參數(shù)資料
型號: MMDF2C02ER2
廠商: ON SEMICONDUCTOR
元件分類: JFETs
英文描述: 3.6 A, 25 V, 0.1 ohm, 2 CHANNEL, N AND P-CHANNEL, Si, POWER, MOSFET
封裝: MINIATURE, CASE 751-07, SO-8
文件頁數(shù): 7/10頁
文件大?。?/td> 231K
代理商: MMDF2C02ER2
MMDF2C02E
http://onsemi.com
6
TYPICAL ELECTRICAL CHARACTERISTICS
NChannel
PChannel
Figure 6. DraintoSource Leakage Current
versus Voltage
Figure 6. DraintoSource Leakage Current
versus Voltage
1
VDS, DRAINTOSOURCE VOLTAGE (VOLTS)
I DSS
,LEAKAGE
(nA)
100
10
04
8
12
16
VGS = 0 V
TJ = 125°C
100
°C
I DSS
,LEAKAGE
(nA)
1
100
VDS, DRAINTOSOURCE VOLTAGE (VOLTS)
10
510
15
20
VGS = 0 V
TJ = 125°C
100
°C
1000
10000
25
°C
25
POWER MOSFET SWITCHING
Switching behavior is most easily modeled and predicted
by recognizing that the power MOSFET is charge
controlled. The lengths of various switching intervals (Δt)
are determined by how fast the FET input capacitance can
be charged by current from the generator.
The published capacitance data is difficult to use for
calculating rise and fall because draingate capacitance
varies greatly with applied voltage. Accordingly, gate
charge data is used. In most cases, a satisfactory estimate of
average input current (IG(AV)) can be made from a
rudimentary analysis of the drive circuit so that
t = Q/IG(AV)
During the rise and fall time interval when switching a
resistive load, VGS remains virtually constant at a level
known as the plateau voltage, VSGP. Therefore, rise and fall
times may be approximated by the following:
tr = Q2 x RG/(VGG VGSP)
tf = Q2 x RG/VGSP
where
VGG = the gate drive voltage, which varies from zero to VGG
RG = the gate drive resistance
and Q2 and VGSP are read from the gate charge curve.
During the turnon and turnoff delay times, gate current is
not constant. The simplest calculation uses appropriate
values from the capacitance curves in a standard equation for
voltage change in an RC network. The equations are:
td(on) = RG Ciss In [VGG/(VGG VGSP)]
td(off) = RG Ciss In (VGG/VGSP)
The capacitance (Ciss) is read from the capacitance curve at
a voltage corresponding to the offstate condition when
calculating td(on) and is read at a voltage corresponding to the
onstate when calculating td(off).
At high switching speeds, parasitic circuit elements
complicate the analysis. The inductance of the MOSFET
source lead, inside the package and in the circuit wiring
which is common to both the drain and gate current paths,
produces a voltage at the source which reduces the gate drive
current. The voltage is determined by Ldi/dt, but since di/dt
is a function of drain current, the mathematical solution is
complex. The MOSFET output capacitance also
complicates the mathematics. And finally, MOSFETs have
finite internal gate resistance which effectively adds to the
resistance of the driving source, but the internal resistance
is difficult to measure and, consequently, is not specified.
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