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11
LT1513/LT1513-2
APPLICATIO
S I
FOR
ATIO
U
(from the Electrical Characteristics). Amplifier output resis-
tance is modeled with a 330k resistor. The power stage
(modulator section) of the LT1513 is modeled as a transcon-
ductance whose value is 4(V
IN
)/(V
IN
+ V
BAT
). This is a very
simplified model of the actual power stage, but it is sufficient
when the unity-gain frequency of the loop is low compared
to the switching frequency. The output filter capacitor model
includes its ESR (R
CAP
). A series resistance (R
BAT
) is also
assigned to the battery model.
Analysis of this loop normally shows an extremely stable
system for all conditions, even with 0
for R5. The one
condition which can cause reduced phase margin is with a
very large battery resistance (>5
), or with the battery
replaced with a resistive load. The addition of R5 gives good
phase margin even under these unusual conditions. R5
should not be increased above 330
without checking for
two possible problems. The first is instability in the constant
current region (see Constant-Current Mode Loop Stability),
and the second is subharmonic switching where switch duty
cycle varies from cycle to cycle. This duty cycle instability is
caused by excess switching frequency ripple voltage on the
V
C
pin. Normally this ripple is very low because of the
filtering effect of C5, but large values of R5 can allow high
ripple on the V
C
pin. Normal loop analysis does not show this
W
U
U
Figure 7. Constant-Current Small-Signal Model
problem, and indeed small signal loop stability can be
excellent even in the presence of subharmonic switching.
The primary issue with subharmonics is the presence of EMI
at frequencies below 500kHz.
Constant-Current Mode Loop Stability
The LT1513 is normally very stable when operating in con-
stant-current mode (see Figure 7), but there are certain con-
ditions which may create instabilities. The combination of
higher value current sense resistors (low programmed charg-
ing current), higher input voltages, and the addition of a loop
compensation resistor (R5) on the V
C
pin may create an un-
stable current mode loop. (A resistor is sometimes added in
series with C5 to improve loop phase margin when the loop
is operating in voltage mode.) Instability results
because loop gain is too high in the 50kHz to 150kHz region
where excess phase occurs in the current sensing amplifier
and the modulator. The I
FBA
amplifier (gain of –12.5) has a
pole at approximately 150kHz. The modulator section con-
sisting of the current comparator, the power switch and the
magnetics, has a pole at approximately 50kHz when the
coupled inductor value is 10
μ
H. Higher inductance will reduce
the pole frequency proportionally. The design procedure pre-
sented here is to roll off the loop to unity-gain at a frequency
of 25kHz or lower to avoid these excess phase regions.
–
+
–
+
R
P
**
1M
g
m
1500
μ
mho
I
P
MODULATOR SECTION
I
P
=V
IN
)
IN
+ V
BAT
V1
FB
V
C
1513 F07
1.245V
EA
I
FBA
VOLTAGE
GAIN = 12
R
330k
R5
330
C5
0.1
μ
F
C
A
10pF
R
A
100k
R4
24
R3
0.1
C
P
3pF
C4
0.22
μ
F
I
FB
THIS IS A SIMPLIFIED AC MODEL FOR THE LT1513 IN
CONSTANT-CURRENT MODE. RESISTOR AND CAPACITOR
NUMBERS CORRESPOND TO THOSE USED IN FIGURE 1.
R
AND C
MODEL THE PHASE DELAY IN THE PowerPath.
C3 IS 3pF FOR A 10
μ
H INDUCTOR. IT SHOULD BE SCALED
PROPORTIONALLY FOR OTHER INDUCTOR VALUES (6pF
FOR 20
μ
H). THE PowerPath IS A TRANSCONDUCTANCE
WHOSE GAIN IS A FUNCTION OF INPUT AND BATTERY
VOLTAGE AS SHOWN.
THE CURRENT AMPLIFIER HAS A FIXED VOLTAGE GAIN OF 12.
ITS PHASE DELAY IS MODELED WITH R
A
AND C
A
.
THE ERROR AMPLIFIER HAS A TRANSCONDUCTANCE OF
1500
μ
mho AND AN INTERNAL OUTPUT SHUNT RESISTANCE OF
330k.
AS SHOWN, THIS LOOP HAS A UNITY-GAIN FREQUENCY OF
ABOUT 27kHz. R5 IS NOT USED IN ALL APPLICATIONS, BUT IT
GIVES BETTER PHASE MARGIN IN CONSTANT VOLTAGE MODE.