This static DC load line produces a straight line equation whose slope is given as: -1/(R L + R E) and that it crosses the vertical Ic axis at a point equal to Vcc/(R L + R E).
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Calculate the values of all the other circuit resistors assuming a standard NPN silicon transistor. Also find the value of the Emitter resistor, R E if it has a voltage drop of 1v across it. Calculate the maximum Collector current ( Ic) flowing through the load resistor when the transistor is switched fully “ON” (saturation), assume Vce = 0. Common Emitter Amplifier Example No1Ī common emitter amplifier circuit has a load resistance, R L of 1.2kΩ and a supply voltage of 12v. The Collector current, Ic can be approximated, since it is almost the same value as the Emitter current. If the voltage across the Emitter resistor is known then the Emitter current, Ie can be easily calculated using Ohm’s Law. This is because Beta ( β ) is an inherent characteristic of the transistors construction and not of its operation.Īs the Base/Emitter junction is forward-biased, the Emitter voltage, Ve will be one junction voltage drop different to the Base voltage. So one BC107 may have a Beta value of 110, while another one may have a Beta value of 450, but they are both BC107 npn transistors. For example, the BC107 NPN Bipolar transistor has a DC current gain Beta value of between 110 and 450 (data sheet value). Transistors of the same type and part number will have large variations in their Beta value. Beta (h FE) has no units as it is a fixed ratio of the two currents, Ic and Ib so a small change in the Base current will cause a large change in the Collector current. Beta is an electrical parameter built into the transistor during manufacture. The Common Emitter Amplifier CircuitĪ transistors Beta value, sometimes referred to as h FE on datasheets, defines the transistors forward current gain in the common emitter configuration. Consider the Common Emitter Amplifier circuit shown below. The best possible position for this Q-point is as close to the center position of the load line as reasonably possible, thereby producing a Class A type amplifier operation, ie. This is in fact the DC operating point of the amplifier and its position may be established at any point along the load line by a suitable biasing arrangement. To obtain low distortion when used as an amplifier the operating quiescent point needs to be correctly selected.
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The aim of any small signal amplifier is to amplify all of the input signal with the minimum amount of distortion possible to the output signal, in other words, the output signal must be an exact reproduction of the input signal but only bigger (amplified).
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This can be achieved using a process known as Biasing.īiasing is very important in amplifier design as it establishes the correct operating point of the transistor amplifier ready to receive signals, thereby reducing any distortion to the output signal.Īlso, the use of a static or DC load line drawn onto the output characteristics curves of an amplifier allows us to see all the possible operating points of the transistor from fully “ON” to fully “OFF”, and to which the quiescent operating point or Q-point of the amplifier can be found. Then some way of “presetting” the amplifier’s circuit configuration is required so that the transistor can operate between these two maximum or peak values. Transistor amplifier’s amplify an AC input signals that alternates between some positive value and a corresponding negative value.