VBE 0.7 V Re www Rc 2 25 20 15 10 5 Vcc +11+ Ves - IsRs - VBE = 0 Rc 1k VBB - VBE = la Ra Base-bias Silicon small signal transistors typically have a ß in the range of 100-300. Complete the following table of values. Beta Vcc= VBB 100 150 200 250 300 1.2k 900 750 500 VBB - VBE RB E = (B + 1) | B = BlB Vaa - VBE RB/B le = RB 1k 500 300 450 250 (KVL) (IE base-bias) Ів IE

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Solve IB and IE
VBE =
0.7 V
Ro Rc
Vcc = VBB
25
20
15
10
Vcc
5
Ves - IsRs - VBE = 0
VBB
Base-bias
Silicon small signal transistors typically have a ß in the range of 100-300.
Complete the following table of values.
Beta
100
150
200
250
300
Rc
1k
1.2k
900
750
500
B = 100
=
R₁ =
B = 100
1 =
VBE BRB
Example Calculations:
Assuming that we have a ß-100 transistor, what value of the base-bias resistor is required to
yield an emitter current of 1mA? Solving the IE base-bias equation for RB and substituting B, VBB,
VBE, and IE yield 930kn. The closest standard value is 910kn.
B = 300
Vn-V₁
/B
Vra-Ver
R/B
=
VBB - VBE
RB
E = (B + 1) B = BlB
VBB - VBE
RB/B
V₁ = 10V c = = 1mA
RB
1k
500
300
450
250
=
What is the emitter current with a 910k resistor? What is the emitter current if we randomly get
a ß-300 transistor?
10-0.7
910k/300
10-0.7
1mA/100
= 930k
Vi= 10V R₁ = 910k VHF = 0 7V
10 -0.7
910k/100
(KVL)
(IE base-bias)
= 102mA
= 307mA
IB
The emitter current is little changed in using the standard value 910k2 resistor. However, with a
change in ß from 100 to 300, the emitter current has tripled. This is not acceptable in a power
amplifier if we expect the collector voltage to swing from near VCC to near ground. However, for
low level signals from micro-volts to about a volt. the bias point can be centered for a ß of the
square root of (100-300)=173. The bias point will still drift by a considerable amount. However.
low-level signals will not be clipped.
Base-bias is not suitable for high emitter currents, as used in power amplifiers. The base-biased
emitter current is not temperature stable.
Thermal runaway is the result of high emitter current causing a temperature increase which
causes an increase in emitter current, which further increases temperature.
IE
Transcribed Image Text:VBE = 0.7 V Ro Rc Vcc = VBB 25 20 15 10 Vcc 5 Ves - IsRs - VBE = 0 VBB Base-bias Silicon small signal transistors typically have a ß in the range of 100-300. Complete the following table of values. Beta 100 150 200 250 300 Rc 1k 1.2k 900 750 500 B = 100 = R₁ = B = 100 1 = VBE BRB Example Calculations: Assuming that we have a ß-100 transistor, what value of the base-bias resistor is required to yield an emitter current of 1mA? Solving the IE base-bias equation for RB and substituting B, VBB, VBE, and IE yield 930kn. The closest standard value is 910kn. B = 300 Vn-V₁ /B Vra-Ver R/B = VBB - VBE RB E = (B + 1) B = BlB VBB - VBE RB/B V₁ = 10V c = = 1mA RB 1k 500 300 450 250 = What is the emitter current with a 910k resistor? What is the emitter current if we randomly get a ß-300 transistor? 10-0.7 910k/300 10-0.7 1mA/100 = 930k Vi= 10V R₁ = 910k VHF = 0 7V 10 -0.7 910k/100 (KVL) (IE base-bias) = 102mA = 307mA IB The emitter current is little changed in using the standard value 910k2 resistor. However, with a change in ß from 100 to 300, the emitter current has tripled. This is not acceptable in a power amplifier if we expect the collector voltage to swing from near VCC to near ground. However, for low level signals from micro-volts to about a volt. the bias point can be centered for a ß of the square root of (100-300)=173. The bias point will still drift by a considerable amount. However. low-level signals will not be clipped. Base-bias is not suitable for high emitter currents, as used in power amplifiers. The base-biased emitter current is not temperature stable. Thermal runaway is the result of high emitter current causing a temperature increase which causes an increase in emitter current, which further increases temperature. IE
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