• Nie Znaleziono Wyników

BUT13

N/A
N/A
Protected

Academic year: 2022

Share "BUT13"

Copied!
6
0
0

Pełen tekst

(1)

/ I T SCS-THOMSON

* 7 1 l * ! f 3® i ! L I O T ® « S B U T 1 3 / 1 3 P / 1 3 P F I HIGH VOLTAGE POWER SWITCH

■ HIGH POWER

■ INTEGRATED SPEED-UP DIODE

DESCRIPTION

The BUT13 . BUT13P and BUT13PFI are silicon multiepitaxial planar NPN transistors in monolithic darlington configuration with integrated base-emit­

ter speed-up diode, mounted respectively in TO-3 metal case, TO-218 plastic package and ISO- WATT218 fully isolated package.

They are particularly suited for output stages in po­

wer, fast switching applications.

ABSOLUTE MAXIMUM RATINGS

Symbol Parameter Value Unit

Vc b o Collector-base Voltage (Ie = 0 ) 600 V

Vc e o Collector-emitter Voltage ( Ib = 0) 400 V

oCD>

Emitter-base Voltage (lc = 0) 10 V

l c Collector Current 28 A

ICM Collector Peak Current 35 A

Ib Base Current 6 A

TO-3 TO -218 ISO W ATT218

P t o t Total Dissipation at T c < 25°C 175 125 60 W

T s t g Storage Temperature - 65 to 200 - 65 to 150 - 65 to 150 °C

Ti Max. Operating Junction Temperature 200 150 150 °C

December 1988 1/6

(2)

THERMAL DATA

T 0 -3 T 0 -2 1 8 IS 0W A T T 218

Rth j-case Thermal Resistance Junction-case Max 1 1 2.08 °C/W

ELECTRICAL CHARACTERISTICS (Tcase = 25 -C unless otherwise specified)

Symbol Parameter Test Conditions Min. Typ. Max. Unit

I c E V Collector Cutoff Current VCE = 600 V 100 M A

VCE = 600 V T c a s e — 1 0 0 ° C 2 mA

oUJO Collector Cutoff Current

(la = 0 ) V 0E = 400 V 1 mA

Ie b o Emitter Cuttoff Current

(lc = 0)

>CVJIIm>

2 0 mA

VcEO(sus)* Collector-emitter Sustaining

Voltage lc = 100 mA 400 V

VcE(sat)* Collector-emitter Saturation lc = 10 A l B = 0 .5 A 1.3 2 V

Voltage l c = 18 A Is = 1 .8 A 1.7 2.5 V

lc = 2 2 A l B = 2 .2 A 2 3 V

lc = 2 8 A l B = 5 .6 A 2.35 5 V

VBE(sat)* Base-emitter Saturation lc = 10 A l B = 0 .5 A 2.5 V

Voltage lc = 1 8 A l B = 1.8 A 2.5 3 V

lc = 2 2 A l B = 2 .2 A 3.3 V

h FE * DC Current Gain lc = 10 A VCE = 5 V 30 300

lc = 18 A VCE = 5 V 30 90

V F* Diode Forward Voltage l F = 2 2 A 2 . 2 4 V

RESISTIVE SWITCHING TIMES

Symbol Parameter Test Conditions Min. Typ. Max. Unit

ton Turn-on Time V Cc = 250 V lc = 10 A 0.5 0.6 ps

Storage Time IB1 = 0 .5 A 1.1 1.5 ps

tf Fall Time VBE(off) = - 5 V

0.3 0.6 ps

INDUCTIVE SWITCHING TIMES

Symbol Parameter Test Conditions Min. Typ. Max. Unit

t. Storage Time

Vclamp = 250 V lc = 10 A IB1 - 0.2 A ; Vb e(oM ) - 5 V

1.3 2 ps

tt Fall Time 0.11 0.5 ps

tc Crossover Time 0.4 0.8 ps

ts Storage Time

Vclamp = 250 V lc = 20 A Ib i= 0 . 4 A ; VBE(off) = - 5 V

1.4 2.6 ps

tf Fall Time 0.4 0.7 ps

to Crossover Time 0.8 1.5 ps

* Pulsed : pulse duration = 300 ps, duty cycle = 1.5 %.

f Z T SGS-THOMSON

^ 7 # ^oicnmiBOTR@a!iocs 2/6

(3)

Safe Operating Areas (for BUT13). Safe Operaging Areas (for BUT13P and BUT13PFI).

10’ 1 10 l c (A )

Collector-emitter Saturation Voltage.

- I i < I J 4 6 0 1 4 « 8

10 1 10 I c ( A )

Collector-emitter Saturation Voltage.

101 1 10 l c (A)

f Z T SGS-THOMSON

^ 7 # ifflCSI®G&IICirR©Q90C3

(4)

Base-emitter Saturation Voltage.

G- 5604

10'1 1 10 ! c ( A )

Collector-emitter Saturation Voltage Dynamic.

Freewheel Diode Forward Voltage.

Vp

(V)

3.2 2.8 2. 4 2 1.6 1.2 0 .8

0 .4

0

1 0 1 1 10 I F ( A )

Switching Times Resistive Load (test circuit fig. 1).

6-5606

Vc c = 250 V h F E * 5 0

I_____i_____ _____ I____

o 2 « 6 8 ! ( MS)

Switching Times Percentage Variation vs. Tease.

2 5 5 0 7 5 100 125 T<

Switching Times inductive Load Test (test circuit fig. 1).

4/6

5 7

SCS-THOMSON

RSI0(B^®SIL[SCTK®0i50(SS

(5)

Switching Times Percentage Variation vs. Tease- Clamped Reverse Bias Safe Operating Area.

T EST CIRCUITS Figure 1.

SGS-THOMSON

MlCSBfflLSCTBSSiOOS

5/6

(6)

I S 0 W A T T 2 1 8 PACKAGE CHARA CTERISTICS AND AP PLIC ATION 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 di­

stances between the pins and heatsink. These di­

stances are in agreement with VDE and UL cree- page 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 break­

down rating and is less fragile than mica or plastic sheets. Power derating for ISOWATT218 packages is determined b y :

THE RM A L IMPEDANCE OF ISOW AT T218 PACKAGE Figure 2 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 impedance, Zth for different pulse durations can be estimated as follows : 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 seconds or gre ater:

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

sient thermal impedance curves.

Figure 2.

RthJ-C R thC-HS R thHS-amb

—W V — W V — V W —

6/6 £ Z T SGS-THOMSON

“ -T# M1GBMUSCTWWMC8

Cytaty

Powiązane dokumenty

Stack-losses of ammonia Y were measured in course of 21 days of operation of a plant for the oxidation of ammonia (NH3) to nitric acid (HNO 3 ).. Discuss the

1) Show that the invariancy of Hamiltonian H with respect to infinitesimal shifts in space leads to the momentum conservation in the quantum system governed by H, i.e. Define

the discrete model of the hyperbolic heat conduction of the periodic unbounded laminated medium under consideration..

- support posts rammed into the ground by means of pile drivers (D - the ramming depth of the posts is determined individually depending on the soil quality at the installation

The book consists of 17 chapters, each comprising a selection of source texts and a number of dedicated exercises whose aim is to practise the lexical items and use the

In this note we are to apply mentioned above Lapunov exponents notation properties to the discussion of the wave-type solutions in the hyperbolic heat con- duction in

By Hajnal’s set mapping theorem (see [5]), we can find an uncountable index set in which for α 6= β, no nonzero difference or sum occurs both in s α and s β , except of course

Here, we introduce a factor graph structure learning approach in the context of an evolutionary algorithm, which is polynomial in the number of variables and the number of