Bipolar Junction Transistor Circuits:The Basic BJT Switch
The Basic BJT Switch
In digital circuits, the BJT is used as a switch to generate one of only two possible output voltage levels, depending on the input voltage level. Each voltage level is associated with one of the binary digits, for example, the high voltage level may fall between 2.8 and 5 V while the low voltage level may fall between 0 and 0.8 V.
Logic circuits are based on BJT stages that are either in cutoff with both junctions reverse-biased or in a conducting mode with the emitter–base junction forward-biased. When the BJT is “on” or conducting emitter current, it can be in the active regionor the saturation region. If it is in the saturation region, the collector–base region is also forward-biased. The three possible regions of operation are summarized in Table 10.2.
The BJT very closely approximates certain switch configurations. For example, when the switch of Figure 10.16(a) is open, no current flows through the resistor and the output voltage is +12 V. Closing the switch causes the output voltage to drop to 0 V and a current of 12/R flows through the resistance. When the base voltage of the BJT of Figure 10.16(b) is zero or negative, the device is cut off and no collector current flows. The output voltage is +12 V just as in the case of the open switch. If a large enough current is now driven into the base to saturate the BJT, the output voltage becomes very small, ranging from 20 to 500 mV, depending on the BJT used. The saturated state corresponds closely to the closed switch. During the time that the BJT switches from cutoff to saturation, the active region equivalent circuit applies. For high-speed switching of this circuit, appropriate reactive effects must be considered. For low-speed switching these reactive effects can be neglected.
Saturation occurs in the basic switching circuit of Figure 10.16(b) when the entire power supply voltage drops across the load resistance. No voltage, or perhaps a few tenths of volts, then appears from collector to emitter. This occurs when the base current exceeds the value
When a transistor switch is driven into saturation, the collector–base junction becomes forward-biased. This situation results in the electron distribution across the base region as shown in Figure 10.17.
The forward bias of the collector–base junction leads to a nonzero concentration of electrons at the right edge of the base region. This results in an excess concentration of electrons in the base that is unnecessary to support the gradient of carriers across this region. When the input signal to the base switches to a lower level to either turn the device off or decrease the current flow, the excess charge must be removed from the base region before the current can begin to decrease.
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