Figure 2B). In that case the last power consumption value determined is substantially equal to the maximum value, which means that the corresponding frequency is substantially equal to the optimum frequency fopt fo the energising current, so that the subroutine Fopt is terminated. In practice, it has been found that for reasons of stability it may be desirable not to set the frequency of the alternating current to a value for which the power consumption is maximal but to a frequency which is slightly lower than this frequency. After the optimum frequency has been determined in accordance with the said subroutine Fopt the frequency of alternating current may then be set to the optimum frequency thus determined minus a predetermined value. It will be obvious to those skilled in the art that the program, described by way of example with reference to Figure 5, for determining a maximum in the relationship between the power consumption and the frequency setting may readily be replaced by any other known program for determining the maximum. The main program Main is interrupted at constant intervals. During these interruptions a control program Control for determining the desired amplitude of the energising current is carried out. A flow chart of an example of this control program is given in Figure 6. During the first step S1 of this control program Control the digitised value Tin is applied to the outputs of the analog-to-digital converter 35 by the central processing unit 31. Subsequently, during the step S2 a new desired value Iref for the amplitude of the energising current is determined in accordance with a customary control algorithm of a kind which adjusts the desired Iref to a value at which the desired temperature Tg and the measurement temperature in the space to be cooled are maintained substantially equal to each other. Further, during the step S2 the flat FL is set to the logic value "1" to indicate that the setting of the amplitude of the energising current must be adapted during the next time that the steps S11 and S12 of the main program are carried out. After termination of the control program Control the main program Main is resumed. In the embodiment of the invention described in the foregoing the optimum frequency of the energising current is determined by changing the frequency of the energising current and at the same determining the power consumption of the motor while the amplitude of the energising current is maintained constant. The maximum power consumption is then derived from the value of the power consumption thus determined. However, the optimum frequency can be determined in various other ways, for example by maintaining the power consumption of the motor constant by means of a control system, the frequency of the energising current being varied. By simultaneously determining the amplitude of the corresponding energising current and subsequently deriving the frequency for which the amplitude of the energising current is minimal from the value of the amplitude and the associated frequency thus determined, it is also possible to find the optimum frequency. In the embodiment described in the preceding the measure for determining the optimal frequency is directly derived from the motor current and voltage over the motor. It will be clear that this measure also may be derived from the current and voltage of th e electric power source. In the event that the control device is fed from the mains via a rectifier the said measure also may be derived from the mains voltage and the current taken from the mains from the control device, because the electric power consumption of the electronics of the control circuit is negligible with respect to the power consumption of the motor, so that it can be considered that all the power taken from the mains is consumed by the motor. It is alternatively possible to derive a frequency for which the power consumption is substantially maximal from the phase difference between the energising current and the energising voltage as a function of the frequency. This method is particularly suitable for motors in which the voltage drop across the inductance is very small relative to the counter-emf generated in the motor coils by the rotor motion. In that case the phase difference between the counter-emf and the energising current is substantially equal to the phase difference between the voltage across the motor and the energising current. Since the power delivered by the motor and hence the cold production is substantially maximal if the energising current and the counter-emf are in phase, the maximum power consumption as a function of the frequency in a motor with a very low inductance is substantially optimal if the phase difference  between the energising current and the energising voltage is zero. By now varying the frequency and determining the cos  for different frequencies by means of a cos  detector and subsequently deriving the frequency for which cos  is maximal from the values determined for cos  and the corresponding frequencies, it is also possible to find a substantially optimum frequency. However, a signal by means of which the frequency can be adapted can also be derived directly from the phase difference. Figure 7 gives the power consumption P and the phase difference  between the energising current and the energising voltage as a function of the frequency f of the energising current. If the frequency f is lower than the optimum frequency fopt the energising voltage leads the energising current ( < 0). In the case that the frequency f is substantially higher than the optimum frequency fopt the energising voltage lags the energising current ( > 0). If the frequency is situated near the optimum frequency the phase difference  is small. For a frequency f′opt for which the phase difference  is zero the power consumption P′opt is equal to the optimum value Popt but for a small error. Figure 8 shows an embodiment of a control device in which the frequency of the energising current is adapted depending on the phase difference . In Figure 7 the elements corresponding to the elements already shown in Figure 3 bear the same reference numerals. The signals Um and Im representing the instantaneous values of the energising voltage across the motor and the energising current through the motor are applied to a phase detector 60 of the customary type for determining the phase difference between the signals Um and Im. The output signal of the phase detector 60, which represents the phase difference, is applied to a control circuit of a customary type which adapts Fr depending on the output signal of the phase detector 60 in such a way that the phase difference  remains substantially zero. Figure 9 shows an example of the energising circuit 44. One terminal 72 of the series arrangement of the coils 16A and 16B of the motor 3 is coupled to a positive power-supply terminal 70 and a negative power-supply terminal 71 of the direct voltage source 44 via electronic switches 74 and 75 respectively, comprising for example power transistors of the FET type. The other terminal 73 of the series arrangement of the coils 16A and 16B is coupled to the positive power-supply terminal 70 and the negative powe ly terminal 71 via similar electronic switches 76 and 77 respectively. The switches 74, 77 are each arranged in parallel with a protection circuit, not shown, of a customary type. A low-impedance resistor 78 and a low-impedance resistor 79 arranged respectively in the connection between the switch 75 and the power-supply terminal 71 and in the connection between the switch 77 and the power-supply terminal 71. The switches 74, ..., 77 are controlled by means of control circuits 80, ...,83. The control circuits 80, ..., 83 are of a customary type which generate a control signal for opening the switch in response to a pulse on an "R" input and which generate a control signal for closing the switch in response to a pulse on an "S" input. The "S" inputs of the control circuits 80 and 83 of the two diagonally opposed switches 74 and 77 are connected to the output of the pulse generator 85 via a delay circuit 84. Similarly, the "S" inputs of the control circuits 81 and 82 of the other two diagonally opposed switches 75 and 76 are connected to output of a pulse generator 87 via a delay circuit 86. The "R" inputs of the control circuits 80, 83, and 81, 82 are connected to the outputs of the respective pulse generators 87 and 85. The pulse generator 85 is of a type which generates a pulse in response to a logic 0-1 transition on its input, for example a monostable multivibrator. The pulse generator 87 is of the type which generates a pulse in response to a logic 1-0 transition on its input. The inputs of the pulse generators 85 and 87 are connected to the output of a pulse-width modulator 88 of a type generating a pulse-width modulated output signal whose frequency is substantially higher than the frequency of the desired energising current and which has a duty cycle which is determined by the amplitude of the signal on its input. By means of the control system described herein, in response to a 0-1 transition of the output signal of the pulse-width modulator 88, the diagonally opposed switches 75, 76 are opened (turned off) and a short time afterwards, determined by the delay switch 84 the two other diagonally opposed switches 74 and 77 are closed (turned on). The coils 16A and 16B are then connected to the power-supply terminals 70 and 71 via the switches 74 and 77. Upon the next logic 1.0 transition of the output signal of the pulse-width modulator 88 the switches 74 and 77 are opened and briefly after this the switches 75 and 76 are closed. The coils 16A and 16B are then connected to the power-supply terminals 70 and 71 via the switches 75 and 76. In this way the coils 16A and 16B are energized with an average voltage which is determined by the duty cycle of the output signal of the pulse-width modulator 88. The high-frequency voltage component produced by change-over of the switches 74, ..., 77 hardly affects the energising current of the motor as a result of the inductance of the motor coils. The energising current through the motor is determined by means of a differential amplifier 89, whose inverting input is connected to the junction point between the resistor 78 and the switch 75 and whose non-inverting input is connected to the junction point between the switch 77 and the resistor 79. The output signal Im of the differential amplifier 89, which is proportional to the voltage difference between said junction points, is consequently proportional to the energising current through the coils 16A and 16B. The signal Im is applied to the inverting input of the differential amplifier 90. The signal Ig from the multiplier 43 is applied to the non-inverting input of the differential amplifier 90, which signal Ig is representative of the desired instantaneous value of the energising current. The output signal of the differential amplifier 90, which is representative of the difference between the desired value Ig and the measure value Im of the energising current, is applied to a control c ircuit 91 of the customary type, for example and integrating control circuit. The control circuit 91 is dimensioned in such a way that depending on the difference between Ig and Im it generates such a control signal for the pulse-width modulator 88 that the duty cycle of the output signal is set to a value for which the energising current produced by the average voltage across the coils 16A and 16B is set to a value for which said difference between Ig and Im is maintained substantially equal to zero.

Claims: A control device for controlling the power supply to an oscillating motor (3) for driving a compressor unit (1) of the resonant-piston type, comprising a circuit (44) for supplying an alternating current from an electric power source (45) to the oscillating motor (3), frequency control means (40,42) for controlling the frequency of the alternating current to an optimal frequency value which substantially corresponds with the resonance frequency of the compressor unit (1), characterized in that the control device is provided with measurement means for determining the optimal frequency value during measurement cycles which are executed at regular intervals, which measurement means being means (40) for setting the frequency of the alternating current to a plurality of different values, means (46,47,48) for determining a measure for the power absorbed by the oscillating motor (3) for each of the different frequency settings, means (40) for determining on basis of the measure of the power absorbed for the different frequency settings the frequency for which the absorbed power is maximal, and in that the control means (40,42) are adapted to set the frequency in the interval following the measurement cycle to a value which substantially corresponds to the optimal frequency determined during the previous measurement cycle. A control device as claimed in Claim 1, characterized in that the control device is provided with means (88,90,91) for maintaining the amplitude of the alternating current constant during at least the determining of the power absorbed. A control device as claimed in Claim 1 or 2, characterized in that the control device comprises comparator means for determining the difference between the instantaneous value of the measure for the power absorbed and the value of the power absorbed which corresponds with the optimal frequency determined in the previous measurement cycle, and initiation means for initiating a measurement cycle if the difference thus determined exceeds predetermined limits. A control device as claimed in any one of the Claims 1, 2 or 3, characterized in that the control device comprises means for iteratively determining the optimal frequency. A control device as claimed in any one of the preceding Claims, characterized in that the control means (40,42) are adapted to adjust the frequency of the alternating current to a frequency equal to the optimum frequency minus a specific value. A compressor unit of the resonant-piston type, comprising an oscillating motor (3) for driving the mechanical resonant system, characterized in that the compressor unit (1) comprises a control device as claimed in any one of the Claims 1 to 5.

Inventors: BOON, FIDELUS ADRIANUS, HEYMANS, PETER MICHEL SILVESTER MARIA, LISSENBURG, ROKUS CORNELIS DIRK, VAN HERK, JOHANNES JOHANNA
Applicants: N.V. PHILIPS' GLOEILAMPENFABRIEKEN
Application year: 1987
Main classification: G05D19
IPC codes: H02K33, F04B35, H02P25, G05D19