NCV8843
http://onsemi.com
10
W
DRV
+ 12 mA (V
IN
* V
O
)
V
O
2
V
IN
)
The base current of a bipolar transistor is equal to collector
current divided by beta of the device. Beta of 60 is used here
to estimate the base current. The Boost pin provides the base
current when the transistor needs to be on. The power
dissipated by the IC due to this current is
W
BASE
+
V
O
2
V
IN
I
S
60
where:
I
S
= DC switching current.
When the power switch turns on, the saturation voltage
and conduction current contribute to the power loss of a
nonideal switch. The power loss can be quantified as
W
SAT
+
V
O
V
IN
I
S
V
SAT
where:
V
SAT
= saturation voltage of the power switch which is
shown in Figure 7.
The switching loss occurs when the switch experiences
both high current and voltage during each switch transition.
This regulator has a 30 ns turnoff time and associated
power loss is equal to
W
S
+
I
S
V
IN
2
30 ns f
S
The turnon time is much shorter and thus turnon loss is
not considered here.
The total power dissipated by the IC is sum of all the above
W
IC
+ W
Q
) W
DRV
) W
BASE
) W
SAT
) W
S
The IC junction temperature can be calculated from the
ambient temperature, IC power dissipation and thermal
resistance of the package. The equation is shown as follows,
T
J
+ W
IC
R
qJA
) T
A
Minimum Load Requirement
As pointed out in the previous section, a minimum load is
required for this regulator due to the predriver current
feeding the output. Placing a resistor equal to V
O
divided by
12 mA should prevent any voltage overshoot at light load
conditions. Alternatively, the feedback resistors can be
valued properly to consume 12 mA current.
COMPONENT SELECTION
Input Capacitor
In a buck converter, the input capacitor supplies pulsed
current with an amplitude equal to the load current. This
pulsed current and the ESR of the input capacitors determine
the V
IN
ripple voltage, which is shown in Figure 13. For V
IN
ripple, low ESR is a critical requirement for the input
capacitor selection. The pulsed input current has a
significant AC component, which is absorbed by the input
capacitors. The RMS current of the input capacitor can be
calculated using:
I
RMS
+ I
O
D(1 * D)
Ǹ
where:
D = switching duty cycle which is equal to V
O
/V
IN
.
I
O
= load current.
Figure 13. Input Voltage Ripple in a Buck Converter
To calculate the RMS current, multiply the load current
with the constant given by Figure 14 at each duty cycle. It is
a common practice to select the input capacitor with an RMS
current rating more than half the maximum load current. If
multiple capacitors are paralleled, the RMS current for each
capacitor should be the total current divided by the number
of capacitors.
Figure 14. Input Capacitor RMS Current can be
Calculated by Multiplying Y Value with Maximum Load
Current at any Duty Cycle
0 0.2 0.4 1.0
DUTY CYCLE
0
0.1
0.3
0.4
0.5
0.6
0.2
0.6 0.8
I
RMS
(XI
O
)
NCV8843
http://onsemi.com
11
Input capacitor type selection is determined by design
constraints and emphasis (such as cost, performance, or
size). Aluminum electrolytic capacitors are widely available
in a broad selection of values, and are generally economical.
Their ESR and ESL (effective series inductance), however,
are relatively high. Multiple capacitors are often connected
in parallel to reduce ESR, and ceramic capacitors added in
parallel to reduce high frequency noise. OSCON types
exhibit lower ESR. Solid tantalum capacitors combine low
ESR with small physical size.
Output Capacitor
In a buck converter, the requirements on the output
capacitor are not as critical as those on the input capacitor.
The current to the output capacitor comes from the inductor
and thus is triangular. In most applications, this makes the
RMS ripple current not an issue in selecting output
capacitors.
The output ripple voltage is the sum of a triangular wave
caused by ripple current flowing through ESR, and a square
wave due to ESL. Capacitive reactance is assumed to be
small compared to ESR and ESL. The peak to peak ripple
current of the inductor is:
I
P * P
+
V
O
(V
IN
* V
O
)
(V
IN
)(L)(f
S
)
V
RIPPLE(ESR)
, the output ripple due to the ESR, is equal
to the product of I
PP
and ESR. The voltage developed
across the ESL is proportional to the di/dt of the output
capacitor. It is realized that the di/dt of the output capacitor
is the same as the di/dt of the inductor current. Therefore,
when the switch turns on, the di/dt is equal to (V
IN
V
O
)/L,
and it becomes V
O
/L when the switch turns off. The total
ripple voltage induced by ESL can then be derived from
V
RIPPLE(ESL)
+ ESL(
VO
L
) ) ESL(
V
IN
* V
O
L
) + ESL(
V
IN
L
)
The total output ripple is the sum of the V
RIPPLE(ESR)
and
V
RIPPLE(ESL)
.
Figure 15. Output Voltage Ripple Using Two 10 mF
Ceramic Capacitors in Parallel
Figure 16. Output Voltage Ripple Using One 100 mF
POSCAP Capacitor
Figure 17. Output Voltage Ripple Using One
100 mF OSCON
Figure 18. Output Voltage Ripple Using One
100 mF Tantalum Capacitor
NCV8843
http://onsemi.com
12
Figure 15 to Figure 18 show the output ripple of a 5.0 V
to 3.3 V/500 mA regulator using 22 mH inductor and various
capacitor types. At the switching frequency, the low ESR
and ESL make the ceramic capacitors behave capacitively
as shown in Figure 15. Additional paralleled ceramic
capacitors will further reduce the ripple voltage, but
inevitably increase the cost. “POSCAP”, manufactured by
SANYO, is a solid electrolytic capacitor. The anode is
sintered tantalum and the cathode is a highly conductive
polymerized organic semiconductor. TPC series, featuring
low ESR and low profile, is used in the measurement of
Figure 16. It is shown that POSCAP presents a good balance
of capacitance and ESR, compared with a ceramic capacitor.
In this application, the low ESR generates less than 5.0 mV
of ripple and the ESL is almost unnoticeable. The ESL of the
throughhole OSCON capacitor give rise to the inductive
impedance. It is evident from Figure 17 which shows the
step rise of the output ripple on the switch turnon and large
spike on the switch turnoff. The ESL prevents the output
capacitor from quickly charging up the parasitic capacitor of
the inductor when the switch node is pulled below ground
through the catch diode conduction. This results in the spike
associated with the falling edge of the switch node. The D
package tantalum capacitor used in Figure 18 has the same
footprint as the POSCAP, but doubles the height. The ESR
of the tantalum capacitor is apparently higher than the
POSCAP. The electrolytic and tantalum capacitors provide
a lowcost solution with compromised performance. The
reliability of the tantalum capacitor is not a serious concern
for output filtering because the output capacitor is usually
free of surge current and voltage.
Diode Selection
The diode in the buck converter provides the inductor
current path when the power switch turns off. The peak
reverse voltage is equal to the maximum input voltage. The
peak conducting current is clamped by the current limit of
the IC. The average current can be calculated from:
I
D(AVG)
+
I
O
(V
IN
* V
O
)
V
IN
The worse case diode average current occurs during
maximum load current and maximum input voltage. Diode
power dissipation can be estimated by (Iavg x Vf) x
(100duty cycle) / Average power, ambient temperature and
thermal characteristics must all be considered when
selecting a diode. For the diode to survive a short circuit
condition, the current rating of the diode should be equal to
the Foldback Current Limit.
Inductor Selection
When choosing inductors, one might have to consider
maximum load current, core and copper losses, component
height, output ripple, EMI, saturation and cost. Lower
inductor values are chosen to reduce the physical size of the
inductor. Higher value cuts down the ripple current, core
losses and allows more output current. For most
applications, the inductor value falls in the range between
2.2 mH and 22 mH. The saturation current ratings of the
inductor shall not exceed the I
L(PK)
, calculated according to
I
L(PK)
+ I
O
)
V
O
(V
IN
* V
O
)
2(f
S
)(L)(V
IN
)
The DC current through the inductor is equal to the load
current. The worse case occurs during maximum load
current. Check the vendor’s spec to adjust the inductor value
under current loading. Inductors can lose over 50% of
inductance when it nears saturation.
The core materials have a significant effect on inductor
performance. The ferrite core has benefits of small physical
size, and very low power dissipation. But be careful not to
operate these inductors too far beyond their maximum
ratings for peak current, as this will saturate the core.
Powered Iron cores are low cost and have a more gradual
saturation curve. The cores with an open magnetic path, such
as rod or barrel, tend to generate high magnetic field
radiation. However, they are usually cheap and small. The
cores providing a close magnetic loop, such as potcore and
toroid, generate low electromagnetic interference (EMI).
There are many magnetic component vendors providing
standard product lines suitable for the NCV8843. Table 1
lists three vendors, their products and contact information.
Table 1.
Vendor Product Family Web Site
Coiltronics UNIPac1/2: SMT, barrel
THINPAC: SMT, toroid, low profile
CTX: Leaded, toroid
www.coiltronics.com
Coilcraft DO1608: SMT, barrel
DS/DT 1608: SMT, barrel, magnetically shielded
DO3316: SMT, barrel
DS/DT 3316: SMT, barrel, magnetically shielded
DO3308: SMT, barrel, low profile
www.coilcraft.com
TDK SLF10145, SLF12555, VLF10040 www.tdk.com

NCV8843DG

Mfr. #:
Manufacturer:
ON Semiconductor
Description:
Switching Voltage Regulators 340 KHZ REGULATOR
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
Payment:
T/T Paypal Visa MoneyGram Western Union