In known claw-pole generators, the energy for the excitation is taken from the electrical system of the respective motor vehicle. This takes place using a generator controller that has a switched semiconductor as a switching element. The generator controller sets the excitation voltage between 0 V and the electrical system voltage. This is shown in
From German Published Patent Application No. 196 34 096, a voltage supply system is known that has an increased output power, produced when an increased power requirement is signaled by an external control signal. The known system has a three-phase generator whose windings supply the voltage for a vehicle electrical system via rectifiers. In addition, the generator contains an exciter winding through which the excitation voltage, which can be influenced by a voltage controller, flows. The exciter winding can be operated with a voltage that is higher than the supply voltage during times that can be predetermined. This increased voltage is produced through the activation of additional windings having rectifiers in the generator, or by a direct-current converter allocated to the generator. In this way, the controlling of the generator takes place through the voltage controller, which has controlled transistors, in such a way that the output voltage of the generator remains at the level of the electrical system.
In contrast, the present invention achieves an increased output power of the generator by using, as an improved magnetic utilization of the generator, the ripple at the exciter winding ends in order to achieve a capacitive voltage increase. This takes place economically through the use of a passive additional circuit that has no transistors. In comparison with circuit topologies that, for example, use direct-current converters for voltage multiplication, this results in advantages with respect to the electromagnetic compatibility.
In comparison to all actively controlled additional circuits, advantages result the fact that no actively controlled components are required. Conventional diodes and capacitors can be used. In addition, no saturation effects occur. The additional circuit according to the present invention is secure against short-circuiting and against open-circuit operation.
An additional voltage increase can advantageously be achieved through the use of a cascade connection.
According to the present invention, an additional circuit that uses only passive components is inserted into a three-phase generator, preferably a claw-pole generator, and through the use of said circuit an increase is achieved in the excitation voltage drop at the excitation winding of the generator. In this way, the excitation current flowing through the excitation winding, and thus the output power provided by the generator, are also increased.
With an additional circuit according to the present invention, the output voltage of the generator can for example be doubled or tripled. A further increase of the output voltage of the generator is possible through the additional use of a cascade connection.
In alternative exemplary embodiments, not shown in the drawing, the additional circuit has only one parallel circuit having two signal branches, or simply has only one signal branch, each of these signal branches being constructed in the same way as one of the signal branches shown in
If a booster circuit according to
In addition, if such a booster circuit is additionally placed into the connection branch between the terminal adjacent to ground of excitation winding WE and ground, there results the device shown in
The curve of the winding voltages at taps U, V, W is shown in
In the following, the functioning of the voltage increase circuit in the exemplary embodiment according to
A voltage of 14V is present at the capacitor situated in the U phase, said capacitor being connected to the electrical system via a diode of the additional circuit. A flow of current takes place from the electrical system to the capacitor via the diode. In this way, the potential at tap U increases to a value that corresponds to the sum of the electrical system voltage and the forward voltage of the diode, i.e., to a value (UBN÷0.7 V). This corresponds to an increase in the charge of the capacitor.
Subsequently, charge flows from the capacitor into the exciter circuit via the second diode of the additional circuit. In this way, the potential at tap U sinks again to −0.7 V. This process, which is constantly repeated, takes place in each of phases U, V, W, with a time offset of 120°.
For example, let exciter current Ierr=8 A and let exciter voltage Uerr=24V. The energy output of the capacitor is then calculated as
For the power of the booster circuit, the following holds:
In this way, the following is obtained:
C≈1500 μF, if f=180 Hz.
If the boundary conditions change, different values will result.
Number | Date | Country | Kind |
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101 50 373 | Oct 2001 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/DE02/03795 | 10/2/2002 | WO | 00 | 10/19/2004 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO03/034583 | 4/24/2003 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
4092712 | Harrigill et al. | May 1978 | A |
4389703 | Morel et al. | Jun 1983 | A |
5986439 | Pletta et al. | Nov 1999 | A |
6272031 | Shona | Aug 2001 | B1 |
Number | Date | Country |
---|---|---|
196 34 096 | Feb 1998 | DE |
0 325 454 | Jul 1989 | EP |
Number | Date | Country | |
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20050041344 A1 | Feb 2005 | US |