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Formula One engines
This article gives an outline of Formula One engines, also called Formula One power units since the hybrid era starting in 2014. Since its inception in 1947, Formula One has used a variety of engine regulations. Formulae limiting engine capacity had been used in Grand Prix racing on a regular basis since after World War I. The engine formulae are divided according to era.
Formula One currently uses 1.6 litre four-stroke turbocharged 90 degree V6 double-overhead camshaft (DOHC) reciprocating engines. They were introduced in 2014 and have been developed over the subsequent seasons. Mostly from the 2023 season, specifications on Formula One engines, including the software used to control them and the maximum per-engine price to F1 teams of €15,000,000, have been frozen until the end of 2025, when the completely new 2026 spec will come into effect.
The history of F1 engines has always been a quest for more power, and the enormous power a Formula One engine produces had been generated by operating at a very high rotational speed, reaching over 20,000 revolutions per minute (rpm) during the 2004–2005 seasons. This is because an engine, theoretically, produces double the power when operated twice as fast if combustion (thermal) efficiency and energy loss remain the same. High-revving engines won races no matter how much fuel it consumed and how much wasted heat it generated, as long as they produced more power over the competition. However, with the skyrocketing cost of exotic materials and production methods enabling the high-speed operation, and the realisation that such advancements in technology would likely never applied to production vehicles (because the resultant product is very inefficient), it was decided to limit the maximum rotational speed (rev) to 19,000 rpm in 2007. The maximum rev was further limited to 18,000 rpm in 2009, and to 15,000 rpm for the 2014–2021 seasons.
Still, the high speed operation of F1 engines contrasts with road car engines of a similar size, which typically operate at less than 6,000 rpm.
The high-speed rotation created a vibration problem caused by secondary imbalance inherent in piston engines. Tony Rudd found in BRM 1.5L P56 V8 engine (11,000rpm redline) of 1961-1962 that a long conrod, much longer than required, was key to reducing the secondary vibration, enabling a high revolution. Coventry Climax FWMV Mk.III, using a much longer conrod in the same cylinder block as Mk.II, proved this concept in 1963. Other teams gradually found this secret, but this concept was not used in mass-produced cars for a long time until Daihatsu applied it to the extremely long-stroke 1.5L 3SZ-VE engine introduced with desaxe crankshaft, 4-valves, and variable valve timing in October 2005.
Notes:
Until the mid-1980s Formula One engines were limited to around 12,000 rpm due to the traditional metal springs used to close the valves. The speed required to close the valves at a higher rpm called for ever stiffer springs, which increased the power required to drive the camshaft to open the valves, to the point where the loss nearly offset the power gain through the increase in rpm. They were replaced by pneumatic valve springs introduced by Renault in 1986, which inherently have a rising rate (progressive rate) that allowed them to have an extremely high spring rate at larger valve strokes without much increasing the driving power requirements at smaller strokes, thus lowering the overall power loss. Since the 1990s, all Formula One engine manufacturers have used pneumatic valve springs with pressurised air.
In addition to the use of pneumatic valve springs, a Formula One engine's high rpm output has been made possible due to advances in metallurgy and design, allowing lighter pistons and connecting rods to withstand the accelerations necessary to attain such high speeds. Improved design also allows narrower connecting rod ends and so narrower main bearings. This permits higher rpm with less bearing-damaging heat build-up. For each stroke, the piston goes from a virtual stop to almost twice the mean speed (approximately 40 m/s), then back to zero. This occurs once for each of the four strokes in the cycle: one Intake (down), one Compression (up), one Power (ignition-down), one Exhaust (up). Maximum piston acceleration occurs at top dead center (TDC) and is in the region of 95,000 m/s2, about 9,700 times standard gravity (9,700 G).
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Formula One engines
This article gives an outline of Formula One engines, also called Formula One power units since the hybrid era starting in 2014. Since its inception in 1947, Formula One has used a variety of engine regulations. Formulae limiting engine capacity had been used in Grand Prix racing on a regular basis since after World War I. The engine formulae are divided according to era.
Formula One currently uses 1.6 litre four-stroke turbocharged 90 degree V6 double-overhead camshaft (DOHC) reciprocating engines. They were introduced in 2014 and have been developed over the subsequent seasons. Mostly from the 2023 season, specifications on Formula One engines, including the software used to control them and the maximum per-engine price to F1 teams of €15,000,000, have been frozen until the end of 2025, when the completely new 2026 spec will come into effect.
The history of F1 engines has always been a quest for more power, and the enormous power a Formula One engine produces had been generated by operating at a very high rotational speed, reaching over 20,000 revolutions per minute (rpm) during the 2004–2005 seasons. This is because an engine, theoretically, produces double the power when operated twice as fast if combustion (thermal) efficiency and energy loss remain the same. High-revving engines won races no matter how much fuel it consumed and how much wasted heat it generated, as long as they produced more power over the competition. However, with the skyrocketing cost of exotic materials and production methods enabling the high-speed operation, and the realisation that such advancements in technology would likely never applied to production vehicles (because the resultant product is very inefficient), it was decided to limit the maximum rotational speed (rev) to 19,000 rpm in 2007. The maximum rev was further limited to 18,000 rpm in 2009, and to 15,000 rpm for the 2014–2021 seasons.
Still, the high speed operation of F1 engines contrasts with road car engines of a similar size, which typically operate at less than 6,000 rpm.
The high-speed rotation created a vibration problem caused by secondary imbalance inherent in piston engines. Tony Rudd found in BRM 1.5L P56 V8 engine (11,000rpm redline) of 1961-1962 that a long conrod, much longer than required, was key to reducing the secondary vibration, enabling a high revolution. Coventry Climax FWMV Mk.III, using a much longer conrod in the same cylinder block as Mk.II, proved this concept in 1963. Other teams gradually found this secret, but this concept was not used in mass-produced cars for a long time until Daihatsu applied it to the extremely long-stroke 1.5L 3SZ-VE engine introduced with desaxe crankshaft, 4-valves, and variable valve timing in October 2005.
Notes:
Until the mid-1980s Formula One engines were limited to around 12,000 rpm due to the traditional metal springs used to close the valves. The speed required to close the valves at a higher rpm called for ever stiffer springs, which increased the power required to drive the camshaft to open the valves, to the point where the loss nearly offset the power gain through the increase in rpm. They were replaced by pneumatic valve springs introduced by Renault in 1986, which inherently have a rising rate (progressive rate) that allowed them to have an extremely high spring rate at larger valve strokes without much increasing the driving power requirements at smaller strokes, thus lowering the overall power loss. Since the 1990s, all Formula One engine manufacturers have used pneumatic valve springs with pressurised air.
In addition to the use of pneumatic valve springs, a Formula One engine's high rpm output has been made possible due to advances in metallurgy and design, allowing lighter pistons and connecting rods to withstand the accelerations necessary to attain such high speeds. Improved design also allows narrower connecting rod ends and so narrower main bearings. This permits higher rpm with less bearing-damaging heat build-up. For each stroke, the piston goes from a virtual stop to almost twice the mean speed (approximately 40 m/s), then back to zero. This occurs once for each of the four strokes in the cycle: one Intake (down), one Compression (up), one Power (ignition-down), one Exhaust (up). Maximum piston acceleration occurs at top dead center (TDC) and is in the region of 95,000 m/s2, about 9,700 times standard gravity (9,700 G).