NCV898032
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13
2. Select Current Sense Resistor
Current sensing for peak current mode control and current
limit relies on the MOSFET current signal, which is
measured with a ground referenced amplifier. Note that the
I
CL
equals the sum of the currents from both inductors. The
easiest method of generating this signal is to use a current
sense resistor from the source of the MOSFET to device
ground. The sense resistor should be selected as follows:
R
S
+
V
CL
I
CL
Where: R
S
: sense resistor [W]
V
CL
: current limit threshold voltage [V]
I
CL
: desire current limit [A]
3. Select SEPIC Inductors
The output inductor controls the current ripple that occurs
over a switching period. A high current ripple will result in
excessive power loss and ripple current requirements. A low
current ripple will result in a poor control signal and a slow
current slew rate in case of load steps. A good starting point
for peak to peak ripple is around 20−40% of the inductor
current at the maximum load at the worst case V
IN
, but
operation should be verified empirically. The worst case V
IN
is the minimum input voltage. After choosing a peak current
ripple value, calculate the inductor value as follows:
L +
V
IN(WC)
D
WC
DI
L,max
f
s
Where: V
IN(WC)
: V
IN
value as close as possible to half of
V
OUT
[V]
D
WC
: duty cycle at V
IN(WC)
DI
L,max
: maximum peak to peak ripple [A]
The maximum average inductor current can be calculated as
follows:
I
L,AVG
+
V
OUT
I
OUT(max)
V
IN(min)
h
The Peak Inductor current can be calculated as follows:
I
L1,peak
+ I
L1,avg
)
DI
L1
2
I
L2,peak
+ I
OUT(max)
)
DI
L2
2
Where (if L1 = L2): DI
L1
= DI
L2
4. Select Coupling Capacitor
Coupling capacitor RMS current is significant. A low
ESR ceramic capacitor is required as a coupling capacitor.
Selecting a capacitor value too low will result in high
capacitor ripple voltage which will distort ripple current and
diminish input line regulation capability. Budgeting 2−5%
coupling capacitor ripple voltage is a reasonable guideline.
DV
coupling
+
I
out
D
WC
C
coupling
f
s
Current mode control helps resolve some of the resonant
frequencies that create issues in voltage mode SEPIC
converter designs, but some resonance issues may occur. A
resonant frequency exists at
f
resonance
+
1
2p (L1 ) L2)C
coupling
Ǹ
It may become necessary to place an RC damping network
in parallel with the coupling capacitor if the resonance is
within ~1 decade of the closed−loop crossover frequency.
The capacitance of the damping capacitor should be ~5
times that of the coupling capacitor. The optimal damping
resistance (including the ESR of the damping capacitor) is
calculated as
R
damping
+
L1 ) L2
C
coupling
Ǹ
5. Select Output Capacitors
The output capacitors smooth the output voltage and
reduce the overshoot and undershoot associated with line
transients. The steady state output ripple associated with the
output capacitors can be calculated as follows:
V
OUT(ripple)
+
I
OUT(max)
D
WC
C
OUT
f
s
)
ǒ
I
OUT(max)
1 * D
WC
)
D
WC
V
IN(min)
2 f
s
L
2
Ǔ
R
esr
The capacitors need to survive an RMS ripple current as
follows:
I
Cout(RMS)
+
I
OUT(max)
2
D
WC
)
ǒ
I
2
a
)
I
2
r
3
* I
a
I
r
Ǔ
DȀ
WC
Ǹ
where
I
a
+ I
L1_peak
) I
L2_peak
* I
out
I
r
+ DI
L1
) DI
L2
The use of parallel ceramic bypass capacitors is strongly
encouraged to help with the transient response.
6. Select Input Capacitors
The input capacitor reduces voltage ripple on the input to
the module associated with the ac component of the input
current.
I
Cin(RMS)
+
DI
L1
12
Ǹ
7. Select Feedback Resistors
The feedback resistors form a resistor divider from the
output of the converter to ground, with a tap to the feedback
pin. During regulation, the divided voltage will equal V
ref
.
The lower feedback resistor can be chosen, and the upper
feedback resistor value is calculated as follows:
R
upper
+ R
lower
ǒ
V
out
* V
ref
Ǔ
V
ref
NCV898032
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14
The total feedback resistance (R
upper
+ R
lower
) should be
in the range of 1 kW – 100 kW.
8. Select Compensator Components
Current Mode control method employed by the
NCV898032 allows the use of a simple, Type II
compensation to optimize the dynamic response according
to system requirements.
9. Select MOSFET(s)
In order to ensure the gate drive voltage does not drop out
the MOSFET(s) chosen must not violate the following
inequality:
Q
g(total)
v
I
drv
f
s
Where: Q
g(total)
: Total Gate Charge of MOSFET(s) [C]
I
drv
: Drive voltage current [A]
f
s
: Switching Frequency [Hz]
The maximum RMS Current can be calculated as follows:
I
D(max)
+ D
WC
ǒ
I
Q(peak)
2
)
ǒ
DI
L1
) DI
L2
Ǔ
2
3
* I
Q(peak)
ǒ
DI
L1
) DI
L2
Ǔ
Ǔ
Ǹ
where
I
Q(peak)
+ I
L1_peak
) I
L2_peak
The maximum voltage across the MOSFET will be the
maximum output voltage, which is the higher of the
maximum input voltage and the regulated output voltaged:
V
Q(max)
+ V
OUT(max)
) V
IN(max)
10. Select Diode
The output diode rectifies the output current. The average
current through diode will be equal to the output current:
I
D(avg)
+ I
OUT(max)
Additionally, the diode must block voltage equal to the
higher of the output voltage and the maximum input voltage:
V
D(max)
+ V
OUT(max)
) V
IN(max)
The maximum power dissipation in the diode can be
calculated as follows:
P
D
+ V
f(max)
I
OUT(max)
Where: P
d
: Power dissipation in the diode [W]
V
f(max)
: Maximum forward voltage of the diode [V]
NCV898032
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15
BOOST TOPOLOGY APPLICATION INFORMATION
Oscillator
Slope
Compensation
+
NCV898032
Voltage Error
VEA
CSA
PWM Comparator
Gate
Drive
Compensation
L
GDRV
Figure 12. Boost Current Mode Schematic
S
R
Q
C
O
R
L
V
OUT
V
FB
I
SNS
V
IN
Boost Converter Design Methodology
This section details an overview of the component
selection process for the NCV898032 in continuous
conduction mode boost. It is intended to assist with the
design process but does not remove all engineering design
work. Many of the equations make heavy use of the small
ripple approximation. This process entails the following
steps:
1. Define Operational Parameters
2. Select Current Sense Resistor
3. Select Output Inductor
4. Select Output Capacitors
5. Select Input Capacitors
6. Select Feedback Resistors
7. Select Compensator Components
8. Select MOSFET(s)
9. Select Diode
10. Determine Feedback Loop Compensation Network
1. Define Operational Parameters
Before beginning the design, define the operating
parameters of the application. These include:
V
IN(min)
: minimum input voltage [V]
V
IN(max):
maximum input voltage [V]
V
OUT
: output voltage [V]
I
OUT(max)
: maximum output current [A]
I
CL
: desired typical cycle−by−cycle current limit [A]
From this the ideal minimum and maximum duty cycles can
be calculated as follows:
D
min
+ 1 *
V
IN(max)
V
OUT
D
WC
+ 1 *
V
IN(WC)
V
OUT
Both duty cycles will actually be higher due to power loss
in the conversion. The exact duty cycles will depend on
conduction and switching losses. If the maximum input
voltage is higher than the output voltage, the minimum duty
cycle will be negative. This is because a boost converter
cannot have an output lower than the input. In situations
where the input is higher than the output, the output will
follow the input, minus the diode drop of the output diode
and the converter will not attempt to switch.
If the calculated D
WC
is higher than the D
max
limit of the
NCV898032, the conversion will not be possible. It is
important for a boost converter to have a restricted D
max
,
because while the ideal conversion ratio of a boost converter
goes up to infinity as D approaches 1, a real converters
conversion ratio starts to decrease as losses overtake the
increased power transfer. If the converter is in this range it
will not be able to regulate properly.
If the following equation is not satisfied, the device will
skip pulses at high V
IN
:
D
min
f
s
w t
on(min)
Where: f
s
: switching frequency [Hz]
t
on(min)
: minimum on time [s]

NCV898032D1R2G

Mfr. #:
Manufacturer:
ON Semiconductor
Description:
Switching Controllers AUTOMOTIVE SWITCHER
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