# Superheterodyne receiver
**The superheterodyne receiver**, often shortened to superhet, is a radio receiver architecture that converts every incoming station to one fixed intermediate frequency before doing almost all of its amplifying and filtering, rather than trying to amplify and filter each station at whatever frequency it happens to arrive on. A local oscillator tuned alongside the desired station is mixed with the incoming signal, and only the difference frequency, always the same value regardless of which station is tuned in, is passed on to a fixed amplifier and filter chain built to do one job extremely well. The microsim on this page lets the reader drag a station's frequency across the tuning dial and watch the local oscillator track it so the intermediate frequency never moves, while a second, unwanted frequency called the image drifts across the band in the opposite direction.
This separation of concerns is what makes the architecture powerful: the front end only has to make a rough first selection of the wanted station, and the fixed intermediate-frequency stages, tuned once and never retuned, can be built with far sharper filtering and far steadier gain than any single amplifier that had to work across an entire tuning range. Nearly every mass-produced radio receiver built since the 1930s, and most software-defined receivers today, still down-converts every station this same way before anything else happens to it.
The architecture grew up alongside broadcast [[Amplitude_modulation|AM radio]] in the 1920s, and it now reaches far beyond consumer sets: the same mix-to-a-fixed-frequency trick tunes [[Radar|radar]] receivers, and a synthesizer built from a [[Phase-locked_loop|phase-locked loop]] usually supplies the tunable local oscillator that a modern set mixes against the incoming [[Carrier_wave|carrier]].
That power comes with one structural cost. Because a mixer responds only to the difference between two frequencies, a second, unwanted input frequency exists that mixes down to the very same intermediate frequency as the wanted station, called the image, and rejecting it shapes almost every other design choice a superheterodyne receiver makes.
## History
Edwin Armstrong developed the superheterodyne while serving with the Signal Corps of the American Expeditionary Forces in France during the First World War, work motivated by the problem of receiving faint, high-frequency signals more reliably than existing sets allowed.[^cn-ww1] He described the technique in a paper to the Institute of Radio Engineers in 1921,[^armstrong1921] building on the older heterodyne principle that radio experimenters had already been using for continuous-wave reception for roughly two decades.[^cn-heterodyne]
Turning the idea into a commercial product took most of the 1920s. Early superheterodyne sets needed more vacuum tubes than a simple regenerative or tuned-radio-frequency set, which made them costlier at a time when tubes and licensing fees already dominated a receiver's price, and control of the key patents sat largely with the Radio Corporation of America, which shaped who could manufacture a superheterodyne set and on what terms.[^cn-rca] Other engineers pursued closely related heterodyne-conversion ideas around the same period, and questions of priority between these parallel efforts were never fully settled to everyone's satisfaction.[^cn-parallel] As tubes fell in price and improved through the late 1920s, the superheterodyne's sharper selectivity and steadier gain won out against the era's biggest practical problem: separating a crowded band of [[Amplitude_modulation|AM]] stations without a set drifting out of tune, and by the 1930s it had displaced the designs that came before it as the standard broadcast-receiver architecture.
## Why the superheterodyne displaced other technologies
Before the superheterodyne, a receiver either amplified the incoming station directly at its own [[Amplitude_modulation|AM]] broadcast frequency, a tuned radio-frequency (TRF) design, or used positive feedback to coax extra gain from a single stage, a regenerative design that was Armstrong's own earlier invention. Both had problems a listener felt directly. A TRF set needed two or three tuned circuits ganged on one dial, and building capacitors that tracked each other accurately across an entire band was hard and expensive; get the tracking even slightly wrong and the set's sensitivity and selectivity swung wildly across the dial. A regenerative set delivered startling gain from very few tubes, but pushing the feedback close to the threshold of oscillation, where the gain was highest, made it prone to radiating its own signal back out through the antenna and interfering with a neighbour's reception.
The superheterodyne sidestepped both problems by moving almost all of the amplification and selectivity to one intermediate frequency that never changes, so a designer could optimise that filter and amplifier chain once, at the factory, rather than asking a listener's hands to reproduce that optimum at every setting of the dial. Its extra tube count briefly counted against it commercially, and RCA's own patent control added friction of its own;[^cn-rca] but once tube costs fell far enough, the technical case for stable, dial-independent selectivity outweighed the extra tube count, and rival designs faded from the mass market.
## Principle of operation
A superheterodyne's central trick is heterodyning: mixing the incoming radio-frequency (RF) [[Carrier_wave|carrier]] against a locally generated tone, the local oscillator (LO), in a deliberately nonlinear device called a mixer. Multiplying two cosines produces both their sum and their difference, `cos(2*pi*fRF*t) * cos(2*pi*fLO*t) = (1/2)*cos(2*pi*(fLO-fRF)*t) + (1/2)*cos(2*pi*(fLO+fRF)*t)`, and the receiver keeps only the difference term, filtering the sum away; the result is the intermediate frequency, `fIF = |fLO - fRF|`. To tune to a different station, the receiver does not retune the IF filter at all — it retunes the local oscillator so the difference stays fixed at `fIF` no matter which station is selected.
### Example: medium-wave broadcast receiver
A standard AM broadcast receiver tunes the 530–1,700 kHz medium-wave band and converts every station in it down to a fixed intermediate frequency of 455 kHz, a value chosen historically as a compromise: high enough to push the image usefully far from the wanted station, yet low enough that an affordable IF filter could still separate stations spaced only 10 kHz apart. With high-side injection the local oscillator runs 455 kHz above whatever station is tuned in, from about 985 kHz to 2,155 kHz across the band.
### RF stage
Ahead of the mixer sits the RF stage: a [[Filter_(signal_processing)|preselector filter]], sometimes followed by a low-noise amplifier, tuned loosely to the wanted station. Its job is not the receiver's main selecting, which belongs to the fixed IF filter, but rejecting the image and any other strong out-of-band signal before it reaches the mixer, since a nonlinear mixer overloaded by a strong unwanted signal can generate spurious products of its own. A preselector with a higher Q rejects the image more strongly but is harder to track accurately across a tuning range, the central tension the microsim's preselector control is built to show. The low-noise amplifier's other job is dominating the receiver's overall noise figure: a first stage with 25 [[Decibel|dB]] of gain and a 2.7 dB noise figure, followed by a lossy cable and a mixer with a 7.4 dB noise figure of its own, still leaves the whole chain at only about 2.7–2.8 dB, because so little of the later stages' noise makes it through the first stage's gain undiminished.[^ell102]
### Local oscillator and mixer
The local oscillator must track the RF tuning exactly, staying a fixed `fIF` away from the wanted station at every setting of the dial; historically this was done mechanically, by ganging the oscillator's tuning capacitor to the RF preselector's shaft, and in a modern set a synthesizer built around a [[Phase-locked_loop|phase-locked loop]] does the same job electronically. With high-side injection, `fLO = fRF + fIF`; low-side injection instead sets `fLO = fRF - fIF`, and either choice works, but it fixes which side of the dial the image falls on. The mixer itself is built from a [[Semiconductor_device|semiconductor]] such as a [[Transistor|transistor]] or diode, driven hard enough by the local oscillator to switch rather than merely amplify, since a perfectly linear device could never produce the sum and difference products heterodyning depends on.
### IF amplifier
Because the intermediate frequency never changes, the IF amplifier is the one stage that can be optimised once and left alone: it runs at a frequency chosen for good, stable transistor or integrated-circuit performance, and it can supply most of the receiver's gain without ever being retuned as the front end is. This is the payoff for the extra stage a superheterodyne needs compared with a receiver that tried to do the same amplifying directly at the incoming radio frequency: a fixed design problem, solved thoroughly once, replaces a moving one that would otherwise have to be solved afresh at every point on the dial.
### IF bandpass filter
Most of a superheterodyne's selectivity, meaning its ability to reject a station on an adjacent channel while passing the wanted one, comes from the fixed IF bandpass filter, built from ceramic resonators, a crystal filter, or several tuned transformers depending on how sharp a cutoff the application needs. Because this filter never retunes, it can use a far higher-order response than any single tuned circuit that had to track the front end across a whole band, the main technical reason a superheterodyne out-selects a comparable tuned-radio-frequency design.
### Demodulator
The last stage recovers the original baseband signal from the fixed-frequency IF using whatever detector matches the [[Signal_modulation|modulation]] in use: a simple diode envelope detector for AM broadcast signals, a discriminator or ratio detector for FM, or a product detector supplied with a locally regenerated carrier for single-sideband and Morse-code reception. Because this stage always sees the same intermediate frequency regardless of which station is tuned in, it can be designed and aligned once for that one frequency rather than for every frequency the receiver might ever cover.
## Multiple conversion
A single conversion forces a trade-off the sim's own IF control makes plain: a high intermediate frequency pushes the image far from the wanted signal and eases rejection, but it also makes a narrow, sharp filter harder to build relative to that frequency, so selectivity suffers; a low IF does the opposite, sharpening selectivity while dragging the image in close. Multiple conversion escapes the trade-off by using two mixers and two intermediate frequencies in series: a first conversion to a high IF, where the image is easy to reject, followed by a second conversion down to a much lower IF, where a sharp, high-selectivity [[Filter_(signal_processing)|filter]] is cheap to build. Communications and surveillance receivers that must reject both a nearby image and a nearby adjacent-channel signal at once routinely use double conversion for exactly this reason, and some demanding designs add a third conversion stage to push the trade-off further apart still.
## Modern designs
Modern receivers keep the superheterodyne's front end largely unchanged (a preselector, a mixer, a local-oscillator synthesizer, and at least one fixed IF) but increasingly digitize the signal as soon as possible after the IF filter rather than continuing with more analog stages. An [[Analog-to-digital_converter|analog-to-digital converter]] samples the fixed intermediate frequency directly, and everything after that, including demodulation, filtering finer than the analog IF filter provides, and following whatever [[Communication_protocol|protocol]] the transmission uses, is carried out in software rather than dedicated analog circuitry. This is the essence of a software-defined radio: the mix-to-a-fixed-IF idea barely changes, but almost everything downstream of it becomes reconfigurable code instead of fixed hardware.
Digital broadcasting keeps the same division of labour. A digital radio or television tuner still down-converts the received channel with an ordinary superheterodyne front end to get a manageable, fixed-frequency signal cheaply, and only then hands it to entirely digital processing: [[Data_compression|data-compression]] schemes such as the [[Discrete_cosine_transform|discrete cosine transform]], the technique behind [[Image_compression|compressing]] the video pictures a digital broadcast carries, run downstream of the analog front end and work the same way regardless of how the RF signal was converted down to baseband in the first place.
## Advantages and disadvantages
The superheterodyne's advantages are the ones already described: stable, high gain and sharp, adjustable selectivity from stages that never need to retune, at the cost of a more complex circuit than a receiver that tried to do everything at the incoming radio frequency. Its disadvantages are a family of ways the extra mixing stage can go wrong.
### Image frequency (fIMAGE)
Because a mixer responds only to the difference between two frequencies, a second input frequency exists that produces exactly the same intermediate frequency as the wanted station: the image, `f_image = fRF + 2*fIF` under high-side injection, since `|fLO - f_image| = |(fRF+fIF)-(fRF+2*fIF)| = fIF` as well. Any energy at the image that reaches the mixer lands directly on top of the wanted signal after conversion, and no amount of IF filtering afterward can separate the two once both have folded onto the same intermediate frequency; the only defence is keeping the image out of the mixer in the first place, with the RF stage's [[Filter_(signal_processing)|preselector]]. A larger `fIF` pushes the image farther from the wanted frequency and makes it easier for a modest preselector to reject, the central design trade the microsim's IF control is built to show.
### Spurious responses
The image is the best-known unwanted response but not the only one: any combination of harmonics of the RF input and the local oscillator that happens to mix down into the IF passband produces a spurious response, letting through a station the receiver was never tuned to. A perfectly linear mixer would produce only the wanted sum and difference products, but every real mixer is imperfect enough to generate weaker versions of these higher-order combinations too, and a well-engineered front end keeps them below the noise floor rather than eliminating them outright.
### Local oscillator radiation
A local oscillator strong enough to drive the mixer efficiently can also leak backward through the mixer and out through the antenna's [[Transmission_line|feed line]], radiating a signal of the receiver's own making. In a crowded band, or with many identical receivers operating close together, this self-generated emission can interfere with other receivers tuned to whatever frequency the leaking oscillator sits on, which is why regulators limit how much a receiver may radiate from its own local oscillator.
### Mixing noise from image
A mixer converts noise as readily as it converts signal, from both the wanted RF frequency and the image frequency at once, so a receiver with no preselector filtering effectively adds the noise power arriving at the image to the noise power arriving at the wanted frequency, degrading the noise figure by up to 3 [[Decibel|dB]] compared with a receiver whose front end suppresses the image first. This is one more reason the receiver's very first stage of gain matters more than any stage after it: in a cascade of amplifiers and mixers, the first stage's noise figure and gain dominate the whole chain's noise figure almost completely,[^ell102] so a low-noise, image-rejecting amplifier ahead of the mixer earns back most of the 3 dB a bare, unprotected mixer would otherwise give up.
### Local oscillator phase noise and reciprocal mixing
A local oscillator is never a perfectly pure tone; it carries phase noise, energy spread into a skirt on either side of its nominal frequency. When a strong nearby signal is present, that skirt mixes with it and lands noise-like energy directly on top of the wanted, much weaker station at the intermediate frequency, a problem called reciprocal mixing, which no amount of IF filtering afterward can remove, since the damage is done before the signal ever reaches that filter. A receiver meant to work well next to strong nearby signals, such as one sharing a tower with other transmitters, needs a local-oscillator [[Phase-locked_loop|synthesizer]] with especially low phase noise for exactly this reason, independent of anything the IF filter's own selectivity offers.
## Microsims
The primary microsim shows two stacked spectrum panes sharing one frequency axis: the top pane is the antenna's RF spectrum, showing the wanted station, its image, the local-oscillator spike, and a translucent [[Filter_(signal_processing)|preselector]] response curve that tracks the tuning; the bottom pane is the spectrum after the mixer, where both the wanted signal and whatever image energy the preselector let through fold onto the same fixed intermediate frequency. **TUNING** sets the wanted station's frequency, with the local oscillator automatically tracking it so the intermediate frequency never moves; **IF** sets the intermediate frequency itself, pushing the image toward or away from the wanted station; **PRESELECTOR Q** sets how sharply the front-end filter rejects everything outside a narrow band around the tuned frequency. An "injection" button switches between high-side and low-side local-oscillator injection, flipping which side of the dial the image falls on. A diagnostics readout reports the wanted, local-oscillator, intermediate and image frequencies together with the live image-rejection figure in decibels. A three.js companion renders the full frequency plan (RF, LO, IF and the image, together with the preselector) in more depth.
*Try:* Raise IF while watching the top pane: the image moves farther from the wanted station, and the diagnostics readout's image-rejection figure climbs as the same preselector now has more room to work with.
## Wikipedia : Wikitube
**Strict pair:** [Wikipedia](https://en.wikipedia.org/wiki/Superheterodyne_receiver) : [Wikitube](https://en.wikitube.io/wiki/Superheterodyne_receiver)
Skeleton mirrored at revision 1374472395. Prose, emphasis and the microsims are Wikitube's own.
## See also
- [[Radar]]
- [[Amplitude_modulation]]
- [[Phase-locked_loop]]
- [[Carrier_wave]]
- [[Filter_(signal_processing)]]
- [[Semiconductor_device]]
- [[Analog-to-digital_converter]]
## References
[^armstrong1921]: Armstrong, E. H. "A New System of Short-Wave Amplification." *Proceedings of the Institute of Radio Engineers* 9, no. 1 (1921): pp. 3–11.
[^ell102]: Ellingson, S. *Radio Systems Engineering – Revised First Edition*. 2023, pp. 102–103 (PDF pages). Open Textbook Library: https://open.umn.edu/opentextbooks/textbooks/radio-systems-engineering . CC BY-NC.
[^cn-ww1]: Citation needed: a primary biographical source (letters, patent file, or Armstrong's own account) for the WWI Signal Corps context in which he developed the superheterodyne.
[^cn-heterodyne]: Citation needed: a primary source (publication or patent) for the earliest heterodyne-detection technique and who is credited with it.
[^cn-rca]: Citation needed: a primary licensing or patent-pool record documenting RCA's control of superheterodyne patents in the 1920s.
[^cn-parallel]: Citation needed: names, dates and patent numbers of engineers who filed closely related heterodyne-conversion patents contemporaneously with Armstrong.
## Further reading
- Ellingson, S. *Radio Systems Engineering – Revised First Edition*. 2023. Open Textbook Library: https://open.umn.edu/opentextbooks/textbooks/radio-systems-engineering . CC BY-NC.
- Tiberius, C.; Mulder, M. *Engineering Signal Analysis: From Fourier to Filtering: Theory*. 2026. Open Textbook Library: https://open.umn.edu/opentextbooks/textbooks/engineering-signal-analysis-from-fourier-to-filtering-theory . CC BY.
- Johnson, D. *Fundamentals of Electrical Engineering I*. 2014. Open Textbook Library: https://open.umn.edu/opentextbooks/textbooks/fundamentals-of-electrical-engineering-1 . CC BY.
- Stiber, M.; Stiber, B.; Larson, E. *Signal Computing: Digital Signals in the Software Domain*. 2020. Open Textbook Library: https://open.umn.edu/opentextbooks/textbooks/signal-computing-digital-signals-in-the-software-domain . CC BY-SA.
- Downey, A. *Think DSP: Digital Signal Processing in Python*. 2012. Open Textbook Library: https://open.umn.edu/opentextbooks/textbooks/think-dsp-digital-signal-processing-in-python . CC BY-NC.
- Dyer, J.; Davis, C. *Measurement and Instrumentation: An Introduction to Concepts and Methods – 1st Edition*. 2020. Open Textbook Library: https://open.umn.edu/opentextbooks/textbooks/measurement-and-instrumentation-an-introduction-to-concepts-and-methods . CC BY-NC-SA.
## External links
- [Superheterodyne (live sketch)](https://editor.p5js.org/sciencenibber/full/EMZke8Hlz)
- [Superheterodyne (editor)](https://editor.p5js.org/sciencenibber/sketches/EMZke8Hlz)
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