MIC2588-2YM Micrel Inc, MIC2588-2YM Datasheet - Page 16
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MIC2588-2YM
Manufacturer Part Number
MIC2588-2YM
Description
Negative Voltage Hot-swap Controller -
Manufacturer
Micrel Inc
Type
Hot-Swap Controllerr
Datasheet
1.MIC2588-1YM_TR.pdf
(21 pages)
Specifications of MIC2588-2YM
Applications
General Purpose
Internal Switch(s)
No
Current Limit
Adjustable
Voltage - Supply
-19 V ~ -80 V
Operating Temperature
-40°C ~ 85°C
Mounting Type
Surface Mount
Package / Case
8-SOIC (0.154", 3.90mm Width)
Family Name
MIC2588
Package Type
SOIC
Operating Supply Voltage (min)
-19V
Operating Supply Voltage (max)
-80V
Operating Temperature (min)
-40C
Operating Temperature (max)
85C
Operating Temperature Classification
Industrial
Product Depth (mm)
3.94mm
Product Height (mm)
1.48mm
Product Length (mm)
4.93mm
Mounting
Surface Mount
Pin Count
8
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Available stocks
Company
Part Number
Manufacturer
Quantity
Price
Company:
Part Number:
MIC2588-2YM
Manufacturer:
MICREL
Quantity:
61
Part Number:
MIC2588-2YM
Manufacturer:
MICREL
Quantity:
20 000
the drain-source breakdown voltage of the MOSFET must
be greater than V
The second breakdown voltage criterion that must be met
is the gate-source voltage. For the MIC2588/MIC2594, the
gate of the external MOSFET is driven up to a maximum of
11V above VEE. This means that the external MOSFET must
be chosen to have a gate-source breakdown voltage of 12V
or more; 20V is recommended. Most power MOSFETs with
a 20V gate-source voltage rating have a 30V drain-source
breakdown rating or higher. For many 48V telecom applica-
tions, transient voltage spikes can approach, and sometimes
exceed, 100V. The absolute maximum input voltage rating
of the MIC2588/MIC2594 is 100V; therefore, a drain-source
breakdown voltage of 100V is suggested for the external
MOSFET. Additionally, an external input voltage clamp is
strongly recommended for applications that do not utilize
conditioned power supplies.
Power 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 datasheet will almost always give a value of on resistance
for a given MOSFET at a gate-source voltage of 4.5V and
10V. For MIC2588/MIC2594 applications, choose the gate-
source ON resistance at 10V and call this value R
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
this is that MOSFETs have a slight increase in R
creasing die temperature. A good approximation for this value
is 0.5% increase in R
above the point at which R
manufacturer. For instance, if the selected MOSFET has a
calculated R
tion temperature ends up at 110°C, a good first cut at the
operating value for R
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:
September 2005
MIC2588/MIC2594
R
ON
•The value of I
(see Sense Resistor Selection).
•The manufacturer’s datasheet for the candidate MOS-
FET.
•The maximum ambient temperature in which the device
will be required to operate.
•Any knowledge you can get about the heat sinking avail-
able 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?).
1. The heat from a TO-263 power MOSFET flows
almost entirely out of the drain tab. If the drain tab
can be soldered down to one square inch or more,
the copper will act as the heat sink for the part. This
copper must be on the same layer of the board as
≈ 10mΩ[1 + (110 – 25)(0.005)] ≈14.3mΩ
ON
of 10mΩ at aT
IN(MAX)
LOAD(CONT, MAX.)
ON
ON
would be:
, or V
per °C rise in junction temperature
ON
DD
J
was initially specified by the
= 25°C, and the actual junc-
2
– V
R. The one addendum to
for the output in question
EE
(min).
ON
ON
with in-
. Since
16
Power MOSFET Transient Thermal Issues
If the prospecitve MOSFET has been shown to withstand the
environmental voltage stresses and the worse-case steady-
state power dissipation is addressed, the remaining task is to
verify if the MOSFET is capable of handling extreme overcur-
rent load faults, such as a short circuit, without overheating.
A power MOSFET can handle a much higher pulsed power
without damage than its continuos power dissipation ratings
imply due to an inherent trait, thermal inertia. With respect to
the specification and use of power MOSFETs, the parameter
of interest is the “Transient Thermal Impedence”, or Z
is a real number (variable factor) used as a multiplier of the
thermal resistance (R
the given “Transient Thermal Imepedence Graph”, normalized
to R
power pulse duration and duty cycle. The single-pulse curve
is appropriate for most hot swap applications. Z
from junction-to-case for power MOSFETs typically used in
telecom applications.
The following example provides a method for estimating the
peak junction temperature of a power MOSFET in determin-
ing if the MOSFET is suitable for a particular application.
V
is SUM110N10-09 (TO-263 package) from Vishay-Siliconix.
This MOSFET has an R
tion-to-case thermal resistance (R
tion-to-ambient thermal resistance (R
the Transient Thermal Impedence Curve is shown in Figure
7. Consider, say, the MOSFET is switched on at time t1 and
the steady-state load current passing through the MOSFET
is 3A. At some point in time after t1, at time t2, there is an
unexpected short-circuit applied to the load, causing the
MIC2588/MIC2594 controller to adjust the GATE output
voltage and regulate the load current for 400µs at the pro-
grammed current limit value, 4.2A in this example. During this
short-circuit load condition, the dissipation in the MOSFET
is calculated by:
At first glance, it would appear that a very hefty MOSFET is
required to withstand this extreme overload condition. Upon
further examination, the calculation to approximate the peak
junction temperature is not a difficult task. The first step is to
determine the maximum steady-state junction temperature,
IN
P
P
D
D
(VDD – VEE) = 48V, I
2. Airflow works. Even a few LFM (linear feet per-
3. The best test of a candidate MOSFET for an ap-
θ
(short) = V
(short) = 48V × 4.2A = 201.6W for 400µs.
, that displays curves for the thermal impedence versus
the MOSFET drain.
minute) of air will cool a MOSFET down substan-
tially. 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.
plication (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 pyrom-
eter on the package, will then give a reasonable
idea of the device’s junction temperature.
DS
× I
LIM
θ
). The multiplier is determined using
ON
LIM
of 9.5mΩ (T
= 4.2A, and the power MOSFET
V
DS
θ(J-C)
= 0V – (-48V) = 48V
θ(J-A)
J
) is 0.4°C/W, junc-
= 25°C), the junc-
) is 40°C/W, and
θ
M9999-083005
is specified
θ
, which
Micrel