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Metrovick F.1
Metrovick F.2 Freda
Metrovick F.2/4 Beryl
Metropolitan-Vickers F.2 / Beryl
Metropolitan-Vickers F.5




Alan Arnold Griffith published a seminal paper in 1926, An Aerodynamic Theory of Turbine Design, that for the first time clearly demonstrated that a gas turbine could be used as a practical, and even desirable, aircraft powerplant. The paper started by demonstrating that existing axial compressor designs were "flying stalled" due to their use of flat blades, and that dramatic improvements could be made by using aerofoil designs instead, improvements that made a gas turbine practical. It went on to outline a complete compressor and turbine design, using the extra exhaust power to drive a second turbine that would power a propeller. In today's terminology the design was a turboprop. In order to prove the design, Griffith and several other engineers at the Royal Aircraft Establishment built a testbed example of the compressor in 1928 known as Anne, the machinery being built for them by Fraser and Chalmers. After Anne's successful testing they planned to follow this up with a complete engine known as Betty.

In 1929 Frank Whittle's thesis on pure jet engines was published, and sent to Griffith for comment. After pointing out an error in Whittle's mathematics, he went on to deride the entire concept, saying that the centrifugal compressor Whittle used would be impractical for aircraft use due to its large frontal area, and that the use of the jet exhaust directly for power would be extremely inefficient. Whittle was distraught, but was convinced that he should patent the idea anyway. Five years later a group of investors persuaded him to start work on what would be the first working British jet engine.

Griffith continued development of his own concepts, eventually developing an advanced compressor design using two contra-rotating stages that improved efficiency. His partner, Hayne Constant, started discussions in 1937 with Manchester-based Metrovick, a maker of steam turbines, to produce the new machinery. Incidentally, Metrovick had recently merged with British Thomson-Houston, another turbine builder who were supporting Whittle's efforts.

A contract for development work was eventually given by the Air Ministry the next year, and work on Betty, also known as the B.10, started. In 1939 the team, including Metrovick engineers led by David Smith, started work on a flyable design, the F.1. Compared to the centrifugal-flow Whittle designs, the F.1 was extremely advanced, using a nine-stage axial compressor, annular combustion chamber, and a two-stage turbine (the second driving a propeller).

In April 1939, Whittle gave a startling demonstration of his experimental engine, the WU, running it for 20 minutes at high power. This led to a rash of contracts to build a production quality design suitable for aircraft use. Development had just started on the F.1 when Whittle started building his W.1 design, planning to install one for flight in the Gloster E.28/39 the next year. Smith decided to end development of the F.1 and move on to a pure-jet instead, starting work on the otherwise similar F.2, Freda, in July 1940.

Development of the F.2 progressed rapidly, and the engine ran for the first time in November 1941. By this point there were a number of engines in development based on the Whittle concept, but the F.2 looked considerably more capable than any of them. Flyable versions, the F.2/1, received its test rating in 1942 and were flown on an Avro Lancaster test-bed (the first prototype Lancaster, s/n BT308) on 29 June 1943, mounted in the rear fuselage. Production quality versions were tested on the F.9/40M (Gloster Meteor) s/n DG204/G which made its first flight on November 13, 1943. These were installed in Messerschmitt Me 262 type underslung nacelles.

As expected, the engines were more powerful than the Whittle design, first delivering 1,800 lbf (8 kN) but soon scaling up to well over 2,000 lbf (8.9 kN). Around this time, the Whittle W.2B was developing 1,600 lbf (7.11 kN). However, the engine suffered from a number of problems that cast doubts on its reliability. These were primarily due to hot spots building up on the turbine bearing and combustion chamber. The latter, in turn, caused warping and fractures of the turbine inlet nozzles.

To address these problems, in August 1942 a minor redesign delivered the F.2/2, which changed the turbine material from Rex 75 to Nimonic 75, and lengthened the combustion chamber by 6 inches (150 mm). Thrust was improved to 2,400 lbf (11,000 N) static, but the problems with overheating remained.

Another attempt to solve the overheating problems resulted in the more highly modified F.2/3 during 1943. This version replaced the original annular combustion chamber with can-type burners like those on the Whittle designs. This appears to have solved the problems, raising the thrust to 2,700 lbf (12,000 N) in the process. However, by this time it was decided to move on to a much more powerful version of the engine.

Development of the F.2 continued on a version using a ten-stage compressor for additional airflow driven by a single stage turbine. The new F.2/4 - the Beryl - initially developed 3,250 lbf (14.45 kN) and was test flown in Avro Lancaster Mk.II s/n LL735 before being installed in the Saunders-Roe SR.A/1 flying boat fighter. Thrust had already improved to 3,850 lbf (17.1 kN) for the third prototype, and eventually settled at 4,000 lbf (17.8 kN). In comparison, the Derwent developed only 10.9 kN in its ultimate form; making the Beryl one of the most powerful engines of the era. Development of the SR.A/1 ended in 1947, ending development of the Beryl along with it. Nevertheless a Beryl from the SR.A/1 prototype was removed and used by Donald Campbell for early runs in his famous 1955 Bluebird K7 hydroplane in which he set seven water speed records between 1955 and 1964.

In 1942 MV started work on thrust augmentation. The resulting Metropolitan-Vickers F.3 was the first British turbofan engine to be designed, built and tested. Indeed, it could be said that the F.3 was also the very first 3-shaft jet engine to be built, although the configuration was completely different to that of the much later Rolls-Royce RB211 turbofan series, since the fan was located at the rear of the engine, not unlike that of the General Electric CJ805-23. Using a stock F.2/2, MV added a separate module to the rear of the engine (directly behind the HP turbine) which comprised contra-rotating LP turbines attached to two contra-rotating fans. Apart from the first stage nozzle guide vanes, the LP turbine was completely statorless, with four consecutive rotor stages. Rotors 1 and 3 drove the front fan clockwise (viewed from front), whereas the rear fan was driven anticlockwise by rotors 2 and 4. Although the front fan had inlet guide vanes, there were no vanes between the contra-rotating fan rotors or, downstream, any exit guide vanes. The core and bypass streams exhausted through separate coaxial propelling nozzles.

The project was generally successful, raising static thrust from around 2,400 lbf (11,000 N) to 4,000 lbf (18 kN). More importantly, specific fuel consumption fell from 1.05 to 0.65 lb/hr/lbf, which was the true aim of the project. The weight increase for all the extra turbomachinery and ducting was fairly significant, however. A bonus was that the team noticed that the cold air from the fan mixed with the hot exhaust from the gas generator, resulted in a marked decrease in noise levels, the first time such an effect had been recorded (it was re-discovered during a major NASA project in the 1960s).

Although the F.3 progressed nicely, development was curtailed by the pressures of war. When the war ended the F.2/2 was no longer current, so some of the ideas were applied to the more up-to-date F.2/4 to produce the Metropolitan-Vickers F.5 propfan.

Following on where the F.3 left off, the F.5 was a version of the F.2/4 with an open rotor (unducted) thrust augmenter added to the end of the jet pipe, somewhat remote from the HP turbine The 5 ft 6 in diameter fixed pitch propellers, which contra-rotated, were driven by a 4-stage statorless LP turbine unit, similar to that of the F.3. The General Electric GE36 UDF demonstrator of the 1980s also used a similar LP turbine arrangement, albeit with many more stages. In addition, the GE36 propellers were variable pitch. With both propfans, the LP turbine arrangement enabled the propellers to rotate at optimum speed, without the need for a reduction gearbox.

Static thrust increased from the 3500lbf of the F.2/2 to in excess of 4,710 lbf (21,000 N), with a corresponding reduction in specific fuel consumption. Relative to the parent turbojet, the weight increase for this propfan configuration was about 26%, compared to 53% for the F.3 turbofan.
Unfortunately, the company cancelled development when they sold their gas turbine business to Armstrong Siddeley in 1946.

Development of the F.2 ended in 1944. Development of the basic concept continued, however, eventually leading to the considerably larger F.9 Sapphire. However, in 1947, Metrovick left jet engine production and their design team moved to Armstrong Siddeley. The Sapphire matured into a successful design, initially besting the power of its Rolls-Royce contemporary, the Avon. Design features of the Metrovick line were worked into Armstrong Siddeley's own line of axial compressor turboprops, although Armstrong Siddeley dropped Metrovick's use of gemstone names for their engines in favour of continuing with animal names, in particular snakes.



Type: Axial flow turbojet
Length: 159 in (4,038.6 mm)
Diameter: 34.9 in (886.5 mm)
Dry weight: ~1,500 lb (680.4 kg)
Compressor: 9-stage axial flow compressor
Combustors: 1x Annular stainless steel combustion chamber
Turbine: 2-stage axial flow turbine
Fuel type: Kerosene (R.D.E. / F / KER)
Maximum thrust: 2,400 lbf (10.68 kN) at sea level static, take-off
Overall pressure ratio: 3.5:1
Turbine inlet temperature: 1,382 °F (750 °C)
Specific fuel consumption: 1.07 lb/lbf/hr (30.31g/s/KN)
Thrust-to-weight ratio: ~1.6:1


F.2/4 Beryl
Type: Axial flow turbojet
Length: 159 in (4,038.6 mm)
Diameter: 36.7 in (932.2 mm)
Dry weight: 1,750 lb (793.8 kg)
Compressor: 10-stage axial flow compressor
Combustors: cannular combustion chamber
Turbine: Single stage axial flow turbine
Fuel type: Kerosene (R.D.E. / F / KER)
Oil system: 1 x Pleesey 8-feed pressure spray at 650 psi (4,481.6 kPa) dry sump, 80 S.U. secs (10.2 cs) (D.E.D. 2472D) grade oil
Maximum thrust: 3,500 lbf (15.57 kN) at 7,700 rpm at sea level for take-off
Overall pressure ratio: 4:1
Turbine inlet temperature: 1,472 °F (800 °C)
Specific fuel consumption: 1.05 lb/lbf/hr (29.74g/s/KN)
Thrust-to-weight ratio: 2:1
Military thrust, static: 3,300 lbf (14.68 kN) at 18,000 rpm at sea level
Cruising thrust, static: 2,970 lbf (13.21 kN) at 7,300 rpm at sea level
Idling thrust, static: 200 lbf (0.89 kN) at 2,560 rpm at sea level


Type: Axial flow turbofan
Length: ~140 in (3,556.0 mm)
Diameter: ~46 in (1,168.4 mm) fan; ; ~34.9 in (886.5 mm) gas generator
Dry weight: ~2300lb (1043kg)
Compressor: 9-stage axial flow compressor;2-stage contra-rotating aft fan
Combustors: 1x Annular stainless steel combustion chamber
Turbine: 2-stage axial flow HP turbine; close-coupled, 4-stage statorless contra-rotating LP turbine
Fuel type: Kerosene (R.D.E. / F / KER)
Maximum thrust: 4,000 lbf (17.79 kN) at sea level static, take-off
Overall pressure ratio: 3.5:1
Bypass ratio: ~2.9
Turbine inlet temperature: ~ 1,382 °F (750 °C)
Specific fuel consumption: ~0.65 lb/lbf/hr (18.41g/s/KN)
Thrust-to-weight ratio: ~1.739


Type: Axial flow turboprop
Length: 146.25 in (3,714.8 mm)
Diameter: ~66 in (1,676.4 mm)propeller; ~37.25 in (946.2 mm) gas generator
Dry weight: 2200 lb (998kg)
Compressor: 10-stage axial flow compressor; 2-stage contra-rotating aft propeller
Combustors: cannular combustion chamber
Turbine: Single-stage axial flow HP turbine; 4-stage statorless contra-rotating power turbine
Fuel type: Kerosene (R.D.E. / F / KER)
Maximum thrust: 4,710 lbf (20.95 kN) at Mach 0.067 , sea level, take-off
Overall pressure ratio: 4:1
Turbine inlet temperature: ~ 1,473 °F (801 °C)
Thrust-to-weight ratio: ~2.14




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