Editing Cavity magnetron (section)

===Hull or single-anode magnetron===
The idea of using a grid for control was invented by [[Philipp Lenard]], who received the [[Nobel Prize for Physics]] in 1905. In the  USA it was later patented by [[Lee de Forest]], resulting in considerable research into alternate tube designs that would avoid his patents. One concept used a magnetic field instead of an electrical charge to control current flow, leading to the development of the magnetron tube. In this design, the tube was made with two electrodes, typically with the cathode in the form of a metal rod in the center, and the anode as a cylinder around it. The tube was placed between the poles of a [[horseshoe magnet]]<ref name=mag>{{cite web |url=http://electriciantraining.tpub.com/14183/css/14183_103.htm |title=The Magnetron |website=electriciantraining.tpub.com |access-date=5 May 2018 |url-status=live |archive-url=https://web.archive.org/web/20160303222027/http://electriciantraining.tpub.com/14183/css/14183_103.htm |archive-date=3 March 2016}}</ref>{{Better source needed|date=October 2019}} arranged such that the magnetic field was aligned parallel to the axis of the electrodes.

With no magnetic field present, the tube operates as a diode, with electrons flowing directly from the cathode to the anode. In the presence of the magnetic field, the electrons will experience a force at right angles to their direction of motion (the [[Lorentz force]]). In this case, the electrons follow a curved path between the cathode and anode. The curvature of the path can be controlled by varying either the magnetic field using an [[electromagnet]], or by changing the electrical potential between the electrodes.

At very high magnetic field settings the electrons are forced back onto the cathode, preventing current flow. At the opposite extreme, with no field, the electrons are free to flow straight from the cathode to the anode. There is a point between the two extremes, the critical value or Hull cut-off magnetic field (and cut-off voltage), where the electrons just reach the anode. At fields around this point, the device operates similar to a triode. However, magnetic control, due to [[hysteresis]] and other effects, results in a slower and less faithful response to control current than electrostatic control using a control grid in a conventional triode (not to mention greater weight and complexity), so magnetrons saw limited use in conventional electronic designs.

It was noticed that when the magnetron was operating at the critical value, it would emit energy in the [[radio frequency]] spectrum. This occurs because a few of the electrons, instead of reaching the anode, continue to circle in the space between the cathode and the anode. Due to an effect now known as [[cyclotron radiation]], these electrons radiate radio frequency energy. The effect is not very efficient. Eventually the electrons hit one of the electrodes, so the number in the circulating state at any given time is a small percentage of the overall current. It was also noticed that the frequency of the radiation depends on the size of the tube, and even early examples were built that produced signals in the microwave regime.

Early conventional tube systems were limited to the [[high frequency]] bands, and although [[very high frequency]] systems became widely available in the late 1930s, the ultra high frequency and microwave bands were well beyond the ability of conventional circuits. The magnetron was one of the few devices able to generate signals in the microwave band and it was the only one that was able to produce high power at centimeter wavelengths.