Cavity magnetron
High-power vacuum tube enabling compact radar and microwave ovens.
The cavity magnetron is a high-power vacuum tube that first found use in early radar, and later became common in microwave ovens and linear particle accelerators. It produces microwaves by directing a stream of electrons past a set of small, open cavities in a metal block, with a magnetic field influencing their motion. This interaction causes the microwaves to oscillate within the cavities, much like a whistle produces a tone when air is blown past its opening. The physical size of the cavities determines the resonant frequency. Unlike a klystron or traveling-wave tube, the magnetron cannot amplify an incoming microwave signal; it only acts as an oscillator, converting direct-current electricity into a microwave signal.
The idea of using magnetic fields to control electric current gained momentum after Lee de Forest invented the Audion in 1906. Albert Hull at General Electric Research Laboratory began developing magnetrons to bypass de Forest’s patents, but his efforts were not fully successful. Other researchers built on Hull’s work, and in 1924, Habann in Germany introduced a key improvement: the use of two cathodes. Progress slowed until 1929, when Okabe in Japan published a paper on generating centimeter-wavelength signals, sparking global interest. In 1934, A. L. Samuel of Bell Telephone Laboratories proposed magnetrons with multiple cathodes, leading to designs by Klaas Posthumus in 1934 and Hans Hollmann in 1935. Companies like Philips, General Electric Company (GEC), and Telefunken began production, but output was limited to about 10 watts. At that time, the klystron could produce more power, so the magnetron saw little use, though a 300-watt device was built by N.F. Alekseev and D.D. Malairov in the USSR in 1936 (published in 1940).
A major breakthrough came in 1940, when John Randall and Harry Boot at the University of Birmingham, England, introduced a cavity magnetron far better than earlier versions. Their first working model produced hundreds of watts at a 10-centimeter wavelength—an unprecedented feat. Within weeks, engineers at GEC boosted this to over a kilowatt, then to 25 kilowatts within months, over 100 kilowatts by 1941, and nearly a megawatt by 1943. These high-power pulses came from a device the size of a small book, transmitted from an antenna only centimeters long. This shrank practical radar systems dramatically, allowing them to be installed in fighter aircraft. New radars emerged for night-fighters, anti-submarine aircraft, and even the smallest escort ships. From that point, the Allies of World War II held a radar lead that Germany and Japan could never close. By the war’s end, nearly every Allied radar relied on the magnetron.
After the war, the magnetron continued in radar use but lost favor in the 1960s as high-power klystrons and traveling-wave tubes appeared. A key drawback is that the magnetron’s output signal changes in frequency and phase from pulse to pulse, making it less suitable for moving target indication and removing clutter from radar displays. It still appears in some radar systems, but has become far more common as a low-cost source for microwave ovens. In that form, over one billion magnetrons are now in use.
**Construction and operation**
**Conventional tube design** In a standard vacuum tube, electrons are emitted from a heated, negatively charged cathode and attracted to a positively charged anode. These components are usually arranged concentrically inside an evacuated glass or metal container, allowing electrons to move freely. If a third electrode—a control grid—is placed between the cathode and anode, varying its voltage regulates the electron flow. This three-electrode tube, called a triode, can act as an amplifier: small changes in the grid’s charge produce identical changes in the larger current flowing between cathode and anode.
**Hull or single-anode magnetron** The concept of using a grid for control was pioneered by Philipp Lenard (Nobel Prize in Physics, 1905) and later patented in the U.S. by Lee de Forest. This spurred research into alternative tube designs that avoided de Forest’s patents. One approach used a magnetic field instead of an electrical charge to control current, leading to the magnetron. In this design, the tube had two electrodes: a central rod-shaped cathode and a cylindrical anode around it. The tube was placed between the poles of a horseshoe magnet, with the magnetic field aligned parallel to the electrodes’ axis. Without a magnetic field, the tube acts as a diode, with electrons flowing straight from cathode to anode. With the magnetic field present, electrons experience a force at right angles to their motion (the Lorentz force), curving their path between the electrodes. The curvature can be controlled by adjusting the magnetic field strength (via an electromagnet) or the electrical potential between the electrodes. At very high...
- field
- Electronics, Radar, Microwave Engineering
- known_for
- High-power microwave generation for radar and microwave ovens
- key_developers
- John Randall, Harry Boot (1940 cavity magnetron); earlier contributions by Albert Hull, Habann, Okabe, A. L. Samuel, Klaas Posthumus, Hans Hollmann, N.F. Alekseev, D.D. Malairov
- first_high_power_example
- 1940, University of Birmingham, England
Lore & Background
The cavity magnetron is a high-power vacuum tube that generates microwaves through the interaction of a stream of electrons with a magnetic field as they move past a series of small, open cavity resonators in a metal block. This process is analogous to a whistle producing a tone when air is blown past its opening. The resonant frequency is determined by the physical dimensions of the cavities. Unlike a klystron or traveling-wave tube, the magnetron cannot amplify an applied microwave signal; it functions solely as an electronic oscillator, converting direct-current electricity into a microwave signal. A key characteristic is that its output signal changes from pulse to pulse in both frequency and phase, making it less suitable for pulse-to-pulse comparisons needed for moving target indication and clutter removal in radar displays. The device typically consists of a central cathode (not always visible in cross-section) surrounded by an anode block containing the cavities, with an antenna for emitting microwaves. Magnets, often horseshoe-shaped alnico types in older models or more compact rare-earth, electromagnet, or ferrite magnets in modern tubes, create a magnetic field along the tube’s axis. The magnetron’s defining breakthrough came in 1940 when John Randall and Harry Boot at the University of Birmingham produced hundreds of watts at 10 cm wavelength, an unprecedented achievement. Within weeks, engineers improved this to over a kilowatt, and by 1943, outputs approached a megawatt. This high power, generated from a device the size of a small book and transmitted from an antenna only centimeters long, drastically reduced the size of practical radar systems, enabling installation in fighter aircraft and small ships. By the end of World War II, nearly all Allied radar relied on the magnetron. Post-war, it fell from favor for radar in the 1960s as high-power klystrons and traveling-wave tubes emerged, but it remains common as a low-cost source for microwave ovens, with over one billion units in use.
Reader's Guide
The cavity magnetron introduced by John Randall and Harry Boot at the University of Birmingham, England in 1940 was an improvement over earlier versions. Their first working example produced hundreds of watts at 10 cm wavelength, an unprecedented achievement. The high power pulses were generated from a device the size of a small book and transmitted from an antenna only centimeters long, reducing the size of practical radar systems by orders of magnitude, enabling installation in fighter aircraft. New radars appeared for night-fighters, anti-submarine aircraft and even the smallest escort ships, and from that point on the Allies of World War II held a lead in radar that their counterparts in Germany and Japan were never able to close. By the end of the war, practically every Allied radar was based on the magnetron. The magnetron continued in radar post-war but fell from favour in the 1960s as high-power klystrons and traveling-wave tubes emerged, because its output signal changes from pulse to pulse in frequency and phase, making it less suitable for moving target indication. It remains in use in some radar systems but has become much more common as a low-cost source for microwave ovens, with over one billion magnetrons in use.
Did You Know?
- The cavity magnetron generates microwaves using the interaction of a stream of electrons with a magnetic field, moving past cavity resonators, similar to a whistle producing a tone when excited by an air stream.
- The first working cavity magnetron by Randall and Boot produced hundreds of watts at 10 cm wavelength in 1940.
- Over one billion magnetrons are in use today, primarily in microwave ovens.
Operating Principle: Oscillation by Electron-Cavity Interaction
The cavity magnetron is fundamentally an oscillator rather than an amplifier. It converts direct-current electricity into a microwave signal by exploiting the interaction between a stream of electrons and a magnetic field. As those electrons travel past a series of small, open cavities carved into a metal block, they excite microwave oscillations within each cavity. The mechanism is often likened to a whistle: just as a stream of air blown across an opening sets up a standing tone, the passing electron stream sets up electromagnetic oscillation in the resonant cavities. The frequency at which the device operates is not set by electronic tuning but by the physical dimensions of those cavities themselves. This distinguishes it sharply from other vacuum tubes such as klystrons or traveling-wave tubes, which can amplify an incoming microwave signal. The magnetron has no such capability; it generates its own signal from scratch, making it a pure source rather than a gain device.
A Scattered Pre-War Lineage Across Three Continents
The road to the practical cavity magnetron was long and scattered across multiple countries. Albert Hull at General Electric's research lab pursued magnetron development along these lines but never achieved full success. L. Manufacturers such as Philips, GEC, and Telefunken began production, but output was capped at roughly ten watts. Meanwhile, the klystron was already delivering more power, leaving the magnetron in a secondary role. A notable exception came from the Soviet Union, where N. F. Alekseev and D. D.
Randall, Boot, and the Radar Revolution of 1940
In 1940, John Randall and Harry Boot at the University of Birmingham in England delivered a cavity magnetron that represented a quantum leap over every predecessor. Their first working unit produced hundreds of watts at a ten-centimeter wavelength, an output previously unattainable. Crucially, all this power was generated from a tube no larger than a small book, with a transmitting antenna only a few centimeters long. That dramatic reduction in radar system size meant the equipment could finally be mounted inside fighter aircraft. New radar suites appeared on night-fighters, anti-submarine patrol planes, and even the smallest escort vessels. From that moment onward, the Allies maintained a radar advantage over Germany and Japan that the Axis powers never managed to close. By the war's end, virtually every Allied radar system relied on the magnetron.
From Wartime Weapon to Kitchen Staple
After World War II, the magnetron continued serving in radar applications, but its dominance eroded during the 1960s as high-power klystrons and traveling-wave tubes matured. A fundamental limitation became increasingly apparent: the magnetron's output signal drifts in both frequency and phase from one pulse to the next. This characteristic makes it poorly suited for pulse-to-pulse comparison techniques essential to moving target indication and for filtering out ground clutter from a radar display. While the device still finds a place in certain radar systems, its most widespread modern role is far removed from military technology. The cavity magnetron has become the standard low-cost microwave source in household and commercial microwave ovens. In that domestic application, more than one billion magnetrons are in active use worldwide, making the device one of the most numerous high-power vacuum tubes ever manufactured. What began as a wartime radar enabler has thus become an everyday kitchen appliance component.
Frequently Asked Questions
What is a cavity magnetron?
It is a high-power vacuum tube that acts as a pure electronic oscillator, converting direct-current electricity into microwave radiation. It served as the core component of early radar systems and later became the heart of the household microwave oven.
Who invented the cavity magnetron?
John Randall and Harry Boot produced the first practical high-power cavity magnetron at the University of Birmingham in 1940, building on earlier groundwork by Albert Hull and several other researchers. Their design quickly became the standard for microwave generation during World War II.
How does a cavity magnetron generate microwaves?
A stream of electrons is driven past a series of small open cavities machined into a metal block while a magnetic field bends the electrons into a curved trajectory. The interaction between the moving electron cloud and the cavity resonators sustains the microwave oscillation.
Can a cavity magnetron amplify a signal like a klystron or traveling-wave tube?
No — the magnetron is strictly an oscillator and cannot function as an amplifier. It produces its microwave output directly from DC input power rather than boosting an incoming signal.
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