Switch-mode supply draws 43-mW standby power
Christophe Basso and Francois Lhermite, Motorola SPS, Toulouse, France -- EDN, 6/10/1999
Switch-mode offline supplies offer better efficiency than linear supplies. However, the efficiency of a switchmode power supply (SMPS) seriously degrades with light loads, and commutation losses provoke power dissipation well above 1W even with no load. A good way to build a low-standby-current SMPS is to use a hysteretic architecture, which delivers high-frequency pulses until the output passes a threshold and then no pulses until the output again drops below the threshold. The SMPS consumes little energy delivering the refreshment pulses. Figure 1 shows a circuit that uses an MC34063 controller IC and an insulated-gate bipolar-transistor (IGBT) output device. The MC34063 operates in current mode. Q3 trips the IC when the voltage on sense resistor R16 drops to approximately 550 mV. (IPEAK=160 mA in this example.) You can adjust the peak current to compensate for the transformer's magnetorestrictive effects. Any transformer you use in an SMPS produces audible noise at a low frequency. You can either buy an expensive transformer whose construction ensures low audible noise or keep peak current low, as in Figure 1's circuit. When reducing the peak current, you need to increase either the primary inductance or the switching frequency (by varying C8) to keep the output power constant. The MMG05N60D IGBT has low parasitic capacitance that degrades efficiency at low peak currents. When you open the high-voltage switch in a MOSFET-based flyback converter, the peak current does not immediately drop to zero. Depending on the amount of parasitic capacitance, the current keeps circulating while the drain voltage rises, and efficiency suffers. Figure 2a illustrates this wasteful behavior in a high-voltage, MOSFET-based switcher. The MMG05N60D IGBT has low parasitic capacitance; its total gate charge at VGS=10V is only 4 nC. Figure 2b shows the current in Figure 1's circuit with zero output power. The start-up circuit for the MC34063 uses Q4 and Q2. When you apply the power main, the voltage on C14 starts to rise. The ratio of R20 and R22 causes Q4 and Q2 to remain open. The IC receives no power, and the current that flows in from C14 is small. When the voltage reaches a threshold, Q4 starts to conduct and pulls Q2's gate toward ground. Q2's drain voltage rises and strengthens the conduction in Q4. C14 rapidly discharges into C10, and the MC34063 oscillates. The circuit offers efficiency ranging from 59.4 to 73%. It dissipates no-load power levels of 42.5, 65, and 82.8 mW at dc input voltages of 120, 325, and 360V, respectively.(DI #2363).














