Electric lamp and discharge devices: systems – Pulsating or a.c. supply – Transformer in the supply circuit
Reexamination Certificate
2001-07-24
2002-11-19
Wong, Don (Department: 2821)
Electric lamp and discharge devices: systems
Pulsating or a.c. supply
Transformer in the supply circuit
C315S224000
Reexamination Certificate
active
06483256
ABSTRACT:
TECHNICAL FIELD
The invention proceeds from an operating device for discharge lamps in accordance with the preamble of claim 1. This is, in particular, a circuit in which the possibilities for heating electrode filaments (W
1
, W
2
) are improved.
PRIOR ART
It is known that gas discharge lamps reach a longer service life when their electrodes are heated up before being started. It is customary to employ the term preheating for this. As a rule, the electrodes are designed for this purpose as filaments to which a preheating current is applied for the purpose of the preheating. A heating current through the filaments can also be desired during operation of the lamp in order to maintain a specific filament temperature. This is the case, in particular, in the dimming of a lamp.
A circuit for heating filaments which seems to be independent of the operation of the gas discharge is disclosed in patent EP 0 707 438. The primary winding (L
11
) of a filament transformer (L
11
, L
12
, L
13
) is connected in parallel with one of the two half-bridge switches for this purpose. Connected in series therewith is a coupling capacitor (CB
1
) so as substantially to absorb the DC component of the AC voltage supplied by the half bridge. Moreover, an electronic switch (S
3
) can also be present in series with the primary winding and can be used to turn the heating of the filaments on and off, or the level of heating can be set by means of a pulse control operation. The filament transformer (L
11
, L
12
, L
13
) has a plurality of secondary windings (L
12
, L
13
) which supply the heating current for the filaments (W
1
, W
2
). Some operating devices have filament-monitoring circuits which operate with a direct current which is small by comparison with the lamp current. In order not to impair the functioning of these circuits, the flow of direct current through the secondary windings must be prevented in at least one direction. This can be achieved by the series circuit of a capacitor or a diode in relation to the respective secondary winding. If only one lamp is being operated, a secondary winding (L
12
, L
13
) is present as a rule for each filament. It may be desired in exceptional cases to heat only one filament. When a plurality of lamps connected in series are being operated, a common secondary winding suffices for the interconnected filaments. As explained below, the possibility of the free selection of the heating current for the filaments by appropriate dimensioning of the filament transformer and/or pulse control operation is limited.
An electronic operating device generally has a generator which is constructed with the aid of electronic switches and outputs a voltage at high frequency by comparison with the system voltage frequency. The energy for operating lamps is thereby made available via suitable reactance two-port networks. The high operating frequency entails a high switching rate for the electronic switches, as a result of which it becomes important for the individual switching operation of an electronic switch to proceed with as little loss as possible. The literature discloses several circuit topologies which permit resonant and/or quasi-resonant switching and thus keep the switching losses low. The half bridge has become established as standard topology for the field of electronic operating devices for lamps. What is involved here is a series circuit, connected between an intermediate circuit potential (P) and a reference potential (E) of an operating voltage (DC), of two electronic switches (S
1
, S
2
). The connecting point (M) of the switches is connected by alternate closing and opening of the switches to the intermediate circuit potential (P) and the reference potential (E). If a switch is now to effect a change in potential of the connecting point (M) by means of a closing operation, there is at first a high voltage at the switch, which drops to a low value in the course of the switching operation. Since the switch must carry current right at the start of a switching operation, this gives rise to high switching losses. The aim is therefore that a switch is turned on only when a low voltage is present across it. The half bridge now offers the possibility of such ZVS (Zero-Voltage-Switching). If specific preconditions are fulfilled, the potential of the connecting point (M) changes automatically (in a quasi-resonant fashion) upon opening of a switch from one potential of the operating voltage (DC) to the other without the need for another switch to be closed. After the automatic change in potential, the other switch can be turned on virtually without loss. In order not to let the automatic change in potential proceed too quickly, a load-relieving capacitor (CT) is frequently connected in parallel to at least one of the two switches. As a result, the losses in the opening switch are reduced and the interference produced by the switching operation is diminished.
It is therefore necessary to attempt to create conditions which deflect an automatic change in potential at the connecting point (M) upon opening of a switch of a half bridge. A necessary condition for this consists in that the load fed by the half bridge must exhibit inductive behavior. The reactance two-port network (Z) for coupling the lamps to the half bridge generally includes a lamp inductor (L
2
). In normal operation of the lamp, it is therefore easy to set an operating frequency at which the load of the half bridge acts inductively. If, by contrast, the above-described filament transformer (L
11
, L
12
, L
13
) is used to preheat the filaments (W
1
, W
2
), and if the lamps are in the preheating phase, the contribution of the lamp inductor (L
2
) to the load impedance is too low to relieve the half-bridge switches (S
1
, S
2
) reliably. The inductance of the lamp inductor (L
2
) can be adapted in order to counteract this effect. However, this is seldom possible since a the lamp inductor (L
2
) must be optimized for normal operation. It is also possible to reduce the capacitance of the load-relieving capacitor (CT) in order to increase the inductance of the load impedance. However, this entails the following disadvantages: the turn-off losses of the half-bridge switches (S
1
, S
2
) are increased, the radio interference which the operating device generates becomes stronger and the possibilities for building up an energy supply from auxiliary circuits from the current through the load-relieving capacitor (CT) are constrained.
SUMMARY OF THE INVENTION
It is an object of the present invention to provide an operating device in accordance with the preamble of claim 1 which also ensures in preheating operation that the half-bridge switches (S
1
, S
2
) are turned on in a virtually de-energized fashion.
This object is achieved in the case of an operating device with the features of the preamble of claim 1 by means of the features of the characterizing part of claim 1. Particularly advantageous refinements are to be found in the dependent claims.
The lamps are connected via a reactance network to the AC voltage supplied by the half bridge at the midpoint potential (M). Said network mostly comprises a series resonant circuit comprising the lamp inductor (L
2
) and a resonance capacitor (CR). There is a need for there to be connected in series with the lamps a coupling capacitor (CB
2
), which absorbs the DC voltage component of the AC voltage supplied by the half bridge. This coupling capacitor (CB
2
) can also be of dual design, in which case one is connected to the intermediate circuit potential (P) and one is connected to the reference potential (E). For starting purposes, the switching frequency of the half bridge is close to the resonant frequency of the resonant circuit (L
2
, CR).
The lamps are not started during preheating, that is to say no lamp current flows. The lamp voltage must not be high during preheating, in order to avoid a premature gas discharge in the lamp. The current through the resonant circuit is therefore also low. It follows that the lamp current is substantially influenced during preheating
Bessone Carlo S.
Nguyen Hoang
Patent-Treuhand-Gesellschaft fuer elektrische Gluehlampen mbH
Wong Don
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