2 Motorola Bipolar Power Transistor Device Data
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ELECTRICAL CHARACTERISTICS (TC = 25
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C unless otherwise noted)
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Collector–Emitter Breakdown Voltage(1) (IC = 100 mAdc, IB = 0) MJ1000
MJ1001
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Collector Emitter Leakage Current
(VCB = 60 Vdc, RBE = 1.0k ohm) MJ1000
(VCB = 80 Vdc, RBE = 1.0k ohm) MJ1001
(VCB = 60 Vdc, RBE = 1.0k ohm, TC = 150
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C) MJ1000
(VCB = 80 Vdc, RBE = 1.0k ohm, TC = 150
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C) MJ1001
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Emitter Cutoff Current (VBE = 5.0 Vdc, IC = 0)
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Collector Emitter Leakage Current (VCE = 30 Vdc, IB = 0) MJ1000
(VCE = 40 Vdc, IB = 0) MJ1001
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DC Current Gain(1) (IC = 3.0 Adc, VCE = 3.0 Vdc)
(IC = 4.0 Adc, VCE = 3.0 Vdc)
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Collector Emitter Saturation Voltage(1) (IC = 30 Adc, IB = 12 mAdc)
(IC = 8.0 Adc, IB = 40 mAdc)
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Base Emitter Voltage(1) (IC = 3.0 Adc, VCE = 3.0 Vdc)
Vdc
(1)Pulse Test: Pulse Width
v
300 µs, Duty Cycle
v
2.0%.
IC, COLLECTOR CURRENT (AMPS)
1.0
VCE, COLLECTOR–EMITTER VOLTAGE (VOLTS)
2.0 10
5.0
1.0
0.7
0.5
3.5
IC, COLLECTOR CURRENT (AMP)
3.0
2.5
2.0
1.5
1.0
0.5
0.3
50,000
0.01
Figure 2. DC Current Gain
IC, COLLECTOR CURRENT (AMP)
50 0.05 0.1 0.2 0.5 1.0 2.0 5.0 10
10,000
5000
2000
Figure 3. Small–Signal Current Gain
f, FREQUENCY (Hz)
30
1000
20,000
hFE, DC CURRENT GAIN
1000
500
200
TJ = 200
°
C
Figure 4. “On” Voltages
500.01 0.02 0.05 0.5 1.0 102.0 5.00.2
Figure 5. DC Safe Operating Area
3000
2000
500
0
25
°
C
TC = 25
°
C
TJ = 25
°
C
TJ = 150
°
C
hfe, SMALL–SIGNAL CURRENT GAIN
100
VBE(sat) @ IC/IB = 250 SECONDARY BREAKDOWN
LIMITATION
THERMAL LIMITATION @ TC = 25
°
C
BONDING WIRE LIMITATION
VBE @ VCE = 3.0 V
VCE(sat) @ IC/IB = 250
V, VOLTAGE (VOLTS)
300
200
100
50
VCE = 3.0 Vdc
IC = 3.0 Adc
MJ1000
0.1 7.0 20 10030 705.03.0
10
3.0
2.0
0.2
0.1
7.0
–55
°
CVCE = 3.0 V
103106
105
104
MJ1001
There we two limitations on the power handling ability of a
transistor: average junction temperature and secondary
breakdown. Safe operating area curves indicate IC – VCE lim-
its of the transistor that must be observed for reliable opera-
tion; e.g., the transistor must not be subjected to greater
dissipation than the curves indicate.
At high case temperatures, thermal limitations will reduce
the power that can be handled to values less than the limita-
tions imposed by secondary breakdown.