The BUV48/BUV48A transistors are designed for high–voltage, high–speed, power
switching in inductive circuits where fall time is critical. They are particularly suited for
line–operated switchmode applications such as:
• Switching Regulators
• Inverters
• Solenoid and Relay Drivers
• Motor Controls
• Deflection Circuits
Fast Turn–Off Times
60 ns Inductive Fall Time — 25_C (Typ)
120 ns Inductive Crossover Time — 25_C (Typ)
Operating Temperature Range –65 to +175_C
100_C Performance Specified for:
Reverse–Biased SOA with Inductive Loads
Switching Times with Inductive Loads
Saturation Voltage
Leakage Currents (125_C)
15 AMPERES
NPN SILICON
POWER TRANSISTORS
400 AND 450 VOLTS
V
(BR)CEO
850–1000 VOLTS
V
(BR)CEX
150 WATTS
CASE 340D–02
TO–218 TYPE
MAXIMUM RATINGS
Rating
Collector–Emitter Voltage
Collector–Emitter Voltage (VBE = –1.5 V)
Emitter Base Voltage
Collector Current — Continuous
ОООООООООООООООООООО
— Peak (1)
— Overload
Base Current — Continuous
ОООООООООООООООООООО
— Peak (1)
Total Power Dissipation — TC = 25_C
ОООООООООООООООООООО
— TC = 100_C
Derate above 25_C
Operating and Storage Junction Temperature Range
THERMAL CHARACTERISTICS
ОООООООООООООООООООООООООООООООО
Characteristic
Thermal Resistance, Junction to Case
Maximum Lead Temperature for Soldering Purposes:
(1) Pulse Test: Pulse Width = 300 µs, Duty Cycle v 2%.
Vcl = 300 V, V
= 5 V, Lc = 180 µH
BE(off)
2
Motorola Bipolar Power Transistor Device Data
Page 3
DC CHARACTERISTICS
, DC CURRENT GAIN
FE
h
0.7
0.5
50
30
20
10
7
5
3
2
1
5
3
2
1
VCE = 5 V
1
90%
10%
2358 10203050
IC, COLLECTOR CURRENT (AMPS)
Figure 1. DC Current Gain
βf = 5
90%
10%
, COLLECTOR–EMITTER VOL TAGE (VOLTS)
CE
V
10
0.5
0.3
0.1
0.7
0.5
5
3
1
0.1
7.5 A
IC = 5 A
TC = 25°C
0.30.5
IB, BASE CURRENT (AMPS)
10 A15 A
Figure 2. Collector Saturation Region
βf = 5
2
1
TJ = 25°C
1234
TJ = 100°C
0.3
0.2
, COLLECTOR–EMITTER VOL TAGE (VOLTS)
CE
V
0.1
IC, COLLECTOR CURRENT (AMPS)
Figure 3. Collector–Emitter Saturation V oltage
4
10
VCE = 250 V
3
µ
10
TJ = 150°C
2
10
125°C
100°C
1
10
, COLLECTOR CURRENT ( A)
0
C
10
I
–1
10
–0.4
REVERSE
°
C
75
25°C
–0.200.20.40.6
VBE, BASE–EMITTER VOLTAGE (VOLTS)
FORWARD
Figure 5. Collector Cutoff Region
, BASE–EMITTER VOLTAGE (VOLTS)
BE
V
C, CAPACITANCE (pF)
0.3
10 k
1 k
100
10
0.1
1
0.33
IC, COLLECTOR CURRENT (AMPS)
Figure 4. Base–Emitter V oltage
C
ib
C
ob
TJ = 25°C
10
VR, REVERSE VOLTAGE (VOLTS)
Figure 6. Capacitance
1011237105020305
1001000
Motorola Bipolar Power Transistor Device Data
3
Page 4
V
CEO(sus)
T able 1. Test Conditions for Dynamic Performance
RBSOA AND INDUCTIVE SWITCHINGRESISTIVE SWITCHING
+10 V
INPUT
0
CONDITIONS
PW Varied to Attain
IC = 200 mA
L
= 25 mH, VCC = 10 V
coil
R
= 0.7 Ω
coil
VALUES
CIRCUIT
SEE ABOVE FOR
DETAILED CONDITIONS
TEST CIRCUITS
20
1
INPUT
2
1
2
INDUCTIVE TEST CIRCUIT
TUT
1N4937
OR
EQUIVALENT
V
clamp
RS =
Ω
0.1
PULSES
δ
= 3%
220100
680 pF
L
R
VCC = 20 V
R
coil
L
coil
V
CC
= 180 µH
coil
coil
100
= 0.05 Ω
I
C
V
CE
I
C(pk)
D1
1N4934D1 D2 D3 D4
D3
= 300 V
t
f
t
2
22 µF
22
22
0.22
tf Clamped
t
33
2 W
160
MM3735
680 pF
680 pF
2N3763
160
33
2 W
V
clamp
RB ADJUSTED TO ATTAIN DESIRED I
t
1
VCE
or
V
clamp
TIME
+10 V
2N6438
D3
0.1
D4
2N6339
µ
F
t
MR854
Ib1 ADJUST
µ
F
Ib2 ADJUST
dTb ADJUST
dT
MR854
V
CC
B1
t1 Adjusted to
Obtain I
C
L
coil (IC
t1 ≈
V
L
coil (IC
t2 ≈
V
Clamp
Test Equipment
Scope — Tektronix
475 or Equivalent
CC
)
pk
)
pk
TURN–ON TIME
I
B1
IB1 adjusted to
obtain the forced
hFE desired
TURN–OFF TIME
Use inductive switching
driver as the input to
the resistive test circuit.
VCC = 300 V
RL = 83 Ω
Pulse Width = 10 µs
RESISTIVE TEST CIRCUITOUTPUT WAVEFORMS
TUT
1
2
1
2
R
L
V
CC
IC pk
90% V
CE(pk)
I
C
t
sv
t
rv
90% I
t
fi
V
CE(pk)
C(pk)
t
ti
10
βf = 5
8
IC = 10 A
6
t
c
V
CE
I
B
90% I
B1
TIME
10% V
CE(pk)
10%
IC pk
2% I
4
C
, BASE CURRENT (AMPS)I
2
B2(pk)
0
0
123456
V
, BASE–EMITTER VOLTAGE (VOLTS)
BE(off)
Figure 7. Inductive Switching MeasurementsFigure 8. Peak–Reverse Current
4
Motorola Bipolar Power Transistor Device Data
Page 5
SWITCHING TIMES NOTE
In resistive switching circuits, rise, fall, and storage times
have been defined and apply to both current and voltage
waveforms since they are in phase. However, for inductive
loads which are common to SWITCHMODE power supplies
and hammer drivers, current and voltage waveforms are not
in phase. Therefore, separate measurements must be made
on each waveform to determine the total switching time. For
this reason, the following new terms have been defined.
tsv= Voltage Storage Time, 90% IB1 to 10% V
trv= Voltage Rise Time, 10–90% V
tfi= Current Fall Time, 90–10% I
tti= Current Tail, 10–2% I
C
tc= Crossover Time, 10% V
clamp
clamp
C
to 10% I
clamp
C
An enlarged portion of the inductive switching waveforms is
INDUCTIVE SWITCHING
5
3
2
TC = 100°C
1
µ
0.7
0.5
t, TIME ( s)
0.3
0.2
βf = 5
0.1
1
25
37
IC, COLLECTOR CURRENT (AMPS)
TC = 25°C
201030
50
shown in Figure 7 to aid in the visual identity of these terms.
For the designer, there is minimal switching loss during
storage time and the predominant switching power losses
occur during the crossover interval and can be obtained using the standard equation from AN–222:
P
= 1/2 VCCIC(tc) f
SWT
In general, trv + tfi ] tc. However, at lower test currents this
relationship may not be valid.
As is common with most switching transistors, resistive
switching is specified at 25_C and has become a benchmark
for designers. However, for designers of high frequency converter circuits, the user oriented specifications which make
this a “SWITCHMODE” transistor are the inductive switching
speeds (tc and tsv) which are guaranteed at 100_C.
1
0.5
0.3
0.2
µ
0.1
t, TIME ( s)
0.05
0.03
0.02
0.01
1255037 201030
t
c
t
fi
β
= 5
f
IC, COLLECTOR CURRENT (AMPS)
TC = 100°C
TC = 100°C
TC = 25°C
TC = 25°C
3
2
1
0.5
0.3
µ
0.2
0.1
t, TIME ( s)
0.05
0.03
0.02
0.01
0
Figure 9. Storage Time, t
t
sv
t
c
t
fi
1245
3
βf, FORCED GAIN
sv
689710
Figure 11a. Turn–Off Times versus Forced Gain
TC = 25°C
IC = 10 A
V
= 5 V
BE(off)
Figure 10. Crossover and Fall Times
3
2
1
t
0.5
0.3
µ
0.2
0.1
t, TIME ( s)
0.05
0.03
0.02
0.01
01 2453689710
Ib2/Ib
sv
t
c
t
fi
1
Figure 11b. Turn–Off Times versus Ib2/Ib
T
= 25°C
C
IC = 10 A
βf = 5 V
1
Motorola Bipolar Power Transistor Device Data
5
Page 6
The Safe Operating Area figures shown in Figures 12 and 13 are
specified for these devices under the test conditions shown.
30
10
5
2
1
0.5
0.2
0.1
0.05
, COLLECTOR CURRENT (AMPS)
C
I
0.02
0.01
1
DC
TC = 25°C
LIMIT ONLY
FOR TURN ON
220500
550
VCE, COLLECTOR–EMITTER VOL TAGE (VOLTS)
1 ms
tr ≤ 0.7 µs
200
100010100
Figure 12. Forward Bias Safe Operating Area
50
40
30
20
10
, COLLECTOR CURRENT (AMPS)
C
I
0
0
V
BE(off)
TC = 100°C
IC/IB
VCE, COLLECTOR–EMITTER VOL TAGE (VOLTS)
BUV48BUV48A
= 5 V
≥
5
200400
600
8001000
FIgure 13. Reverse Bias Safe Operating Area
SAFE OPERATING AREA INFORMATION
FORWARD BIAS
There are two limitations on the power handling ability of a
transistor: average junction temperature and second breakdown. Safe operating area curves indicate IC – VCE limits of
the transistor that must be observed for reliable operation;
i.e., the transistor must not be subjected to greater dissipation than the curves indicate.
The data of Figure 12 is based on TC = 25_C; T
variable depending on power level. Second breakdown pulse
limits are valid for duty cycles to 10% but must be derated
when TC v 25_C. Second breakdown limitations do not derate the same as thermal limitations. Allowable current at the
voltages shown on Figure 12 may be found at any case temperature by using the appropriate curve on Figure 14.
T
may be calculated from the data in Figure 11. At high
J(pk)
case temperatures, thermal limitations will reduce the power
that can be handled to values less than the limitations imposed by second breakdown.
REVERSE BIAS
For inductive loads, high voltage and high current must be
sustained simultaneously during turn–off, in most cases, with
the base to emitter junction reverse biased. Under these
conditions the collector voltage must be held to a safe level
at or below a specific value of collector current. This can be
accomplished by several means such as active clamping,
RC snubbing, load line shaping, etc. The safe level for these
devices is specified as Reverse Bias Safe Operating Area
and represents the voltage current conditions during reverse
biased turn–off. This rating is verified under clamped conditions so that the device is never subjected to an avalanche
mode. Figure 13 gives RBSOA characteristics.
J(pk)
is
100
SECOND BREAKDOWN
DERATING
120
160200
POWER DERATING F ACT OR (%)
80
60
40
20
THERMAL DERATING
0
0
4080
TC, CASE TEMPERATURE (°C)
Figure 14. Power Derating
6
Motorola Bipolar Power Transistor Device Data
Page 7
0.5
1
D = 0.5
0.2
0.1
0.05
RESISTANCE (NORMALIZED)
0.02
r(t), EFFECTIVE TRANSIENT THERMAL
0.01
0.02
0.2
0.1
0.05
0.02
0.01
SINGLE PULSE
0.10.50.2
0.05125102050100200500
OVERLOAD CHARACTERISTICS
100
TC = 25°C
80
60
40
20
, COLLECTOR CURRENT (AMPS)
C
I
0
tp = 10 µs
VCE, COLLECTOR–EMITTER VOL TAGE (VOLTS)
Figure 16. Rated Overload Safe Operating Area
(OLSOA)
BUV48A
BUV48
300
R
(t) = r(t) R
θ
JC
θ
= 1
JC
D CURVES APPLY FOR POWER
PULSE TRAIN SHOWN
READ TIME AT t
T
J(pk)
t, TIME (ms)
°
C/W MAX
– TC = P
θ
(pk)
JC
1
R
Figure 15. Thermal Response
OLSOA applies when maximum collector current is limited
and known. A good example is a circuit where an inductor is
inserted between the transistor and the bus, which limits the
rate of rise of collector current to a known value. If the transistor is then turned off within a specified amount of time, the
magnitude of collector current is also known.
Maximum allowable collector–emitter voltage versus collector current is plotted for several pulse widths. (Pulse width
is defined as the time lag between the fault condition and the
removal of base drive.) Storage time of the transistor has
been factored into the curve. Therefore, with bus voltage and
maximum collector current known, Figure 16 defines the
500100400
450200
maximum time which can be allowed for fault detection and
shutdown of base drive.
OLSOA is measured in a common–base circuit (Figure 18)
which allows precise definition of collector–emitter voltage
and collector current. This is the same circuit that is used to
measure forward–bias safe operating area.
P
(pk)
t
1
t
(t)
θ
JC
2
DUTY CYCLE, D = t1/t
2
10002000
OLSOA
5
4
3
(AMP)
C
I
2
1
0
RBE = 2.2
RBE = 10
Ω
24
Ω
dV/dt (KV/µs)
RBE = 100
RBE = 0
6810
Figure 17. IC = f(dV/dt)
Motorola Bipolar Power Transistor Device Data
Ω
500 µF
Notes:
• VCE = VCC + V
• Adjust pulsed current source
for desired IC, t
BE
p
500 V
V
EE
V
CC
Figure 18. Overload SOA Test Circuit
7
Page 8
P ACKAGE DIMENSIONS
C
B
U
L
S
K
4
123
Q
E
A
D
J
H
NOTES:
1. DIMENSIONING AND TOLERANCING PER ANSI
Y14.5M, 1982.
Motorola reserves the right to make changes without further notice to any products herein. Motorola makes no warranty , representation or guarantee regarding
the suitability of its products for any particular purpose, nor does Motorola assume any liability arising out of the application or use of any product or circuit, and
specifically disclaims any and all liability, including without limitation consequential or incidental damages. “T ypical” parameters which may be provided in Motorola
data sheets and/or specifications can and do vary in different applications and actual performance may vary over time. All operating parameters, including “Typicals”
must be validated for each customer application by customer’s technical experts. Motorola does not convey any license under its patent rights nor the rights of
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applications intended to support or sustain life, or for any other application in which the failure of the Motorola product could create a situation where personal injury
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and its officers, employees, subsidiaries, affiliates, and distributors harmless against all claims, costs, damages, and expenses, and reasonable attorney fees
arising out of, directly or indirectly, any claim of personal injury or death associated with such unintended or unauthorized use, even if such claim alleges that
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8
◊
Motorola Bipolar Power Transistor Device Data
BUV48/D
*BUV48/D*
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