Download Battery-Charger Load Switch Approximates An Ideal Diode

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Transcript
Battery-Charger Load Switch
Approximates An Ideal Diode
Budge Ing, Hubert Bugajski
July 19, 2010
Most rechargeable battery-powered systems include a switch that connects
the load either to the battery or to a source of charging power. This switch
allows a system with a depleted battery to operate immediately when
plugged in, running on adapter power while the battery is charging.
The simplest and least expensive switch is a diode-OR connection. The load
connects to each power source (battery and adapter) through separate
Schottky diodes, so power is applied by the higher voltage of the two
sources.
The drawback to this approach is the power dissipation (PD = Ibatt × Vdiode)
and voltage drop (Vdiode = 350 mV at 0.5 A for the PMEG2010AEH) incurred
when the battery services the load. Such losses may not be significant
for high-voltage multicell batteries. But for one-cell Li+ batteries or
two- to four-cell nickel-metal-hydride (NiMH) batteries, the power loss
and diode drop across the blocking diode are considerable.
An alternative technique using a battery-charging IC with a Power OK (POK)
output, like the MAX8814, switches loads with a voltage drop of only 45
mV at 0.5 A, an improvement of 305 mV (Fig. 1). This technique cuts power
dissipation by 152.5 mW (175 mW – 22.5 mW) compared with the diode-OR
connection. Performance improves at lower currents. At 100 mA, for
instance, a diode drops about 270 mV but the alternative circuit drops
only 10 mV.
This circuit switches loads without intervention from a microcontroller
or system software. When operating on batteries and with Vdc In
disconnected, U1’s POK output is high. This condition connects load and
battery by turning on Q4 and Q3. Node 1 is biased to the battery voltage
through R2, which maintains Q1 and Q2 off. When Vdc In connects to a dc
source, Q1 and Q2 are held off because C1 raises node 1 to Vbatt + Vdc.
High voltage at the gates of Q1 and Q2 is generated instantly when Vdc
In is applied. To prevent damage at the POK input, Q5 is configured as
a source follower (voltage buffer). With its gate biased to the battery
voltage, POK sees no voltage higher than the battery voltage. When POK
goes low, current flows through Q5 and pulls down the gates of Q1 and Q2,
turning them on. Vdc In services the load, and U1 charges the battery. C1
and R1 provide a short delay that allows Q3 time to turn off, preventing
unregulated current from flowing to the battery.
When Vdc In is removed, POK becomes a high-impedance node, and battery
current flows through the body diode of Q3. The load voltage is Vbatt –
Vdiode. Because Q5’s gate is biased at the battery voltage, Q5 conducts
until POK reaches a voltage level sufficient to service the load by turning
on Q4 and Q3. Figure 2 shows the circuit’s response (with battery
installed) when Vdc In is applied and removed.
A modified circuit is suitable for battery-charging ICs such as the
MAX1507, which does not provide a POK output (Fig. 3). The comparator (U3)
supplies a POK output by comparing Vdc In to the battery voltage. This
modified circuit’s response is very similar to that of the original
circuit (Fig. 4).