# BUV48

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## SGS-THOMSON BUX48 V48 V48FI B UX4 8A/ V 48 A/ V4 8AFI HIGH VOLTAGE POWER SWITCH

DESCRIPTION

The BUX48/A, BUV48/A, and BUV48FI/AFI are multiepitaxial mesa NPN transistors mounted res­

pectively in TO-3 metal case, TO-218 plastic package and ISOWATT218 fully isolated package.

They are particulary intended for switching applica­

tions directly from the 220V and 380V mains.

ABSO LU TE M AXIM UM RATING S

S ym bo l P a r a m e t e r

V a lu e B UX4 8 Unit B UV4 8 B U V 4 8F I

B UX4 8A B UV4 8A B U V 4 8A F I

VcER Collector-emitter Voltage (Rbe = 10 Q) 850 1000 V

Vces Collector-emitter Voltage (VBe= 0) 850 1000 V

< O o Collector-emitter Voltage (Ib= 0) 400 450 V

Vebo Emitter-base Voltage (lc = 0) 7 V

lc Collector Current 15 A

ICM Collector Peak Current (t„ < 5 ms) 30 A

Icp Collector Peak Current non Repetitive (t„ < 20 gs) 55 A

Ib Base Current 4 A

Ib m Base Peak Current 20 A

T O - 3 T O - 2 1 8 I S O W A T T 2 1 8

P tot Total Dissipation at T c < 25 °C 175 125 65 W

T stq Storage Temperature - 65 to 200 - 65 to 150 - 65 to 150 °C

Ti Max. Operating Junction Temperature 200 125 125 °C

November 1988 1/10

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THERM AL DATA

T O - 3 T 0 - 2 1 8 IS O W A T T 2 1 8

Rth j-case Thermal Resistance Junction-case max 1 1 1.92 °C/W

ELECTR IC AL CHARACTERISTICS (Tcase = 25 “C unless otherwise specified)

S y m b o l P a r a m e t e r T e s t C o n d it io n s Min. Typ. Max. Unit

Ices Collector Cutoff Current Vce = rated Vces 200 pA

< 03m II O Vce = rated VCEs, T c = 1 2 5 °C 2 mA

Icer Collector Cutoff Current Vce = rated Vcer 500 pA

(Rbe = 1 0 0 ) Vce = rated Vc er. Tc = 125 °C 4 mA

Iebo Emitter Cutoff Current

(lc = 0 ) Veb = 5 V 1 mA

VcEO(sus) Collector-emitter Sustaining lc = 200 mA L = 2 5 m H

Voltage (Ib = 0 ) for B U X 4 8 /B U V 4 8 /B U V 4 8 F I 400 V

for B U X 4 8 A /B U V 4 8 A /B U V 4 8 A F I 450 V

Vebo Emitter-base Voltage

(lc = 0 ) Ie = 50 mA 7 30 V

VcE(sat)* Collector-emitter Saturation for B U X 4 8 /B U V 4 8 /B U V 4 8 F I

Voltage l c = 10 A l B = 2 A 1.5 V

lc = 15 A l B = 4 A 3.5 V

lc = 15 A l B = 3 A for B U X 4 8 A /B U V 4 8 A /B U V 4 8 A F I

5 V

l c = 8 A I e = 1.6 A 1.5 V

lc = 12 A l B = 2.4 A 5 V

VBE(sat) Base-emitter Saturation for B U X 4 8 /B U V 4 8 /B U V 4 8 F I

voltage l c = 10 A l B = 2 A

for B U X 4 8 A /B U V 4 8 A /B U V 4 8 A F I

1.6 V

l c = 8 A l B = 1.6 A 1.6 V

* Pulsed : pulse duration = 300 ps, duty cycle < 2 %.

RESISTIVE SWITCHING TIMES (see fig. 2)

S ym bo l P a r a m e t e r T e s t C o n d it io n s Min. Ty p. Max. Unit

Ion Turn-on Time for B U X 4 8 /B U V 4 8 /B U V 4 8 F I V c c = 150 V l c = 10 A IB1= 2 A

for B U X 4 8 A /B U V 4 8 A /B U V 4 8 A F I V c c = 150 V l c = 8 A

1 ps

I b1 = 1 .6 A 1 ps

ts Storage Time for B U X 4 8 /B U V 4 8 /B U V 4 8 F I V c c = 150 V l c = 10 A IB1 = - l B2 = 2 A

for B U X 4 8 A /B U V 4 8 A /B U V 4 8 A F I V c c = 150 V lc = 8 A

3 ps

IB1 = — Ib2 = 1 -6 A 3 ps

tf Fall Time for B U X 4 8 /B U V 4 8 /B U V 4 8 F I V c c = 150 V lc = 10 A Ibi = - Ib2 = 2 A

for B U X 4 8 A /B U V 4 8 A /B U V 4 8 A F I V c c = 150 V l c = 8 A

0.8 ps

IB1 = — IB2 = 1 -6 A 0.8 ps

r Z J SCS-THOMSON

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B U X48/B UV48/B UV48FI-BUX48A/B UV48A/B UV48AFI

INDUCTIVE SWITCHING TIMES (see fig. 1)

Sy mb o l P a r a m e t e r T e s t C o n d it io n s Min. Ty p. Max. Unit

ts Storage Time for B U X 4 8 /B U V 4 8 /B U V 4 8 F I Voc = 3 0 0 V, l c = 1 0 A, Lb = 3 hH

Vbe = — 5 V, I si = 2 A 2.7 PS

same T case = 125 °C

for B U X 48A B U V 4 8 A /B U V 4 8 A F I

5 ps

V cc = 300 V, l c = 8 A, Lb = 3 .uH

Vbe = — 5 V, Ib i = 1.6 A 3 ps

same, T case = 125 °C 5 ps

ti Fall Time for B U X 4 8/B U V 4 8 /B U V 4 8 F I V cc = 3 0 0 V, lc = 10 A, L B = 3 jiH

Vbe = — 5 V, l Bi = 2 A 0.16 ps

same T caS8 = 125 °C

for B U X 4 8 A /B U V 4 8 A /B U V 4 8 A F I

0.4 ps

V cc = 300 V, lc = 8 A, L e = 3 pH

Vbe = — 5 V, l B) = 1 .6 A 0.13 ps

same. T case = 125 °C 0.4 ps

Safe Operating Area (TO-3). Safe Operating Area (TO-218, ISOWATT218).

SCS-THOMSON

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Clamped Reverse Bias Safe Operating Areas. Forward Biased Accidental Overload Area.

(see fig. 3).

DC Current Gain..

0.5 2 3.5 5 6.5 8 9.5 1 c (A)

Saturation Voltage.

6-5 2 2 8

Collector-emitter Saturation Voltage.

G - 52 26/1

Collector Current Spread vs. Base Emitter Voltage.

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B U X48/B UV48/B UV48FI-BUX48A/B UV48A/B UV48AFI

Switching Times vs. Collector Current with Ib Constant.

Switching Times with and without Antisaturation Network (see fig.1).

Switching Times vs. Collector Current (see fig.2).

0 2 U 6 8 10 12 1c (A )

Switching Times Percentage Variation vs. Case Temperature.

Switching Times Percentage vs. Case Tempera­

ture.

25 50 75 100 TcaseTC)

Fall Times vs. Voltage Slope (see fig.2)..

0 1000 2000 3000 d v /d l (V/^js)

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Switching Times Percentage Variation vs. Case Dynamic Collector-emitter Saturation Voltage

Temperature. (see fig. 4).

Figure 1 : Switching Times Test Circuit on Inductive Load, with and without Antisaturation Network.

+6V

D1, D2 : Fast recovery diodes

Q1, Q2 : Transistors SGS 2N519 1 ,2N5195.

r r j SGS-THOMSON Moewmijicmsiwiics 6/10

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B U X48/B UV48/B UV48FI-BUX48A/B UV48A/B UV48AFI Figure 2 : Switching Times Test Circuit on resistive Load.

Figure 3 : Forward Biased Accidental Overload Area Test Circuit.

f ZT SGS-THOMSON

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Figure 4 : VcE(sat) Dyn. Test Circuit.

+ v BB =14 v

Figure 5 : Equivalent Input Schematic Circuit Circuit at Turn-on.

c

i f C » C ; AVq = AVj s- 6605/1

8/10 f ZT SGS-THOMSON

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B U X48/B UV48/B UV48FI-BUX48A/B UV48A/B UV48AFI

Figure 6 : Remarks to VcE(sat) Dyn. Test Circuit (fig.4).

## \ /

b

### S-660 3 t

The speed-up capacitor decreases the VCE (sat) dyn. as shown in diagram (figure 6). The 50 nF capacitor modifies the shape of base current with a overshoot.

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IS 0 W A T T 2 1 8 P AC KA G E C H A R A C T E R IS T IC S AND A P P LIC A TIO N ISOWATT218 is fully isolated to 4000V dc. Its ther­

mal impedance, given in the data sheet, is optimi­

sed to give efficient thermal conduction together with excellent electrical isolation. The structure of the case ensures optimum distances between the pins and heatsink. These distances are in agree­

ment with VDE and UL creepage and clearance standards. The ISOWATT218 package eliminates the need for external isolation so reducing fixing hardware.

The package is supplied with leads longer than the standard TO-218 to allow easy mounting on pcbs.

Accurate moulding techniques used in manufacture assures consistent heat spreader-to-heatsink capa­

citance.

ISOWATT218 thermal performance is equivalent to that of the standard part, mounted with a 0.1 mm mi­

ca washer. The thermally conductive plastic has a higher breakdown rating and is less fragile than mi­

ca or plastic sheets. Power derating for ISO- WATT218 packages is determined by :

Tj - Tc Pd= ---

Rth

T H E R M A L IM PED AN C E OF ISO W ATT218 PAC KA G E Figure 6 illustrates the elements contributing to the

thermal resistance of a transistor heatsink assem­

bly, using ISOWATT218 package.

The total thermal resistance Rth(tot) is the sum of each of these elements. The transient thermal im­

pedance, Zth for different pulse durations can be estimated as follow s:

1 - For a short duration power pulse of less than 1 m s :

Zth < RthJ-C

2 - For an intermediate power pulse of 5ms to 50ms seconds :

Zth = RthJ-C

3 - For long power pulses of the order of 500ms se­

conds or gre ater:

Zth = RthJ-C + RthC-HS + RthHS-amb It is often possible to discern these areas on trans­

ient thermal impedance curves.

Figure 6.

R thJ-C R thC-HS R thHS-amb

T SGS-THOMSON

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