The invention relates to a secondary side rectifier of an inductive energy transmission system, wherein the energy transmission system has a single-phase resonant circuit, which has at least one inductor and at least one capacitor and can be magnetically coupled to a primary side resonant tuned circuit, and wherein the secondary side rectifier has a B2 bridge circuit, which consists of four diodes and is connected on the input side to the secondary side resonant circuit, and the output voltage of which is smoothed by at least one smoothing capacitor.
In contactless energy transmission, an induced voltage in the secondary circuit of an air gapped transformer is generally rectified, the resulting DC voltage subsequently being used to supply loads. A simple rectifier in this case consists of a B2 bridge comprising of four diodes D1-D4 and an additional smoothing capacitor, as represented in
The rectifier described above is also suitable for rectifying an inductive energy transmission system that has a single-phase primary side resonant circuit and a single-phase secondary side resonant circuit, which are magnetically coupled to one another. The resonant circuits may be formed as parallel or series circuits, consisting of inductors and capacitors.
It is an object of the present invention to provide a controlled secondary side rectifier with the output voltage can be regulated or adjusted, and which consists of few components.
This object is achieved according to the invention by a secondary side rectifier having the features of claim 1. Other advantageous configurations of the rectifier according to the invention are given by the features of the dependent claims.
The secondary side rectifier according to the invention is advantageously distinguished in that it requires only one controlled switching means, with which it is possible to switch to and fro between two modes. The switching means is connected in parallel with one of the diodes of the B2 bridge. When the switching means is open, the parallel diode is not short-circuited, so that the secondary side rectifier operates as a conventional uncontrolled B2 bridge rectifier. In this mode, there is therefore full bridge rectification. This typically delivers simple peak value rectification of the AC value, with
U
A=√2*Ui in no-load operation.
In the second mode, the diode is short-circuited by means the switching means, so that the rectifier operates together with the at least one capacitor of the secondary side resonant circuit as a voltage doubler. In the second mode, the doubled voltage value UA=2*√2*Ui is set up after several oscillation periods of the resonant circuit in no-load operation.
By the on-state time of the switching means, it is therefore possible to switch the output voltage between the values UA,min=√2*Ui and UA,max=2*√2*Ui, or permanently to UA,min or UA,max.
It is in this case advantageous for the switching means to be soft-switched, that is to say no current flows through the switching means when it switched, and it is switched without voltage. This leads to advantageously low switching losses. It is, however, also possible for the switching means to be hard-switched.
The secondary side rectifier according to the invention therefore allows regulation of the output voltage in a sufficiently large adjustment range with only one additional switching means. The one switching means therefore advantageously replaces an otherwise required DC/DC converter.
The rectifier according to the invention is distinguished because of the few components required and by a compact design and low weight, and it is furthermore favourable in terms of production.
Owing to the possibility of operating the rectifier in voltage doubler mode, the reactive power in the secondary side resonant tuned circuit can advantageously be reduced, since the resonant capacitors merely need to be dimensioned for the sum of the active voltage and half the reactive voltage of the conventional passive rectifier.
If the rectifier according to the invention is used in a pickup, the latter can advantageously be dimensioned smaller and manufactured more favourably. The invention likewise claims an energy transmission system and a pickup, which the secondary rectifier according to the invention is used.
The rectifier according to the invention will be explained in more detail below with the aid of drawings, in which:
The switching means S, with which the rectifier can be switched to and fro between a first mode and a second mode, is connected in parallel with an arbitrary diode D1 to D4. In the first mode, when the semiconductor switch S is switched off, the rectifier behaves as a B2 full bridge, as represented in
U
A,min=√2*Ui
is then set up at the output.
If the switching means S is closed, then the potential at point P1 is set to earth, or the potential of the terminal A1, and the rectifier is in the second mode and therefore in doubling mode. If the switching means S is closed, or switched on, for long enough, an output voltage
U
A,max=2*√2*Ui
is set up.
Depending on the on-state time, the output voltage UA can therefore be regulated to an arbitrary value between the two limit values and UA,min and UA,max.
In the second mode, the negative half wave of the induced voltage flows through the diode D3, so that the resonant capacitor CS is charged to its peak value before subsequently charging the smoothing capacitor Cgr during the positive half-wave via the diode D4 to the sum of the induced voltage of the positive half-wave and the resonant capacitor voltage which was stored during the negative half-wave, so that the voltage UA,max is set up after a few oscillation periods.
At time T1, the drive signal S for the switching means S is set to ONE, so that the diode D1 is short-circulated by the switching means S. From time T1 onwards, the rectifier operates together with the capacitor CS of the resonant tuned circuit as a voltage doubler. The potential of the point P1, and therefore a potential of the tuned circuit, is thereby—as represented—set to ground or a fixed potential, in so far as an upper diode is short circuited by means of the switching means S. The rectifier current Igr flows in the positive half-period. Since the output voltage UA at the smoothing capacitor Cgr cannot be doubled abruptly, the peak current increases and more power is fed to the output circuit as an average value. The output voltage UA increases with the time constant which derives from the Q-factor of the overall passive circuit. The drive signal G generally has a frequency which is less than the transmission frequency of the energy transmission system. As already mentioned above, the value of the output voltage UA or of the output current of the rectifier can be regulated by means of the on-state/off-state time of the semiconductor switch S.
Number | Date | Country | Kind |
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10 2011 119 261.5 | Nov 2011 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP2012/070852 | 10/22/2012 | WO | 00 | 5/23/2014 |