Map of content for microelectronic circuits — how semiconductor physics gives rise to devices (diodes, MOSFETs, BJTs), and how those devices are biased and combined into amplifiers, op-amps, and signal-processing circuits. The path: semiconductor physics → pn junction → diodes and their circuits → MOSFET and BJT operation → DC biasing → small-signal models → single-transistor amplifiers → operational amplifiers → frequency response.

Signal and circuit preliminaries

The vocabulary for the signals these circuits process and the basic tools used to analyze them.

  • Signal — the general concept; the time-varying quantity an amplifier acts on.
  • Sinusoid — the test signal for everything; AC analysis is sinusoidal steady state.
  • Amplitude (signal) — peak, peak-to-peak, and the size of a swing.
  • Phase (waveform) — the shift between input and output a circuit introduces.
  • Frequency and period — the rate and its reciprocal.
  • Root mean square — the effective DC-equivalent value used for power and ripple.
  • Capacitive reactance; why coupling and bypass caps are frequency-dependent.
  • Voltage divider — the most-reused result in biasing and small-signal analysis.
  • Fourier series — harmonic decomposition; the basis for talking about distortion and spectral content.

Semiconductor physics

Why silicon conducts the way it does, and how doping turns it into a controllable material.

The pn junction

What happens when n-type meets p-type — the structure underneath every diode and transistor.

Diodes

The two-terminal device built from a single pn junction, and the models used to analyze it.

Diode application circuits

Rectifiers, regulators, and waveform-shaping circuits built from diodes.

MOSFET — structure and operation

The voltage-controlled transistor that dominates modern electronics.

MOSFET — DC biasing

Setting the transistor’s operating point so it amplifies.

BJT — structure and operation

The current-controlled transistor: two coupled pn junctions.

BJT — DC biasing

Establishing a stable collector current.

Small-signal modelling

Linearizing a nonlinear device around its Q-point so AC analysis becomes linear circuit analysis.

Single-transistor amplifier configurations

The standard ways to wire one transistor as an amplifier, and what each is good for.

Operational amplifiers and feedback

The idealized high-gain differential amplifier and the feedback circuits built around it.

Op-amp non-idealities

Where the real op-amp departs from the ideal model.

  • Input bias current — the small DC current the inputs actually draw.
  • Input offset voltage — the small input mismatch that appears as a DC output error.
  • Slew rate — the maximum output rate of change; a large-signal speed limit.
  • Full-power bandwidth — the highest frequency for a full-amplitude undistorted output, set by slew rate.

Frequency response and the Miller effect

How gain rolls off with frequency, and why.


The signal-analysis machinery here — Transfer function, Bode plot, Frequency response, filters, and the Fourier series — is developed in full in Signals and systems; this course applies it to transistor and op-amp circuits. The AC math (complex impedance, phasors, the -plane) rests on the complex analysis in Mathematical methods. Digital logic is where this meets the gate level: CMOS, NMOS transistor, and PMOS transistor are the transistor-level substrate that digital gates are built from, and the Voltage-transfer characteristic is the bridge between the analog device curve and the digital logic level. The underlying device physics — PN junction, Depletion region, carrier drift and diffusion — is the circuit-side counterpart of the field theory in Electromagnetics.