MIC2198 Micrel, Inc.
MIC2198 10 October 2005
where:
I
G[high-side](avg)
=
average high-side MOSFET gate current.
Q
G
= total gate charge for the high-side MOSFET
taken from manufacturer’s data sheet
with V
GS
= 5V.
f
s
= 500kHz
The low-side MOSFET is turned on and off at V
DS
= 0 because
the freewheeling diode is conducting during this time. The
switching losses for the low-side MOSFET is usually negli-
gible. Also, the gate drive current for the low-side MOSFET
is more accurately calculated using C
ISS
at V
DS
= 0 instead
of gate charge.
For the low-side MOSFET:
I C V f
G[low-side](avg) ISS GS S
= × ×
Since the current from the gate drive comes from the input
voltage, the power dissipated in the MIC2198 due to gate
drive is:
P V I I
GATEDRIVE IN G[high-side](avg) G[low-side](avg)
= +
( )
A convenient figure of merit for switching MOSFETs is the
on-resistance times the total gate charge (R
DS(on)
× Q
G
).
Lower numbers translate into higher efficiency. Low gate-
charge logic-level MOSFETs are a good choice for use with
the MIC2198. Power dissipation in the MIC2198 package
limits the maximum gate drive current.
Parameters that are important to MOSFET switch selection
are:
Voltage rating
On-resistance
Total gate charge
The voltage rating of the MOSFETs are essentially equal to
the input voltage. A safety factor of 20% should be added to
the V
DS(max)
of the MOSFETs to account for voltage spikes
due to circuit parasitics.
The power dissipated in the switching transistor is the sum
of the conduction losses during the on-time (P
CONDUCTION
)
and the switching losses that occur during the period of time
when the MOSFETs turn on and off (P
AC
).
P P P
SW CONDUCTION AC
= +
where:
P I R
CONDUCTION
SW(rms)
SW
2
= ×
P P P
AC AC(off) AC(on)
= +
R
SW
= on-resistance of the MOSFET switch.
Making the assumption the turn-on and turnoff transition times
are equal, the transition time can be approximated by:
t
C V C V
I
T
ISS GS OSS IN
G
=
× + ×
where:
C
ISS
and C
OSS
are measured at V
DS
= 0.
I
G
= gate drive current (1A for the MIC2198)
The total high-side MOSFET switching loss is:
P
AC
= (V
IN
+ V
D
) × I
PK
× t
T
×f
S
where:
t
T
= switching transition time (typically 20ns to 50ns).
V
D
= freewheeling diode drop, typically 0.5V.
f
S
it the switching frequency, nominally 500kHz
The low-side MOSFET switching losses are negligible and
can be ignored for these calculations.
RMS Current and MOSFET Power Dissipation
Calculation
Under normal operation, the high-side MOSFETs RMS cur-
rent is greatest when V
IN
is low (maximum duty cycle). The
low-side MOSFETs RMS current is greatest when V
IN
is high
(minimum duty cycle). However, the maximum stress the
MOSFETs see occurs during short circuit conditions, where
the output current is equal to I
OVERCURRENT(max)
. (See the
“Sense Resistor” section). The calculations below are for
normal operation. To calculate the stress under short circuit
conditions, substitute I
OVERCURRENT(max)
for I
OUT(max)
. Use
the formula below to calculate D under short circuit condi-
tions.
D 0.063 1.8 10 V
SHORTCIRCUIT
3
IN
= × ×
The RMS value of the high-side switch current is:
I D I
I
12
SW(high side)(rms) OUT(max)
2
PP
2
= × +
I 1 D I
I
12
SW(low side)(rms) OUT(max)
2
PP
2
=
( )
+
where:
D = duty cycle of the converter
D
V
V
OUT
IN
=
×η
η = efficiency of the converter.
Converter efficiency depends on component parameters,
which have not yet been selected. For design purposes, an
efficiency of 90% can be used for V
IN
less than 10V and 85%
can be used for V
IN
greater than 10V. The efficiency can be
more accurately calculated once the design is complete. If the
assumed efficiency is grossly inaccurate, a second iteration
through the design procedure can be made.
October 2005 11 MIC2198
MIC2198 Micrel, Inc.
For the high-side switch, the maximum DC power dissipa-
tion is:
P R I
SWITCH1(dc) DS(on)1
SW1(rms)
2
= ×
For the low-side switch (N-Channel MOSFET), the DC power
dissipation is:
P R I
SWITCH2(dc) DS(on)2
SW 2(rms)
2
= ×
Since the AC switching losses for the low-side MOSFET is
near zero, the total power dissipation is:
P P
low-side MOSFET(max) SWITCH2(dc)
=
The total power dissipation for the high-side MOSFET is:
P P P
high sideMOSFET(max) SWITCH 1(dc) AC
= +
External Schottky Diode
An external freewheeling diode is used to keep the inductor
current flow continuous while both MOSFETs are turned off.
This dead time prevents current from flowing unimpeded
through both MOSFETs and is typically 80ns The diode
conducts twice during each switching cycle. Although the
average current through this diode is small, the diode must
be able to handle the peak current.
I I 2 80ns f
D(avg) OUT S
= × × ×
The reverse voltage requirement of the diode is:
V V
DIODE(rrm)
IN
=
The power dissipated by the Schottky diode is:
P I V
DIODE D(avg) F
= ×
where:
V
F
= forward voltage at the peak diode current
The external Schottky diode, D2, is not necessary for circuit
operation since the low-side MOSFET contains a parasitic
body diode. The external diode will improve efficiency and
decrease high frequency noise. If the MOSFET body diode
is used, it must be rated to handle the peak and average cur-
rent. The body diode has a relatively slow reverse recovery
time and a relatively high forward voltage drop. The power
lost in the diode is proportional to the forward voltage drop
of the diode. As the high-side MOSFET starts to turn on, the
body diode becomes a short circuit for the reverse recovery
period, dissipating additional power. The diode recovery and
the circuit inductance will cause ringing during the high-side
MOSFET turn-on.
An external Schottky diode conducts at a lower forward voltage
preventing the body diode in the MOSFET from turning on.
The lower forward voltage drop dissipates less power than
the body diode. The lack of a reverse recovery mechanism
in a Schottky diode causes less ringing and less power loss.
Depending on the circuit components and operating condi-
tions, an external Schottky diode will give a 1/2% to 1%
improvement in efficiency.
Output Capacitor Selection
The output capacitor values are usually determined by the
capacitors ESR (equivalent series resistance). Voltage rating
and RMS current capability are two other important factors in
selecting the output capacitor. Recommended capacitors are
tantalum, low-ESR aluminum electrolytics, and OS-CON.
The output capacitor’s ESR is usually the main cause of output
ripple. The maximum value of ESR is calculated by:
R
V
I
ESR
OUT
PP
where:
V
OUT
= peak-to-peak output voltage ripple
I
PP
= peak-to-peak inductor ripple current
The total output ripple is a combination of the ESR and the
output capacitance. The total ripple is calculated below:
∆V
I (1 D
)
C f
I R
OUT
PP
OUT S
2
PP ESR
2
=
×
×
+ ×
( )
where:
D = duty cycle
C
OUT
= output capacitance value
f
S
= switching frequency
The voltage rating of capacitor should be twice the output
voltage for a tantalum and 20% greater for an aluminum
electrolytic or OS-CON.
The output capacitor RMS current is calculated below:
I
I
12
C
PP
OUT(rms)
=
The power dissipated in the output capacitor is:
P
DISS(C
OUT
)
= I
C
OUT(rms)
2
× R
ESR(C
OUT
)
Input Capacitor Selection
The input capacitor should be selected for ripple current rating
and voltage rating. Tantalum input capacitors may fail when
subjected to high inrush currents, caused by turning the input
supply on. Tantalum input capacitor voltage rating should
be at least 2 times the maximum input voltage to maximize
reliability. Aluminum electrolytic, OS-CON, and multilayer
polymer film capacitors can handle the higher inrush currents
without voltage derating.
The input voltage ripple will primarily depend on the input
capacitors ESR. The peak input current is equal to the peak
inductor current, so:
∆V I R
IN INDUCTOR(peak) ESR(C )
IN
= ×
The input capacitor must be rated for the input current ripple.
The RMS value of input capacitor current is determined at
the maximum output current. Assuming the peak-to-peak
inductor ripple current is low:
I I D (1 D)
C (rms) OUT(max)
IN
× ×
MIC2198 Micrel, Inc.
MIC2198 12 October 2005
The power dissipated in the input capacitor is:
P I R
DISS(C )
C (rms)
ESR(C )
IN
IN
2
IN
= ×
Voltage Setting Components
The MIC2198 requires two resistors to set the output voltage
as shown in Figure 6.
Error
3
MIC2198
FB
V
REF
0.8V
R2
R1
Amp
Figure 6. Voltage-Divider Configuration
The output voltage is determined by the equation:
V V 1
R1
R2
O REF
= × +
Where: V
REF
for the MIC2198 is typically 0.8V.
A typical value of R1 can be between 3k and 10k. If R1 is
too large it may allow noise to be introduced into the voltage
feedback loop. If R1 is too small in value it will decrease
the efficiency of the power supply, especially at low output
loads.
Once R1 is selected, R2 can be calculated using:
R2
V R
1
V V
REF
O REF
=
×
Voltage Divider Power Dissipation
The reference voltage and R2 set the current through the
voltage divider.
I
V
R2
DIVIDER
REF
=
The power dissipated by the divider resistors is:
P (R1 R2) I
DIVIDER DIVIDER
2
= + ×
Efficiency Calculation and Considerations
Efficiency is the ratio of output power to input power. The
difference is dissipated as heat in the buck converter. Under
light output load, the significant contributors are:
Supply current to the MIC2198
MOSFET gate-charge power (included in the IC
supply current)
Core losses in the output inductor
To maximize efficiency at light loads:
Use a low gate-charge MOSFET or use the small-
est MOSFET, which is still adequate for maximum
output current.
Use a ferrite material for the inductor core, which
has less core loss than an MPP or iron power
core.
Under heavy output loads the significant contributors to power
loss are (in approximate order of magnitude):
Resistive on-time losses in the MOSFETs
Switching transition losses in the MOSFETs
Inductor resistive losses
Current-sense resistor losses
Input capacitor resistive losses (due to the capaci-
tors ESR)
To minimize power loss under heavy loads:
Use logic-level, low on-resistance MOSFETs.
Multiplying the gate charge by the on-resistance
gives a figure of merit, providing a good balance
between low and high load efficiency.
Slow transition times and oscillations on the voltage
and current waveforms dissipate more power during
turn-on and turnoff of the MOSFETs. A clean layout
will minimize parasitic inductance and capacitance
in the gate drive and high current paths. This will
allow the fastest transition times and waveforms
without oscillations. Low gate-charge MOSFETs
will transition faster than those with higher gate-
charge requirements.
For the same size inductor, a lower value will
have fewer turns and therefore, lower winding re-
sistance. However, using too small of a value will
require more output capacitors to filter the output
ripple, which will force a smaller bandwidth, slower
transient response and possible instability under
certain conditions.
Lowering the current-sense resistor value will
decrease the power dissipated in the resistor.
However, it will also increase the overcurrent
limit and will require larger MOSFETs and inductor
components.
Use low-ESR input capacitors to minimize the
power dissipated in the capacitors ESR.
Decoupling Capacitor Selection
The 4.7µF decoupling capacitor is used to minimize noise on
the V
DD
pin. The placement of this capacitor is critical to the
proper operation of the IC. It must be placed right next to the
pins and routed with a wide trace. The capacitor should be a
good quality tantalum. An additional 1µF ceramic capacitor
may be necessary when driving large MOSFETs with high
gate capacitance. Incorrect placement of the V
DD
decoupling
capacitor will cause jitter or oscillations in the switching wave-
form and large variations in the overcurrent limit.
A 0.1µF ceramic capacitor is required to decouple the V
IN
.
The capacitor should be placed near the IC and connected
directly to between pin 6 (V
IN
) and pin 9 (GND).

MIC2198YML-TR

Mfr. #:
Manufacturer:
Microchip Technology / Micrel
Description:
Switching Controllers 500KHz Sync Buck Controller
Lifecycle:
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