Proximity fuze

A proximity fuze (or fuse[1][2][3]) is a fuze that detonates an explosive device automatically when the distance to the target becomes smaller than a predetermined value. Proximity fuzes are designed for targets such as planes, missiles, ships at sea, and ground forces. They provide a more sophisticated trigger mechanism than the common contact fuze or timed fuze. It is estimated that it increases the lethality by 5 to 10 times, compared to these other fuzes.[4]

Proximity fuze MK53 removed from shell, circa 1950s

Background

Before the invention of the proximity fuze, detonation was induced by direct contact, a timer set at launch or an altimeter. All of these earlier methods have disadvantages. The probability of a direct hit on a small moving target is low; a shell that just misses the target will not explode. A time- or height-triggered fuze requires good prediction by the gunner and accurate timing by the fuze. If either is wrong, then even accurately aimed shells may explode harmlessly before reaching the target or after passing it. At the start of The Blitz, it was estimated that it took 20,000 rounds to shoot down a single aircraft.[5] Other estimates put the figure as high as 100,000[6] or as low as 2,500 rounds for each aircraft.[7] With a proximity fuze, the shell or missile need only pass close by the target at some time during its flight. The proximity fuze makes the problem simpler than the previous methods.

Proximity fuzes are also useful for producing air bursts against ground targets. A contact fuze would explode when it hit the ground; it would not be very effective at scattering shrapnel. A timer fuze can be set to explode a few meters above the ground but the timing is vital and usually requires observers to provide information for adjusting the timing. Observers may not be practical in many situations, the ground may be uneven, and the practice is slow in any event. Proximity fuzes fitted to such weapons as artillery and mortar shells solve this problem by having a range of set burst heights [e.g. 2, 4 or 10 m (7, 13 or 33 ft)] above ground that are selected by gun crews. The shell bursts at the appropriate height above ground.

World War II

The idea of a proximity fuse had long been considered militarily useful. Several ideas had been considered, including optical systems that shone a light, sometimes infrared, and triggered when the reflection reached a certain threshold, various ground-triggered means using radio signals, and capacitive or inductive methods similar to a metal detector. All of these suffered from the large size of pre-WWII electronics and their fragility, as well as the complexity of the required circuitry.

British military researchers at the Telecommunications Research Establishment (TRE) Samuel C. Curran, William A. S. Butement, Edward S. Shire, and Amherst F. H. Thomson conceived of the idea of a proximity fuze in the early stages of World War II.[8] Their system involved a small, short range, Doppler radar. British tests were then carried out with "unrotated projectiles," in this case rockets. However, British scientists were uncertain whether a fuze could be developed for anti-aircraft shells, which had to withstand much higher accelerations than rockets. The British shared a wide range of possible ideas for designing a fuze, including a photoelectric fuze and a radio fuze, with United States during the Tizard Mission in late 1940. To work in shells, a fuze needed to be miniaturized, survive the high acceleration of cannon launch, and be reliable.[9]

The National Defense Research Committee assigned the task to the physicist Merle A. Tuve at the Department of Terrestrial Magnetism. Also eventually pulled in were researchers from the National Bureau of Standards (this research unit of NBS later became part of the Army Research Laboratory). Work was split in 1942, with Tuve's group working on proximity fuzes for shells, while the National Bureau of Standards researchers focused on the technically easier task of bombs and rockets. Work on the radio shell fuze was completed by Tuve's group, known as Section T, at The Johns Hopkins University Applied Physics Lab (APL).[10] Over 100 American companies were mobilized to build some 20 million shell fuzes.[11]

The proximity fuze was one of the most important technological innovations of World War II. It was so important that it was a secret guarded to a similar level as the atom bomb project or D-Day invasion.[12][13][14] Adm. Lewis L. Strauss wrote that,

"One of the most original and effective military developments in World War II was the proximity, or 'VT', fuze. It found use in both the Army and the Navy, and was employed in the defense of London. While no one invention won the war, the proximity fuze must be listed among the very small group of developments, such as radar, upon which victory very largely depended."[15]

The fuze was later found to be able to detonate artillery shells in air bursts, greatly increasing their anti-personnel effects.[16]

In Germany, more than 30 (perhaps as many as 50)[17] different proximity fuze designs were developed, or researched, for anti-aircraft use, but none saw service.[9] These included acoustic fuzes triggered by engine sound, one based on electrostatic fields developed by Rheinmetall Borsig, and radio fuzes. In mid-November 1939, a German neon lamp tube and a design of a prototype proximity fuze based on capacitive effects was received by British Intelligence as part of the Oslo Report.

In the post-World War II era, a number of new proximity fuze systems were developed, including radio, optical, and other means. A common form used in modern air-to-air weapons uses a laser as an optical source and time-of-flight for ranging.

Design in the UK

The first reference to the concept of radar in the UK was made by W. A. S. Butement and P. E. Pollard, who constructed a small breadboard model of a pulsed radar in 1931. They suggested the system would be useful for the coast artillery units, who could accurately measure the range to shipping even at night. The War Office proved uninterested in the concept and told the two to work on other issues.[18][19]

In 1936, the Air Ministry took over Bawdsey Manor to further develop their prototype radar systems that would emerge the next year as Chain Home. The Army was suddenly extremely interested in the topic of radar, and sent Butement and Pollard to Bawdsey to form what became known as the "Army Cell". Their first project was a revival of their original work on coast defense, but they were soon told to start a second project to develop a range-only radar to aid anti-aircraft guns.[20]

As these projects moved from development into prototype form in the late 1930s, Butement turned his attention to other concepts, and among these was the idea of a proximity fuse:

...Into this stepped W. A. S. Butement, designer of radar sets CD/CHL and GL, with a proposal on 30 October 1939 for two kinds of radio fuze: (1) a radar set would track the projectile, and the operator would transmit a signal to a radio receiver in the fuze when the range, the difficult quantity for the gunners to determine, was the same as that of the target and (2) a fuze would emit high-frequency radio waves that would interact with the target and produce, as a consequence of the high relative speed of target and projectile, a Doppler-frequency signal sensed in the oscillator.[21]

In May 1940 a formal proposal from Butement, Edward S. Shire, and Amherst F.H. Thompson was sent to the British Air Defence Establishment based on the second of the two concepts.[8] A breadboard circuit was constructed and the concept was tested in the laboratory by moving a sheet of tin at various distances. Early field testing connected the circuit to a thyratron trigger operating a tower-mounted camera which photographed passing aircraft to determine distance of fuze function.

Prototype fuzes were then constructed in June 1940, and installed in "unrotated projectiles", the British cover name for solid-fueled rockets, and fired at targets supported by balloons.[8] Rockets have relatively low acceleration and no spin creating centrifugal force, so the loads on the delicate electronic fuze are relatively benign. It was understood that the limited application was not ideal; a proximity fuze would be useful on all types of artillery and especially anti-aircraft artillery, but those had very high accelerations.

As early as September 1939, John Cockcroft began a development effort at Pye Ltd. to develop tubes capable of withstanding these much greater forces.[22] Pye's research was transferred to the United States as part of the technology package delivered by the Tizard Mission when the United States entered the war. Pye's group was apparently unable to get their rugged pentodes to function reliably under high pressures until 6 August 1941, which was after the successful tests by the American group.[23][24]

Looking for a short-term solution to the valve problem, in 1940 the British ordered 20,000 miniature tubes from Western Electric Company and Radio Corporation of America that were intended for use in hearing aids. An American team under Admiral Harold G. Bowen, Sr. correctly deduced that the tubes were meant for experiments with proximity fuzes for bombs and rockets.[9]

In September 1940, the Tizard Mission travelled to the US to introduce their researchers to a number of UK developments, and the topic of proximity fuses was raised. The details of the British experiments were passed to the United States Naval Research Laboratory and National Defense Research Committee (NDRC).[8] Information was also shared with Canada in 1940 and the National Research Council of Canada delegated work on the fuze to a team at the University of Toronto.[25]

Improvement in the US

Prior to and following receipt of circuitry designs from the British, various experiments were carried out by Richard B. Roberts, Henry H. Porter, and Robert B. Brode under the direction of NDRC Section T Chairman Merle Tuve.[8] Tuve's group was known as Section T, not APL, throughout the war.[26] As Tuve later put it in an interview: "We heard some rumors of circuits they were using in the rockets over in England, then they gave us the circuits, but I had already articulated the thing into the rockets, the bombs and shell."[24][27] As Tuve understood, the circuitry of the fuze was rudimentary. In his words, "The one outstanding characteristic in this situation is the fact that success of this type of fuze is not dependent on a basic technical idea—all of the ideas are simple and well known everywhere."[24] The critical work of adapting the fuze for anti-aircraft shells was done in the United States, not in England.[28] Tuve claimed that despite being pleased by the outcome of the Butement et al. vs. Varian patent suit (which saved the U.S. Navy millions of dollars), the fuze design delivered by the Tizard Mission was "not the one we made to work!"[29]

A key improvement was introduced by Lloyd Berkner, who developed a system using separate transmitter and receiver circuits. In December 1940, Tuve invited Harry Diamond and Wilbur S. Hinman, Jr, of the United States National Bureau of Standards (NBS) to investigate Berkner's improved fuze and develop a proximity fuze for rockets and bombs to use against the German Luftwaffe.[8][30][31]

In just two days, Diamond was able to come up with a new fuze design and managed to demonstrate its feasibility through extensive testing at the Naval Proving Ground at Dahlgren, Virginia.[32][33] On 6 May 1941, the NBS team built six fuzes which were placed in air-dropped bombs and successfully tested over water.[8]

Given their previous work on radio and radiosondes at NBS, Diamond and Hinman developed the first all solid-state radio doppler proximity fuze, which employed the Doppler effect of reflected radio waves using a diode detector arrangement that they devised.[31][34][35] The use of the Doppler effect developed by this group was later incorporated in all radio proximity fuzes for bomb, rocket, and mortar applications.[30] Later, the Ordnance Development Division of the National Bureau of Standards (which became the Harry Diamond Laboratories – and later merged into the Army Research Laboratory – in honor of its former chief in subsequent years) developed the first automated production techniques for manufacturing radio proximity fuzes at a low cost.[35]

While working for a defense contractor in the mid-1940s, Soviet spy Julius Rosenberg stole a working model of an American proximity fuze and delivered it to Soviet intelligence.[36] It was not a fuze for anti-aircraft shells, the most valuable type.[37]

In the US, NDRC focused on radio fuzes for use with anti-aircraft artillery, where acceleration was up to 20,000 g as opposed to about 100 g for rockets and much less for dropped bombs.[38] In addition to extreme acceleration, artillery shells were spun by the rifling of the gun barrels to close to 30,000 rpm, creating immense centrifugal force. Working with Western Electric Company and Raytheon Company, miniature hearing-aid tubes were modified to withstand this extreme stress. The T-3 fuze had a 52% success against a water target when tested in January, 1942. The United States Navy accepted that failure rate. A simulated battle conditions test was started on 12 August 1942. Gun batteries aboard cruiser USS Cleveland (CL-55) tested proximity-fuzed ammunition against radio-controlled drone aircraft targets over Chesapeake Bay. The tests were to be conducted over two days, but the testing stopped when drones were destroyed early on the first day. The three drones were destroyed with just four projectiles.[8][39]

A particularly successful application was the 90 mm shell with VT fuze with the SCR-584 automatic tracking radar and the M-9 electronic fire control computer. The combination of these three inventions was successful in shooting down many V-1 flying bombs aimed at London and Antwerp, otherwise difficult targets for anti-aircraft guns due to their small size and high speed.

VT (Variable Time)

The Allied fuze used constructive and destructive interference to detect its target.[40] The design had four or five tubes.[41] One tube was an oscillator connected to an antenna; it functioned as both a transmitter and an autodyne detector (receiver). When the target was far away, little of the oscillator's transmitted energy would be reflected to the fuze. When a target was nearby, it would reflect a significant portion of the oscillator's signal. The amplitude of the reflected signal corresponded to the closeness of the target.[notes 1] This reflected signal would affect the oscillator's plate current, thereby enabling detection.

However, the phase relationship between the oscillator's transmitted signal and the signal reflected from the target varied depending on the round trip distance between the fuze and the target. When the reflected signal was in phase, the oscillator amplitude would increase and the oscillator's plate current would also increase. But when the reflected signal was out of phase then the combined radio signal amplitude would decrease, which would decrease the plate current. So the changing phase relationship between the oscillator signal and the reflected signal complicated the measurement of the amplitude of that small reflected signal.

This problem was resolved by taking advantage of the change in frequency of the reflected signal. The distance between the fuze and the target was not constant but rather constantly changing due to the high speed of the fuze and any motion of the target. When the distance between the fuze and the target changed rapidly, then the phase relationship also changed rapidly. The signals were in-phase one instant and out-of-phase a few hundred microseconds later. The result was a heterodyne beat frequency which corresponded to the velocity difference. Viewed another way, the received signal frequency was Doppler-shifted from the oscillator frequency by the relative motion of the fuze and target. Consequently, a low frequency signal, corresponding to the frequency difference between the oscillator and the received signal, developed at the oscillator's plate terminal. Two of the four tubes in the VT fuze were used to detect, filter, and amplify this low frequency signal. Note here that the amplitude of this low frequency 'beat' signal corresponds to the amplitude of the signal reflected from the target. If the amplified beat frequency signal's amplitude was large enough, indicating a nearby object, then it triggered the 4th tube - a gas-filled thyratron. Upon being triggered, the thyratron conducted a large current that set off the electrical detonator.

In order to be used with gun projectiles, which experience extremely high acceleration and centrifugal forces, the fuze design also needed to utilize many shock hardening techniques. These included planar electrodes and packing the components in wax and oil to equalize the stresses.

The designation VT means variable time.[42] Captain S. R. Shumaker, Director of the Bureau of Ordnance's Research and Development Division, coined the term to be descriptive without hinting at the technology.[43]

Development

The anti-aircraft artillery range at Kirtland Air Force Base in New Mexico was used as one of the test facilities for the proximity fuze, where almost 50,000 test firings were conducted from 1942 to 1945.[44] Testing also occurred at Aberdeen Proving Ground in Maryland, where about 15,000 bombs were fired.[34] Other locations include Ft. Fisher in North Carolina and Blossom Point, Maryland.

US Navy development and early production was outsourced to the Wurlitzer company, at their barrel organ factory in North Tonawanda, New York.[45]

Production

First large scale production of tubes for the new fuzes[8] was at a General Electric plant in Cleveland, Ohio formerly used for manufacture of Christmas-tree lamps. Fuze assembly was completed at General Electric plants in Schenectady, New York and Bridgeport, Connecticut.[46] Once inspections of the finished product were complete, a sample of the fuzes produced from each lot was shipped to the National Bureau of Standards, where they were subjected to a series of rigorous tests at the specially built Control Testing Laboratory.[34] These tests included low- and high-temperature tests, humidity tests, and sudden jolt tests.

By 1944, a large proportion of the American electronics industry concentrated on making the fuzes. Procurement contracts increased from $60 million in 1942, to $200 million in 1943, to $300 million in 1944 and were topped by $450 million in 1945. As volume increased, efficiency came into play and the cost per fuze fell from $732 in 1942 to $18 in 1945. This permitted the purchase of over 22 million fuzes for approximately one billion dollars. The main suppliers were Crosley, RCA, Eastman Kodak, McQuay-Norris and Sylvania. There were also over two thousand suppliers and subsuppliers, ranging from powder manufacturers to machine shops.[47][48] It was among the first mass-production applications of printed circuits.[49]

Deployment

Vannevar Bush, head of the U.S. Office of Scientific Research and Development (OSRD) during the war, credited the proximity fuze with three significant effects.[50]

  • It was important in defense from Japanese Kamikaze attacks in the Pacific. Bush estimated a sevenfold increase in the effectiveness of 5-inch antiaircraft artillery with this innovation.[51]
  • It was an important part of the radar-controlled antiaircraft batteries that finally neutralized the German V-1 attacks on England.[51]
  • It was used in Europe starting in the Battle of the Bulge where it was very effective in artillery shells fired against German infantry formations, and changed the tactics of land warfare.

At first the fuzes were only used in situations where they could not be captured by the Germans. They were used in land-based artillery in the South Pacific in 1944. Also in 1944, fuzes were allocated to the British Army's Anti-Aircraft Command, that was engaged in defending Britain against the V-1 flying bomb. As most of the British heavy anti-aircraft guns were deployed in a long, thin coastal strip, dud shells fell into the sea, safely out of reach of capture. Over the course of the German V-1 campaign, the proportion of flying bombs flying through the coastal gun belt that were destroyed rose from 17% to 74%, reaching 82% during one day. A minor problem encountered by the British was that the fuzes were sensitive enough to detonate the shell if it passed too close to a seabird and a number of seabird "kills" were recorded.[52]

The Pentagon refused to allow the Allied field artillery use of the fuzes in 1944, although the United States Navy fired proximity-fuzed anti-aircraft shells during the July 1943 invasion of Sicily.[53] After General Dwight D. Eisenhower demanded he be allowed to use the fuzes, 200,000 shells with VT fuzes or (code named "POZIT"[54]) were used in the Battle of the Bulge in December 1944. They made the Allied heavy artillery far more devastating, as all the shells now exploded just before hitting the ground.[55] German divisions were caught out in open as they had felt safe from timed fire because it was thought that the bad weather would prevent accurate observation. U.S. General George S. Patton credited the introduction of proximity fuzes with saving Liege and stated that their use required a revision of the tactics of land warfare.[56]

Bombs and rockets fitted with radio proximity fuzes were in limited service with both the USAAF and USN at the end of WW2.  The main targets for these proximity fuze detonated bombs and rockets were anti-aircraft emplacements and airfields.[57]

Sensor types

Radio

Radio frequency sensing is the main sensing principle for artillery shells.

The device described in World War II patent[58] works as follows: The shell contains a micro-transmitter which uses the shell body as an antenna and emits a continuous wave of roughly 180–220 MHz. As the shell approaches a reflecting object, an interference pattern is created. This pattern changes with shrinking distance: every half wavelength in distance (a half wavelength at this frequency is about 0.7 meters), the transmitter is in or out of resonance. This causes a small cycling of the radiated power and consequently the oscillator supply current of about 200–800 Hz, the Doppler frequency. This signal is sent through a band pass filter, amplified, and triggers the detonation when it exceeds a given amplitude.

Optical

Optical sensing was developed in 1935, and patented in Great Britain in 1936, by a Swedish inventor, probably Edward W. Brandt, using a petoscope. It was first tested as a part of a detonation device for bombs that were to be dropped over bomber aircraft, part of the UK's Air Ministry's "bombs on bombers" concept. It was considered (and later patented by Brandt) for use with anti-aircraft missiles fired from the ground. It used then a toroidal lens, that concentrated all light from a plane perpendicular to the missile's main axis onto a photo cell. When the cell current changed a certain amount in a certain time interval, the detonation was triggered.

Some modern air-to-air missiles (e.g. the ASRAAM and AA-12 Adder) use lasers to trigger detonation. They project narrow beams of laser light perpendicular to the flight of the missile. As the missile cruises towards its target the laser energy simply beams out into space. As the missile passes its target some of the energy strikes the target and is reflected to the missile, where detectors sense it and detonate the warhead.

Acoustic

Acoustic proximity fuzes are actuated by the acoustic emissions from a target (example an aircraft's engine or ship's propeller).  Actuation can be either through an electronic circuit coupled to a microphone, or hydrophone, or mechanically using a resonating vibratory reed connected to diaphragm tone filter. [59] [60]

During WW2, the Germans had at least five acoustic fuzes for anti-aircraft use under development, though none saw operational service.   The most developmentally advanced of the German acoustic fuze designs was the Rheinmetall-Borsig Kranich (German for Crane) which was a mechanical device utilizing a diaphragm tone filter sensitive to frequencies between 140 and 500Hz connected to a resonating vibratory reed switch used to fire an electrical igniter.  The Schmetterling, Enzian, Rheintochter and X4 guided missiles were all designed for use with the Kranich acoustic proximity fuze. [59] [61]

During WW2, the National Defense Research Committee (NDRC) investigated the use of acoustic proximity fuzes for anti-aircraft weapons but concluded that there were more promising technological approaches.  The NDRC research highlighted the speed of sound as a major limitation in the design and use of acoustic fuzes, particularly in relation to missiles and high-speed aircraft.[60]

Hydroacoustic influence is widely used as a detonation mechanism for naval mines and torpedoes. A ship's propeller rotating in water produces a powerful hydroacoustic noise which can be picked up using a hydrophone and used for homing and detonation. Influence firing mechanisms often use a combination of acoustic and magnetic induction receivers.[62] [63]

Magnetic
German World War II magnetic mine that landed on the ground instead of the water.
Main article: Magnetic proximity fuze

Magnetic sensing can only be applied to detect huge masses of iron such as ships. It is used in mines and torpedoes. Fuzes of this type can be defeated by degaussing, using non-metal hulls for ships (especially minesweepers) or by magnetic induction loops fitted to aircraft or towed buoys.

Pressure

Some naval mines use pressure fuzes which are able to detect the pressure wave of a ship passing overhead. Pressure sensors are usually used in combination with other fuze detonation technologies such as acoustic and magnetic induction.[63]

During WW2, pressure activated fuzes were developed for sticks (or trains) of bombs to create above ground airbursts.  The first bomb in the stick was fitted with an impact fuze while the other bombs were fitted with pressure sensitive diaphragm actuated detonators.  The blast from the first bomb was used to trigger the fuze of the second bomb which would explode above ground and in this turn would detonate the third bomb with the process repeated all the way till the last bomb in the string.  Due to the forward speed of the bomber, bombs fitted with pressure detonators would all explode at about the same height above ground along a horizontal trajectory.  This design was used in both the British No44 “Pistol” and the German Rheinmetall-Borsig BAZ 55A fuzes.[59] [60]

  • 120mm HE mortar shell fitted with proximity fuze
  • 120mm HE mortar shell fitted with M734 proximity fuze
  • 60mm HE mortar shell fitted with proximity fuze
  • A 155mm artillery fuze with selector for point/proximity detonation (currently set to proximity).

See also

Notes
  1. The return signal is inversely proportional to the fourth power of the distance.

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  59. Hogg, Ian (1999). German Secret Weapons of the Second World War. Frontline Books. pp. 120–122. ISBN 978-1-8483-2781-8.
  60. "Chapter 2 Proximity and Time Fuzes". Summary Technical Report of the National Defence Research Council (PDF) (Report). 1946. pp. 17–18.
  61. Zaloga, Steven (2019). German Guided Missiles of World War II. Bloomsbury Publishing. ISBN 978-1-4728-3179-8.
  62. Beloshitskiy, V.P; Baginskiy, Yu.M (1960). Oruzhiye Podvodnogo Udara (Underwater Weapons) (Report). Military Publishing House.
  63. Erickson, Andrew; Goldstein, Lyle; Murray, William (2009). Chinese Mine Warfare. Naval War College. pp. 12–17. ISBN 978-1-884733-63-5.

Bibliography
  • Baldwin, Ralph B. (1980), The Deadly Fuze: The Secret Weapon of World War II, San Rafael, CA: Presidio Press, ISBN 978-0-89141-087-4. Baldwin was a member of the (APL) team headed by Tuve that did most of the design work.
  • Baxter, James Phinney III (1968) [1946], Scientists Against Time, Cambridge, MA: MIT Press, ISBN 978-0-262-52012-6
  • Bureau of Ordnance (15 May 1946), VT Fuzes For Projectiles and Spin-Stabilized Rockets, Ordnance Pamphlet, OP 1480, U. S. Navy Bureau of Ordnance
  • Bush, Vannevar (1970), Pieces of the Action, New York: William Morrow and Company, Inc.
  • Gibbs, Jay (2004). "Question 37/00: Effectiveness of Shipboard Anti-Aircraft Fire". Warship International. XLI (1): 29. ISSN 0043-0374.
  • Holmes, Jamie (2020), 12 Seconds of Silence: How a Team of Inventors, Tinkerers, and Spies Took Down a Nazi Superweapon, Boston, MA: Houghton Mifflin Harcourt.
  • Hogg, Ian V. (2002), British & American Artillery of World War Two (revised ed.), Greenhill Books, ISBN 978-1-85367-478-5
  • Sharpe, Edward A. (2003), "The Radio Proximity Fuze: A survey", Vintage Electrics, 2 (1)

Further reading
  • Allard, Dean C. (1982), "The Development of the Radio Proximity Fuze" (PDF), Johns Hopkins APL Technical Digest, 3 (4): 358–59
  • Bennett, Geoffrey (1976), "The Development of the Proximity Fuze", Journal of the Royal United Service Institution, 121 (1): 57–62, ISSN 0953-3559
  • Collier, Cameron D. (1999), "Tiny Miracle: the Proximity Fuze", Naval History, U. S. Naval Institute, 13 (4): 43–45, ISSN 1042-1920
  • Fuzes, Proximity, Electrical: Part One (PDF), Engineering Design Handbook: Ammunition Series, United States Army Materiel Command, July 1963, AMCP 706-211
  • Fuzes, Proximity, Electrical: Part Two, Engineering Design Handbook: Ammunition Series, United States Army Materiel Command, AMCP 706-212
  • Fuzes, Proximity, Electrical: Part Three, Engineering Design Handbook: Ammunition Series, United States Army Materiel Command, AMCP 706-213
  • Fuzes, Proximity, Electrical: Part Four, Engineering Design Handbook: Ammunition Series, United States Army Materiel Command, AMCP 706-214
  • Fuzes, Proximity, Electrical: Part Five, Engineering Design Handbook: Ammunition Series, United States Army Materiel Command, August 1963, AMCP 706-215
  • US 3166015, Tuve, Merle A. & Richard B. Roberts, "Radio Proximity Fuze", issued 19 January 1965, assigned to United States of America
  • Allen, Kevin. "Artillery Proximity Fuses". Warfare History Network. Retrieved 4 June 2018.
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