• Nie Znaleziono Wyników

BC140

N/A
N/A
Protected

Academic year: 2022

Share "BC140"

Copied!
3
0
0

Pełen tekst

(1)

BC140 BC141

GENERAL PURPOSE TRANSISTORS

DESCRIPTION

The BC140 and BC141 are silicon planar epitaxial

\iPN transistors in TO-39 metal case. They are par- : cularly designed for audio amplifiers and switching applications up to 1 A. The complementary PNP r/pes are the BC160 and BC161.

INTERNAL SCH EMATIC DIAGRAM

ABSOLUTE MAXIMUM RATINGS

S ym bo l P a r a m e t e r V al ue

Uni t

BC 14 0 BC141

VcBO Collector-base Voltage ( Ie = 0 ) 80 100 V

VcEO Collector-emitter Voltage (l B = 0) 40 60 V

Ve b o Emitter-base Voltage (lc = 0) 7 V

lc Collector Current 1 A

Ib Base Current 0.1 A

P tot Total Power Dissipation at T amb £ 45 °C 0.65 W

3t Tc a s e — 45 "C 3.7 W

T s t g Storage Temperature - 55 to 175 °C

T | Junction Temperature 175 °C

January 1989 1/3

(2)

B C 1 40 -B C 1 41

TH ER M AL DATA

R th j-case Thermal Resistance Junction-case Max 35 :C/W

Rth j-amb Thermal Resistance Junction-ambient Max 200 :C/W

ELE CTRICAL CHARACTERISTICS (Tamb = 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 Vces =60 V 100 nA

(Ie= 0) Vces= 60 V Tamb =150 °C 100 pA

V ( B R ) C B O Collector-base Breakdown

Voltage

lc = 100 pA

for B C 1 4 0 80 V

Oe = 0 ) for BC141 100 V

V ( B R ) C E O * Collector-emitter

Breakdown Voltage

lc = 30 mA

for B C 1 4 0 40 V

(Ib =0) for BC141 60 V

V ( B R ) E B O Emitter-base

Breakdown Voltage (lc =0)

lE = 100 pA 7 V

V c E ( s a t ) * Collector-emitter lc = 100 mA Ib= 10 mA 0.1 V

Saturation Voltage lc = 500 mA Ib= 50 mA 0.35 V

l c = 1 A lB =0.1 A 0.6 1 V

CO>

Base-emitter Voltage l c = 1 A < o m II < 1.25 1.8 V

h F E * DC Current Gain l c = 100 pA < o m II <

for B C 14 0- 14 1 75

for B C 1 4 0 - 1 4 1 Gr. 6 28

for B C 1 4 0 - 1 4 1 Gr. 10 40

for B C 1 40 -14 1 Gr. 16 90

lc = 100 mA < Om II <

for B C 1 4 0 - 1 4 1 40 140 250

for B C 1 4 0 - 1 4 1 Gr 6 40 63 100

for B C 1 4 0 - 1 4 1 Gr.10 63 100 160

for B C 1 4 0 - 1 4 1 Gr.16 100 160 250

lC = 1 a

>II

o>

for B C 1 4 0 - 1 4 1 26

for B C 1 4 0 - 1 4 1 Gr. 6 15

for B C 1 4 0 - 1 4 1 Gr.10 20

for B C 1 4 0 - 1 4 1 Gr.16 30

t T Transition Frequency lc = 50 mA Vqe= 10 V 50 MHz

C c B O Collector-base lE = 0 Vcb= 10 V

Capacitance f = 1 MHz 12 25 pF

t o n Turn-on Time lc = 100 mA

let = 5 mA 250 ns

t o f f Turn-off Time l c = 100 mA

I b 1= I b2= 5 mA 850 ns

* Pused : pulse duration = 300 ps, duty cycle = 1 %.

T SGS-THOMSON

^ 7 # M fl»[iLiKgirK© [iaD© i

(3)

BC 1 40 -B C 1 41

Collector-emitter Saturation Voltage. Base-emitter Voltage.

G-1869

ZC Curent Gain. Transiition Frequency.

1 0 ' 1 10 10' l c (m A ) 1 K> 10! Ic (m A )

n ? Z SCS'THOMSON

^ 7 # ' t

3/3

Cytaty

Powiązane dokumenty

signals [6.6). As aresuIt, the gain accuracy and linearity of the -ÓL modulator is not limited by component matching. Furthermore, as shown in Figure 6.1, the ADC 's reference

This work is dedicated to the development of high brightness 100-electron-beam sources to increase the throughput of electron beam lithography, inspection, and electron beam

According to Hasan and Handzic (2003), all integrated frameworks consider KM as a complex and multidimensional concept; synthesise the object and human

Niknejad, “A compact 1V 18.6dBm 60GHz power amplifier in 65nm CMOS,” in IEEE International Solid-State Circuits Conference Digest of Technical Papers. (ISSCC),

Awangarda jako zjawisko społczne, bunt ob­ darzony imieniem w świadomości uczestników kultury — zrodziła się w wyniku powstania alternatywnej publiczności, i

Visualization is the conversion of data into a visual or tabular format so that the characteristics of the data and the relationships among data items or attributes can be

The selected development process thus implies sticking to the railway standards from the beginning, considering the fi re detection system as any other electronic

We now present a construction of an un- countable family of Toeplitz sequences over two symbols with the following properties: the corresponding Toeplitz flows are strictly ergodic