In most amplifiers applications we want fidelity of amplification (=>output wave shape identical to the input shape form). If the input signal is nonsinusoidal (the principles of Fourier analysis show that such signal consist of broad spectrum of harmonically related frequencies) to achieve undistorted output all component frequencies (to 3  5 harmonics of repetition frequency) must be equally amplified in magnitude. Unequal gain for the frequency components causes (gain  frequency curve and phase  frequency curve)) distortion. In middlefrequency range the gain and phase angle are reasonable constant => circuits reactances have negligible effect (seriescapacitive reactances approximate short circuits, all shuntcapacitive reactances appear as effective open circuits) In highfrequency range shunt capacitance (result of the internal transistor capacitance) reduces the load impedance and output voltage. In lowfrequency range the series capacitance increase in reactance and progressively cause a drop in the response with falling frequency. The amplifier bandwidth BW=f_{H0}f_{L0}since
the low frequency limit BW can be extended to zero frequency, the highfrequency
limit restricts the amplifier bandwidth.
Gain versus frequency curves driven in logarithmic scale are known as Bode plots => we can employ straightline approximation to obtain the performance characteristic corner frequency at which asymptotes of the dB curves intersect. => correction for curve in corner frequency (10 log2=3dB). Gainfrequencies curves in dB being additive.
(The gain of 2stage identical amplifier fall at 40dB per frequency decade
(12 dB per octave), 3stage circuits will have a gain curve that falls
at 60dB per decade. The phase angle will be multiplied by the number
of stages +90^{o }and at extreme frequency in nstage amplifier
=> critical condition for oscillation. When stages of the amplifier
are cascaded the bandwidth is reduced.
Black box width feedback (voltage) illustrates
the sampling by the b
(beta) network and reverse transmissions of signal in feedback system.
(=> giving on output bU_{2}
=> is subtracted from the voltage U_{1} at the mixing point, to
yield the error signal U_{D.}
Openloop gain A_{D}
internal gain of the amplifier.
Closedloop gain A=
A_{D}/(1+bA_{D})~1/b.
Output sampling: Output resistance
in:
Effect of feedback on input resistance:
Inverting op amp, noninverting
op amp and the unitygain buffer
The integration operation amplifier (in fig (a)
above, if Z_{f} is a capacitance will perform mathematical
operation of integration on the input signal). By considering property
of the integration operation amplifier the Miller effect can be explained
as increasing equivalent input capacitance C'=(1+A_{D})C and so
a very large time constant circuits can be achieved. Example of such a
circuit see active integrator called "charge sensitive
amplifier"
The application of negative feedback to amplifiers is effective in increasing the amplifier bandwidth. In general, instability of the voltage feedback never differs as much as 180^{o }from its middlerange => reduce by corrective RC circuits in 1 stage. The compensation network seriously reduces the amplifier bandwidth.
Monolithic construction, with a complete amplifier integrated into tiny silicon chip, leads very small size, balancing of temperature effects, reduced cost, and improved reliability by elimination of much interconnecting wiring. By addition of negative feedback to a highgain (A>5000) integrated amplifier => operational amplifier ("opamp"). This circuits closely approaches an ideal package of gain, with high input resistance and low output resistance. Use of negative feedback
sacrifices gain, reduce distortion, improve stability
of gain, alter frequency response and modify
input and output impedance.
When a pnjunction is under reverse voltage U_{D} (case of semiconductor detector) the transition region is depleted of mobile charges (=> More mobile charge is removed and the depleted region increases whit increasing U_{D}) and takes on the properties of a dielectric, with only fixed charges present. The dynamic transition capacitance depends on r.m.s. of applied voltage (U_{B}+U_{D})~U_{D}, where U_{B}  barrier potential of junction, U_{D}  applied outside voltage: To make charge response independent of variance
in detector capacitance is necessary use active
integrator called "charge sensitive amplifier"


