Radio receiver

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Early broadcast radio receiver. Truetone model from about 1940

In radio communications, a radio receiver (commonly also called a radio) is an electronic device that receives radio waves and converts the information carried by them to a usable form. It is used with an antenna. The antenna intercepts radio waves (electromagnetic waves) and converts them to tiny alternating currents which are applied to the receiver, and the receiver extracts the desired information. The receiver uses electronic filters to separate the desired radio frequency signal from all the other signals picked up by the antenna, an electronic amplifier to increase the power of the signal for further processing, and finally recovers the desired information through demodulation.

The information produced by the receiver may be in the form of sound (an audio signal), images (a video signal) or digital data.[1] A radio receiver may be a separate piece of electronic equipment, or an electronic circuit within another device. Devices that contain radio receivers include television sets, radar equipment, two-way radios, cell phones, wireless computer networks, GPS navigation devices, satellite dishes, radio telescopes, bluetooth enabled devices, garage door openers, and baby monitors.

In consumer electronics, the terms radio and radio receiver are often used specifically for receivers designed to reproduce the audio (sound) signals transmitted by radio broadcasting stations, historically the first mass-market commercial radio application.

Broadcast radio receivers[edit]

The most familiar form of radio receiver is a broadcast receiver, often just called a radio, which receives audio programs intended for public reception transmitted by local radio stations. The sound is produced either by a loudspeaker in the radio or an earphone which plugs into a jack on the radio. The radio requires electric power, provided either by batteries inside the radio or a power cord which plugs into an electric outlet. All radios have a volume control to adjust the loudness of the audio, and some type of "tuning" control to select the radio station to be received.

Tuning[edit]

Radio waves transmitted by multiple radio stations travel through the air simultaneously without interfering with each other because they have different frequencies; their carrier waves oscillate at different rates, measured in kilohertz (kHz) or megahertz (MHz). The frequency of radio stations is usually listed prominently in their advertising. In order to select a particular station to receive, the radio is adjusted ("tuned") to the frequency of the desired transmitter. In some radios this is done by the user turning a "tuning" knob until the desired station is heard in the radio's loudspeaker. In newer radios this is often done by pressing a "channel up" or "channel down" button, which causes the radio to automatically receive the next radio station it finds going up or down the frequency band. The radio has a dial or LCD display showing the frequency it is tuned to.

AM and FM[edit]

In most countries radio broadcasting is permitted using two different methods of modulation, that is, methods of adding the sound signal to the radio wave, AM and FM, on different frequency bands. In amplitude modulation (AM) the strength of the radio signal is varied by the audio signal. AM broadcasting is permitted on AM broadcast bands between 148 and 283 kHz in the low frequency (LF) range and 526 and 1706 kHz in the medium frequency (MF) range of the radio spectrum. In frequency modulation (FM) the frequency of the radio signal is varied slightly by the audio signal. FM broadcasting is permitted in the FM broadcast bands between about 65 and 108 MHz in the very high frequency (VHF) range. The exact frequency ranges vary somewhat in different countries; radios sold in each country receive the correct frequency range for that country. Most broadcast radios, called "AM/FM" radios, can receive both AM and FM bands, and have a switch to select which band to receive.

Limited AM broadcasting is also permitted in parts of the high frequency (HF) band called the shortwave band, between about 2.3 and 26 MHz. Shortwave listening requires a receiver that can receive these bands, called a shortwave receiver. At these frequencies, radio waves transmitted into the sky can reflect from a layer in the atmosphere called the ionosphere, returning to earth at transcontinental distances (this path is called "skip" or skywave) So shortwaves are used for long distance international broadcasting, often by governmental broadcasting organizations like the BBC.

Stereo[edit]

Main article: FM stereo

FM radio stations broadcast in stereophonic sound (stereo), they transmit two sound (audio) channels representing left and right microphones. There are two types of FM receiver: monaural receivers cannot reproduce the stereo sound; only stereo receivers can. In monaural FM receivers both channels are combined and reproduced by a single loudspeaker. In stereo receivers the two channels are reproduced by two separate speakers, allowing the listener to hear stereophonic sound. There is also a standard for AM stereo transmission, but few AM radio stations broadcast in stereo, so few radios are sold that are capable of producing AM stereo sound.

Reception[edit]

The signal strength (power per square meter) of radio waves decreases the farther they travel from the transmitter, so receivers can only receive a transmitter within a limited distance, depending on the power of the transmitter and the sensitivity of the receiver. AM radio waves travel as ground waves which follow the contour of the Earth and can travel beyond the horizon, so AM radio stations can be received at hundreds of miles. Due to their higher frequency, FM radio signals do not travel far beyond the visual horizon; limiting reception distance to about 40 miles (64 km), and can be blocked by hills between the transmitter and receiver. However FM radio is less susceptible to interference from radio noise (RFI, sferics, static) and has higher fidelity; better frequency response and less audio distortion, than AM. So in many countries serious music is only broadcast by FM stations, and AM stations specialize in radio news, talk radio, and sports.

Types of broadcast receiver[edit]

Radios are made in a range of styles

  • Table radio - A self-contained radio with speaker designed to sit on a table.
  • Clock radio - A bedside table radio that also includes an alarm clock. The alarm clock can be set to turn on the radio in the morning instead of an alarm, to wake the owner.
  • Tuner - A high fidelity AM/FM radio receiver in a component home audio system. It has no speakers but outputs an audio signal which is fed into the system and played through the system's speakers.
  • Portable radio - a radio powered by batteries that can be carried with a person. Radios are now often integrated with other audio sources in CD players and portable media players.
    • Boom box - a portable battery-powered high fidelity stereo sound system in the form of a box with a handle. It usually also includes a CD player in addition to an AM/FM radio. It has integral stereo speakers which can often be detached from the box and separated for better listening.
    • Transistor radio - an older term for a portable pocket-sized broadcast radio receiver. Made possible by the invention of the transistor and developed in the 1960s, transistor radios were hugely popular during the 1960s and 70s, and changed the public's listening habits.
  • Car radio - An AM/FM radio integrated into the dashboard of a vehicle, used for entertainment while driving. Virtually all cars and trucks come with car radios. It usually also includes a CD player.
  • Satellite radio receiver - subscription radio receiver that receives radio channels over an S band or L band microwave downlink signal from a geostationary direct broadcast satellite 22,000 miles above the Earth. The subscriber must pay a monthly fee. They are mostly designed as car radios.
  • Shortwave radio - This is a broadcast radio that also receives the shortwave bands. It is used for shortwave listening.
  • Crystal radio - an antique type of radio from the turn of the century that doesn't require a power source but works off the power from the radio transmitter. They are now mainly sold as educational devices for children.

Hi-Fi / Home theater[edit]

Main article: Home cinema

Today AV receivers are a common component in a high-fidelity or home-theatre system. The receiver is generally the nerve centre of a sophisticated home-theatre system providing selectable inputs for a number of different audio components like record players, CD players, tape decks and video components like VCRs, DVD players, video game consoles and television sets.

With the decline of gramophone record vinyl discs, modern receivers tend to omit inputs for phonograph turntables, which have separate requirements of their own. All other common audio/visual components can use any of the identical line-level inputs on the receiver for playback, regardless of how they are marked (the "name" on each input is mostly for the convenience of the user). For instance, a second CD player can be plugged into an "AUX" input, and will work the same as it will in the "CD" input jacks.

Some receivers can also provide digital signal processors (DSP) to give a more realistic auditory illusion of listening in a concert hall. Digital audio S/PDIF and USB connections are also common today. The home theater receiver, in the vocabulary of consumer electronics, comprises both the 'radio receiver' and other functions, such as control, sound processing, and power amplification. The standalone radio receiver is usually known in consumer electronics as a tuner.

Some modern integrated receivers can send audio out to seven loudspeakers and an additional channel for a subwoofer and often include connections for headphones. Receivers vary greatly in price, and support stereophonic or surround sound. A high-quality receiver for dedicated audio-only listening (two channel stereo) can be relatively inexpensive. Excellent ones can be purchased for $300 or less. Because modern receivers are purely electronic devices with no moving parts unlike electromechanical devices like turntables and cassette decks, they tend to offer many years of trouble-free service. In recent years, the home theater in a box has become common, which often integrates a surround-capable receiver with a DVD player. The user simply connects it to a television, perhaps other components, and a set of loudspeakers.

Other applications[edit]

Radio receivers are essential components of all systems that use radio. Besides broadcast receivers, described above, radio receivers are used in a huge variety of electronic systems in modern technology. They can be a separate piece of equipment (a radio), or a subsystem incorporated into other electronic devices. A transceiver is a transmitter and receiver combined in one unit. Below is a list of a few of the most common types, organized by function

  • Two-way (duplex) voice communications - A two-way radio is an audio transceiver, a receiver and transmitter in the same device, used for bidirectional person-to-person voice communication. The radio link may be half-duplex, using a single radio channel in which only one radio can transmit at a time. so different users take turns talking, pressing a push to talk button on their radio which switches on the transmitter. Or the radio link may be full duplex, a bidirectional link using two radio channels so both people can talk at the same time, as in a cell phone.
    • Cellphone - a portable telephone that is connected to the telephone network by radio signals exchanged with a local antenna called a cell tower. Cellphones have highly automated digital receivers working in the UHF and microwave band that receive the incoming side of the duplex voice channel, as well as a control channel that handles dialing calls and switching the phone between cell towers. They usually also have several other receivers that connect them with other networks: a WiFi modem, a bluetooth modem, and a GPS receiver. The cell tower has sophisticated multichannel receivers that receive the signals from many cell phones simultaneously.
    • Cordless phone - a landline telephone in which the handset is portable and communicates with the rest of the phone by a short range duplex radio link, instead of being attached by a cord. Both the handset and the base station have radio receivers operating in the UHF band that receive the short range bidirectional duplex radio link.
    • Citizens band radio - a limited power half-duplex two-way radio operating in the 27 MHz band that can be used without a license. They are often installed in vehicles and used by truckers and delivery services.
    • Walkie-talkie - a handheld short range half-duplex two-way radio that communicates on VHF or UHF bands with other walkie-talkies.
Handheld scanner
    • Scanner - a receiver that continuously monitors multiple frequencies or radio channels by stepping through the channels repeatedly, listening briefly to each channel for a transmission. When a transmitter is found the receiver stops at that channel. Scanners are used to monitor emergency police, fire, and ambulance frequencies, as well as other two way radio frequencies such as citizens band. Scanning capabilities have also become a standard feature in communications receivers, walkie-talkies, and other two-way radios.
Modern communications receiver, ICOM RC-9500
  • One-way (simplex) voice communications
Baby monitor. The receiver is on the left
    • Baby monitor - this is a cribside appliance for mothers of infants that transmits the baby's sounds to a receiver carried by the mother, so she can monitor the baby while she is in other parts of the house. Many baby monitors now have video cameras to show a picture of the baby.
  • Data communications
    • Wireless (WiFi) modem - an automated short range digital data transmitter and receiver on a portable wireless device that communicates by microwaves with a nearby access point, a router or gateway, connecting the portable device with a local computer network (WLAN) to exchange data with other devices.
    • Bluetooth modem - a very short range (up to 10 m) 2.4-2.83 GHz data transceiver on a portable wireless device used as a substitute for a wire or cable connection, mainly to exchange files between portable devices and connect cellphones and music players with wireless earphones.
    • Microwave relay - a long distance high bandwidth point-to-point data transmission link consisting of a dish antenna and transmitter that transmits a beam of microwaves to another dish antenna and receiver. Since the antennas must be in line-of-sight, distances are limited by the visual horizon to 30-40 miles. Microwave links are used for private business data, wide area computer networks (WANs), and by telephone companies to transmit distance phone calls and television signals between cities.
  • Remote control - Remote control receivers are automated receivers in autonomous (unmanned) devices such as drone vehicles that receive digital commands that control the device. Remote control systems often also incorporate a telemetry channel to transmit data on the state of the controlled device back to the controller.
    • Drone receiver - unmanned drone aircraft are controlled by encrypted commands from a satellite.
    • Radio controlled model receiver - A receiver used to receive commands transmitted from a nearby handheld controller to steer radio-controlled toy cars, boats, airplanes, and helicopters. Usually operates on the 2.4 GHz band.
    • Garage door opener - Residential garage doors are opened and closed by the owner pressing a button on a transmitter in his car. The device transmits a short-range 2.45 GHz coded signal to a receiver in the garage door opener. The digital signal is encrypted and changes with each use, to prevent thieves from recording and copying it.
    • Keyless lock - most modern cars have keyless entry systems. To unlock the door, instead of inserting a key in a lock, the owner presses a button on a small transmitter on a keyring, which transmits a short range 2.45 GHz coded signal to a receiver in the car.
  • Radiolocation - This is the use of radio waves to determine the location or direction of an object.
    • Radar - a device that transmits a narrow beam of microwaves which reflect from a target back to a receiver, used to locate objects such as aircraft, spacecraft, missiles, ships or land vehicles. The reflected waves from the target are received by a receiver usually connected to the same antenna, indicating the direction to the target. Widely used in aviation, shipping, navigation, weather forecasting, space flight, vehicle collision avoidance systems, and the military.
    • Global navigation satellite system (GNSS) receiver, such as a GPS receiver used with the US Global Positioning System - the most widely used electronic navigation device. A sophisticated automated digital receiver that receives simultaneous data signals at 1.575 and 1.227 GHz from several satellites in low Earth orbit. Using extremely precise time signals it calculates the distance to the satellites, and from this the location on Earth (longitude and latitude and altitude) of the receiver. GNSS receivers are sold as portable devices, and are also incorporated in cell phones, vehicles and military weapons, even artillery shells.
    • VOR receiver - navigational instrument on an aircraft that uses the VHF signal from VOR navigational beacons between 108 to 117.95 MHz to determine the direction to the beacon very accurately, for air navigation.
    • Wild animal tracking receiver - a receiver with a directional antenna used to track wild animals which have been tagged with a small VHF transmitter, for wildlife management purposes.

How receivers work[edit]

Symbol for an antenna

A radio receiver is connected to an antenna which converts the energy from the incoming radio wave into a tiny radio frequency AC voltage which is applied to the receiver's input. An antenna typically consists of an arrangement of metal conductors. The oscillating electric and magnetic fields of the radio wave push the electrons in the antenna back and forth, creating an oscillating voltage.

The antenna may be enclosed inside the receiver's case, as with the ferrite loop antennas of AM radios and the flat inverted F antenna of cell phones; attached to the outside of the receiver, as with whip antennas used on FM radios, or mounted separately and connected to the receiver by a cable, as with rooftop television antennas and satellite dishes.

Filtering, amplification, and demodulation[edit]

Although they may have additional functions, almost all radio receivers perform three basic functions on the signal from the antenna; filtering, amplification, and demodulation:[2]

Symbol for a bandpass filter used in block diagrams of radio receivers
  • Bandpass filtering: The receiver uses a circuit called a bandpass filter to select the radio signal of the desired radio transmitter from the multiple radio signals picked up by the antenna. In radio communication, radio waves from many transmitters pass through the air simultaneously without interfering with each other because they have different frequencies, that is, the carrier wave of each transmitter oscillates at a different rate, measured in megahertz (MHz) or gigahertz (GHz). See graphs below. Vin shows the voltage from the antenna. The antenna typically receives a broad range of frequencies, so the oscillating voltage from the antenna is a composite that contains signals from other transmitters at other frequencies (S2, S3, and S4) and radio noise (RFI or static) from the atmosphere (N), in addition to the desired radio station's signal (S1), superposed on each other. To separate out the desired radio transmission, the bandpass filter allows the frequency of the radio transmission to pass though, and blocks signals at all other frequencies.
The frequency spectrum of a typical radio signal from an AM or FM radio transmitter. It consists of a strong signal (C) at the carrier wave frequency fC, with the modulation contained in narrow frequency bands called sidebands (SB) just above and below the carrier.
How the bandpass filter selects a single radio signal S1 from all the radio signals received by the antenna. From top, the graphs show the voltage from the antenna applied to the filter Vin, the transfer function of the filter T, and the voltage at the output of the filter Vout as a function of frequency f. The transfer function T is the amount of signal that gets through the filter at each frequency:
The bandpass filter consists of one or more resonant circuits (tuned circuits). A simple resonant circuit is composed of an inductor (coil of wire) and a capacitor connected together. It has a natural resonant frequency similar to a tuning fork, which is set equal to the frequency of the desired radio station. The resonant circuit is connected between the signal line and ground. When the incoming radio signal is at the resonant frequency, it sets up sympathetic oscillations (resonance) in the resonant circuit, giving it a high impedance, so the radio signal from the desired station is passed on to the following stages of the receiver. At all other frequencies the tuned circuit has low impedance, so signals at these frequencies are conducted to ground and not passed on.
    • Bandwidth and selectivity: See graphs. The information (modulation) in a radio transmission is contained in two narrow bands of frequencies called sidebands (SB) on either side of the carrier frequency (C), so the filter has to pass a band of frequencies, not just a single frequency. The band of frequencies received by the receiver is called its passband (PB), and the width of the passband in kilohertz is called the bandwidth (BW). The bandwidth of the filter must be wide enough to allow the sidebands through without distortion, but narrow enough to block any interfering transmissions on adjacent frequencies (such as S2 in the diagram). The ability of the receiver to reject unwanted radio stations near in frequency to the desired station is an important parameter called selectivity determined by the filter. In modern receivers quartz crystal, ceramic resonator, or surface acoustic wave (SAW) filters are often used in place of tuned circuits, which have sharper selectivity.
    • Tuning: Some receivers (for example those in garage door openers and radar sets) are fixed to receive a single frequency, but most receivers (such as AM, FM, and television broadcast receivers), are adjustable so they can receive transmitters on different frequencies. Tuning is the process of adjusting the frequency of the receiver's passband to the frequency of the desired radio transmitter. In many modern receivers such as television sets this is accomplished automatically by the user pressing a "channel up" or "channel down" button, but others use the traditional method of turning a "tuning" knob until the desired station is heard in the speaker. Tuning a radio has similarities to tuning a musical instrument to resonate with another. Turning the tuning knob changes the resonant frequency of the tuned circuit. When the resonant frequency is equal to the radio transmitter's frequency the tuned circuit oscillates in sympathy, passing the signal on to the rest of the receiver. The range of frequencies a receiver can be tuned to is called its tuning range. For example, FM receivers cover the FM band of frequencies, from 88 MHz to 108 MHz in the US.
Symbol for an amplifier
  • Amplification: The power of the radio waves picked up by a receiving antenna decreases with the square of its distance from the transmitting antenna. Even with the powerful transmitters used in radio broadcasting stations, if the receiver is more than a few miles from the transmitter the power intercepted by the receiver's antenna is very small, in the range of microwatts, nanowatts or picowatts. In order to increase the power of the signal to a level capable of driving the loudspeaker or earphone, electric power from a battery or wall socket is used to amplify the signal in a circuit called an amplifier.
In the amplifier circuits transistors perform the actual amplification. A transistor functions somewhat similarly to a water valve. In it, the weak current from the radio signal controls a stronger current from the power supply. Receivers usually have several stages of amplification: the radio signal from the bandpass filter is amplified to make it powerful enough to drive the demodulator, then the audio signal from the demodulator is amplified to make it powerful enough to operate the speaker. The degree of amplification of a radio receiver is measured by a parameter called its sensitivity, which is the minimum signal strength of a station at the antenna, measured in microvolts, necessary to receive the signal clearly, with a certain signal-to-noise ratio. Since it is easy to amplify a signal to any desired degree, the limit to the sensitivity of many modern receivers is not the degree of amplification but random electronic noise present in the circuit, which can drown out a weak radio signal.
Symbol for a demodulator
  • Demodulation: After the radio signal is filtered and amplified, the receiver must extract the information-bearing modulation signal from the modulated radio frequency carrier wave. This is done by a circuit called a demodulator (detector). Radio communication systems use several different ways of adding the modulation signal to the radio frequency carrier wave at the transmitter, and receivers are classified by which type of modulation they receive:
    • AM receivers receive amplitude modulation (AM) in which the amplitude (strength) of the radio wave is varied by the modulation signal.
    • FM receivers receive frequency modulation (FM) in which the frequency of the radio wave is varied by the modulation signal.
    • FSK receivers receive frequency shift keying (FSK) modulation, in which the frequency of the radio wave is switched between two frequencies representing the binary digits 0 and 1. These are used in wireless devices to transmit digital information.
Many other types of modulation are also used for specialized purposes. These different types of modulation require different demodulation circuits. Broadcast radio receivers typically receive both AM and FM modulation.

The modulation signal output by the demodulator is usually amplified to increase its strength, then the information is converted back to a human-usable form by some type of transducer. An audio signal, representing sound, as in a broadcast radio, is converted to sound waves by an earphone or loudspeaker. A video signal, representing moving images, as in a television receiver, is converted to light by a display. Digital data, as in a wireless modem, is applied as input to a computer or microprocessor, which interacts with human users.

AM demodulation[edit]

Main article: Envelope detector
Envelope detector circuit
How an envelope detector works
The easiest type of demodulation to understand is AM demodulation, used in AM radios to recover the audio modulation signal, which represents sound and is converted to sound waves by the radio's speaker. It is accomplished by a circuit called an envelope detector (see circuit), consisting of a diode (D) with a bypass capacitor (C) across its output.
See graphs. The amplitude modulated radio signal from the tuned circuit is shown at (A). The rapid oscillations are the radio frequency carrier wave. The audio signal (the sound) is contained in the slow variations (modulation) of the amplitude (size) of the waves. If it was applied directly to the speaker, this signal cannot be converted to sound, because the audio excursions are the same on both sides of the axis, averaging out to zero, which would result in no net motion of the speaker's diaphragm. (B) When this signal is applied as input VI to the detector, the diode (D) conducts current in one direction but not in the opposite direction, thus allowing through pulses of current on only one side of the signal. In other words, it rectifies the AC current to a pulsing DC current. The resulting voltage VO applied to the load RL no longer averages zero; its peak value is proportional to the audio signal. (C) The bypass capacitor (C) is charged up by the current pulses from the diode, and its voltage follows the peaks of the pulses, the envelope of the audio wave. It performs a smoothing (low pass filtering) function, removing the radio frequency carrier pulses, leaving the low frequency audio signal to pass through the load RL. The audio signal is amplified and applied to earphones or a speaker.

Tuned radio frequency (TRF) receiver[edit]

Block diagram of TRF receiver

In the simplest type of radio receiver, called a tuned radio frequency (TRF) receiver, the three functions above are performed consecutively:[3] (1) the mix of radio signals from the antenna is filtered to extract the signal of the desired transmitter; (2) this oscillating voltage is sent through a radio frequency (RF) amplifier to increase its strength to a level sufficient to drive the demodulator; (3) the demodulator recovers the modulation signal (which in broadcast receivers is an audio signal, a voltage oscillating at an audio frequency rate representing the sound waves) from the modulated radio carrier wave; (4) the modulation signal is amplified further in an audio amplifier, then is applied to a loudspeaker or earphone to convert it to sound waves.

Single transistor TRF receiver circuit, an example of a very simple radio.

The single transistor TRF receiver circuit (right) shows how a very simple radio works. The inductor L and capacitor C1 form a tuned circuit that passes the signal from the desired transmitter to the transistor, and conducts other radio signals to ground. The transistor Q functions as both a demodulator and audio amplifier (there is no RF amplifier). The base-emitter junction of the transistor acts as a diode that conducts current only during the positive half-cycles of the RF signal, thus rectifying the current to a pulsing DC current. This small current controls a larger current from the battery B through the collector of the transistor which powers the loudspeaker SP. The collector current is an amplified copy of the base current : . The capacitor C2 performs a smoothing function, acting as a low pass filter to remove the radio frequency pulses of carrier, leaving the audio signal to pass through the speaker.

Although the TRF receiver is used in a few applications, it has practical disadvantages which make it inferior to the superheterodyne receiver below, which is used in most applications.[3] The drawbacks stem from the fact that in the TRF the filtering, amplification, and demodulation are done at the high frequency of the incoming radio signal. The bandwidth of a filter increases with its center frequency, so as the TRF receiver is tuned to different frequencies its bandwidth varies. Most important, the increasing congestion of the radio spectrum requires that radio channels be spaced very close together in frequency. It is extremely difficult to build filters operating at radio frequencies that have a small enough bandwidth to separate closely spaced radio stations. TRF receivers typically must have many cascaded tuning stages to achieve adequate selectivity. The Advantages section below describes how the superheterodyne receiver overcomes these problems.

The superheterodyne design[edit]

Block diagram of a superheterodyne receiver. The parts of the circuit colored red (known as the RF front end) operate at the original incoming radio frequency; those colored green operate at the intermediate frequency (IF); while those colored blue operate at audio frequency. The dotted line indicates that the RF filter and local oscillator must be tuned in tandem.
How a superheterodyne radio works. The incoming radio signal from the antenna (top) consists of the desired radio signal S1 plus others at different frequencies. The RF filter (2nd graph) removes any signal such as S2 at the image frequency LO - IF, which would otherwise pass through the IF filter and interfere. The output of the filter is applied to the mixer along with a local oscillator signal (LO) (3rd graph). In the mixer the signal S1 at frequency RF combines with the LO frequency to create a heterodyne at the difference between these frequencies, the intermediate frequency (IF). The unwanted signals create heterodynes at other frequencies. The IF bandpass filter (4th graph) removes the heterodynes created by the other signals, leaving the desired signal (5th graph) which is demodulated.

The superheterodyne receiver, invented in 1918 by Edwin Armstrong[4] is the design used in almost all modern receivers[5][3][6][7] except a few specialized applications.

In the superheterodyne, the radio frequency signal from the antenna is shifted down to a lower "intermediate frequency" (IF), before it is processed.[8][9][10][11] An unmodulated sinusoidal signal LO generated by a local oscillator (LO) in the receiver is mixed with the incoming radio frequency signal RF from the antenna in a nonlinear transistor or diode called the "mixer". The result at the output of the mixer is a heterodyne or beat frequency at the difference between these two frequencies: IF = |RF − LO|. This is similar to the way two musical notes at different frequencies played together produce a beat note at the difference between their frequencies. This lower frequency is called the intermediate frequency (IF). The IF also contains the modulation (sidebands) that was present in the original RF signal. This signal is bandpass filtered and amplified as in the TRF receiver, by the IF filter and amplifier,[6] then is demodulated in a detector, producing an audio signal.

The receiver is easy to tune; in order to receive a different frequency it is only necessary to change the local oscillator frequency LO. The frequency received is LO + IF. The rest of the receiver after the mixer operates at the fixed intermediate frequency (IF) so the IF bandpass filter does not have to be adjusted to different frequencies, as the bandpass filter in the TRF receiver did. The fixed frequency allows modern receivers to use sophisticated quartz crystal, ceramic resonator, or surface acoustic wave (SAW) IF filters that have very high Q factors, to improve selectivity.

RF filter and image response[edit]

The RF filter on the front end of the receiver is needed to prevent interference from any radio signals at the image frequency. When the incoming radio signal RF is mixed with the local oscillator signal LO, two new frequencies (heterodynes) are created,[11] one at the sum RF + LO, and one at the difference RF − LO of the frequencies. Because of this, without an input filter the receiver can receive incoming RF signals at two different frequencies,[12][7][11][13] one above the LO frequency: RF1 = LO + IF, and one below the LO frequency: RF2 = LO − IF. The receiver can be designed to receive on either of these two frequencies; the former is called low-side injection because the LO signal frequency is below the received frequency, while the latter is high-side injection.[11] Whichever is chosen, the other frequency is called the image frequency. If the receiver is designed to receive on LO + IF, for example, any other radio station or radio noise on the frequency LO − IF will also produce a heterodyne at the IF and therefore will pass through the IF filter, interfering with the desired signal. Therefore, the superheterodyne requires a bandpass filter, the RF filter, on the input to reject this image frequency.[7] The RF filter also serves to limit the bandwidth applied to the RF amplifier, preventing it from being overloaded (saturated) by strong out-of-band signals. This filter does not need great selectivity, but as the receiver is tuned to different frequencies it must "track" in tandem with the LO.

Advantages[edit]

The superheterodyne design is superior to other receivers for these reasons:[8][12]

  • At the high frequencies used for radio transmission, signal processing circuitry often performs poorly.[3] Amplifying devices have little gain, and are prone to instability and parasitic oscillation.[8] At the microwave frequencies used in modern wireless devices, ordinary circuits using capacitors and inductors must be replaced with cumbersome high frequency techniques such as striplines and waveguides. By shifting the signal down to a lower intermediate frequency, the amplification, filtering and detection can be done at a more convenient frequency where the electronics works better.
  • The different frequencies of different stations are all converted to the same frequency, the IF, for filtering, so the bandwidth and gain of the receiver is constant over its frequency range. To tune the receiver to a different frequency, only the frequency of the local oscillator LO needs to be changed. The rest of the receiver after the mixer operates at a fixed frequency, the IF. The TRF receiver (as well as other types of receiver described in the History section below) require that the bandpass filter (tuned circuit) be adjustable to different frequencies. The bandwidth of a filter of a given Q factor is proportional to its center frequency, so the bandwidth of these receivers increases as they are tuned to higher frequencies.[6] It is also easier to build tunable oscillators than tunable electronic filters. In an analog television set, for example, if the superheterodyne design was not used, all the complicated filters that separate out the luminance carrier, chroma carrier and the audio subcarrier from the television signal would have to be made adjustable, and retuned each time the channel was changed.
  • The total amplification of the receiver is divided between three amplifiers at different frequencies; the RF, IF, and audio amplifier. This reduces problems with feedback and parasitic oscillations that are encountered in receivers where most of the amplifier stages operate at the same frequency, as in the TRF receiver.[8]
  • The most important advantage is that better selectivity can be achieved by doing the filtering at the lower intermediate frequency.[3][6][8] One of the most important parameters of a receiver is its bandwidth, the band of frequencies it accepts. In order to reject nearby interfering stations or noise, a narrow bandwidth is required. In all known filtering techniques, the bandwidth of the filter increases in proportion with the frequency, so by performing the filtering at the lower IF, rather than the frequency of the original radio signal RF, a narrower bandwidth can be achieved. Modern FM and television broadcasting, cellphones and other communications services, with their narrow channel widths, would be impossible without the superheterodyne.[6]

Terminology[edit]

As the superheterodyne is the most developed and widely used radio circuit, a terminology has grown up around it:

  • Balanced mixer - An improved type of mixer circuit in which the local oscillator frequency or input signal frequency (or both in a double balanced mixer) are cancelled in the output to the IF filter. This reduces the unwanted frequencies which the IF filter must remove.
  • Beat frequency oscillator (BFO) - This is an electronic oscillator which is only found in communications receivers, used in the reception of radiotelegraph (CW) or single-sideband modulation (SSB). It produces a fixed frequency offset from the IF which is mixed with the IF in the demodulator. The IF and BFO frequencies produce a heterodyne (beat) in the audio range which sounds like a musical tone in the speaker. In CW the "dots" and "dashes" of the Morse code are audible as beeps.
  • Converter - in many superhet circuits the same tube or transistor functions as both the local oscillator and the mixer. This is called a converter.
  • First detector, second detector - the mixer tube or transistor is sometimes called the "first detector", while the demodulator that extracts the modulation from the IF signal is called the "second detector". In a dual-conversion superhet there are two mixers, so the demodulator is called the "third detector".
  • IF strip - The IF filter and amplifier usually consists of several tuned amplifier stages as in the TRF receiver. This is called the IF strip.
  • Image frequency - a frequency on the opposite side of the local oscillator frequency LO from the received radio signal, which the receiver can also receive. The RF filter on the input is needed to block any signal at this frequency to prevent interference. In the usual low side injection receiver the incoming signal is at LO + IF and the image frequency is LO − IF.
  • Local oscillator (LO) - part of every superheterodyne circuit, a radio frequency electronic oscillator which produces a signal that mixes with the incoming radio signal from the antenna in the mixer to generate the intermediate frequency.
  • RF front end - refers to all the components of the receiver up to and including the mixer; all the parts that process the signal at the original incoming radio frequency. In the block diagram above the RF front end components are colored red.

Dual-conversion superheterodyne[edit]

Dual conversion superheterodyne block diagram

In choosing the intermediate frequency (IF) used in a superhet, there is a tradeoff between image rejection and selectivity.[3][7][11] Since the separation between the desired frequency and the image is 2IF, the higher the IF, the farther apart these two frequencies are, and the better the image rejection the RF filter can achieve. However, the lower the IF, the narrower the bandwidth the IF filter can achieve, and the better the selectivity. In order to achieve both good image rejection and selectivity, many modern superhet receivers use two intermediate frequencies; this is called a dual-conversion or double-conversion superheterodyne.[3] The incoming RF signal is first mixed with one local oscillator signal in the first mixer to convert it to a high IF frequency, to allow efficient filtering out of the image frequency, then this first IF is mixed with a second local oscillator signal in a second mixer to convert it to a low IF frequency for good bandpass filtering. Some receivers even use triple-conversion.

Automatic gain control (AGC)[edit]

The signal strength (amplitude) of the radio signal from a receiver's antenna varies drastically, by orders of magnitude, depending on how far away the radio transmitter is, how powerful it is, and propagation conditions along the path of the radio waves.[14] The strength of the signal received from a given transmitter varies with time due to changing propagation conditions of the path through which the radio wave passes, such as multipath interference; this is called fading.[14][3] In an AM receiver the amplitude of the audio signal from the detector, and the sound volume, is proportional to the amplitude of the radio signal, so fading causes variations in the volume. In addition as the receiver is tuned between strong and weak stations, the volume of the sound from the speaker would vary drastically. Without an automatic system to handle it, in an AM receiver constant adjustment of the volume control would be required.

With other types of modulation like FM or FSK the amplitude of the modulation does not vary with the radio signal strength, but in all types the demodulator requires a certain range of signal amplitude to operate properly.[3][15] Insufficient signal amplitude will cause an increase of noise in the demodulator, while excessive signal amplitude will cause amplifier stages to overload (saturate), causing distortion (clipping) of the signal.

Therefore, almost all modern receivers include a feedback system which monitors the average level of the radio signal at the detector, and adjusts the gain of the amplifiers to give the optimum signal level for demodulation.[3][15][14] This is called automatic gain control (AGC). AGC can be compared to the dark adaptation mechanism in the human eye; on entering a dark room the gain of the eye is increased by the iris opening.[14] In its simplest form an AGC system consists of a rectifier which converts the RF signal to a varying DC level, a lowpass filter to smooth the variations and produce an average level.[15] This is applied as a control signal to an earlier amplifier stage, to control its gain. In a superheterodyne receiver AGC is usually applied to the IF amplifier, and there may be a second AGC loop to control the gain of the RF amplifier to prevent it from overloading, too.

In certain receiver designs such as modern digital receivers, a related problem is DC offset of the signal. This is corrected by a similar feedback system.

History[edit]

Radio waves were first identified in German physicist Heinrich Hertz's 1887 series of experiments to prove James Clerk Maxwell's electromagnetic theory. Hertz used spark-excited dipole antennas to generate the waves and micrometer spark gaps attached to dipole and loop antennas to detect them.[16][17][18] These primitive devices are more accurately described as radio wave sensors, not "receivers", as they could only detect radio waves within about 100 feet of the transmitter, and were not used for communication but instead as laboratory instruments in scientific experiments.

Spark era[edit]

Main article: Wireless telegraphy
Guglielmo Marconi who built the first radio receivers, with his early spark transmitter (right) and coherer receiver (left) from the 1890s. The receiver records the Morse code on paper tape
Generic block diagram of an unamplified radio receiver from the wireless telegraphy era[19]
Example of transatlantic radiotelegraph message recorded on paper tape by a siphon recorder at RCA's New York receiving center in 1920. The translation of the Morse code is given below the tape.

The earliest radio communication systems, used during the first three decades of radio, 1887-1917, called the wireless telegraphy or "spark" era, used spark gap transmitters which generated radio waves by discharging a capacitance through an electric spark.[20][21][22] Each spark produced a transient pulse of radio waves consisting of a sinusoidal wave which decreased rapidly exponentially to zero.[16][18] Spark transmitters produced strings of these damped waves, and could not generate the sinusoidal continuous waves which are modulated to carry sound in modern AM and FM transmission. Thus spark transmitters could not transmit audio (sound), and instead transmitted information by radiotelegraphy; the transmitter was switched on and off rapidly by the operator using a telegraph key, creating different length pulses of these damped radio waves ("dots" and "dashes") to spell out text messages in Morse code.[18][21]

Therefore, the first radio receivers did not have to demodulate the radio signal - extract an audio signal from it as modern receivers do - just detect the presence or absence of the radio signal, and produce a sound in the earphone during the "dots" and "dashes" of the Morse code.[18] The device which did this was called a "detector". Since there were no amplifying devices during this era, the sensitivity of the receiver mostly depended on the detector, and many different detector devices were tried. Radio receivers during the spark era (see diagram) consisted of these parts:[3]

  • An antenna, to intercept the radio waves and convert them to tiny radio frequency electric currents.
  • A resonant circuit (tuned circuit), consisting of a capacitor connected to a coil of wire (an inductor), which acted as a bandpass filter to select the desired signal out of all the signals picked up by the antenna. Either the capacitor or inductor was adjustable to tune the receiver to the frequency of different transmitters. The earliest receivers, before 1897, did not have tuned circuits, they responded to all radio signals picked up by their antennas, so they had little frequency-discriminating ability and received any transmitter in their vicinity.[23] Most receivers used a pair of tuned circuits with their coils magnetically coupled, called a resonant transformer (oscillation transformer) or "loose coupler".
  • A detector, which produced a pulse of DC current for each damped wave received.
  • An indicating device such as an earphone, which converted the pulses of current into sound waves. The first receivers used an electric bell instead. Later receivers in commercial wireless systems used a Morse siphon recorder,[16] which consisted of an ink pen mounted on a needle swung by an electromagnet (a galvanometer) which drew a line on a moving paper tape. Each string of damped waves constituting a Morse "dot" or "dash" caused the needle to swing over, creating a displacement of the line, which could be read off the tape. With such an automated receiver a radio operator didn't have to continuously monitor the receiver.

The signal from the spark gap transmitter consisted of damped waves repeated at an audio frequency rate, from 120 to perhaps 4000 per second, so in the earphone the signal sounded like a musical tone or buzz, and the Morse code "dots" and "dashes" sounded like beeps.

The first person to use radio waves for communication was Guglielmo Marconi.[21][24] Marconi invented little himself, but he was first to believe that radio could be a practical communication medium, and singlehandedly developed the first wireless telegraphy systems, transmitters and receivers, beginning in 1895,[24] mainly by improving technology invented by others.[21][25][26][27] [28][29] Oliver Lodge and Alexander Popov were also experimenting with similar radio wave receiving apparatus at the same time in 1895,[26][30] but they are not known to have transmitted Morse code during this period,[21][24] just strings of random pulses. Therefore, Marconi is usually given credit for building the first radio receivers.

Coherer receiver[edit]

Main article: Coherer
Coherer from 1904 as developed by Marconi.
One of Marconi's first coherer receivers, used in his "black box" demonstration at Toynbee Hall, London, 1896. The coherer is at right, with the "tapper" just behind it, The relay is at left, batteries are in background
A typical commercial radiotelegraphy receiver from the first decade of the 20th century. The coherer (right) detects the pulses of radio waves, and the "dots" and "dashes" of Morse code were recorded in ink on paper tape by a siphon recorder (left) and transcribed later.

The first radio receivers invented by Marconi, Oliver Lodge and Alexander Popov in 1894-5 used a primitive radio wave detector called a coherer, invented in 1890 by Edouard Branly and improved by Lodge and Marconi.[16][21][23][26][30][31][32] The coherer was a glass tube with metal electrodes at each end, with loose metal powder between the electrodes.[16][21][33] It initially had a high resistance. When a radio frequency voltage was applied to the electrodes, its resistance dropped and it conducted electricity. In the receiver the coherer was connected directly between the antenna and ground. In addition to the antenna, the coherer was connected in a DC circuit with a battery and relay. When the incoming radio wave reduced the resistance of the coherer, the current from the battery flowed through it, turning on the relay to ring a bell or make a mark on a paper tape in a siphon recorder. In order to restore the coherer to its previous nonconducting state to receive the next pulse of radio waves, it had to be tapped mechanically to disturb the metal particles.[16][21][30][34] This was done by a "decoherer", a clapper which struck the tube, operated by an electromagnet powered by the relay.

The coherer is an obscure antique device, and even today there is some uncertainty about the exact physical mechanism by which the various types worked.[16][25][35] However it can be seen that it was essentially a bistable device, a radio-wave-operated switch, and so it did not have the ability to rectify the radio wave to demodulate the later amplitude modulated (AM) radio transmissions that carried sound.[16][25]

In a long series of experiments Marconi found that by using an elevated wire monopole antenna instead of Hertz's dipole antennas he could transmit longer distances, beyond the curve of the Earth, demonstrating that radio was not just a laboratory curiosity but a commercially viable communication method. This culminated in his historic transatlantic wireless transmission on December 12, 1901 from Poldhu, Cornwall to St. John's, Newfoundland, a distance of 3500 km (2200 miles), which was received by a coherer.[25][29] However the usual range of coherer receivers even with the powerful transmitters of this era was limited to a few hundred miles.

The coherer remained the dominant detector used in early radio receivers for about 10 years,[33] until replaced by the crystal detector and electrolytic detector around 1907. In spite of much development work, it was a very crude unsatisfactory device.[16][21] It was not very sensitive, and also responded to impulsive radio noise (RFI), such as nearby lights being switched on or off, as well as to the intended signal.[21][33] Due to the cumbersome mechanical "tapping back" mechanism it was limited to a data rate of about 12-15 words per minute of Morse code, while a spark-gap transmitter could transmit Morse at up to 100 WPM with a paper tape machine.[36][37]

Other early detectors[edit]

The coherer's poor performance motivated a great deal of research to find better radio wave detectors, and many were invented. Some strange devices were tried; researchers experimented with using frog legs and even a human brain from a cadaver as detectors.[16][38]

By the first years of the 20th century, experiments in using amplitude modulation (AM) to transmit sound by radio (radiotelephony) were being made. So a second goal of detector research was to find detectors that could demodulate an AM signal, extracting the audio (sound) signal from the radio carrier wave. It was found by trial and error that this could be done by a detector that exhibited "asymmetrical conduction"; a device that conducted current in one direction but not in the other.[39] This rectified the alternating current radio signal, removing one side of the carrier cycles, leaving a pulsing DC current whose amplitude varied with the audio modulation signal. When applied to an earphone this would reproduce the transmitted sound.

Below are the detectors that saw wide use before vacuum tubes took over around 1920.[40][41] All except the magnetic detector could rectify and therefore receive AM signals:

Magnetic detector
  • Magnetic detector - Developed by Guglielmo Marconi in 1902 from a method invented by Ernest Rutherford and used by the Marconi Co. until it adopted the Audion vacuum tube around 1912, this was a mechanical device consisting of an endless band of iron wires which passed between two pulleys turned by a windup mechanism.[42][43][44][45] The iron wires passed through a coil of fine wire attached to the antenna, in a magnetic field created by two magnets. The hysteresis of the iron induced a pulse of current in a sensor coil each time a radio signal passed through the exciting coil. The magnetic detector was used on shipboard receivers due to its insensitivity to vibration. One was part of the wireless station of the RMS Titanic which was used to summon help during its famous 15 April 1912 sinking.[46]
Electrolytic detector
  • Electrolytic detector ("liquid barretter") - Invented in 1903 by Reginald Fessenden, this consisted of a thin silver-plated platinum wire enclosed in a glass rod, with the tip making contact with the surface of a cup of nitric acid.[16][43][47][48][49] The electrolytic action caused current to be conducted in only one direction. The detector was used until about 1910.[43] Electrolytic detectors that Fessenden had installed on US Navy ships received the first AM radio broadcast on Christmas Eve, 1906, an evening of Christmas music transmitted by Fessenden using his new alternator transmitter.[16]
Early Fleming valve.
Marconi valve receiver for use on ships had two Fleming valves (top) in case one burned out. It was used on the RMS Titanic.
  • Thermionic diode (Fleming valve) - The first vacuum tube, invented in 1904 by John Ambrose Fleming, consisted of an evacuated glass bulb containing two electrodes: a cathode consisting of a hot wire filament similar to that in an incandescent light bulb, and a metal plate anode.[23][50][51][52] Fleming, a consultant to Marconi, invented the valve as a more sensitive detector for transatlantic wireless reception. The filament was heated by a separate current through it and emitted electrons into the tube by thermionic emission, an effect which had been discovered by Thomas Edison. The radio signal was applied between the cathode and anode. When the anode was positive, a current of electrons flowed from the cathode to the anode, but when the anode was negative the electrons were repelled and no current flowed. The Fleming valve was used to a limited extent but was not popular because it was expensive, had limited filament life, and was not as sensitive as electrolytic or crystal detectors.[50]
A galena cat's whisker detector from a 1920s crystal radio
  • Crystal detector (cat's whisker detector) - invented around 1904-1906 by Henry H. C. Dunwoody and Greenleaf Whittier Pickard, based on Karl Ferdinand Braun's 1874 discovery of "asymmetrical conduction" in crystals, these were the most successful and widely used detectors before the vacuum tube era[39][40] and gave their name to the crystal radio receiver (below).[43][53][54] One of the first semiconductor electronic devices, a crystal detector consisted of a pea-sized pebble of a crystalline semiconductor mineral such as galena (lead sulfide) whose surface was touched by a fine springy metal wire mounted on an adjustable arm.[23] This functioned as a primitive diode which conducted electric current in only one direction. In addition to their use in crystal radios, carborundum crystal detectors were also used in some early vacuum tube radios because they were more sensitive than the vacuum tube grid-leak detector.

During the vacuum tube era, the term "detector" changed from meaning a radio wave detector to mean a demodulator, a device that could extract the audio modulation signal from a radio signal. That is its meaning today.

Tuning[edit]

The word "tuning" means adjusting the frequency of the receiver (its passband) to the frequency of the desired radio transmitter, to receive the desired radio transmission. The first receivers had no tuned circuit, the detector was connected directly between the antenna and ground. Due to the lack of any frequency selective components besides the antenna, the bandwidth of the receiver was equal to the broad bandwidth of the antenna.[22][23][31][55] This was acceptable and even necessary because the first Hertzian spark transmitters also lacked a tuned circuit. Due to the impulsive nature of the spark, they radiated a very "noisy" signal, the energy of the radio waves was spread over a very wide band of frequencies, a wide bandwidth.[56][57] To receive enough energy from this wideband signal the receiver had to have a wide bandwidth also.

It was found that when more than one spark transmitter was radiating in a given area, their frequencies overlapped, so their signals interfered with each other, resulting in garbled reception.[22][55][58] It became clear that, if multiple transmitters were to operate simultaneously, some method of selective signaling was needed, to allow the receiver to select which transmitter's signal to receive.[58][59] As radio transmission and detection systems were being developed it was also theorized that the multiple wavelengths produced by a poorly tuned transmitter were overlapping each other causing the signal to "dampen", or die down, greatly reducing the power and range of transmission.[60] In 1892, William Crookes gave a lecture[61] on radio in which he suggested using resonance to reduce the bandwidth of transmitters and receivers. Different transmitters could then be "tuned" to transmit on different frequencies so they didn't interfere.[29][56][62] The receiver would also have a resonant circuit (tuned circuit), and could receive a particular transmission by "tuning" its resonant circuit to the same frequency as the transmitter, analogously to tuning a musical instrument to resonance with another. This is the system used in all modern radio.

Tuning was used in Hertz's original experiments[63] and practical application of tuning showed up in the early to mid 1890s in wireless systems not specifically designed for radio communication. Nikola Tesla's March 1893 lecture demonstrating the wireless transmission of power for lighting (mainly by what he thought was ground conduction[64]) included elements of tuning. The wireless lighting system consisted of a spark-excited grounded resonant transformer with a wire antenna which transmitted power across the room to another resonant transformer tuned to the frequency of the transmitter, which lighted a Geissler tube.[26][62] Use of tuning in free space "Hertzian waves" (radio) was explained and demonstrated in Oliver Lodge's 1894 lectures on Hertz's work.[65] At the time Lodge was demonstrating the physics and optical qualities of radio waves instead of attempting to build a communication system but he would go on to develop methods (patented in 1897) of tuning radio (what he called "syntony"), including using variable inductance to tune antennas.[66][67][68]

By 1897 the advantages of tuned systems had become clear, and Marconi and the other wireless researchers had incorporated tuned circuits, consisting of capacitors and inductors connected together, into their transmitters and receivers.[22][26][29][31][55][67] The tuned circuit acted like an electrical analog of a tuning fork. It had a high impedance at its resonant frequency, but a low impedance at all other frequencies. Connected between the antenna and the detector it served as a bandpass filter, passing the signal of the desired station to the detector, but routing all other signals to ground.[23] The frequency of the station received f was determined by the capacitance C and inductance L in the tuned circuit:

Inductive coupling[edit]
Marconi's inductively coupled coherer receiver from his controversial April 1900 "four circuit" patent no. 7,777.
Braun receiving transformer from 1904
Crystal receiver from 1914 with "loose coupler" tuning transformer. The secondary coil (1) can be slid in or out of the primary (in box) to adjust the coupling. Other components: (2) primary tuning capacitor, (3) secondary tuning capacitor, (4) loading coil, (5) crystal detector, (8) headphones

In order to reject radio noise and interference from other transmitters near in frequency to the desired station, the bandpass filter (tuned circuit) in the receiver has to have a narrow bandwidth, allowing only a narrow band of frequencies through.[22][23] The form of bandpass filter that was used in the first receivers, which has continued to be used in receivers until recently, was the double-tuned inductively-coupled circuit, or resonant transformer (oscillation transformer or RF transformer).[22][26][29][31][67][69] The antenna and ground were connected to a coil of wire, which was magnetically coupled to a second coil with a capacitor across it, which was connected to the detector.[23] The RF alternating current from the antenna through the primary coil created a magnetic field which induced a current in the secondary coil which fed the detector. Both primary and secondary were tuned circuits;[55] the primary coil resonated with the capacitance of the antenna, while the secondary coil resonated with the capacitor across it. Both were adjusted to the same resonant frequency.

This circuit had two advantages.[23] One was that by using the correct turns ratio, the impedance of the antenna could be matched to the impedance of the receiver, to transfer maximum RF power to the receiver. Impedance matching was important to achieve maximum receiving range in the unamplified receivers of this era.[19][23] The coils usually had taps which could be selected by a multiposition switch. The second advantage was that due to "loose coupling" it had a much narrower bandwidth than a simple tuned circuit, and the bandwidth could be adjusted.[22][69] Unlike in an ordinary transformer, the two coils were "loosely coupled"; separated physically so not all the magnetic field from the primary passed through the secondary, reducing the mutual inductance. This gave the coupled tuned circuits much "sharper" tuning, a narrower bandwidth than a single tuned circuit. In the "Navy type" loose coupler (see picture), widely used with crystal receivers, the smaller secondary coil was mounted on a rack which could be slid in or out of the primary coil, to vary the mutual inductance between the coils.[22][70] When the operator encountered an interfering signal at a nearby frequency, the secondary could be slid further out of the primary, reducing the coupling, which narrowed the bandwidth, rejecting the interfering signal. A disadvantage was that all three adjustments in the loose coupler - primary tuning, secondary tuning, and coupling - were interactive; changing one changed the others. So tuning in a new station was a process of successive adjustments.

Selectivity became more important as spark transmitters were replaced by continuous wave transmitters which transmitted on a narrow band of frequencies, and broadcasting led to a proliferation of closely spaced radio stations crowding the radio spectrum.[23] Resonant transformers continued to be used as the bandpass filter in vacuum tube radios, and new forms such as the variometer were invented.[70][71] Another advantage of the double-tuned transformer for AM reception was that when properly adjusted it had a "flat top" frequency response curve as opposed to the "peaked" response of a single tuned circuit.[72] This allowed it to pass the sidebands of AM modulation on either side of the carrier with little distortion, unlike a single tuned circuit which attenuated the higher audio frequencies. Until recently the bandpass filters in the superheterodyne circuit used in all modern receivers were made with resonant transformers, called IF transformers.

Patent disputes[edit]

Marconi's initial radio system had relatively poor tuning limiting its range and adding to interference.[73] To overcome this drawback he developed a four circuit system with tuned coils in "symphony" at both the transmitters and receivers.[73] His 1900 British #7,777 (four sevens) patent for tuning filed in April 1900 and granted a year later opened the door to patents disputes since it infringed on the Syntonic patents of Oliver Lodge, first filed in May 1897, as well as patents filed by Ferdinand Braun.[73] Marconi was able to obtain patents in the UK and France but the US version of his tuned four circuit patent, filed in November 1900, was initially rejected based on it being anticipated by Lodge's tuning system, and refiled versions were rejected because of the prior patents by Braun, and Lodge.[74] A further clarification and re-submission was rejected because it infringed on parts of two prior patents Tesla had obtained for his wireless power transmission system.[75] Marconi's lawyers managed to get a resubmitted patent reconsidered by another examiner who initially rejected it due to a pre-existing John Stone Stone tuning patent, but it was finally approved it in June 1904 based on it having a unique system of variable inductance tuning that was different from Stone[76][77] who tuned by varying the length of the antenna.[74] When Lodge's Syntonic patent was extended in 1911 for another 7 years the Marconi Company agreed to settle that patent dispute, purchasing Lodge's radio company with its patent in 1912, giving them the priority patent they needed.[78][79] Other patent disputes would crop up over the years including a 1943 US Supreme Court ruling on the Marconi Companies ability to sue the US government over patent infringement during World War I. The Court rejected the Marconi Companies suit saying they could not sue for patent infringement when their own patents did not seem to have priority over the patents of Lodge, Stone, and Tesla.[26][62]

Crystal radio receiver[edit]

Main article: Crystal radio
Prior to 1920 the crystal receiver was the main type used in wireless telegraphy stations, and sophisticated models were made, like this Marconi Type 106 from 1915.
Family listening to the first broadcasts around 1920 with a crystal receiver. The mother and father have to share an earphone
After vacuum tube receivers appeared around 1920, the crystal set became a simple cheap alternative radio used by youth and the poor.
Simple crystal radio. The capacitance of the wire antenna connected to the coil serves as the capacitor in the tuned circuit.
Typical "loose coupler" crystal radio circuit

Although it was invented in 1904 in the wireless telegraphy era, the crystal radio receiver could also rectify AM transmissions and served as a bridge to the broadcast era. In addition to being the main type used in commercial stations during the wireless telegraphy era, it was the first receiver to be used widely by the public.[80] During the first two decades of the 20th century, as radio stations began to transmit in AM voice (radiotelephony) instead of radiotelegraphy, radio listening became a popular hobby, and the crystal was the simplest, cheapest detector. The millions of people who purchased or homemade these inexpensive reliable receivers created the mass listening audience for the first radio broadcasts, which began around 1920.[81] In the 1920s the crystal receiver was superseded by vacuum tube receivers and became obsolete. However it continued to be used by youth and the poor until World War 2.[80] Today crystal radios, the simplest type of radio receivers, are constructed by students as educational science projects.

The crystal radio used a crystal detector called a cat's whisker detector, invented by Harrison H. C. Dunwoody and Greenleaf Whittier Pickard in 1904, to rectify the radio signal to extract the audio from the radio frequency carrier.[23][43][82] It consisted of a mineral crystal, usually galena (PbS, lead sulfide) which was lightly touched by a fine springy wire (the "cat whisker") on an adjustable arm.[43][83] The resulting crude semiconductor junction functioned as a Schottky barrier diode, it only conducted current in one direction. Only particular sites on the crystal surface functioned as rectifying junctions, and the junction could be disrupted by the slightest vibration. So a usable site was found by trial and error before each use; the operator would drag the cat's whisker across the crystal until the radio began functioning. Frederick Seitz, a later semiconductor researcher, wrote:

Such variability, bordering on what seemed the mystical, plagued the early history of crystal detectors and caused many of the vacuum tube experts of a later generation to regard the art of crystal rectification as being close to disreputable.[84]

Like other receivers of this era the crystal radio was unamplified and ran off the power of the radio waves received from the radio station, so it had to be listened to with earphones; it could not drive a loudspeaker.[23][83] It required a long wire antenna, and its sensitivity depended on how large the antenna was. During the wireless era it was used in commercial and military longwave stations with huge antennas to receive long distance radiotelegraphy traffic, even including transatlantic traffic.[85][86] However, when used to receive broadcast stations a typical home crystal set had a more limited range of about 25 miles.[87] In sophisticated crystal radios the "loose coupler" inductively coupled tuned circuit was used to increase the Q. However it still had poor selectivity compared to modern receivers.[83]

Heterodyne receiver and BFO[edit]

Main article: Heterodyne
Radio receiver with Poulsen "tikker" consisting of a commutator disk turned by a motor to interrupt the carrier.

Beginning around 1905 continuous wave (CW) transmitters began to replace spark transmitters for radiotelegraphy because they had much greater range. The first continuous wave transmitters were the Poulsen arc invented in 1904 and the Alexanderson alternator developed 1906-1910, which were replaced by vacuum tube transmitters beginning around 1920.[18]

The continuous wave radiotelegraphy signals produced by these transmitters required a different method of reception.[88][89] The radiotelegraphy signals produced by spark gap transmitters consisted of strings of damped waves repeating at an audio rate, so the "dots" and "dashes" of Morse code were audible as a tone or buzz in the receivers' earphones. However the new continuous wave radiotelegraph signals simply consisted of pulses of unmodulated carrier (sine waves). These were inaudible in the receiver headphones. To receive this new modulation type, the receiver had to produce some kind of tone during the pulses of carrier.

The first crude device that did this was the "ticker" or "tikker", invented in 1908 by Valdemar Poulsen.[40][88] [90] This was a vibrating interrupter with a capacitor at the tuner output which served as a rudimentary modulator, interrupting the carrier at an audio rate, thus producing a buzz in the earphone when the carrier was present.[5] A similar device was the "tone wheel" invented by Rudolph Goldschmidt, a wheel spun by a motor with contacts spaced around its circumference, which made contact with a stationary brush.

Fessenden's heterodyne radio receiver circuit

In 1901 Reginald Fessenden had invented a better means of accomplishing this.[88][90][91][92] In his heterodyne receiver an unmodulated sine wave radio signal at a frequency fO offset from the incoming radio wave carrier fC was applied to a rectifying detector such as a crystal detector or electrolytic detector, along with the radio signal from the antenna. In the detector the two signals mixed, creating two new heterodyne (beat) frequencies at the sum fC + fO and the difference fC − fO between these frequencies. By choosing fO correctly the lower heterodyne fC − fO was in the audio frequency range, so it was audible as a tone in the earphone whenever the carrier was present. Thus the "dots" and "dashes" of Morse code were audible as musical "beeps". A major attraction of this method during this pre-amplification period was that the heterodyne receiver actually amplified the signal somewhat, the detector had "mixer gain".[90]

The receiver was ahead of its time, because when it was invented there was no oscillator capable of producing the radio frequency sine wave fO with the required stability.[93] Fessenden first used his large radio frequency alternator,[5] but this wasn't practical for ordinary receivers. The heterodyne receiver remained a laboratory curiosity until a cheap compact source of continuous waves appeared, the vacuum tube electronic oscillator[90] invented by Edwin Armstrong and Alexander Meissner in 1913.[40][94] After this it became the standard method of receiving CW radiotelegraphy. The heterodyne oscillator is the ancestor of the beat frequency oscillator (BFO) which is used to receive radiotelegraphy in communications receivers today. The heterodyne oscillator had to be retuned each time the receiver was tuned to a new station, but in modern superheterodyne receivers the BFO signal beats with the fixed intermediate frequency, so the beat frequency oscillator can be a fixed frequency.

Armstrong later used Fessenden's heterodyne principle in his superheterodyne receiver (below).[90][5]

Vacuum tube era[edit]

Unlike today, when almost all radios use a variation of the superheterodyne design, during the 1920s vacuum tube radios used a variety of competing circuits.
During the "Golden Age of Radio" (1920 to 1950), families gathered to listen to the home radio in the evening, such as this Zenith console model 12-S-568 from 1938, a 12 tube superheterodyne with pushbutton tuning and 12 inch cone speaker.

The Audion (triode) vacuum tube invented by Lee De Forest in 1906 was the first practical amplifying device and revolutionized radio.[50] Vacuum tube transmitters replaced spark transmitters and made possible four new types of modulation: continuous wave (CW) radiotelegraphy, amplitude modulation (AM) around 1915 which could carry audio (sound), frequency modulation (FM) around 1938 which had much improved audio quality, and single sideband (SSB).

The amplifying vacuum tube used energy from a battery or electrical outlet to increase the power of the radio signal, so vacuum tube receivers could be more sensitive and have a greater reception range than the previous unamplified receivers. The increased audio output power also allowed them to drive loudspeakers instead of earphones, permitting more than one person to listen. The first loudspeakers were produced around 1915. These changes caused radio listening to evolve explosively from a solitary hobby to a popular social and family pastime. The development of amplitude modulation (AM) and vacuum tube transmitters during World War I, and the availability of cheap receiving tubes after the war, set the stage for the start of AM broadcasting, which sprang up spontaneously around 1920.

The advent of radio broadcasting increased the market for radio receivers greatly, and transformed them into a consumer product.[95][96][97] At the beginning of the 1920s the radio receiver was a forbidding high-tech device, with many cryptic knobs and controls requiring technical skill to operate, housed in an unattractive black metal box, with a tinny-sounding horn loudspeaker.[96] By the 1930s, the broadcast receiver had become a piece of furniture, housed in an attractive wooden case, with standardized controls anyone could use, which occupied a respected place in the home living room. In the early radios the multiple tuned circuits required multiple knobs to be adjusted to tune in a new station. One of the most important ease-of-use innovations was "single knob tuning", achieved by linking the tuning capacitors together mechanically.[96][97] The dynamic cone loudspeaker invented in 1924 greatly improved audio frequency response over the previous horn speakers, allowing music to be reproduced with good fidelity.[96][98] Convenience features like large lighted dials, tone controls, pushbutton tuning, tuning indicators and automatic gain control (AGC) were added.[95][97] The receiver market was divided into the above broadcast receivers and communications receivers, which were used for two-way radio communications such as shortwave radio.[99]

A vacuum tube receiver required several power supplies at different voltages, which in early radios were supplied by separate batteries. These were the standard batteries used in early radios:[100][101][102]

  • "A" battery - This supplied current to heat the filaments of the tubes, which consumed the bulk of the power in early radios. The first tubes used 6V at several amperes, so lead-acid automobile batteries were often used, as they could be recharged. Later tubes used 3V or 1.5V from dry cell batteries.
  • "B" battery - this supplied the plate (anode) voltage for the tubes, including the audio output power to the earphone or loudspeaker. These were rectangular multicell carbon-zinc batteries. They were made in multiples of 22.5 volts: 22.5, 45, 67.5, and 90 volts, and often had taps to give different voltages.
  • "C" battery - a few radios required a third voltage of about 4V to bias the grid of the tubes negative.

By 1930 adequate rectifier tubes were developed, and the expensive batteries were replaced by a transformer power supply that worked off the house current.[95][96]

Vacuum tubes were bulky, expensive, had a limited lifetime, consumed a large amount of power and produced a lot of waste heat, so the number of tubes a receiver could economically have was a limiting factor. Therefore, a goal of tube receiver design was to get the most performance out of a limited number of tubes. The major radio receiver designs, listed below, were invented during the vacuum tube era.

A defect in many early vacuum tube receivers was that the amplifying stages could oscillate, act as an oscillator, producing unwanted radio frequency alternating currents.[23][103][104] These parasitic oscillations mixed with the carrier of the radio signal in the detector tube, producing audible beat notes (heterodynes); annoying whistles, moans, and howls in the speaker. The oscillations were caused by feedback in the amplifiers; one major feedback path was the capacitance between the plate and grid in early triodes.[103][104] This was solved by the Neutrodyne circuit, and later the development of the tetrode and pentode around 1930.

Edwin Armstrong is one of the most important figures in radio receiver history, and during this period invented technology which continues to dominate radio communication.[5] He was the first to give a correct explanation of how De Forest's triode tube worked. He invented the feedback oscillator, regenerative receiver, the superregenerative receiver, the superheterodyne receiver, and modern frequency modulation (FM).

The first vacuum tube receivers[edit]

De Forest's first commercial Audion receiver, the RJ6 which came out in 1914. The Audion tube was always mounted upside down, with its delicate filament loop hanging down, so it did not sag and touch the other electrodes in the tube.
Example of single tube triode grid-leak receiver from 1920, the first type of amplifying radio receiver. In the grid leak circuit, electrons attracted to the grid during the positive half cycles of the radio signal charge the grid capacitor with a negative voltage of a few volts, biasing the grid near its cutoff voltage, so the tube conducts only during the positive half-cycles, rectifying the radio carrier.

The first amplifying vacuum tube, the Audion, a crude triode, was invented in 1906 by Lee De Forest as a more sensitive detector for radio receivers, by adding a third electrode to the thermionic diode detector, the Fleming valve.[50][71][105][106] It was not widely used until its amplifying ability was recognized around 1912.[50] The first tube receivers, invented by De Forest and built by hobbyists until the mid 1920s, used a single Audion which functioned as a grid-leak detector which both rectified and amplified the radio signal.[71][103][107] The grid-leak detector circuit was also used in regenerative, TRF, and early superheterodyne receivers (below) until the 1930s.

To give enough output power to drive a loudspeaker, 2 or 3 additional Audion stages were needed for audio amplification.[71] Many early hobbyists could only afford a single tube receiver, and listened to the radio with earphones, so early tube amplifiers and speakers were sold as add-ons.

In addition to very low gain of about 5 and a short lifetime of about 30 - 100 hours, the primitive Audion had erratic characteristics because it was incompletely evacuated, some residual air was left in the tube by De Forest, who believed that ionization was key to its operation.[108][109] This made it a more sensitive detector[108] but also caused its electrical characteristics to vary during use.[71][105] As the tube heated up, gas released from the metal elements would change the pressure in the tube, changing the plate current and other characteristics, so it required periodic bias adjustments to keep it at the correct operating point. Each Audion stage usually had a rheostat to adjust the filament current, and often a potentiometer or multiposition switch to control the plate voltage. The filament rheostat was also used as a volume control. The many controls made multitube Audion receivers nightmarishly complicated to operate.

By 1914, Harold Arnold at Western Electric and Irving Langmuir at GE had realized that the residual gas in the tube that caused these problems was not necessary; the Audion could operate on electron conduction alone.[105][108][109] They were able to evacuate tubes to a lower pressure of 10−9 atm, producing the first "hard vacuum" triodes. These more stable tubes did not require bias adjustments and allowed radios to have fewer controls and be more user-friendly.[105] During World War I civilian radio use was prohibited, but by 1920 these tubes came on the market and large-scale production of vacuum tube radios began. The "soft" incompletely evacuated tubes were used as detectors through the 1920s then became obsolete.

Regenerative (autodyne) receiver[edit]

Main article: Regenerative receiver
Block diagram of regenerative receiver
Circuit of single tube Armstrong regenerative receiver
Homemade Armstrong regenerative receiver, 1922. The "tickler" coil (L3) is visible on the front panel, coupled to the input tuning coils.
Commercial regenerative receiver from the early 1920s, the Paragon RA-10 (center) with separate 10R single tube RF amplifier (left) and three tube DA-2 detector and 2-stage audio amplifier unit (right). The 4 cylindrical dry cell "A" batteries (right rear) powered the tube filaments, while the 2 rectangular "B" batteries provided plate voltage.
Homemade one-tube Armstrong regenerative receiver from the 1940s. The tickler coil is a variometer winding mounted on a shaft inside the tuning coil (upper right) which can be rotated by a knob on the front panel.

The regenerative receiver, invented by Edwin Armstrong[110][111] in 1913 when he was a 23-year-old college student,[112] was used very widely until the late 1920s particularly by hobbyists who could only afford a single-tube radio. Today transistor versions of the circuit are still used in a few inexpensive applications like walkie-talkies. In the regenerative receiver the gain (amplification) of a vacuum tube or transistor is increased by using regeneration (positive feedback); some of the energy from the tube's output circuit is fed back into the input circuit with a feedback loop.[23][103][113][114][115] The early vacuum tubes had very low gain (around 5). Regeneration could not only increase the gain of the tube enormously, by a factor of 15,000 or more, it also increased the Q factor of the tuned circuit, decreasing (sharpening) the bandwidth of the receiver by the same factor, improving selectivity greatly.[103][113][114] The receiver had a control to adjust the feedback. The tube also acted as a grid-leak detector to rectify the AM signal.[103]

Another advantage of the circuit was that the tube could be made to oscillate, and thus a single tube could serve as both a beat frequency oscillator and a detector, functioning as a heterodyne receiver to make CW radiotelegraphy transmissions audible.[103][113][114] This mode was called an autodyne receiver. To receive radiotelegraphy, the feedback was increased until the tube oscillated, then the oscillation frequency was tuned to one side of the transmitted signal. The incoming radio carrier signal and local oscillation signal mixed in the tube and produced an audible heterodyne (beat) tone at the difference between the frequencies.

A widely used design was the Armstrong circuit, in which a "tickler" coil in the plate circuit was coupled to the tuning coil in the grid circuit, to provide the feedback.[23][103][115] The feedback was controlled by a variable resistor, or alternately by moving the two windings physically closer together to increase loop gain, or apart to reduce it.[113] This was done by an adjustable air core transformer called a variometer (variocoupler). Regenerative detectors were sometimes also used in TRF and superheterodyne receivers.

One problem with the regenerative circuit was that when used with large amounts of regeneration the selectivity (Q) of the tuned circuit could be too sharp, attenuating the AM sidebands, thus distorting the audio modulation.[116] This was usually the limiting factor on the amount of feedback that could be employed.

A more serious drawback was that it could act as an inadvertent radio transmitter, producing interference (RFI) in nearby receivers.[23][103][113][114][115][117] In AM reception, to get the most sensitivity the tube was operated very close to instability and could easily break into oscillation (and in CW reception did oscillate), and the resulting radio signal was radiated by its wire antenna. In nearby receivers, the regenerative's signal would beat with the signal of the station being received in the detector, creating annoying heterodynes, (beats), howls and whistles.[23] Early regeneratives which oscillated easily were called "bloopers", and were made illegal in Europe. One preventative measure was to use a stage of RF amplification before the regenerative detector, to isolate it from the antenna.[103][113] But by the mid 1920s "regens" were no longer sold by the major radio manufacturers.[23]

Superregenerative receiver[edit]

This was a receiver invented by Edwin Armstrong in 1922 which used regeneration in a more sophisticated way, to give greater gain.[104][118][119][120][121] It was used in a few shortwave receivers in the 1930s, and is used today in a few cheap high frequency applications such as walkie-talkies and garage door openers.

In the regenerative receiver the loop gain of the feedback loop was less than one, so the tube (or other amplifying device) did not oscillate but was close to oscillation, giving large gain.[118] In the superregenerative receiver, the loop gain was made equal to one, so the amplifying device actually began to oscillate, but the oscillations were interrupted periodically.[104][6] This allowed a single tube to produce gains of over 106.

TRF receiver[edit]

Block diagram of a tuned radio frequency receiver. To achieve enough selectivity to reject stations on adjacent frequencies, multiple cascaded bandpass filter stages had to be used. The dotted line indicates that the bandpass filters must be tuned together.
Typical 5 tube TRF circuit from 1924 has 2 stages of RF amplification containing 3 bandpass filters, a grid-leak detector stage, and 2 stages of transformer-coupled audio amplification
Early 6 tube TRF receiver from around 1920. The 3 large knobs adjust the 3 tuned circuits to tune in stations
Atwater-Kent TRF receiver from the 1920s with 2 RF stages (left), detector and two audio amplifier tubes (right). The loudspeaker consists of an earphone coupled to an acoustic horn which amplifies the sound.
Tuning a Neutrodyne TRF receiver with 3 tuned circuits (large knobs), 1924. For each station the index numbers on the dials had to be written down so that the station could be found again.

The tuned radio frequency (TRF) receiver, invented in 1916 by Ernst Alexanderson, improved both sensitivity and selectivity by using several stages of amplification before the detector, each with a tuned circuit, all tuned to the frequency of the station.[23][104][6][122][123] Its operation is briefly described in the How receivers work section above. It was very popular in quality radios during the 1920s until the superheterodyne replaced it in the 1930s. TRF receivers consist of these parts:

  • One or more tuned radio frequency amplifier stages, each consisting of an amplifying tube or transistor and a tuned circuit. In vacuum tube radios these consisted of a tube amplifier followed by an air core interstage coupling transformer with a capacitor across one winding.
  • A detector stage, in tube radios usually a triode grid-leak detector.
  • Usually one or more audio amplifier stages

A major problem of early TRF receivers was that they were complicated to tune, because each resonant circuit had to be adjusted to the frequency of the station before the radio would work.[23][104] In later TRF receivers the tuning capacitors were linked together mechanically ("ganged") on a common shaft so they could be adjusted with one knob, but in early receivers the frequencies of the tuned circuits could not be made to "track" well enough to allow this, and each tuned circuit had its own tuning knob.[6][124] Therefore, the knobs had to be turned simultaneously. For this reason most TRF sets had no more than three tuned RF stages.[103][116]

A second problem was that the multiple radio frequency stages, all tuned to the same frequency, were prone to oscillate,[124][125] and the parasitic oscillations mixed with the radio station's carrier in the detector, producing audible heterodynes (beat notes), whistles and moans, in the speaker.[23][103][104][123] This was solved by the invention of the Neutrodyne circuit (below) and the development of the tetrode later around 1930, and better shielding between stages.[123]

Today the TRF design is used in a few integrated (IC) receiver chips. From the standpoint of modern receivers the disadvantage of the TRF is that the gain and bandwidth of the tuned RF stages are not constant but vary as the receiver is tuned to different frequencies.[125] Since the bandwidth of a filter with a given Q is proportional to the frequency, as the receiver is tuned to higher frequencies its bandwidth increases.[8][12]

Neutrodyne receiver[edit]

Main article: Neutrodyne

The Neutrodyne receiver, invented in 1922 by Louis Hazeltine,[126][127] was a TRF receiver with a "neutralizing" circuit added to each radio amplification stage to cancel the feedback to prevent the oscillations which caused the annoying whistles in the TRF.[23][104][123][124][128] In the neutralizing circuit a capacitor fed a feedback current from the plate circuit to the grid circuit which was 180° out of phase with the feedback which caused the oscillation, canceling it.[103] The Neutrodyne was popular until the advent of cheap tetrode tubes around 1930.

Reflex receiver[edit]

Main article: Reflex receiver
Block diagram of simple single tube reflex receiver

The reflex receiver, invented in 1914 by Wilhelm Schloemilch and Otto von Bronk,[129] and rediscovered and extended to multiple tubes in 1917 by Marius Latour[129][130] and William H. Priess, was a design used in some inexpensive radios of the 1920s[131] which enjoyed a resurgence in small portable tube radios of the 1930s[132] and again in a few of the first transistor radios in the 1950s.[104][133] It is another example of an ingenious circuit invented to get the most out of a limited number of active devices. In the reflex receiver the RF signal from the tuned circuit is passed through one or more amplifying tubes or transistors, demodulated in a detector, then the resulting audio signal is passed again though the same amplifier stages for audio amplification.[104] The separate radio and audio signals present simultaneously in the amplifier do not interfere with each other since they are at different frequencies, allowing the amplifying tubes to do "double duty". In addition to single tube reflex receivers, some TRF and superheterodyne receivers had several stages "reflexed".[133] Reflex radios were prone to a defect called "play-through" which meant that the volume of audio did not go to zero when the volume control was turned down.[133]

Superheterodyne receiver[edit]

Block diagram of a superheterodyne receiver. The dotted line indicates that the RF filter and local oscillator must be tuned in tandem.
The first superheterodyne receiver built at Armstrong's Signal Corps laboratory in Paris during World War I. It is constructed in two sections, the mixer and local oscillator (left) and three IF amplification stages and a detector stage (right). The intermediate frequency was 75 kHz.
During the 1940s the vacuum tube superheterodyne receiver was refined into a cheap-to-manufacture form called the "All American Five" because it only required 5 tubes, which was used in almost all broadcast radios until the end of the tube era in the 1970s.

The superheterodyne, invented in 1918 during World War I by Edwin Armstrong[4] when he was in the Signal Corps, is the design used in almost all modern receivers, except a few specialized applications.[5][6][7] It is a more complicated design than the other receivers above, and when it was invented required 6 - 9 vacuum tubes, putting it beyond the budget of most consumers, so it was initially used mainly in commercial and military communication stations.[9] However, by the 1930s the "superhet" had replaced all the other receiver types above.

In the superheterodyne, the "heterodyne" technique invented by Reginald Fessenden is used to shift the frequency of the radio signal down to a lower "intermediate frequency" (IF), before it is processed.[8][9][10] Its operation and advantages over the other radio designs in this section are described above in The superheterodyne design

By the 1940s the superheterodyne AM broadcast receiver was refined into a cheap-to-manufacture design called the "All American Five", because it only used five vacuum tubes: usually a converter (mixer/local oscillator), an IF amplifier, a detector/audio amp, audio power amp, and a rectifier. This design was used for virtually all commercial radio receivers until the transistor replaced the vacuum tube in the 1970s.

Semiconductor era[edit]

A modern smartphone has several digital radio transmitters and receivers to connect to different devices; a cellular receiver, a wireless modem, a bluetooth modem, and a GPS receiver

The invention of the transistor in 1947 revolutionized radio technology, making truly portable receivers possible, beginning with transistor radios in the late 1950s. Although portable vacuum tube radios were made, tubes were bulky and inefficient, consuming large amounts of power and requiring several large batteries to produce the filament and plate voltage. Transistors did not require a heated filament, reducing power consumption, and were smaller and much less fragile than vacuum tubes.

The development of integrated circuits (ICs) in the 1970s created another revolution, allowing an entire radio receiver to be put on a chip. ICs reversed the economics of radio design used with vacuum tube receivers; since the marginal cost of adding additional amplifying devices (transistors) to the chip was essentially zero, the size and cost of the receiver was dependent not on how many active components were used as with vacuum tubes, but on the passive components; inductors and capacitors, which could not be integrated easily on the chip.[16] As a result, the current trend in receivers is to use digital circuitry on the chip to do functions that were formerly done by analog circuits which require passive components. In a digital receiver the IF signal is sampled and digitized, and the bandpass filtering and detection functions are performed by digital signal processing (DSP) on the chip. Another benefit of DSP is that the properties of the receiver; channel frequency, bandwidth, gain, etc. can be dynamically changed by software to react to changes in the environment; these systems are known as software-defined radios or cognitive radio.

In modern wireless technology, radio transmitters and receivers are embedded in portable digital devices such as laptops, cell phones, GPS receivers, Bluetooth headsets, wireless routers and work automatically, in the background, to keep the device in touch with other devices, without wires. They transmit binary digital data by modulation methods such as frequency shift keying (FSK) allowing portable digital devices to communicate via wireless networks.

Digital technologies[edit]

Many of the functions performed by analogue electronics can be performed by software instead. The benefit is that software is not affected by temperature, physical variables, electronic noise and manufacturing defects.[134] For really high-performance receivers, such as satellite communications receivers and military/naval receivers, two-stage ("double conversion") and even three-stage ("triple conversion") superheterodyne processing is frequently used. Single-conversion receivers are rather simple-minded in their nature.

DSP technology[edit]

DSP technology, short for digital signal processing, is the use of digital means to process signals and is coming into wide use in modern shortwave receivers. It is the basis of many areas of modern technology including cell phones, CD players, video recorders and computers. A digital signal is essentially a stream or sequence of numbers that relay a message through some sort of medium such as a wire. The primary benefit of DSP hardware in shortwave receivers is the ability to tailor the bandwidth of the receiver to current reception conditions and to the type of signal being listened to. A typical analog only receiver may have a limited number of fixed bandwidths, or only one, but a DSP receiver may have 40 or more individually selectable filters.

PC controlled radio receivers[edit]

"PC radios", or radios that are designed to be controlled by a standard PC are controlled by specialized PC software using a serial port connected to the radio. A "PC radio" may not have a front-panel at all, and may be designed exclusively for computer control, which reduces cost.

Some PC radios have the great advantage of being field upgradable by the owner. New versions of the DSP firmware can be downloaded from the manufacturer's web site and uploaded into the flash memory of the radio. The manufacturer can then in effect add new features to the radio over time, such as adding new filters, DSP noise reduction, or simply to correct bugs.

A full-featured radio control program allows for scanning and a host of other functions and, in particular, integration of databases in real-time, like a "TV-Guide" type capability. This is particularly helpful in locating all transmissions on all frequencies of a particular broadcaster, at any given time. Some control software designers have even integrated Google Earth to the shortwave databases, so it is possible to "fly" to a given transmitter site location with a click of a mouse. In many cases the user is able to see the transmitting antennas where the signal is originating from.

Radio control software[edit]

The field of software control of PC radios has grown rapidly in the last several years, with developers making a number of advances. Since the Graphical User Interface or GUI interface PC to the radio has unlimited flexibility, any number of new features can be added by the software designer. Features that can be found in advanced control software programs today include a band table, GUI controls corresponding to traditional radio controls, local time clock and a UTC clock, signal strength meter, an ILG database for shortwave listening with lookup capability, scanning capability, text-to-speech interface, and integrated Conference Server.

Software-defined radios[edit]

The next level in radio / software integration are so-called pure "software defined radios". The distinction here is that all filtering, modulation and signal manipulation is done in software, usually by a PC soundcard or by a dedicated piece of DSP hardware. There may be a minimal RF front-end or traditional radio that supplies an IF to the SDR. SDR's can go far beyond the usual demodulation capability of typical, and even high-end DSP shortwave radios. They can for example, record large swaths of the radio spectrum to a hard drive for "playback" at a later date. The same SDR that one minute is demodulating a simple AM broadcast may also be able to decode an HDTV broadcast in the next. A well known open-source project called GNU Radio is dedicated to evolving a high-performance SDR. All the source code for this SDR is freely downloadable and modifiable by anyone.

All-digital radio[edit]

With the invention of all digital radio transmitter and receiver without any analogue adapters, it opens up for the possibility to build increasingly smaller and cheaper radios.[135]

See also[edit]

References[edit]

  1. ^ Radio-Electronics, Radio Receiver Technology
  2. ^ Ganguly, Partha Kumar (2015). Principles of Electronics. PHI Learning Pvt. Ltd. pp. 286–289. ISBN 812035124X. 
  3. ^ a b c d e f g h i j k Rudersdorfer, Ralf (2013). Radio Receiver Technology: Principles, Architectures and Applications. John Wiley and Sons. ISBN 111864784X.  Chapter 1
  4. ^ a b Armstrong, Edwin H. (February 1921). "A new system of radio frequency amplification". Proceedings of the Inst. of Radio Engineers. New York: Institute of Radio Engineers. 9 (1): 3–11. Retrieved December 23, 2015. 
  5. ^ a b c d e f Lee, Thomas H. (2004) The Design of CMOS Radio Frequency Integrated Circuits, 2nd Ed., p. 14-15
  6. ^ a b c d e f g h i Dixon, Robert (1998). Radio Receiver Design. CRC Press. pp. 57–61. ISBN 0824701615. 
  7. ^ a b c d e Williams, Lyle Russell (2006) The New Radio Receiver Building Handbook, p. 28-30
  8. ^ a b c d e f g Army Technical Manual TM 11-665: C-W and A-M Radio Transmitters and Receivers, 1952, p. 195-197
  9. ^ a b c McNicol, Donald (1946) Radio's Conquest of Space, p. 272-278
  10. ^ a b Terman, Frederick E. (1943) Radio Engineers' Handbook, p. 636-638
  11. ^ a b c d e Carr, Joseph J. (2001). The Technician's Radio Receiver Handbook: Wireless and Telecommunication Technology. Newnes. pp. 8–11. ISBN 0750673192. 
  12. ^ a b c Rembovsky, Anatoly; Ashikhmin, Alexander; Kozmin, Vladimir; et al. (2009). Radio Monitoring: Problems, Methods and Equipment. Springer Science and Business Media. p. 26. ISBN 0387981004. 
  13. ^ Terman, Frederick E. (1943) Radio Engineers' Handbook, p. 645
  14. ^ a b c d Drentea, Cornell (2010). Modern Communications Receiver Design and Technology. Artech House. pp. 325–330. ISBN 1596933100. 
  15. ^ a b c Hagen, Jon B. (1996). Radio-Frequency Electronics: Circuits and Applications. Cambridge Univ. Press. p. 60. ISBN 0521553563. 
  16. ^ a b c d e f g h i j k l m Lee, Thomas H. (2004). The Design of CMOS Radio-Frequency Integrated Circuits, 2nd Ed. UK: Cambridge University Press. pp. 1–8. ISBN 0521835399. 
  17. ^ Appleyard, Rollo (October 1927). "Pioneers of Electrical Communication part 5 - Heinrich Rudolph Hertz" (PDF). Electrical Communication. New York: International Standard Electric Corp. 6 (2): 67. Retrieved December 19, 2015. 
  18. ^ a b c d e Phillips, Vivian J. (1980). Early Radio Wave Detectors. London: Inst. of Electrical Engineers. pp. 4–12. ISBN 0906048249. 
  19. ^ a b Rudersdorfer, Ralf (2013). Radio Receiver Technology: Principles, Architectures and Applications. John Wiley and Sons. pp. 1–2. ISBN 111864784X. 
  20. ^ Nahin, Paul J. (2001). The Science of Radio: With Matlab and Electronics Workbench Demonstration, 2nd Ed. Springer Science & Business Media. pp. 45–48. ISBN 0387951504. 
  21. ^ a b c d e f g h i j Coe, Lewis (2006). Wireless Radio: A History. McFarland. pp. 3–8. ISBN 0786426624. 
  22. ^ a b c d e f g h McNicol, Donald (1946). Radio's Conquest of Space. Murray Hill Books. pp. 57–68. 
  23. ^ a b c d e f g h i j k l m n o p q r s t u v w Carr, Joseph (1990). Old Time Radios! Restoration and Repair. McGraw-Hill Professional. pp. 5–13. ISBN 0071507663. 
  24. ^ a b c Beauchamp, Ken (2001). History of Telegraphy. IET. pp. 184–186. ISBN 0852967926. 
  25. ^ a b c d Nahin, Paul J. (2001) The Science of Radio, p. 53-56
  26. ^ a b c d e f g Klooster, John W. (2007). Icons of Invention. ABC-CLIO. pp. 159–161. ISBN 0313347433. 
  27. ^ McNicol, Donald (1946). Radio's Conquest of Space. Murray Hill Books. pp. 37–45. 
  28. ^ Hong, Sungook (2001). Wireless: From Marconi's Black-box to the Audion. MIT Press. pp. 1–2. ISBN 0262082985. 
  29. ^ a b c d e Sarkar et al (2006) History of Wireless, p. 349-358, archive
  30. ^ a b c Fleming, John Ambrose (1910). The Principles of Electric Wave Telegraphy and Telephony, 2nd Ed. London: Longmans, Green and Co. pp. 420–428. 
  31. ^ a b c d Stone, Ellery W. (1919). Elements of Radiotelegraphy. D. Van Nostrand Co. pp. 203–208. 
  32. ^ Phillips, Vivian 1980 Early Radio Wave Detectors, p. 18-21
  33. ^ a b c McNicol, Donald (1946) Radio's Conquest of Space, p. 107-113
  34. ^ Phillips, Vivian 1980 Early Radio Wave Detectors, p. 38-42
  35. ^ Phillips, Vivian 1980 Early Radio Wave Detectors, p. 57-60
  36. ^ Maver, William Jr. (August 1904). "Wireless Telegraphy To-Day". American Monthly Review of Reviews. New York: The Review of Reviews Co. 30 (2): 192. Retrieved January 2, 2016. 
  37. ^ Aitken, Hugh G.J. (2014). The Continuous Wave: Technology and American Radio, 1900-1932. Princeton Univ. Press. p. 190. ISBN 1400854601. 
  38. ^ Phillips, Vivian 1980 Early Radio Wave Detectors, p. 198-203
  39. ^ a b Phillips, Vivian 1980 Early Radio Wave Detectors, p. 205-209
  40. ^ a b c d Marriott, Robert H. (September 17, 1915). "United States Radio Development". Proc. of the Inst. of Radio Engineers. US: Institute of Radio Engineers. 5 (3): 184. doi:10.1109/jrproc.1917.217311. Retrieved 2010-01-19. 
  41. ^ Secor, H. Winfield (January 1917). "Radio Detector Development". Electrical Experimenter. New York: Experimenter Publishing Co. 4 (9): 652–656. Retrieved January 3, 2016. 
  42. ^ McNicol, Donald (1946). Radio's Conquest of Space. Murray Hill Books. pp. 121–123. 
  43. ^ a b c d e f Stone, Ellery (1919) Elements of Radiotelegraphy, p. 209-221
  44. ^ Fleming, John Ambrose (1910) The Principles of Electric Wave Telegraphy and Telephony, p. 446-455
  45. ^ Phillips, Vivian 1980 Early Radio Wave Detectors, p. 85-108
  46. ^ Stephenson, Parks (November 2001). "The Marconi Wireless Installation in R.M.S. Titanic". Old Timer's Bulletin. The Antique Wireless Association. 42 (4). Retrieved May 22, 2016.  copied on Stephenson's marconigraph.com personal website
  47. ^ McNicol, Donald (1946) Radio's Conquest of Space, p. 115-119
  48. ^ Fleming, John Ambrose (1910) The Principles of Electric Wave Telegraphy and Telephony, p. 460-464
  49. ^ Phillips, Vivian 1980 Early Radio Wave Detectors, p. 65-81
  50. ^ a b c d e Lee, Thomas H. (2004) The Design of CMOS Radio Frequency Integrated Circuits, 2nd Ed., p. 9-11
  51. ^ McNicol, Donald (1946) Radio's Conquest of Space, p. 157-162
  52. ^ Fleming, John Ambrose (1910) The Principles of Electric Wave Telegraphy and Telephony, p. 476-483
  53. ^ McNicol, Donald (1946) Radio's Conquest of Space, p. 123-131
  54. ^ Fleming, John Ambrose (1910) The Principles of Electric Wave Telegraphy and Telephony, p. 471-475
  55. ^ a b c d Hong, Sungook (2001). Wireless: From Marconi's Black-box to the Audion. MIT Press. pp. 89–100. ISBN 0262082985. 
  56. ^ a b Aitken, Hugh 2014 Syntony and Spark: The origins of radio, p. 70-73
  57. ^ Beauchamp, Ken (2001) History of Telegraphy, p. 189-190
  58. ^ a b Kennelly, Arthur E. (1906). Wireless Telegraphy: An Elementary Treatise. New York: Moffatt, Yard and Co. pp. 173–183. 
  59. ^ Aitken, Hugh 2014 Syntony and Spark: The origins of radio, p. 31-48
  60. ^ Jed Z. Buchwald, Scientific Credibility and Technical Standards in 19th and early 20th century Germany and Britain, Springer Science & Business Media - 1996, page 158
  61. ^ Crookes, William (February 1, 1892). "Some Possibilities of Electricity". The Fortnightly Review. London: Chapman and Hall. 51: 174–176. Retrieved August 19, 2015. 
  62. ^ a b c Rockman, Howard B. (2004). Intellectual Property Law for Engineers and Scientists. John Wiley and Sons. pp. 196–199. ISBN 0471697397. 
  63. ^ Cecil Lewis Fortescue, Wireless Telegraphy, Read Books Ltd - 2013, chapter XIII
  64. ^ Hong, Sungook (2001). Wireless: From Marconi's Black-box to the Audion. MIT Press. p. 199. ISBN 0262082985. 
  65. ^ Peter Rowlands, Oliver Lodge and the Liverpool Physical Society, Liverpool University Press - 1990, page 117
  66. ^ Jed Z. Buchwald, Scientific Credibility and Technical Standards in 19th and early 20th century Germany and Britain, Springer Science & Business Media - 1996, pages 158-159
  67. ^ a b c Aitken, Hugh G.J. (2014). Syntony and Spark: The Origins of Radio. Princeton Univ. Press. p. 255. ISBN 1400857880. 
  68. ^ Thomas H. Lee, The Design of CMOS Radio-Frequency Integrated Circuits, Cambridge University Press - 2004, page 35
  69. ^ a b McNicol, Donald (1946) Radio's Conquest of Space, p. 242-253
  70. ^ a b Marx, Harry J.; Van Muffling, Adrian (1922). Radio Reception. New York: G. Putnam's Sons. pp. 95–103. 
  71. ^ a b c d e McNicol, Donald (1946) Radio's Conquest of Space, p. 254-259
  72. ^ Terman, Frederick E. (1943). Radio Engineers' Handbook (PDF). New York: McGraw-Hill Book Co. p. 170. 
  73. ^ a b c Hong, Sungook (2001). Wireless: From Marconi's Black-box to the Audion. MIT Press. pp. 91-99
  74. ^ a b Howard B. Rockman, Intellectual Property Law for Engineers and Scientists,John Wiley & Sons - 2004, page 198
  75. ^ U.S. Patent No. 649,621, 3/15/1900, and part of 645,576, 3/20/1900 (filed Sept. 2, 1897) MARCONI WIRELESS TELEGRAPH CO. OF AMERICA v. UNITED STATES. UNITED STATES v. MARCONI WIRELESS TELEGRAPH CO. OF AMERICA. 320 U.S. 1 (63 S.Ct. 1393, 87 L.Ed. 1731)
  76. ^ US Patent no. 714,756, John Stone Stone Method of electric signaling, filed: February 8, 1900, granted: December 2, 1902
  77. ^ MARCONI WIRELESS TELEGRAPH CO. OF AMERICA v. UNITED STATES. UNITED STATES v. MARCONI WIRELESS TELEGRAPH CO. OF AMERICA. 320 U.S. 1 (63 S.Ct. 1393, 87 L.Ed. 1731)
  78. ^ Hong, Sungook (2001). Wireless: From Marconi's Black-box to the Audion. MIT Press. p. 48
  79. ^ Susan J. Douglas, Listening in: Radio and the American Imagination, U of Minnesota Press, page 50
  80. ^ a b Basalla, George (1988). The Evolution of Technology. UK: Cambridge University Press. p. 44. ISBN 0-521-29681-1. 
  81. ^ Corbin, Alfred (2006). The Third Element: A Brief History of Electronics. AuthorHouse. pp. 44–45. ISBN 1-4208-9084-0. 
  82. ^ Army Technical Manual TM 11-665: C-W and A-M Radio Transmitters and Receivers. US Dept. of the Army. 1952. pp. 167–169. 
  83. ^ a b c Williams, Lyle Russell (2006). The New Radio Receiver Building Handbook. Lulu. pp. 20–24. ISBN 1847285260. 
  84. ^ Riordan, Michael; Lillian Hoddeson (1988). Crystal fire: the invention of the transistor and the birth of the information age. USA: W. W. Norton & Company. pp. 19–21. ISBN 0-393-31851-6. 
  85. ^ Beauchamp, Ken (2001). History of Telegraphy. Institution of Electrical Engineers. p. 191. ISBN 0852967926. 
  86. ^ Bucher, Elmer Eustice (1917). Practical Wireless Telegraphy. New York: Wireless Press. p. 306. 
  87. ^ Lescarboura, Austin C. (1922). Radio for Everybody. New York: Scientific American Publishing Co. pp. 93–94. 
  88. ^ a b c Lauer, Henri; Brown, Harry L. (1920). Radio Engineering Principles. McGraw-Hill. pp. 135–142. 
  89. ^ Phillips, Vivian 1980 Early Radio Wave Detectors, p. 172-185
  90. ^ a b c d e McNicol, Donald (1946). Radio's Conquest of Space. New York: Murray Hill Books. pp. 133–136. 
  91. ^ US patent no. 1050441, Reginald A. Fessenden, Electrical signaling apparatus, filed July 27, 1905; granted January 14, 1913
  92. ^ Hogan, John V. L. (April 1921). "The Heterodyne Receiver". The Electric Journal. Pittsburgh, USA: The Electric Journal. 18 (4): 116–119. Retrieved January 28, 2016. 
  93. ^ Nahin, Paul J. (2001) The Science of Radio, p. 91
  94. ^ McNicol, Donald (1946) Radio's Conquest of Space, p. 267-270
  95. ^ a b c McNicol, Donald (1946) Radio's Conquest of Space, p. 341-344
  96. ^ a b c d e Wurtzler, Steve J. (2007). Electric Sounds: Technological Change and the Rise of Corporate Mass Media. Columbia Univ. Press. pp. 147–148. ISBN 023151008X. 
  97. ^ a b c Nebeker, Frederik (2009). Dawn of the Electronic Age: Electrical Technologies in the Shaping of the Modern World, 1914 to 1945. John Wiley and Sons. pp. 159–160. ISBN 0470409746. 
  98. ^ McNicol, Donald (1946) Radio's Conquest of Space, p. 336-340
  99. ^ Terman, Frederick E. (1943) Radio Engineers' Handbook, p. 656
  100. ^ Malanowski, Gregory (2011). The Race for Wireless. AuthorHouse. p. 67. ISBN 1463437501. 
  101. ^ Nelson, Phillip I. (1995). "Powering your antique battery radio". Phil's Old Radios. Personal website. Retrieved January 1, 2016. 
  102. ^ Haan, E. R. (December 1925). "Radio batteries, their care and selection". Popular Mechanics. New York: Popular Mechanics Co. 44 (6): 1010–1013. ISSN 0032-4558. Retrieved January 1, 2016. 
  103. ^ a b c d e f g h i j k l m Williams, Lyle Russell (2006). The New Radio Receiver Building Handbook. Lulu. pp. 24–27. ISBN 1847285260. 
  104. ^ a b c d e f g h i j Lee, Thomas H. (2004) The Design of CMOS Radio Frequency Integrated Circuits, 2nd Ed., p. 15-18
  105. ^ a b c d Okamura, Sōgo (1994). History of Electron Tubes. IOS Press. pp. 17–22. ISBN 9051991452. 
  106. ^ De Forest, Lee (January 1906). "The Audion; A New Receiver for Wireless Telegraphy". Trans. of the AIEE. American Institute of Electrical and Electronic Engineers. 25: 735–763. doi:10.1109/t-aiee.1906.4764762. Retrieved January 7, 2013.  The link is to a reprint of the paper in the Scientific American Supplement, No. 1665, November 30, 1907, p.348-350, copied on Thomas H. White's United States Early Radio History website
  107. ^ Terman, Frederick E. (1943). Radio Engineers' Handbook (PDF). New York: McGraw-Hill Book Co. pp. 564–565. 
  108. ^ a b c Langmuir, Irving (September 1915). "The Pure Electron Discharge and its Applications in Radio Telegraphy and Telephony" (PDF). Proceedings of the IRE. New York: Institute of Radio Engineers. 3 (3): 261–293. doi:10.1109/jrproc.1915.216680. Retrieved January 12, 2016. 
  109. ^ a b Tyne, Gerald F. J. (December 1943). "The Saga of the Vacuum Tube, Part 9" (PDF). Radio News. Chicago: Ziff-Davis. 30 (6): 30–31, 56, 58. Retrieved June 17, 2016. 
  110. ^ Armstrong, Edwin H. (September 1915). "Some recent developments in the Audion receiver" (PDF). Proc. of the IRE. New York: Institute of Radio Engineers. 3 (9): 215–247. Retrieved August 29, 2012. 
  111. ^ Armstrong, Edwin H. (September 1915). "Some recent developments in the Audion receiver" (PDF). Proc. of the IRE. New York: Institute of Radio Engineers. 3 (9): 215–247. Retrieved August 29, 2012. 
  112. ^ Armstrong, Edwin H. (April 1921). "The Regenerative Circuit". The Electrical Journal. Pittsburgh, PA: Westinghouse Co. 18 (4): 153–154. Retrieved January 11, 2016. 
  113. ^ a b c d e f Army Technical Manual TM 11-665: C-W and A-M Radio Transmitters and Receivers, 1952, p. 187-190
  114. ^ a b c d Terman, Frederick E. (1943) Radio Engineers' Handbook, p. 574-575
  115. ^ a b c McNicol, Donald (1946) Radio's Conquest of Space, p. 260-262
  116. ^ a b Langford-Smith, F. (1953). Radiotron Designer's Handbook, 4th Ed. (PDF). Wireless Press for RCA. pp. 1223–1224. 
  117. ^ In the early 1920s Armstrong, David Sarnoff head of RCA, and other radio pioneers testified before the US Congress on the need for legislation against radiating regenerative receivers. Wing, Willis K. (October 1924). "The Case Against the Radiating Receiver" (PDF). Broadcast Radio. New York: Doubleday, Page and Co. 5 (6): 478–482. Retrieved January 16, 2016. 
  118. ^ a b Army Technical Manual TM 11-665: C-W and A-M Radio Transmitters and Receivers, 1952, p. 190-193
  119. ^ Terman, Frederick E. (1943). Radio Engineers' Handbook (PDF). New York: McGraw-Hill Book Co. pp. 662–663. 
  120. ^ Williams, Lyle Russell (2006) The New Radio Receiver Building Handbook, p. 31-32
  121. ^ McNicol, Donald (1946) Radio's Conquest of Space, p. 279-282
  122. ^ Army Technical Manual TM 11-665: C-W and A-M Radio Transmitters and Receivers, 1952, p. 170-175
  123. ^ a b c d McNicol, Donald (1946) Radio's Conquest of Space, p. 263-267
  124. ^ a b c Army Technical Manual TM 11-665: C-W and A-M Radio Transmitters and Receivers, 1952, p. 177-179
  125. ^ a b Terman, Frederick E. (1943). Radio Engineers' Handbook (PDF). New York: McGraw-Hill Book Co. pp. 438–439. 
  126. ^ US Patent No. 1450080, Louis Alan Hazeltine, "Method and electric circuit arrangement for neutralizing capacity coupling"; filed August 7, 1919; granted March 27, 1923
  127. ^ Hazeltine, Louis A. (March 1923). "Tuned Radio Frequency Amplification With Neutralization of Capacity Coupling" (PDF). Proc. of the Radio Club of America. New York: Radio Club of America. 2 (8): 7–12. Retrieved March 7, 2014. 
  128. ^ Terman, Frederick E. (1943). Radio Engineers' Handbook (PDF). New York: McGraw-Hill Book Co. pp. 468–469. 
  129. ^ a b Grimes, David (May 1924). "The Story of Reflex and Radio Frequency" (PDF). Radio in the Home. 2 (12): 9–10,. Retrieved January 24, 2016. 
  130. ^ US Patent no. 1405523, Marius Latour Audion or lamp relay or amplifying apparatus, filed December 28, 1917; granted February 7, 1922
  131. ^ McNicol, Donald (1946) Radio's Conquest of Space, p. 283-284
  132. ^ "Reflexing Today: Operating economy with the newer tubes" (PDF). Radio World. New York: Hennessey Radio Publications Co. 23 (17): 3. July 8, 1933. Retrieved January 16, 2016. 
  133. ^ a b c Langford-Smith, F. (1953). Radiotron Designer's Handbook, 4th Ed. (PDF). Wireless Press for RCA. pp. 1140–1141. 
  134. ^ "History of the Radio Receiver". Radio-Electronics.Com. Retrieved 2007-11-23. 
  135. ^ Pizzicato Comes of Age

Further reading[edit]

  • Communications Receivers, Third Edition, Ulrich L. Rohde, Jerry Whitaker, McGraw Hill, New York, 2001, ISBN 0-07-136121-9
  • Buga, N.; Falko A.; Chistyakov N.I. (1990). Chistyakov N.I., ed. Radio Receiver Theory. Translated from the Russian by Boris V. Kuznetsov. Moscow: Mir Publishers. ISBN 5-03-001321-0  First published in Russian as «Радиоприёмные устройства»