Section 2.2: Transistors and Amplification

Status: draft1 — Human-edited draft, may be missing images or figures.

Section 2.2: Transistors and Amplification #

Remember when we talked about semiconductors in your Technician studies? Now it’s time to take a deeper dive into these amazing components. As a General class operator, you’ll want to understand how transistors and tubes amplify signals to help you communicate over longer distances with clearer signals.

Transistors: The Building Blocks of Amplification #

Transistors might be small, but they’re incredibly versatile! These semiconductor devices form the foundation of modern electronics, serving as both switches and amplifiers with remarkable precision. They perform two primary functions in your radio equipment: switching signals on and off, and amplifying weak signals into stronger ones. Let’s look at how they work in your radio equipment.

Bipolar Junction Transistors (BJTs) #

Bipolar transistors consist of three semiconductor layers (collector, base, and emitter). A small current through the base controls a much larger current between collector and emitter.

Key Information: A bipolar transistor used as a switch has two operating points: saturation and cutoff.

When used as a switch:

  • In cutoff, the transistor blocks current flow (like an open switch)
  • In saturation, the transistor allows maximum current flow (like a closed switch)

Field-Effect Transistors (FETs) #

FETs use an electric field, rather than current, to control the flow of current through a semiconductor channel.

Key Information: In MOSFET construction, the gate is separated from the channel by a thin insulating layer.

This insulating layer creates an extremely high input impedance, as virtually no current flows into the gate. The voltage at the gate creates an electric field that controls current flow between the source and drain.

Both transistor types have important roles in your radio. Bipolar transistors are often used in audio and low-level RF stages, while MOSFETs excel in RF power amplifiers and receiver front ends where their high-frequency performance and high input impedance are advantageous.

Vacuum Tubes: Understanding Legacy Technology #

Though largely replaced by solid-state devices in modern equipment, vacuum tubes remain important to understand for several reasons: they appear on your exam, they’re found in older equipment still in use, and they’re still manufactured for specific applications like high-power RF amplifiers. They perform much the same function that we now usually use transistors for, but they can handle much higher voltages and power levels. They are also less “fragile”, being more resistant to things like radiation and EMPs.

Vacuum tubes work by controlling a stream of electrons flowing from a heated cathode to a plate (anode) through a vacuum.

Key Information: The control grid in a vacuum tube regulates the flow of electrons between cathode and plate.

The control grid acts like a gate, varying electron flow based on its voltage. Small voltage changes on the grid cause large changes in plate current, providing amplification.

Key Information: The primary purpose of a screen grid in a vacuum tube is to reduce grid-to-plate capacitance.

The screen grid sits between the control grid and plate, reducing capacitance between them. This prevents unwanted oscillation in RF amplifiers and was a critical advancement in radio technology.

While most new amateur radio equipment uses solid-state technology (transistors), tubes are still found in:

  • Some commercial and amateur high-power amplifiers
  • Vintage equipment that many hams still enjoy using
  • Specialty audio equipment where some prefer their characteristics

Amplifier Classes: Efficiency vs. Fidelity #

Amplifier “classes” (A, B, AB, C) describe when a transistor or tube conducts current during a signal’s waveform cycle. This classification represents the fundamental tradeoff between efficiency and signal fidelity that all amplifiers face.

Amplifier Efficiency #

Key Information: The efficiency of an RF power amplifier is determined by dividing the RF output power by the DC input power.

Efficiency=RFoutputDCinput100%\text{Efficiency} = \frac{RF_{output}}{DC_{input}} \cdot 100\%

For example, if an amplifier draws 200 watts from your power supply but produces only 100 watts of RF output, its efficiency is ( 100200=50%\frac{100}{200} = 50\% ). The remaining power is converted to heat, which explains why some amplifiers need cooling fans.

Different amplifier classes have different typical efficiencies:

  • Class A: 25-30%
  • Class AB: 40-60%
  • Class B: 60-70%
  • Class C: 70-80%

Amplifier Linearity #

Key Information: A linear amplifier preserves the input waveform in the output.

Linearity refers to how faithfully an amplifier reproduces its input signal. In a perfectly linear amplifier, the output is an exact (but larger) copy of the input. This is crucial for modes where the signal’s shape contains information, such as:

  • SSB voice operation
  • AM signals
  • Most digital modes

Now let’s look at the main amplifier classes:

Class A Amplifiers: Maximum Fidelity #

Key Information: In a Class A amplifier, the amplifying device conducts current 100% of the time.

Class A amplifiers provide excellent linearity but low efficiency (typically under 30%). Since the device conducts during the entire waveform cycle, the output faithfully reproduces the input. You’ll find Class A amplification in receiver front ends and low-level stages where signal accuracy is crucial.

Class C Amplifiers: Maximum Efficiency #

Key Information:

  • Class C amplifiers have the highest efficiency of these classes.
  • A Class C power stage is appropriate for amplifying FM signals.

Class C amplifiers conduct for less than 50% of the waveform cycle, achieving high efficiency (up to 80%) but significantly distorting the signal’s amplitude.

Since FM encodes information in frequency rather than amplitude, the distortion introduced by Class C doesn’t affect the information content, making it ideal for FM transmitters.

Class B and AB: The Middle Ground #

Class B (50% conduction) and Class AB (50-100% conduction) offer a compromise between efficiency and linearity. Most SSB transmitters use Class AB in their final stages to balance reasonable efficiency with acceptable linearity.

Oscillators: Signal Generators #

Oscillators generate the RF signals that get amplified in transmitters and used for frequency conversion in receivers:

Key Information: The basic components of a sine wave oscillator are a filter and an amplifier operating in a feedback loop.

An oscillator needs three elements:

  1. Amplification to overcome losses
  2. Frequency selection (filtering)
  3. Positive feedback that reinforces the oscillation

The frequency selection in many oscillators comes from an LC (inductor-capacitor) circuit, where the frequency is determined by the inductance and capacitance in the tank circuit (discussed in Section 1.3).

Modern transceivers often use direct digital synthesis (DDS) for frequency generation. DDS systems use digital techniques to generate analog waveforms, providing fast frequency changes with excellent stability.

Key Information: A direct digital synthesizer (DDS) is characterized by variable output frequency with the stability of a crystal oscillator.

Amplifier Stability #

Preventing unwanted oscillation is critical in amplifier design:

Key Information: The purpose of neutralizing an amplifier is to eliminate self-oscillations.

Self-oscillation occurs when some of an amplifier’s output feeds back to its input in the right phase to create a feedback loop. Neutralization techniques cancel out this unwanted feedback, typically by feeding back an equal but opposite signal.

Inductor Self-Resonance #

One last important concept for amplifier design is inductor self-resonance:

Key Information: When an inductor is operated above its self-resonant frequency, it becomes capacitive.

Every inductor has some parasitic capacitance between its windings. At a certain frequency (the self-resonant frequency), this capacitance resonates with the inductance. Above this frequency, the component behaves more like a capacitor than an inductor—a critical consideration because this unexpected behavior can cause tank circuits to malfunction and amplifiers to become unstable at higher frequencies.


These amplification principles help you understand how your equipment processes signals. Whether you’re selecting a linear amplifier for SSB operation, troubleshooting an oscillation problem, or simply wondering why your radio performs the way it does, these concepts provide valuable insights.

Next, we’ll explore how power supplies convert household electricity into the steady DC voltages your radio equipment requires.

G6A07:What are the operating points for a bipolar transistor used as a switch?
  • →Saturation and cutoff
G6A09:Which of the following describes MOSFET construction?
  • →The gate is separated from the channel by a thin insulating layer
G6A10:Which element of a vacuum tube regulates the flow of electrons between cathode and plate?
  • →Control grid
G6A12:What is the primary purpose of a screen grid in a vacuum tube?
  • →To reduce grid-to-plate capacitance
G7B08:How is the efficiency of an RF power amplifier determined?
  • →Divide the RF output power by the DC input power
G7B10:Which of the following describes a linear amplifier?
  • →An amplifier in which the output preserves the input waveform
G7B04:In a Class A amplifier, what percentage of the time does the amplifying device conduct?
  • →100%
G7B02:Which of these classes of amplifiers has the highest efficiency?
  • →Class C
G7B11:For which of the following modes is a Class C power stage appropriate for amplifying a modulated signal?
  • →FM
G7B07:Which of the following are basic components of a sine wave oscillator?
  • →A filter and an amplifier operating in a feedback loop
G7C05:Which of the following is characteristic of a direct digital synthesizer (DDS)?
  • →Variable output frequency with the stability of a crystal oscillator
G7B01:What is the purpose of neutralizing an amplifier?
  • →To eliminate self-oscillations
G6A11:What happens when an inductor is operated above its self-resonant frequency?
  • →It becomes capacitive