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JWST499-Cetinkunt
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transistor. The diode limits the voltage to the supply voltage by providing a current flow
path during that transient period. The current flow due to inductive voltage is then dissipated
in the diode-load loop within a short period of time. The resistor (R ) which connects the
2
base to the ground is not necessary, but makes the circuit a better one by providing a ground
to the base when the transistor is not turned ON (when the mechanical switch is open).
In the following discussion, assume the components in the dotted blocks do not exist for
simplicity. Let L = 0.0 H and R = 0.0 Ω. When the mechanical switch is OFF, the base
2
voltage and current are zero, the transistor is OFF, no current flows through the load. When
the mechanical switch is ON, the base current and collector current are,
V AB (10 − 0.7)V
i = = = 9.3 mA (5.156)
B
R 1000 Ω
1
i = ⋅ i = 0.93 A (5.157)
C
B
where it is assumed that = 100. But the maximum current that the supply can support is
V CC − V CE 10 − 0.2
i C,max = = = 0.098 A (5.158)
R L 100
Hence, the transistor saturates with the maximum voltage drop across the load, V = 10 −
L
0.2, and the minimum voltage drop across the transistor, V CE = 0.2 V. The transistor acts
like a very low resistance switch when it is saturated. Voltage drop across it is V CE = 0.2V.
Providing excess base current to saturate the transistor is a good idea and provides a safety
margin to make sure the transistor is fully turned ON (in its saturation region) and hence
providing the maximum voltage drop across the load. Notice that when the transistor is
ON, the current drain through the resistor R is
2
V BE 0.7
i = = = 0.07 mA (5.159)
2
R 2 10 000
which is a negligable load.
Example Another common use of a transistor is in a current-source circuit (Fig-
ure 5.20). Notice that this circuit does not have any voltage amplification, but it has current
amplification. Output voltage tracks the base voltage as shown below with the exception of
the small voltage drop across the base and emitter. Let us assume voltage drop across the
base-emitter is V = 0.6V.
BE
V out = V − 0.6; when V ≥ 0.6 V (5.160)
in
in
V out = 0; when V < 0.6 V (5.161)
in
A
C
v in
B
E v out
i E
R
E
FIGURE 5.20: A transistor circuit as a current-source.