NCV8877
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10
THEORY OF OPERATION
+
Figure 16. Current Mode Control Schematic
Oscillator
Slope
Compensation
Q
S
R
NCV8877
Voltage
Error
VEA
CSA
PWM Comparator
Gate
Drive
L
ISNS
GDRV
VOUT
WAKEUP
ROSC
DISB
DISABLE
R
L
C
O
V
OUT
V
IN
R
SNS
R
OSC
VC
R
DAMP
C
DECOUPLING
GND
DISB
The DISB pin provides an IC disable function. When a DC
logic-low voltage is applied to this pin, the NCV8877 enters
a low quiescent sleep mode, permitting an external signal to
either shutdown the IC or disable the wakeup function.
Regulation
The NCV8877 is a non−synchronous boost controller
designed to supply a minimum output voltage during
Start−Stop vehicle operation battery voltage sags. The
NCV8877 is in low quiescent current sleep mode under
normal battery operation (12 V) and is enabled when the
supply voltage drops below the descending threshold (7.3 V
for the NCV887700). Boost operation is initiated when the
supply voltage is below the regulation set point (6.8 V for the
NCV887700). Once the supply voltage sag condition ends
and begins to increase, the NCV8877 boost operation will
cease when the supply voltage increases beyond the
regulation set point. The NCV8877 low quiescent current
sleep mode resumes once the supply voltage increases
beyond the ascending voltage threshold (7.6 V for the
NCV887700).
The NCV8877 VOUT pin serves the dual purpose: (1)
powering the NCV8877 and (2) providing the regulation
feedback signal. The feedback network is imbedded within
the IC to eliminate the constant current battery drain that would
exist with the use of external voltage feedback resistors.
There is no soft−start operating mode. The NCV8877 will
instantly respond to a voltage sag so as to maintain normal
operation of downstream loads. Once the NCV8877 is
enabled, the voltage error operational transconductance
amplifier supplies current to set VC to 1.1 V to minimize the
feedback loop response time when the battery voltage sag
goes below the regulation set point.
Current Mode Control
The NCV8877 incorporates a current mode control
scheme, in which the PWM ramp signal is derived from the
power switch current. This ramp signal is compared to the
output of the error amplifier to control the on−time of the
power switch. The oscillator is used as a fixed−frequency
clock to ensure a constant operational frequency. The
resulting control scheme features several advantages over
conventional voltage mode control. First, derived directly
from the inductor, the ramp signal responds immediately to
line voltage changes. This eliminates the delay caused by the
output filter and the error amplifier, which is commonly
found in voltage mode controllers. The second benefit
comes from inherent pulse−by−pulse current limiting by
merely clamping the peak switching current. Finally, since
current mode commands an output current rather than
voltage, the filter offers only a single pole to the feedback
loop. This allows for a simpler compensation.
The NCV8877 also includes a slope compensation
scheme in which a fixed ramp generated by the oscillator is
added to the current ramp. A proper slope rate is provided to
improve circuit stability without sacrificing the advantages
of current mode control.
Current Limit
The NCV8877 features two current limit protections,
peak current mode and over current latch off. When the
current sense amplifier detects a voltage above the peak
current limit between ISNS and GND after the current limit
leading edge blanking time, the peak current limit causes the
power switch to turn off for the remainder of the cycle. Set
the current limit with a resistor from ISNS to GND, with R
= V
CL
/ I
limit
.
NCV8877
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11
If the voltage across the current sense resistor exceeds the
over current threshold voltage the device enters over current
hiccup mode. The device will remain off for the hiccup time
and then go through the soft−start procedure.
UVLO
Input Undervoltage Lockout (UVLO) is provided to
ensure that unexpected behavior does not occur when VIN
is too low to support the internal rails and power the
controller. The IC will start up when enabled and VIN
surpasses the UVLO threshold plus the UVLO hysteresis
and will shut down when VIN drops below the UVLO
threshold or the part is disabled.
VDRV
An internal regulator provides the drive voltage for the
gate driver. Bypass with a ceramic capacitor to ground to
ensure fast turn on times. The capacitor should be between
0.1 mF and 1 mF, depending on switching speed and charge
requirements of the external MOSFET.
VDRV uses an internal linear regulator to charge the
VDRV bypass capacitor. VOUT must be decoupled at the IC
by a capacitor that is equal or larger in value than the VDRV
decoupling capacitor.
APPLICATION INFORMATION
Design Methodology
This section details an overview of the component selection
process for the NCV8877 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 Operating Frequency
3. Select Current Sense Resistor
4. Select Output Inductor
5. Select Output Capacitors
6. Select Input Capacitors
7. Select Compensator Components
8. Select MOSFET(s)
9. Select Diode
10. Design Notes
11. 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
max
+ 1 *
V
IN(min)
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
max
is higher the D
max
of the NCV8877,
the conversion will not be possible. It is important for a boost
converter to have a restricted D
max
, because while the ideal
conversion ration 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]
2. Select Operating Frequency
The default setting is an open ROSC pin, allowing the
oscillator to operate at the default frequency F
s
. Adding a
resistor to GND increases the switching frequency.
The graph in Figure 17, below, shows the required
resistance to program the frequency. From 200 kHz to
500 kHz, the following formula is accurate to within 3% of
the expected
Figure 17. R
OSC
vs. F
SW
100
90
80
70
60
50
40
30
20
10
0
150 200 250 500450400350300
F
SW
(kHz)
R
OSC
(kW)
550
NCV8877
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12
R
OSC
+
2859
(
F
sw
* 170
)
Where: f
sw
: switching frequency [kHz]
R
OSC
: resistor from ROSC pin to GND [k]
Note: The R
OSC
resistor ground return to the NCV8877 pin
3 must be independent of power grounds.
3. 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. 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]
4. Select Output Inductor
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 half of V
OUT
, or whatever V
IN
is closest to half of V
OUT
.
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
L,peak
+ I
L,avg
)
DI
L,max
2
Where: I
L,peak
: Peak inductor current value [A]
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)
+
DI
OUT(max)
fC
OUT
)
ǒ
I
OUT(max)
1 * D
)
V
IN(min)
D
2fL
Ǔ
R
ESR
The capacitors need to survive an RMS ripple current as
follows:
I
Cout(RMS)
+ I
OUT
D
WC
DȀ
WC
)
D
WC
12
ǒ
DȀ
WC
L
R
OUT
T
SW
Ǔ
2
Ǹ
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)
+
V
IN(WC)
2
D
WC
Lf
s
V
OUT
23
Ǹ
7. Select Compensator Components
Current Mode control method employed by the NCV8877
allows the use of a simple, Type II compensation to optimize
the dynamic response according to system requirements.
8. 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
Q(max)
+ I
out
D
Ǹ
DȀ
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)
9. 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)
The maximum power dissipation in the diode can be
calculated as follows:
P
D
+ V
f(max)
I
OUT(max)

NCV887720D1R2G

Mfr. #:
Manufacturer:
ON Semiconductor
Description:
Switching Controllers AUTO START-STOP BOOST
Lifecycle:
New from this manufacturer.
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