U-97 APPLICATION NOTE
MODELLING, ANALYSIS AND
COMPENSATION OF THE
CURRENT-MODE CONVERTER
A b s t r a c t
As current-mode conversion increases in popularity, several peculiarities associated with fixed-frequency, peak-current
detecting schemes have surfaced These include instability above 50% duty cycle, a tendency towards subharmonic
oscillation, non-ideal loop response, and an increased sensitivity to noise. This paper will attempt to show that the
performance of any current-mode converter can be improved and at the same time all of the above problems reduced or
eliminated by adding a fixed amount of “slope compensation” to the sensed current waveform.
1.0 INTRODUCTION
The recent introduction of integrated control circuits designed specifically
for current mode control has led to a dramatic upswing in the
application of this technique to new designs. Although the advantages of
current-mode control over conventional voltage-mode control has been
amply demonstrated(l-5), there still exist several drawbacks to a fixed
frequency peak-sensing current mode converter. They are (1) open loop
instability above 50% duty cycle, (2) less than ideal loop response
caused by peak instead of average inductor current sensing, (3) tendency
towards subharmonic oscillation, and (4) noise sensitivity, particularly
when inductor ripple current is small. Although the benefits of current
mode control will, in most cases, far out-weight these drawbacks, a
simple solution does appear to be available. It has been shown by a
number of authors that adding slope compensation to the current
waveform (Figure 1) will stabilize a system above 50% duty cycle. If
one is to look further, it becomes apparent that this same compensation
technique can be used to minimize many of the drawbacks stated above.
In fact, it will be shown that any practical converter will nearly always
perform better with some slope compensation added to the current
waveform.
The simplicity of adding slope compensation - usually a single resistor -
adds to its attractiveness. However, this introduces a new problem - that
of analyzing and predicting converter performance. Small signal AC
models for both current and voltage-mode PWM’s have been
extensively developed in the literature. However, the slope compensated
or “dual control” converter possesses properties of both with an
equivalent circuit different from yet containing elements of each.
Although this has been addressed in part by several authors(l,2), there
still exists a need for a simple circuit model that can provide both
qualitative and quantitative results for the power supply designer.
FIGURE 1- A CURRENT-MODE CONTROLLED BUCK REGULATOR WITH SLOPE COMPENSATION.
3-43
APPLICATION NOTE U-97
The first objective of this paper is to familiarize the reader with the
peculiarities of a peak-current control converter and at the same time
demonstrate the ability of slope compensation to reduce or eliminate
many problem areas. This is done in section 2. Second, in section 3, a
circuit model for a slope compensated buck converter in continuous
conduction will be developed using the state-space averaging technique
outlined in (1). This will provide the analytical basis for section 4 where
the practical implementation of slope compensation is discussed.
2.1 OPEN LOOP INSTABILITY
An unconditional instability of the inner current loop exists for any fixed
frequency current-mode converter operating above 50% duty cycle -
regardless of the state of the voltage feedback loop. While some
topologies (most notably two transistor forward converters) cannot
operate above 50% duty cycle, many others would suffer serious input
limitations if greater duty cycle could not be achieved. By injecting a
small amount of slope compensation into the inner loop, stability will
result for all values of duty cycle. Following is a brief review of this
technique.
A.) DUTY CYCLE < 0.5
B.) DUTY CYCLE > 0.5
COMPENSATING
SLOPE
C.) DUTY CYCLE > 0.5 WITH SLOPE COMPENSATION
FIGURE 2- DEMONSTRATION OF OPEN LOOP INSTABILITY IN A
CURRENT-MODE CONVERTER.
Figure 2 depicts the inductor current waveform,
current
it may be seen graphically that
(3)
Therefore, to guarantee current loop stability, the slope of the
compensation ramp must be greater than one-half of the down slope of
the current waveform. For the buck regulator of Figure 1,
constant equal to
waveform should be chosen such that
vs nT for all n as in Figure 3, we observe a damped
sinusoidal response at one-half the switching frequency, similar to that of
an RLC circuit. This ring-out is undesirable in that it (a) produces a
ringing response of the inductor current to line and load transients, and
(b) peaks the control loop gain at ? the switching frequency, producing
a marked tendency towards instability.
FIGURE 3- ANALOGY OF THE INDUCTOR CURRENT RESPONSE TO
THAT OF AN RLC CIRCUIT.
It has been shown in (1), and is easily verified from equation 2, that by
choosing the slope compensation m to be equal to
2.3 SUBHARMONIC OSCILLATION
For steady state condition we can write
Gain peaking by the inner current loop can be one of the most
(8)
significant problems associated with current-mode controllers. This peaking occurs at one-half the switching frequency, and - because of
or loop to break into oscillation at one-half the switching frequency. This By using (9) to reduce (7), we obtain
instability, sometimes called subharmonic oscillation, is easily detected
as duty cycle asymmetry between consecutive drive pulses in the power (10)
in subharmonic oscillation (dotted waveforms with period 2T).
1
to an output current,
From figure 5, two equations may be
written
(4)(5)
Adding slope compensation as in figure 6 gives another equation
(6)
Using (5) to eliminate from (6) and solving for
yields
(7)FIGURE 6- ADDITION OF SLOPE COMPENSATION TO THE CONTROL
SIGNAL
write the small signal gain at f =
is
4TA
Loop gain =
(12)
1
to guarantee stability as
A
1
then for the case of m = 0 (no
compensation) we see the same instability previously discussed at 50%
duty cycle. As the compensation is increased to m =
system, the finite value of
we reach a point, m = where the
maximum. gain becomes independent of duty cycle. This is the point of critical damping as discussed earlier, and increasing m above this value will do little to improve stability for a regulator operating over the full duty cycle range.
2.4 PEAK CURRENT SENSING VERSUS
AVERAGE CURRENT SENSING
True current-mode conversion, by definition, should force the average inductor current to follow an error voltage - in effect replacing the inductor with a current source and reducing the order of the system by one. As shown in Figure 8, however, peak current detecting schemes are generally used which allow the average inductor current to vary with duty cycle while producing less than perfect input to output - or feedforward characteristics. If we choose to add slope compensation
equal to m = -?
APPLICATION NOTE
(A)
(B)
FIGURE 11
- BASIC BUCK CONVERTER (A) AND ITS SMALL SIGNAL EQUIVALENT CIRCUIT MODEL (B).
If we now perturb these equations - that in substitute
D +
+
duty cycle may be written from Figure 6 as
(18)
Perturbing this equation as before gives
(19)
By using 19 to eliminate from 16 and 17 we arrive at the state space equations
(20)
(21)
An equivalent circuit model for these equations is shown in Figure 11B and discussed in the next section.
3.2 A.C. MODEL DISCUSSION
The model of Figure 11B can be used to verify and expand upon our previous observations. Key to understanding this model is the interaction
U-97
between
If
then a double pole response will be formed by the LRC output filter similar to any voltage-mode converter. By appropriately adjusting m,
any condition between these two extremes can be generated.
Of particular interest is the case when Since the down
slope of the inductor current
At this point,
typical 12 volt buck regulator operating under the following conditions:
APPLICATION NOTE U-97
If a small ripple to D.C. current ratio is used. as is the case for
versus
frequency for the same example of Figure 12. The gains have all been
normalized to zero dB at low frequency to reflect the actual difference in
frequency response as slope compensation m is varied. At m =
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