LTC3114-1
25
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For more information www.linear.com/LTC3114-1
applicaTions inForMaTion
is simply a matter of substituting different values in the
equations provided and reviewing the Bode plots, making
minor adjustments as needed. Since the compensation de
-
sign procedure uses a simplified model of the LTC3114-1,
the results from the following compensation design should
always be verified with time domain step load response tests
to validate the effectiveness of the compensation design. It
is assumed that the value and type of output capacitor will
be selected based on the guidelines provided elsewhere
in this data sheet. Particular attention needs to be paid
to the voltage bias effect on ceramic capacitors typically
used for output bypassing. Similarly, it is assumed that
the inductor value and current rating has been selected
as well based on the application requirements.
Example Application Details:
V
IN
= 9V to 36V
V
OUT
= 12V
Maximum I
OUT
(boost mode) = 700mA, R
LOAD
(min)
= 12V/0.7A = 17.1Ω
Maximum I
OUT
(buck mode) = 1A, R
LOAD
(min) = 12Ω
C
OUT
= 44µF
L = 10µH
Since this application includes boost mode operation, the
first step is to calculate the worst-case RHPZ frequency
as this will dictate the maximum loop bandwidth for the
converter:
RHPZ(f)=
V
IN
2
R
LOAD
V
OUT
2
2π L
(Hz)
substituting the values mentioned earlier yields:
RHPZ(f)=
9V
2
17.1Ω
12V
2
2π 10µH
= 153.1kHz
In order to account for internal IC component variations, it
is good practice to set the converter bandwidth or cross-
over frequency at least three times lower than the RHPZ
frequency to avoid excessive phase loss from the RHPZ
when operating in boost mode. In some instances such
as higher output voltage applications, an even greater
separation between the loop crossover frequency and the
RHPZ frequency may be necessar
y
. In this example design,
we’ll plan to achieve a loop bandwidth (f
CC
) of 29kHz or
approximately one-fifth the RHPZ frequency.
The system poles and zeros are as follows:
Output Load Pole (P1) =
1
2π R
LOAD
C
OUT
;
buck mode, where R
LOAD
= output resistance.
In boost mode this equation is slightly different:
2
2π R
LOAD
C
OUT
( )
,
but with the reduced output current capability in boost
(higher R
LOAD
), the load pole location is about the same.
Error Amp Pole (P2) =
1
2π R
EA
C
C
( )
;
this pole is very close to DC, R
EA
= error amp output
resistance, which is approximately 3.6MΩ. It has no
impact on the compensation design, but is included
here for completeness.
Compensation Zero (Z1) =
1
2π R
Z
C
P1
( )
;
R
Z
and C
P1
are the error amp compensation components
that will be selected.
Ignoring very high frequency output capacitor ESR zero
and secondary high frequency error amp pole, the system
has two poles and one zero. The error amp pole (P2) is
always near DC and we have little influence on it. The
output load pole (P1) will move depending on buck-boost
converter load resistance. The highest frequency for P1, the
output load pole, is at maximum load current (minimum
R
LOAD
). If we design the error amp zero (Z1) frequency
so that it coincides with P1(max), then we will get the
maximum phase benefit from the compensation network
at full load and enough phase boost at lighter loads for
stable operation and a single pole response where the
loop crosses zero dB.
LTC3114-1
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applicaTions inForMaTion
Assuming the error amp zero is designed as just described,
at frequencies above P2 (and Z1), the closed-loop gain of
our system simplifies to:
G
CL
=
G
CS
R
LOAD
g
m
R
Z
V
OUT
where:
G
CS
is the inner current loop closed-loop transconduc-
tance = 1.97A/V
R
LOAD
is the minimum load resistance in ohms
g
m
is the transconductance of the error amplifier, 120µS
R
Z
is the compensation zero setting resistor (one of
our design variables)
V
OUT
is the output voltage
Our desired closed-loop frequency (f
CC
) defined earlier is
29kHz. Assuming that we have a single pole response in
our system, we can express the ratio of the closed-loop
crossover frequency to f
P1
in the buck mode of operation
as follows:
f
CC
f
P1
=
G
CS
R
LOAD
g
m
R
z
V
O
We can now calculate R
Z
by rearranging the previous
equation:
R
Z
=
f
CC
V
OUT
2
π
C
OUT
G
CS
g
m
It’s important to note that the value of R
Z
is proportional
to the overall crossover frequency, f
CC
. If we later want to
adjust f
CC
lower, for example, R
Z
can be lowered in value
and C
P1
increased proportionally to keep the compensa-
tion zero at the same frequency.
As mentioned previously, we will place the zero at fre-
quency P1, yielding:
C
P1
=
1
2π R
Z
f
P1
or more simply,
R
LOAD
C
OUT
R
Z
where R
l
is the minimum load resistance in buck mode,
12Ω in this example.
Quickly substituting our values in the above equations
yields:
R
Z
= 407k, C
P1
= 1.3nF,
but please continue reading as this is not the final answer.
If the inner current loop were an ideal V
CCS
, then the
previously derived compensation would be sufficient to
stabilize the converter. However, the inner current loop
utilizes an operational amplifier with an integral compen
-
sation network, which contributes an additional zero and
pole in the power stage response, the gain peaking, as
described previously. The effect of the additional zero/pole
pair pushes out f
CC
, our crossover frequency, beyond what
was predicted by the previous calculations. A simplified
approach to calculating our compensation components
then is to re-use the previous equations but scale f
CC
, the
cross over frequency, by a scaling factor (α), which will
account for the gain boost present in the system:
f
CC
=
f
CC
3
α
( )
, where α = 0.42
So, in our example, this results in:
f
CC
=
29kHz
3
0.42
( )
= 4.06kHz
Using the new value of f
CC
in the previous equations for
R
Z
and C
C
yields:
R
Z
=
4.06kHz12V 2
π
44µF
1.97A
V
120µA
V
R
Z
= 56.9kΩ, use 56.2kΩ
C
P1
=
12Ω 44µF
56.2k
C
P1
= 9.4nF, use 10nF
C
P2
is usually chosen to be a small value around 10pF as
it is meant to filter out high frequency switching frequency
related components.
Keep in mind that this analysis assumes that the zero pro
-
vided by the output capacitor and its ESR is at a frequency
much higher than f
CC
.
LTC3114-1
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31141fb
For more information www.linear.com/LTC3114-1
Typical applicaTions
9V to 36V V
IN
to 12V V
OUT
Regulator
10µH
SW1 SW2
GND PGND
BST1
68nF
4.7µF
10nF
10pF
33nF
56.2k
20k
182k
INDUCTOR: WÜRTH 744 065 100
D1: ON SEMI MBRS260T3G
31141 TA02a
2M
68nF
BST2
V
IN
PV
OUT
PV
IN
LDO
PLDO
FB
RUN
10µF
V
IN
9V TO 36V
VCPROG
MODE
44µF
V
OUT
12V AT 1A, V
IN
> 12V
12V AT 0.7A, V
IN
> 9V
LTC3114-1
D1
OPTIONAL
Efficiency vs Input Voltage Load Step Response
INPUT VOLTAGE (V)
8
EFFICIENCY (%)
87
93
94
95
16
24
28 32
31141 TA02b
91
89
86
92
85
90
88
12
20
36
40
I
LOAD
= 350mA
LOAD CURRENT
500mA/DIV
V
OUT
200mV/DIV
1ms/DIV
31141 TA02c
V
IN
= 15V
100mA to 700mA

LTC3114EDHC-1#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 40V, 1A Sync. Buck-Boost Converter with Programmable Current Limit
Lifecycle:
New from this manufacturer.
Delivery:
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