ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING Theory: 3H preamplifiers. Encyclopedia of radio electronics and electrical engineering Encyclopedia of radio electronics and electrical engineering / Beginner radio amateur Preamplifiers are usually voltage amplifiers, and low-power ones, since their output is designed for a load from 600 ohms to several tens of kilo-ohms. As a rule, they work on the high-impedance input of the power amplifier and therefore their output current is very small. Usually, preamplifiers have several inputs designed to connect various sources: the line output of a tape recorder, an electromagnetic or piezoelectric pickup, a radio receiver, and sometimes (less often) a broadcast line. Requirements for input parameters - sensitivity (the minimum signal voltage required for normal operation) and input resistance - differ for different inputs. Moreover, correction of the frequency response of the amplifier is often required when working with one or another signal source. A magnetic head, for example, develops an EMF proportional to the rate of change of the magnetic flux, and hence to frequency. But at higher frequencies, the EMF drops due to a decrease in the effective thickness of the tape layer at short recording wavelengths, the finite width of the head gap, and other reasons. Therefore, the corrector amplifier must have a rise in the amplitude-frequency characteristic (AFC) at lower and higher frequencies. The necessary amplification to raise the signal level from a few millivolts to fractions of a volt in the AF preamplifier is usually obtained using one or two transistor stages. Moreover, to simplify the amplifier, a direct connection between the cascades by direct current is often used. A practical diagram of such an amplifier is shown in fig. 39. The input signal through the decoupling capacitor C1 is fed to the base of the transistor VT1, and from its load (resistor R1) - to the base / T2. The stabilization of the transistor mode occurs as follows: the collector voltage of the transistor VT1 (usually 1 ... 2 V) is "repeated" at the emitter VT2, where the bias resistor R3 is connected. The amplified signal is removed from the load of the transistor VT2 (resistor R4) and is fed through the isolation capacitor C3 to the UMZCH. Capacitor C2 eliminates AC negative feedback for audio frequencies, thereby increasing the gain, which in this amplifier can reach several thousand. Resistor R2 creates an OOS in the first stage - it reduces the gain, but it increases the input impedance and reduces distortion. Its resistance can be varied over a wide range, when it is reduced to zero, the gain will be maximum. You can also reduce the gain by turning on a resistor in series with capacitor C2, thus creating an OOS in the second stage. By reducing the capacitance of the capacitor, it will be possible to correct the frequency response. providing a rise in the higher frequencies of the audio spectrum due to the fact that the capacitance decreases with frequency, reducing the feedback at these frequencies. To attenuate the higher frequencies, you need to include a small capacitor between the collector and the base of one of the transistors. As a result, an OOS will appear, operating mainly at these frequencies. If it is necessary to increase the input and lower the output impedance of the amplifier, emitter followers are turned on at its input and output. Author: V.Polyakov, Moscow See other articles Section Beginner radio amateur. Read and write useful comments on this article. Latest news of science and technology, new electronics: Machine for thinning flowers in gardens
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