Philips Semiconductors Product specification
SG3524SMPS control circuit
1994 Aug 31 4
TIMING CAPACITOR VALUE (C–)–(µF)
10
5
3
2
1.0
0.5
0.3
.001 .002 .005 .01 .02 .05 1
OUTPUT DEAD TIME – microseconds
SL00178
Figure 5. Output Stage Dead Time as a Function of the Timing
Capacitor Value
TIMING RESISTOR (R ) kohms
T
100
50
20
10
5
2
1
1005020105 200 5001ms2ms
OSCILLATOR PERIOD (µs)
SL00179
Figure 6. Oscillator Period
as a Function of RT and CT
FREQUENCY - (Hz)
VOLTAGE GAIN - dB
80
60
40
20
0
10 100 1k 10k 100k 1M 10M
RL = RESISTANCE FROM
PIN 9 TO GND
RL = 30kΩ
RL = 100kΩ
RL = 1MΩ
RL = 30MΩ
RL = 300kΩ
SL00180
Figure 7. Amplifiers Open-Loop Gain as a Function of
Frequency and Loading on Pin 9
Oscillator
The oscillator in the SG3524 uses an external resistor (RT) to
establish a constant charging current into an external capacitor (CT).
While this uses more current than a series-connected RC, it
provides a linear ramp voltage on the capacitor which is also used
as a reference for the comparator. The charging current is equal to
3.6 V ÷RT and should be kept within the approximate range of 30µA
to 2mA; i.e., 1.8k<RT<100k.
The range of values for CT also has limits as the discharge time of
CT determines the pulse-width of the oscillator output pulse. This
pulse is used (among other things) as a blanking pulse to both
outputs to insure that there is no possibility of having both outputs
on simultaneously during transitions. This output dead time
relationship is shown in Figure 5. A pulse width below approximately
0.5µs may allow false triggering of one output by removing the
blanking pulse prior to the flip-flop’s reaching a stable state. If small
values of CT must be used, the pulse-width may still be expanded
by adding a shunt capacitance (≅100pF) to ground at the oscillator
output. [(Note: Although the oscillator output is a convenient
oscilloscope sync input, the cable and input capacitance may
increase the blanking pulse-width slightly.)] Obviously, the upper
limit to the pulse width is determined by the maximum duty cycle
acceptable. Practical values of CT fall between 0.001 and 0.1 µF.
The oscillator period is approximately t=RTCT where t is in
microseconds when RT=Ω and CT=µF. The use of Figure 6 will allow
selection of RT and CT for a wide range of operating frequencies.
Note that for series regulator applications, the two outputs can be
connected in parallel for an effective 0-90% duty cycle and the
frequency of the oscillator is the frequency of the output. For
push-pull applications, the outputs are separated and the flip-flop
divides the frequency such that each output’s duty cycle is 0-45%
and the overall frequency is one-half that of the oscillator.
External Synchronization
If it is desired to synchronize the SG3524 to an external clock, a
pulse of ≅+3V may be applied to the oscillator output terminal with
RTCT set slightly greater than the clock period. The same
considerations of pulse-width apply. The impedance to ground at
this point is approximately 2kΩ.
If two or more SG3524s must be synchronized together, one must
be designated as master with its RTCT set for the correct period.
The slaves should each have an RTCT set for approximately 10%
longer period than the master with the added requirement that
CT(slave)=one-half CT (master). Then connecting Pin 3 on all units
together will insure that the master output pulse—which occurs first
and has a wider pulse width—will reset the slave units.
Error Amplifier
This circuit is a simple differential input transconductance amplifier .
The output is the compensation terminal, Pin 9, which is a
high-impedance node (RL≅5MΩ). The gain is
AVgMRL8 ICRL
2kT 0.002RL
and can easily be reduced from a nominal of 10,000 by an external
shunt resistance from Pin 9 to ground, as shown in Figure 7.
In addition to DC gain control, the compensation terminal is also the
place for AC phase compensation. The frequency response curves
of Figure 7 show the uncompensated amplifier with a single pole at
approximately 200Hz and a unity gain crossover at 5MHz.
Typically, most output filter designs will introduce one or more
additional poles at a significantly lower frequency. Therefore, the
best stabilizing network is a series RC combination between Pin 9
and ground which introduces a zero to cancel one of the output filter
poles. A good starting point is 50kΩ plus 0.001µF.