Micrel, Inc. MIC2593
September 2008
22
M9999-092208
MOSFET Voltage Requirements
The first voltage requirement for each MOSFET is easily
stated: the drain-source breakdown voltage of the
MOSFET must be greater than V
IN(MAX)
for the slot in
question. For instance, the 5V input may reasonably be
expected to see high-frequency transients as high as
6.5V. Therefore, the drain-source breakdown voltage of
the MOSFET must be at least 7V.
The second breakdown voltage criteria which must be
met is a bit subtler than simple drain-source breakdown
voltage, but is not hard to meet. Low-voltage MOSFETs
generally have low breakdown voltage ratings from gate
to source as well. In MIC2593 applications, the gates of
the external MOSFETs are driven from the +12V input to
the MIC2593 controller. That supply may well be at 12V +
(5% x 12V) = 12.6V. At the same time, if the output of the
MOSFET (its source) is suddenly shorted to ground, the
gate-source voltage will go to (12.6V – 0V) = 12.6V. This
means that the external MOSFETs must be chosen to
have a gate-source breakdown voltage in excess of 13V;
after 12V absolute maximum, the next commonly
available voltage class has a 20V maximum gate-source
voltage. At the present time, most power MOSFETs with a
20V gate-source voltage rating have a 30V drain-source
breakdown rating or higher. As a general tip, look to
surface mount devices with a drain-source rating of 30V
as a starting point.
MOSFET Steady-State Thermal Issues
The selection of a MOSFET to meet the maximum
continuous current is a fairly straightforward exercise.
First, arm yourself with the following data:
The value of I
LOAD(CONT, MAX)
for the output in
question (see Sense Resistor Selection).
The manufacturer’s data sheet for the candidate
MOSFET.
The maximum ambient temperature in which the
device will be required to operate.
Any knowledge you can get about the heat
sinking available to the device (e.g., Can heat be
dissipated into the ground plane or power plane,
if using a surface mount part? Is any airflow
available?).
The data sheet will almost always give a value of on
resistance given for the MOSFET at a gate-source
voltage of 4.5V, and another value at a gate-source
voltage of 10V. As a first approximation, add the two
values together and divide by two to get the on-resistance
of the part with 7V to 8V of enhancement (11.5V nominal
V
GATE
minus the 3.5V to 4.5V gate threshold of the
MOSFET). Call this value R
ON
. Since a heavily enhanced
MOSFET acts as an ohmic (resistive) device, almost all
that’s required to determine steady-state power
dissipation is to calculate I
2
R. The one addendum to this
is that MOSFETs have a slight increase in R
ON
with
increasing die temperature. A good approximation for this
value is 0.5% increase in R
ON
per °C rise in junction
temperature above the point at which R
ON
was initially
specified by the manufacturer. For instance, if the
selected MOSFET has a calculated R
ON
of 10m at T
J
=
25°C and the actual junction temperature ends up at
110°C, a good first cut at the operating value for R
ON
would be:
[
]
14.3m25)(0.05)(110110mR
ON
+
Next, approximate the steady-state power dissipation
(I
2
R) using I
LOAD(CONT,max)
and the approximated R
ON
.
[
]
1.14W14.3m(8.93A)RIR
2
ON
2
MAX)LOAD(CONT,ON
××
The final step is to make sure that the heat sinking
available to the MOSFET is capable of dissipating at least
as much power (rated in °C/W) as that with which the
MOSFET’s performance was specified by the
manufacturer. Here are a few practical tips:
1. The heat from a surface-mount device such as an
SO-8 MOSFET flows almost entirely out of the
drain leads. If the drain leads can be soldered
down to one square inch or more, the copper
trace will act as the heat sink for the part. This
copper trace must be on the same layer of the
board as the MOSFET drain.
2. Airflow works. Even a few LFM (linear feet per
minute) of air will cool a MOSFET down
substantially. If you can, position the MOSFET(s)
near the inlet of a power supply’s fan, or the outlet
of a processor’s cooling fan.
3. The best test of a surface-mount MOSFET for an
application (assuming the above tips show it to be
a likely fit) is an empirical one. Check the
MOSFET's temperature in the actual layout of the
expected final circuit, at full operating current. The
use of a thermocouple on the drain leads, or
infrared pyrometer on the package, will then give
a reasonable idea of the device’s junction
temperature.
MOSFET Transient Thermal Issues
Having chosen a MOSFET that will, a) withstand both the
applied voltage stresses, and b) handle the worst-case
continuous I
2
R power dissipation that it will endure;
verifying the MOSFET’s ability to handle short-term
overload power dissipation without overheating is the lone
item to be determined. A MOSFET can handle a much
higher pulsed power without damage than its continuous
dissipation ratings would imply. The reason for this is that
thermal devices (silicon die, lead frames, etc.) have
thermal inertia.
In terms related directly to the specification and use of
power MOSFETs, this is known as “transient thermal
impedance. ”Almost all power MOSFET data sheets give
a Transient Thermal Impedance Curve. For example, take
the case where t
FLT
for the 5V supply has been set to
Micrel, Inc. MIC2593
September 2008
23
M9999-092208
50ms, I
LOAD(CONT, MAX)
is 5.0A, the slow-trip threshold is
50Mv nominal, and the fast-trip threshold is 100mV. If the
output is connected to a 0.60 load, the output current
from the MOSFET for the slot in question will be regulated
to 5.0A for 50ms before the MIC2593 circuit breaker trips.
During that time, the dissipation in the MOSFET is given
by:
[]
2V5A(0.6A5VE IEP
MOSFET
==×=
()
50ms for 10W5A2VP
MOSFET
=×=
At first glance, it would appear that a really hefty MOSFET
is required to withstand this sort of fault condition. This is
where the transient thermal impedance curves become
very useful. Figure 13 shows the curve for the Vishay
(Siliconix) Si4430DY, a commonly used SO-8 power
MOSFET.
Taking the simplest case first, we’ll assume that once a
fault event such as the one in question occurs, it will be a
long time, several seconds, before the fault is isolated and
the channel is reset. In such a case, we can approximate
this as a “single pulse” event, that is to say, there’s no
significant duty cycle. Then, reading up from the X-axis at
the point where “Square Wave Pulse Duration” is equal to
0.1sec (=100msec), we see that the Z
(JA)
of this MOSFET
to a highly infrequent event of this duration is only 7% of
its continuous R
(JA)
.
This particular part is specified as having an R
(JA)
of
35°C/W for intervals of 10 seconds or less. Thus:
Assume T
A
= 55°C maximum, 1 square inch of copper at
the drain leads, no airflow.
Recalling from our previous approximation hint, the part
has an R
ON
of (0.014/2) = 7m at 25°C.
Assume it has been carrying just about 5A for some time.
When performing this calculation, be sure to use the
highest anticipated ambient temperature (T
A(MAX)
) in which
the MOSFET will be operating as the starting
temperature, and find the operating junction temperature
increase (T
J
) from that point. Then, as shown next, the
final junction temperature is found by adding T
A(MAX)
and
T
J
. Since this is not a closed-form equation, getting a
close approximation may take one or two iterations, but
it’s not a hard calculation to perform and tends to
converge quickly.
Then the starting (steady-state) T
J
is:
JA(MAX)J
TTT
+
[
]
)C)(R)(0.005T(TRT
ONAA(MAX)ONA(MAX)
°
+
+
(JA)
2
RI ××
[
]
7m
m
C)(0.005)(25C(557mC55T
J
°°
+
+
°
C/W)(35(5A)
2
°××
C)(35(0.20125W)C55T
J
°
+
°
C62.0°
Iterate the calculation once to see if this value is within a
few percent of the expected final value. For this iteration
we will start with T
J
equal to the already calculated value
of 62.0°C:
[
]
7m
m
C)(0.005)(25C(62.07mTT
AJ
°°
+
+
C/W)(35(5A)
2
°××
C62.35C)(35(0.20125W)C55T
J
°°
+
°
So our original approximation of 62.0°C was very close to
the correct value. We will use T
J
= 62°C.
Finally, add (10W)(35°C/W)(0.07) = 24.5°C to the steady-
state T
J
to get T
J(TRANSIENT MAX.)
= 86.5°C. This is an
acceptable maximum junction temperature for this part.
10
-4
10
-3
10
-2
10
-1
1 10 100 600
2
1
0.1
0.01
0.2
0.1
0.05
0.02
Single Pulse
Duty Cycle = 0.5
Normalized Thermal Transient Imperance, Juction-to-Ambient
1. Duty Cycle, D =
2. Per Unit Base = R
qJA
= 67°C/W
3. T
JM
– T
A
= P
DM
Z
qJA
(t)
4. Surface Mounted
t
1
t
2
t
1
t
2
Notes:
P
DM
Square Wave Pulse Duration (sec)
Normalized Effective Transient
Thermal Impedance
Figure 13. Si4430DY MOSFET Transient Thermal Impedance Curve
Micrel, Inc. MIC2593
September 2008
24
M9999-092208
MOSFET and Sense Resistor Selection Guide
Listed in Table 5 below, by Manufacturer and Type
Number, are some of the more popular MOSFET and
resistor types used in PCI hot plug applications.
Although far from comprehensive, this information will
constitute a good starting point for most designs.
Power Supply Decoupling
In general, prudent system design requires that power
supplies used for logic functions should have less than
100mV of noise at frequencies of 100kHz and above. In
particular, the –12V supply should have less than 100mV
of peak-to-peak noise at frequencies of 1MHz or higher.
This is because the –12V supply is the most negative
potential applied to the IC, and is therefore connected to
the device's substrate. All of the subcircuits integrated
onto the silicon chip are hence subjected by capacitive
coupling to any HF noise on the –12V supply. While
individual capacitances are quite low, the amount of
injected energy required to cause a "glitch" can also be
quite low at the internal nodes of high speed logic circuits.
Less obviously, but equally important, is the fact that the
internal charge pump for the 3.3V
AUX
supplies is
somewhat susceptible to noise on the +12V input when
that input is at or near zero volts. The +12V supply should
not carry HF noise in excess of 200mV peak-to-peak with
respect to chip ground when it is in the "off" state.
If either the –12V input, the +12V input, of both supplies
do carry significant HF noise (as can happen when they
are locally derived by a switching converter), the solution
is both small and inexpensive. An LC filter made of a
ferrite bead between the noisy power supply input and the
MIC2593, followed by a "composite capacitor" from the
affected MIC2593 input pin to ground, will suffice for
almost any situation. A good composite capacitor for this
purpose is the parallel combination of a 47µF tantalum
bulk decoupling capacitor, and one 1µF and one 0.01µF
ceramic capacitor for high-frequency bypass. A suggested
ferrite bead for such use is Fair-Rite Products Corporation
part number 2743019447 (this is a surface-mountable
part). Similar parts from other vendors or a 0.27µH air-
core coil can also be used.
Noisy V
IN
To MIC2593
SMT Ferrite Bead
Fair-Rite Products
Type 2743019447
47µF
Tanalum
1µF
Ceramic
10nF
Ceramic
Figure 14. Filter Circuit for Noisy Supplies
(+3.3V and/or –12V)
It is theoretically possible that high-amplitude, HF noise
reflected back into one or both of the MIC2593’s –12V
outputs could interfere with proper device operation,
although such noisy loads are unlikely to occur in the real
world. If this becomes an application-specific concern, a
pair of filters similar to that in Figure 14 will provide the
required HF bypassing. The capacitors would be
connected to the MIC2593’s –12V output pins, and the
ferrite beads would be placed between the –12V output
pins and the loads.
MOSFET Vendors Key MOSFET Type(s) Web Address
Vishay (Siliconix) Si4430DY (“LittleFoot
®
” Series)
Si4420DY (“LittleFoot
®
” Series)
www.siliconix.com
International Rectifier IRF7413A (SO-8 package part)
Si4420DY (second source to Vishay)
www.irf.com
Fairchild Semiconductor FDS6644 (SO-8 package part)
FDS6670A (SO-8 package part)
FDS6688 (SO-8 package part)
www.fairchildsemi.com
Resistor Vendors Sense Resistors Web Address
Vishay (Dale) WSL Series
WSL 3637 Series
www.vishay.com/docs/wsl_30100.pdf
IRC OARS Series
LR Series
(second source to WSL)
irctt.com/pdf_files/OARS.pdf
irctt.com/pdf_files/LRC.pdf

MIC2593-2BTQ

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IC CTRLR HOTPLUG PCI DUAL 48TQFP
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