The present invention relates to switching circuits, and more particularly, to a method for detecting a null current condition in a PWM driven inductor, and a related driving circuit implementing such a method.
Switching circuits using reactive components, such as inductors and capacitors, are increasingly used for converting power. These converters may be characterized by those that use a PWM driven inductor. This inductor has one terminal coupled to a rectified voltage supply line, and another terminal coupled to a PWM drive switch. One or more switches alternate between conduction phases and cut-off phases causing the inductance to absorb energy from the supply during the conduction phase, and release it to a load circuit during the successive cut-off phase.
One of the problems that is encountered in forming these circuits is that of precisely determining the instant in which the switch must be switched on. Often, this switching takes places when the current in the inductor becomes null in order to charge again the inductor after it has delivered to the load all of its stored energy.
This situation is encountered, for example, in power supplies using converters functioning at a high frequency. These converters are used for reasons of space and costs, and are often preferred because they do not require the use of transformers for the mains voltage. Because of their widespread use and importance, in the following description reference will be made to power supplies using DC-DC switching converters for highlighting the addressed technical problem. However, the considerations that will be made hold for any circuit using a PWM driven inductor, that is, the current in the inductor becomes null between two consecutive switchings toward the voltage source.
Many of the current electronic devices are powered by power supplies that are directly connected to the mains voltage, as depicted in FIG. 1. The mains voltage is rectified by a rectifying bridge, and then filtered with a relatively large capacitor CBULK. As may be noticed in
These power supplies cause a strong harmonic content of the mains current, which reduces the power factor. Enforced “power quality” specifications impose the use of circuits that correct the non-linearity of the current absorbed from the mains voltage by making it almost sinusoidal for remaining below a certain maximum tolerable limit having a harmonic content.
There are many techniques for improving the power factor. Some techniques contemplate the use of passive networks using capacitors and inductors. Other techniques contemplate the use of active circuits for correcting the power factor. In the latter case, which is the case of interest, the power supply has one or more switches that are switched for charging the bulk capacitor during the whole half-wave of the AC network voltage by absorbing current at high frequency and at a level proportional to the instantaneous value of the mains voltage.
As is well known to those skilled in the art, there are different topologies of power factor correction circuits, and each of them has advantages and drawbacks depending on the output power. One of the most used topologies for circuits having an output power less than 80 W is the so-called “Boost” topology with TM (Transition Mode) control, with a fixed turn on time TON and variable frequency.
The power supply of
According to a transition mode TM control, the switch SW remains in a conduction state for a constant time TON, the value of which depends on the load. The value of the current circulating in the inductor L when this time interval expires is
The inductor is turned off and the stored energy: E=½·L·I2 is transferred through the clamping diode D to the bulk capacitor CBULK in the form of a charging current (discharging current of the inductance). The switch is turned on again when energy transfer is completed, that is, after the current in the inductor has become null.
Generally, two alternative techniques are used for detecting the null current condition in the inductor. One technique is connecting in series to the inductor a sensing resistance and monitoring the voltage drop on it. The other technique forms an auxiliary winding magnetically coupled to the inductor L and uses the induced signal on the auxiliary winding for determining the turn on instant of the switch.
Both techniques have the following drawbacks. The first technique implies a power dissipation on the current sensing resistor, and as a consequence, a reduction of the efficiency of the system. The second technique requires the use of a transformer, which consequently increases cost. None of these techniques are amenable to a complete integration on silicon.
An object of the present invention is to provide a method for detecting a null current condition in an inductor driven in a switched mode that, differently from the known methods, can be implemented in circuits that are fully integrated on silicon with significant advantages in terms of simplification and cost.
In circuits using a PWM driven inductor, a first terminal is coupled to a voltage source node, and a second terminal is coupled to a line for outputting a current toward a load and to a driving switch that alternates conduction phases and non-conduction phases. When the current in the inductor becomes null, there is a drop of the voltage on the second terminal of the inductor which becomes equal to the voltage present on the first terminal.
By detecting this occurrence for establishing a nullification of the current circulating in the inductor, important advantages may be achieved in terms of simplifying the circuit and for allowing the realization of the entire driving circuit in an integrated form. This is because the use of a current sensing resistor or an auxiliary winding is no longer required.
Another object of the invention is to provide a method for detecting the null current condition in a PWM driven inductor having a first terminal connected to a voltage source node and a second terminal connected to a line for outputting current toward a load. The method comprises time differentiating the voltage on the second terminal of the inductor for generating a time derivative signal, monitoring an instant when the derivative signal becomes negative, and signaling the nullification of the current flowing in the inductor each time the derivative signal becomes negative. The voltage on the second terminal of the inductor may also be filtered before being differentiated.
Another object of the present invention is to provide a PWM driving circuit for an inductor while detecting the nullification of the current flowing in the inductor. The PWM driving circuit has a first terminal connected to a voltage source node and a second terminal connected to a line for outputting current toward a load. A power switch is connected between the second terminal and a ground node of the circuit, a PWM control circuit is connected to the switch and operates as a function of load conditions, and a bistable output stage is coupled to a control terminal of the power switch.
The driving circuit of the invention may also comprise a differentiating line or stage coupled to the second terminal of the inductor. A derivative signal is produced by the differentiating stage when the voltage on the second terminal of the inductor drops because of the nullification of the current circulating in the inductor that has become negative. This causes the switching of a monitoring circuit that in turn sets the bistable output circuit, and thus turns on the power switch.
The driving circuit of the invention allows the formation of boost converters and power factor correction circuits for power supplies without requiring external components (non-integrable components), such as current sensing resistors or auxiliary windings magnetically coupled to the inductor for detecting a null current condition in the inductor.
The different aspects and advantages of the invention will become even more evident through a detailed description of embodiments of the invention and by referring to the attached drawings, in which:
a and 5b are basic block diagrams of power supplies embodying the driving circuit of the present invention;
It has been observed that, in boost converters and power factor correction circuits, characterized by comprising a PWM driven inductor having a first terminal connected to a voltage source node and a second terminal connected to a line for outputting current toward a load, that when the current in the inductor becomes null, the voltage on the second terminal diminishes and becomes equal to the voltage on the first terminal. This voltage may correspond to a rectified mains voltage node, for example.
According to the method of the present invention, the null current condition in the inductor is effectively detected by time differentiating the voltage on the second terminal, and causing the signaling of a null current condition when the time derivative signal becomes negative because of a drop of the voltage on the second terminal. If the voltage on the second node is excessively noisy for causing false null current verifications, it may be filtered before being differentiated.
To better illustrate the peculiarity of the driving circuit of the present invention, an application to a common boost converter will be described in detail, but the considerations that will be made hold for any other circuit employing a PWM driven inductor.
a is a basic block diagram of a power supply based on a boost converter that uses the driving circuit of the invention (enclosed by the dashed line). A rectifying bridge rectifies the AC mains voltage and provides a rectified voltage to a boost converter that drives an electrical load LOAD.
b is a basic block diagram of a power supply that includes a power factor correction circuit using the driving circuit of the invention, a bulk capacitor CBULK and a converter, which can be either a DC-DC or an AC-DC converter.
Referring to
The switch is commanded to an off state by applying a voltage on the reset input R of the flip-flop FF. During this off phase, the energy stored in the inductor is transferred to the capacitor C in the form of a charge current flowing through the clamping diode D.
This happens only if the voltage on the second node A of the second terminal of the inductor is:
VA=VOUT+VBE>VIN
where VIN is the instantaneous rectified voltage at the output of the rectifying bridge, and VBE is the base-emitter voltage of the power switch SW.
The voltage VA is substantially constant when the inductor transfers energy toward the load. In this time interval, which is a function of the voltage difference on the terminals of the inductor L, the current in the inductor decreases from the value reached at the end of the previous charging phase, until it becomes null. When this current becomes null, the voltage on the node A drops, becoming equal to the rectified input voltage VIN.
According to this embodiment, the time differentiating element of the block DERIVATIVE is basically a capacitor connected between the DRAIN node and the gate of a second switch SW2 that switches the set input S of the bistable circuit FF to the supply voltage VDD.
When the voltage on the node DRAIN drops because of the nullification of the current in the inductor, the differentiating capacitor absorbs current (i.e., the derivative signal becomes negative) from the gate of the switch SW2 which turns on, thus momentarily coupling the set input S of the bistable circuit FF to the supply voltage VDD of the circuit. The output Q of the bistable circuit FF switches to an active state for turning on the power switch SW.
A distinction from similar known driving circuits is that the circuit of the invention does not require any sensing resistor to be connected in series to the inductor, or any auxiliary winding magnetically coupled to it. Moreover, the time differentiating block DERIVATIVE can be integrated on the same chip as the power switch SW and the relative control and drive circuitry.
The integrated device of
According to the embodiment shown, a turn off circuit for the switch SW includes a comparator COMP and a switch SW3 for generating a reset pulse for the bistable circuit FF after a pre-established time from the last generated set pulse (fixed turn-on time TON). This pre-established time is determined by the capacitance of the capacitor C4 connected to the pin CAP of the device as shown, and by the charging current I. Substantially, when a negative derivative signal is applied to the gate of the switch SW2 in the differentiating block DERIVATIVE, it also switches a third switch SW3 for discharging the capacitor C4. When the voltage on the nodes of the capacitor C4 drops below a pre-established threshold, the comparator COMP generates a reset pulse (R) for the flip-flop FF that turns off the power switch SW.
A hysteresis comparator HYST receives a feedback signal that is fed to the dedicated pin FB. The feedback signal is representative of the output voltage that is provided to the load. The comparator HYST turns off and on the power switch SW when the feedback signal respectively surpasses the upper and lower thresholds.
In the shown embodiment, the feedback signal is also used to regulate the charging current I of the capacitor C4 to vary the turn on time of the power switch SW as a function of load conditions. The feedback signal can be customarily tapped from a resistive voltage divider R3, R4 connected in parallel to the load LOAD, as depicted in FIG. 8.
Optionally, the driving circuit of the invention may also be provided, according to a common technique, for a blanking circuit (not depicted in
Number | Date | Country | Kind |
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02425295 | May 2002 | EP | regional |
Number | Name | Date | Kind |
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5463306 | Berry et al. | Oct 1995 | A |
Number | Date | Country |
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0507393 | Mar 1992 | EP |
Number | Date | Country | |
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20040036450 A1 | Feb 2004 | US |