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AN-7502 Datasheet, PDF (6/9 Pages) Fairchild Semiconductor – Power MOSFET Switching Waveforms
Application Note 7502
For peak gate voltages other than 10 volts, and load resis-
tances other than BVDSS/ID(MAX), the equations of Table 1
may be used in conjunction with slope estimates from the
characterization curves for CX and CGS + CX(1 + gM/gMJ) at
the appropriate drain-current level.
Characterization-Curve Limits
The switching-time range over which the characterization can be
applied is very impressive. For gate currents of the order of
microamperes, device dissipation is the limiting factor. For gate
currents of the order of amperes, the device response will be
slowed by gate propagation delay. This delay, of course,
degrades the linear switching relationship to gate current. How-
ever, as Figure 12 graphically shows, the characterization is valid
across five decades of gate current and switching time, allowing
all but a very few switching applications to be described by the
characterization curves of Figure 9.
104
RFM15N15
tD(OFF)
tR
103
tF
tD(ON)
102
101
100
10-1
10-2
100
101
102
103
104
105
106
GATE CURRENT (IG) - MICROAMPERES
FIGURE 12. FIVE DECADES OF LINEAR RESPONSE
Conclusions
The viability of the proposed characterization curves using con-
stant current has been demonstrated and the limits of applica-
tion defined. The existence of a vertical JFET in a power
MOSFET makes data-sheet capacitances of little use for esti-
mating switching times. The classical method of defining
switching time by 10% and 90% is a poor representation for
power MOSFETs because of the dual-slope nature of the drain
waveforms. Switching influences are masked because the 10%
level is controlled by one mechanism and the 90% level by
another. Device comparisons based on the classical switching
definition can be very misleading.
Appendix A - Analysis for Resistive Step
Voltage Inputs
Step Voltage Gate Drive
To obtain the necessary relationships, six device switching
states must be examined using the same device equivalent
circuit as was used for the constant-gate-current case, but
with the forcing function replaced wIth a step voltage with
internal resistance RO, Figure A-1.
GATE
RO VGS
CX VX gMJ VX VD
DRAIN
VG
CGS
gM VG
RL
CDS
SOURCE
LEGEND
VGS
VX
VD
CGS
- Gate Voltage
CDS
- JFET Driving Voltage gM
- Drain Voltage
gMJ
- Gate Source
RL
Capacitance
CX - MOSFET Feedback IG
Capacitance
- Drain Source Capacitance
- MOSFETTransconductance
- JFET Transconductance
- Drain Load Resistance
- Constant Current Amplitude
FIGURE A-1. POWER MOSFET EQUIVALENT CIRCUIT
State 1: Mos Off, JFET Off
As before, both current generators are open circuits, reducing
the equivalent circuit to simply charging CISS through RO.
t = ROCISSIn(1/(1 - VGS(TH)/VG)]
State 2: Mos Active, JFET Active
Before proceeding, it is wise to examine an actual device
response and make use of available simplifications. Figure A-2
shows iG(t) and iD(t) for a typical power MOSFET driven by a
step gate voltage. For truly resistive switching, realize that these
waveforms are only mirror images of their voltage counterparts
vG(t) and vD(t). Using Figure A-2, applicable gate currents for
each of the device states may be listed.
IPK1
IPK2
IPK3
iG(t)
iD(t)
TIME
IPK4
IPK6
IPK5
FIGURE A-2. iG(t) AND iD(t) FOR A TYPICAL POWER MOSFET
DRIVEN BY A STEP GATE VOLTAGE
©2002 Fairchild Semiconductor Corporation
Application Note 7502 Rev. A1