H-BRIDGE MOSFET POWER MODULE

M.S. KENNEDY CORP.
H-BRIDGE
MOSFET POWER MODULE
3020
4707 Dey Road Liverpool, N.Y. 13088
(315) 701-6751
FEATURES:
•
•
•
•
•
•
Pin Compatible with MPM3002 and MPM3012
P and N Channel MOSFETs for Ease of Drive
N Channel Current Sensing MOSFET for Lossless Sensing
Isolated Package for Direct Heat Sinking, Excellent Thermal Conductivity
Avalanche Rated Devices
100 Volt, 10 Amp Full H-Bridge
DESCRIPTION:
The MSK 3020 is an H-bridge power circuit packaged in a space efficient isolated ceramic tab power SIP package.
The MSK 3020 consists of P-Channel MOSFETs for the top transistors and N-Channel MOSFETs for the bottom
transistors. The N Channel MOSFETS are current sensing to allow lossless current sensing for current controlled
applications. The MSK 3020 uses M.S. Kennedy's proven power hybrid technology to bring a cost effective high
performance circuit for use in today's sophisticated servo motor and disk drive systems. The MSK 3020 is pin
compatible with the MPM3002 and MPM3012 with some differences in specifications.
EQUIVALENT SCHEMATIC
PIN-OUT INFORMATION
TYPICAL APPLICATIONS
•
•
•
•
Stepper Motor Servo Control
Disk Drive Head Control
X-Y Table Control
Az-El Antenna Control
1
2
3
4
5
6
1
Gate Q1
Source Q1
Drain 1, 2
Gate Q2
Sense Q2
Kelvin Source 2, 3
7
8
9
10
11
12
Source 2, 3
Sense Q3
Gate Q3
Drain 3, 4
Gate Q4
Source 4
Rev. C 7/10
ABSOLUTE MAXIMUM RATINGS
VDSS Drain to Source Voltage
VDGDR Drain to Gate Voltage
(RGS=1MΩ)
VGS Gate to Source Voltage
(Continuous)
Continuous Current
ID
Pulsed Current
IDM
Sense Current-Continuous
IM
Sense Current Peak
IMM
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
100V MAX
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
Single Pulse Avalanche Energy
7.9mJ
(Q1,Q4)
69mJ
(Q2,Q3)
+175°C MAX
JunctionTemperature
-55°C to +150°C
Storage Temperature
Case Operating Temperature Range -55°C to +125°C
Lead Temperature Range
200°C MAX
(10 Seconds Lead Only)
Thermal Resistance (Junction to Case)
5.2°C/W
P-Channel @ 25°C
8.0°C/W
P-Channel @ 125°C
3.3°C/W
N-Channel @ 25°C
5.1°C/W
N-Channel @ 125°C
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
±20V
10A
25A
13mA
33mA
○
○
○
○
100V MAX
○
○
MAX
MAX
MAX
MAX
MAX
TJ
TST
TC
TLD
RTH-JC
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
○
ELECTRICAL SPECIFICATIONS
Parameter
Test Conditions 4
Drain-Source Breakdown Voltage
Drain-Mirror Breakdown Voltage
Drain-Source Leakage Current
Gate-Source Leakage Current
Gate-Source Threshold Voltage
Drain-Source on Resistance
2
Drain-Source on Resistance
3
Forward Transconductance
1
N-CHANNEL (Q2, Q3)
Total Gate Charge
1
Gate-Source Charge 1
Gate-Drain Charge
1
Turn-On Delay Time 1
Rise Time
1
Turn-Off Delay Time 1
Fall Time
1
Input Capacitance
1
Output Capacitance 1
Reverse Transfer Capacitance 1
Output Capacitance of Sensing Cells 1
Current Sensing Ratio 1
P-CHANNEL (Q1, Q4)
Total Gate Charge
1
Gate-Source Charge 1
Gate-Drain Charge
1
Turn-On Delay Time 1
Rise Time
1
Turn-Off Delay Time 1
Fall Time
1
Input Capacitance
1
Output Capacitance 1
Reverse Transfer Capacitance 1
BODY DIODE
Forward on Voltage
1
Reverse Recovery Time
1
Reverse Recovery Charge
1
Min.
MSK 3020
Typ.
Max.
Units
ID = 0.25 mA (All Transistors)
VGS = 0
VGS = 0
VDS = 100V, (Q2, Q3)
VDS = 100V VGS = 0V, (Q2, Q3)
VDS = -100V VGS = 0V, (Q1, Q4)
VDS = 0V (All Transistors)
VGS = ±20V
VDS = VGS ID = 250 μA (Q2, Q3)
VDS = VGS ID = 250 μA (Q1, Q4)
VGS = 10V ID = 8.4A (Q2, Q3)
VGS = -10V ID = -8.4A (Q1, Q4)
VGS = 10V ID = 8.4A (Q2, Q3)
VGS = -10V ID = -8.4A (Q1, Q4)
VDS = 50V ID = 8.4A (Q2, Q3)
VDS = -50V ID = -8.4A (Q1, Q4)
100
100
2.0
-2.0
4.7
3.2
-
25
-25
±100
4.0
-4.0
0.26
0.31
0.16
0.20
-
V
V
μA
μA
nA
V
V
Ω
Ω
Ω
Ω
S
S
ID = 14A
VDS = 80V
VGS = 10V
VDD = 50V
ID = 14A
RG = 12Ω
RD = 3.5Ω
VGS = 0V
VDS = 25V
f = 1 MHz
VGS = 10V ID = 14A
1390
9.5
42
22
25
700
320
83
9
-
26
5.5
11
1540
nC
nC
nC
nS
nS
nS
nS
pF
pF
pF
pF
r
ID = -8.4A
VDS = -80V
VGS = -10V
VDD = -50V
ID = -8.4A
RG = 9.1Ω
RD = 6.2Ω
VGS = 0V
VDS = -25V
f = 1 MHz
-
15
58
45
46
760
260
170
58
8.3
32
-
nC
nC
nC
nS
nS
nS
nS
pF
pF
pF
IS = 14A VGS = 0V (Q2, Q3)
IS = -14A VGS = 0V (Q1, Q4)
IS = 14A di/dt = 100A/μS (Q2, Q3)
IS = -8.4A di/dt = 100A/μS (Q1, Q4)
IS = 14A di/dt = 100A/μS (Q2, Q3)
IS = -8.4A di/dt = 100A/μS (Q1, Q4)
-
2.5
-1.6
150
47
0.85
650
310
71
1.2
970
V
V
nS
nS
μC
nC
NOTES:
1 This parameter is guaranteed by design but need not be tested. Typical parameters are representative of actual device performance
but are for reference only.
2 Resistance as seen at package pins.
3 Resistance for die only; use for thermal calculations.
4 TA = 25°C unless otherwise specified.
Rev. C 7/10
2
APPLICATION NOTES
N-CHANNEL GATES (Q2, Q3):
For driving the N-Channel gates, it is important to keep in mind that it is essentially like driving a capacitance to a sufficient
voltage to get the channel fully on. Driving the gates to +15 volts with respect to their sources assures that the transistors
are on. This will keep the dissipation down to a minimum level. How quickly the gate gets turned ON and OFF will
determine the dissipation of the transistor while it is transitioning from OFF to ON and vice-versa. Turning the gate ON and
OFF too slow will cause excessive dissipation, while turning it ON and OFF too fast will cause excessive switching noise in
the system. It is important to have as low a driving impedance as practical for the size of the transistor. Many motor drive
IC's have sufficient gate drive capability for the MSK 3020. If not, paralleled CMOS standard gates will usually be
sufficient. A series resistor in the gate circuit slows it down, but also suppresses any ringing caused by stray iductances
in the MOSFET circuit. The selection of the resistor is determined by how fast the MOSFET wants to be switched. See
Figure 1 for circuit details.
FIGURE 1
P-CHANNEL GATES (Q1, Q4):
Most everything applies to driving the P-Channel gates as the N-Channel gates. The only difference is that the P-Channel
gate to source voltage needs to be negative. Most motor drive IC's are set up with an open collector or drain output for
directly interfacing with the P-Channel gates. If not, an external common emitter switching transistor configuration (see
Figure 2) will turn the P-Channel MOSFET on. All the other rules of MOSFET gate drive apply here. For high supply
voltages, additional circuitry must be used to protect the P-Channel gate from excessive voltages.
FIGURE 2
BRIDGE DRIVE CONSIDERATIONS:
It is important that the logic used to turn ON and OFF the various transistors allow sufficient "dead time" between a high
side transistor and its low side transistor to make sure that at no time are they both ON. When they are, this is called
"shoot-through" and it places a momentary short across the power supply. This overly stresses the transistors and causes
excessive noise as well. See Figure 3.
FIGURE 3
This deadtime should allow for the turn on and turn off time of the transistors, especially when slowing them down with
gate resistors. This situation will be present when switching motor direction, or when sophisticated timing schemes are
used for servo systems such as locked antiphase PWM'ing for high bandwidth operation.
3
Rev. C 7/10
APPLICATION NOTES, CONT.
USING CURRENT SENSING MOSFETS:
A MOSFET transistor is constructed of many individual MOSFET cells connected in parallel. They share the current total
very evenly. If one of these cells are brought out to a pin, that cell will pass an accurate proportional amount of the total
current. This current can be used as a low power sense of the whole current without passing that whole current through a
sensing device like a resistor. This small current multiplied by the ratio specified on the data sheet equals the whole current.
There are several methods of working with the sense function to obtain the actual current.
1. Virtual Earth Sensing
The disadvantage is amplifying a current swing of 10 amps in 100 nSec to produce a 5V output means the op amp has to
slew 50V/μSec. This is beyond the capabilities of a lot of op amps.
2. Resistor Sensing
The disadvantage is RT voltage must be above the offset voltage of the op amp and RT must be much less than RDS(ON) of
the sensing cell or temperature shifts will affect accuracy.
4
Rev. C 7/10
TYPICAL PERFORMANCE CURVES
5
Rev. C 7/10
MECHANICAL SPECIFICATIONS
TORQUE SPECIFICATION 3 TO 5 IN/LBS. TEFLON SCREWS OR WASHERS ARE RECOMMENDED.
ALL DIMENSIONS ARE ±0.010 INCHES UNLESS OTHERWISE SPECIFIED.
ORDERING INFORMATION
PART
NUMBER
SCREENING LEVEL
MSK 3020
Industrial
M.S. Kennedy Corp.
4707 Dey Road, Liverpool, New York 13088
Phone (315) 701-6751
FAX (315) 701-6752
www.mskennedy.com
The information contained herein is believed to be accurate at the time of printing. MSK reserves the right to make
changes to its products or specifications without notice, however, and assumes no liability for the use of its products.
6
Rev. C 7/10