The invention relates to a method and an arrangement for dynamic wave form correction of a power supply of an induction heating device.
Induction heating devices are usually heated and/or powered by working signals, especially by current working signals or the variation of current working signals, which are normally generated or converted in a frequency converter from at least one input power signal provided by an AC power source. The working signals normally comprise a higher frequency than the input power signals.
In many cases, the regulation of the heating power is done by a variation of the frequency of the working signal. Therefore, it is an object of the invention to find a way to vary the frequency of the working signal in a new and advantageous way.
This object is solved by an arrangement and a method for dynamic wave form correction of a power supply of an induction heating device as described below.
Advantageous embodiments are also described.
The invention relates to a method for dynamic wave form correction of a power supply of an induction heating device,
The invention allows a flexible variation of the working signal, as there are at least two working base frequencies between which the working signal can be switched or a zero crossing of the half wave signal is passed within the frequency shifting operation, so that also a shifting in the time or phase direction is possible.
A zero crossing of the half wave signal corresponds in this context to a time where the amplitude of the input power signal is zero, as the current value of the signal changes from a positive to a negative value. Even if the half wave signal should not change from a positive to a negative value at this point, but only touch the value zero, the term zero crossing is also used for this context. As an alternative, the term zero point can be used for the half wave signal.
Particularly, in a subsequent frequency shifting operation the working frequency of the working signal is first increased from the second working frequency to a maximum frequency and then decreased to the first working frequency or to a third working frequency within the half wave duration, where preferably a, particularly further, zero crossing of the half wave signal is passed within the frequency shifting operation.
This enables or eases the repeated execution of frequency shifting operations as, at least after executing the subsequent frequency shifting operation, the first working frequency can be reached again, so that the next frequency shifting operation can be added.
Preferably, a number of n>1 frequency shifting operations is executed one after another,
This embodiment can increase the flexibility for a variation of the frequency even more, as a number of up to n>1 different working base frequencies and/or time lags can be selected.
In an advantageous embodiment,
In another advantageous embodiment, at least one frequency shifting operation comprises a time span before the increasing of the frequency and/or after decreasing the frequency and/or while the working frequency has the maximum value, where the working frequency is hold constant. This can reduce the times where frequency modulation is executed and thus reduce the controlling effort during these times.
Particularly, at least one frequency shifting operation starts and/or ends at a zero-crossing. This has the advantage, that an at least relatively high correlation with respect to the amplitude of the half waves signal is given.
In an alternative, but also advantageous embodiment, at least one frequency shifting operation starts after a timespan of a zero crossing.
In an advantageous embodiment, the working signal, after a working base frequency has been reached, is changing its gradient, particularly from a negative to a zero or a positive value. This is particularly executed at the transition from increasing or decreasing the signal to a period where the signal is constant.
Particularly, the values of the second working base frequency and maximum working frequency are derived from the first working base frequency and from a counter frequency, where especially the ratio of the frequency difference of the second working base frequency from the first working base frequency and the difference of the maximum working frequency from the first working base frequency is constant. This eases the implementation of an controlling algorithm for the generation of the different signals.
In an advantageous embodiment,
Particularly, the first modulation value is 8 and the second modulation value is 25 and/or the counter frequency is between 4 and 100 MHz, especially 10 Mhz.
Furthermore, the invention relates to an arrangement for dynamic wave form correction of a power supply of an induction heating device,
In an advantageous embodiment, the converter comprises at least one full bridge and/or at least one half bridge and/or a single switch.
The invention will be described in further details with references to the drawings, in which
In the embodiments, the input signal Uin is a voltage signal, particularly with an amplitude of about 230 V. Alternatively, a voltage amplitude of about 110 V is possible.
The input power frequency can be 50 Hz or 60 Hz. Alternatively, the input power frequency can be 400 Hz, for example for use in boats or for camping, as this can reduce the size of the device.
The output signal Iw, which is, in the embodiments, a current signal, transmits the generated current for driving the induction heating device 3, which especially contains or is implemented by one or several induction coils.
Inside the frequency converter 2, the input voltage signal Uin is first rectified in the rectifying unit 2a to a voltage signal Uh containing the half waves of the input voltage signal Uin. After that, a high frequency current working signal Iw with a working frequency fW is generated in the inverter unit 2b, for example using IGBTs in a half bridge circuit or a full bridge circuit or a single switch. The behaviour of the frequency converter 2 is controlled by a control unit 4 which is connected to the frequency converter 2 by control lines 7.
In
In the embodiment according to
During the following half waves between t1 and t2, a subsequent frequency shifting operation 6 is executed.
The frequency fw remains constant for the time tv, and is then increased again to a frequency fmax, then held constant for a time tm and finally decreased again to the working base frequency f1, where it remains constant until t2.
Afterwards, the described behaviour is repeated between t2 and t3, and t3 and, not shown, t4.
The time, when the value f2 or f1 is reached again, is arranged after the end t1 of the first half wave. Afterwards, the frequency is constant for a time span tn until t1′.
The same procedure is repeated between t1′ and t2′ and set forth in the following half waves.
The frequency shifting operation 5 is executed between t0′ and t1′ and therefore shifted by a time span ts with respect to the half wave arranged between t0 and t1. The working base frequency f1 is held constant for a time duration tv and then increased to the frequency fmax. Also in the embodiment according to
The time, when the value f2 is reached, is arranged after the end t1 of the first half wave. Afterwards, the frequency is constant for a time span tn until t1′.
The same procedure is repeated between t1′ and t2′ and set forth in the following half waves.
In the embodiments, the ratio between the deviation of fmax with respect to f2 divided by the deviation of f1 with respect to f2 is equal to 31%.
These values are received by dividing the value of the counter frequency by the counter frequency divided by the base frequency f2 after subtracting different values for f1 and fmax. The counter frequency can be 4 MHz to 100 Mhz.
In the following examples, the value for the counter frequency will be 10 MHz, whereas the value for f1 is 8 and the value for fmax is 25.
In a first example, with a value of 19.000 Hz for f2, values of 19.293 for f1 and 19.947 Hz for fmax are received.
In a second example, with a value of 19.000 Hz for f2, a first frequency f1 is located at 25.510 Hz and a maximum frequency fmax is located at a value of 26.666 Hz.
Number | Date | Country | Kind |
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08007985 | Apr 2008 | EP | regional |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP2009/001489 | 3/3/2009 | WO | 00 | 10/15/2010 |
Publishing Document | Publishing Date | Country | Kind |
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WO2009/129889 | 10/29/2009 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
4223195 | Bechtel | Sep 1980 | A |
4713744 | Coston | Dec 1987 | A |
5714739 | Irrera et al. | Feb 1998 | A |
6450241 | Lehman | Sep 2002 | B1 |
6696770 | Nadot et al. | Feb 2004 | B2 |
20020122456 | Fishman et al. | Sep 2002 | A1 |
20060118549 | Fishman et al. | Jun 2006 | A1 |
Number | Date | Country |
---|---|---|
1734789 | Dec 2006 | EP |
Entry |
---|
International Search Report for PCT/EP2009/001489, dated Jul. 23, 2009, 2 pages. |
Number | Date | Country | |
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20110036832 A1 | Feb 2011 | US |