Thrust-specific fuel consumption (TSFC) is the fuel efficiency of an engine design with respect to thrust output. TSFC may also be thought of as fuel consumption (grams/second) per unit of thrust (newtons, or N), hence thrust-specific. This figure is inversely proportional to specific impulse, which is the amount of thrust produced per unit fuel consumed.
TSFC or SFC for thrust engines (e.g. turbojets, turbofans, ramjets, rockets, etc.) is the mass of fuel needed to provide the net thrust for a given period e.g. lb/(h·lbf) (pounds of fuel per hour-pound of thrust) or g/(s·kN) (grams of fuel per second-kilonewton). Mass of fuel is used, rather than volume (gallons or litres) for the fuel measure, since it is independent of temperature. [1]
Specific fuel consumption of air-breathing jet engines at their maximum efficiency is more or less proportional to exhaust speed. The fuel consumption per mile or per kilometre is a more appropriate comparison for aircraft that travel at very different speeds.[ citation needed ] There also exists power-specific fuel consumption, which equals the thrust-specific fuel consumption divided by speed. It can have units of pounds per hour per horsepower.
SFC is dependent on engine design, but differences in the SFC between different engines using the same underlying technology tend to be quite small. Increasing overall pressure ratio on jet engines tends to decrease SFC.
In practical applications, other factors are usually highly significant in determining the fuel efficiency of a particular engine design in that particular application. For instance, in aircraft, turbine (jet and turboprop) engines are typically much smaller and lighter than equivalently powerful piston engine designs, both properties reducing the levels of drag on the plane and reducing the amount of power needed to move the aircraft. Therefore, turbines are more efficient for aircraft propulsion than might be indicated by a simplistic look at the table below.
SFC varies with throttle setting, altitude, climate. For jet engines, air flight speed is an important factor too. Air flight speed counteracts the jet's exhaust speed. (In an artificial and extreme case with the aircraft flying exactly at the exhaust speed, one can easily imagine why the jet's net thrust should be near zero.) Moreover, since work is force (i.e., thrust) times distance, mechanical power is force times speed. Thus, although the nominal SFC is a useful measure of fuel efficiency, it should be divided by speed when comparing engines at different speeds.
For example, Concorde cruised at 1354 mph, or 7.15 million feet per hour, with its engines giving an SFC of 1.195 lb/(lbf·h) (see below); this means the engines transferred 5.98 million foot pounds per pound of fuel (17.9 MJ/kg), equivalent to an SFC of 0.50 lb/(lbf·h) for a subsonic aircraft flying at 570 mph, which would be better than even modern engines; the Olympus 593 used in the Concorde was the world's most efficient jet engine. [2] [3] However, Concorde ultimately has a heavier airframe and, due to being supersonic, is less aerodynamically efficient, i.e., the lift to drag ratio is far lower. In general, the total fuel burn of a complete aircraft is of far more importance to the customer.
This section may be confusing or unclear to readers. In particular, Unclear what the table is all about. How should it be used? For what should it be used? If it is supposed to state the units for different quantities, then established definitions for unit name, unit symbol, quantity name and so on should be used. See examples in the International System of units article: https://en.wikipedia.org/wiki/International_System_of_Units#Derived_units.(February 2020) |
Specific impulse (by weight) | Specific impulse (by mass) | Effective exhaust velocity | Specific fuel consumption | |
---|---|---|---|---|
SI | =X seconds | =9.8066 X N·s/kg | =9.8066 X m/s | =101,972 (1/X) g/(kN·s) / {g/(kN·s)=s/m} |
Imperial units | =X seconds | =X lbf·s/lb | =32.16 X ft/s | =3,600 (1/X) lb/(lbf·h) |
Rocket engines in vacuum | |||||||
---|---|---|---|---|---|---|---|
Model | Type | First run | Application | TSFC | Isp (by weight) | Isp(by weight) | |
lb/lbf·h | g/kN·s | s | m/s | ||||
Merlin 1D | liquid fuel | 2013 | Falcon 9 | 12 | 330 | 310 | 3000 |
Avio P80 | solid fuel | 2006 | Vega stage 1 | 13 | 360 | 280 | 2700 |
Avio Zefiro 23 | solid fuel | 2006 | Vega stage 2 | 12.52 | 354.7 | 287.5 | 2819 |
Avio Zefiro 9A | solid fuel | 2008 | Vega stage 3 | 12.20 | 345.4 | 295.2 | 2895 |
RD-843 | liquid fuel | Vega upper stage | 11.41 | 323.2 | 315.5 | 3094 | |
Kuznetsov NK-33 | liquid fuel | 1970s | N-1F, Soyuz-2-1v stage 1 | 10.9 | 308 | 331 [4] | 3250 |
NPO Energomash RD-171M | liquid fuel | Zenit-2M, -3SL, -3SLB, -3F stage 1 | 10.7 | 303 | 337 | 3300 | |
LE-7A | cryogenic | H-IIA, H-IIB stage 1 | 8.22 | 233 | 438 | 4300 | |
Snecma HM-7B | cryogenic | Ariane 2, 3, 4, 5 ECA upper stage | 8.097 | 229.4 | 444.6 | 4360 | |
LE-5B-2 | cryogenic | H-IIA, H-IIB upper stage | 8.05 | 228 | 447 | 4380 | |
Aerojet Rocketdyne RS-25 | cryogenic | 1981 | Space Shuttle, SLS stage 1 | 7.95 | 225 | 453 [5] | 4440 |
Aerojet Rocketdyne RL-10B-2 | cryogenic | Delta III, Delta IV, SLS upper stage | 7.734 | 219.1 | 465.5 | 4565 | |
NERVA NRX A6 | nuclear | 1967 | 869 |
Jet engines with Reheat, static, sea level | |||||||
---|---|---|---|---|---|---|---|
Model | Type | First run | Application | TSFC | Isp (by weight) | Isp(by weight) | |
lb/lbf·h | g/kN·s | s | m/s | ||||
Turbo-Union RB.199 | turbofan | Tornado | 2.5 [6] | 70.8 | 1440 | 14120 | |
GE F101-GE-102 | turbofan | 1970s | B-1B | 2.46 | 70 | 1460 | 14400 |
Tumansky R-25-300 | turbojet | MIG-21bis | 2.206 [6] | 62.5 | 1632 | 16000 | |
GE J85-GE-21 | turbojet | F-5E/F | 2.13 [6] | 60.3 | 1690 | 16570 | |
GE F110-GE-132 | turbofan | F-16E/F | 2.09 [6] | 59.2 | 1722 | 16890 | |
Honeywell/ITEC F125 | turbofan | F-CK-1 | 2.06 [6] | 58.4 | 1748 | 17140 | |
Snecma M53-P2 | turbofan | Mirage 2000C/D/N | 2.05 [6] | 58.1 | 1756 | 17220 | |
Snecma Atar 09C | turbojet | Mirage III | 2.03 [6] | 57.5 | 1770 | 17400 | |
Snecma Atar 09K-50 | turbojet | Mirage IV, 50, F1 | 1.991 [6] | 56.4 | 1808 | 17730 | |
GE J79-GE-15 | turbojet | F-4E/EJ/F/G, RF-4E | 1.965 | 55.7 | 1832 | 17970 | |
Saturn AL-31F | turbofan | Su-27/P/K | 1.96 [7] | 55.5 | 1837 | 18010 | |
GE F110-GE-129 | turbofan | F-16C/D, F-15EX | 1.9 [6] | 53.8 | 1895 | 18580 | |
Soloviev D-30F6 | turbofan | MiG-31, S-37/Su-47 | 1.863 [6] | 52.8 | 1932 | 18950 | |
Lyulka AL-21F-3 | turbojet | Su-17, Su-22 | 1.86 [6] | 52.7 | 1935 | 18980 | |
Klimov RD-33 | turbofan | 1974 | MiG-29 | 1.85 | 52.4 | 1946 | 19080 |
Saturn AL-41F-1S | turbofan | Su-35S/T-10BM | 1.819 | 51.5 | 1979 | 19410 | |
Volvo RM12 | turbofan | 1978 | Gripen A/B/C/D | 1.78 [6] | 50.4 | 2022 | 19830 |
GE F404-GE-402 | turbofan | F/A-18C/D | 1.74 [6] | 49 | 2070 | 20300 | |
Kuznetsov NK-32 | turbofan | 1980 | Tu-144LL, Tu-160 | 1.7 | 48 | 2100 | 21000 |
Snecma M88-2 | turbofan | 1989 | Rafale | 1.663 | 47.11 | 2165 | 21230 |
Eurojet EJ200 | turbofan | 1991 | Eurofighter | 1.66–1.73 | 47–49 [8] | 2080–2170 | 20400–21300 |
Dry jet engines, static, sea level | |||||||
---|---|---|---|---|---|---|---|
Model | Type | First run | Application | TSFC | Isp (by weight) | Isp(by weight) | |
lb/lbf·h | g/kN·s | s | m/s | ||||
GE J85-GE-21 | turbojet | F-5E/F | 1.24 [6] | 35.1 | 2900 | 28500 | |
Snecma Atar 09C | turbojet | Mirage III | 1.01 [6] | 28.6 | 3560 | 35000 | |
Snecma Atar 09K-50 | turbojet | Mirage IV, 50, F1 | 0.981 [6] | 27.8 | 3670 | 36000 | |
Snecma Atar 08K-50 | turbojet | Super Étendard | 0.971 [6] | 27.5 | 3710 | 36400 | |
Tumansky R-25-300 | turbojet | MIG-21bis | 0.961 [6] | 27.2 | 3750 | 36700 | |
Lyulka AL-21F-3 | turbojet | Su-17, Su-22 | 0.86 | 24.4 | 4190 | 41100 | |
GE J79-GE-15 | turbojet | F-4E/EJ/F/G, RF-4E | 0.85 | 24.1 | 4240 | 41500 | |
Snecma M53-P2 | turbofan | Mirage 2000C/D/N | 0.85 [6] | 24.1 | 4240 | 41500 | |
Volvo RM12 | turbofan | 1978 | Gripen A/B/C/D | 0.824 [6] | 23.3 | 4370 | 42800 |
RR Turbomeca Adour | turbofan | 1999 | Jaguar retrofit | 0.81 | 23 | 4400 | 44000 |
Honeywell/ITEC F124 | turbofan | 1979 | L-159, X-45 | 0.81 [6] | 22.9 | 4440 | 43600 |
Honeywell/ITEC F125 | turbofan | F-CK-1 | 0.8 [6] | 22.7 | 4500 | 44100 | |
PW J52-P-408 | turbojet | A-4M/N, TA-4KU, EA-6B | 0.79 | 22.4 | 4560 | 44700 | |
Saturn AL-41F-1S | turbofan | Su-35S/T-10BM | 0.79 | 22.4 | 4560 | 44700 | |
Snecma M88-2 | turbofan | 1989 | Rafale | 0.782 | 22.14 | 4600 | 45100 |
Klimov RD-33 | turbofan | 1974 | MiG-29 | 0.77 | 21.8 | 4680 | 45800 |
RR Pegasus 11-61 | turbofan | AV-8B+ | 0.76 | 21.5 | 4740 | 46500 | |
Eurojet EJ200 | turbofan | 1991 | Eurofighter | 0.74–0.81 | 21–23 [8] | 4400–4900 | 44000–48000 |
GE F414-GE-400 | turbofan | 1993 | F/A-18E/F | 0.724 [9] | 20.5 | 4970 | 48800 |
Kuznetsov NK-32 | turbofan | 1980 | Tu-144LL, Tu-160 | 0.72-0.73 | 20–21 | 4900–5000 | 48000–49000 |
Soloviev D-30F6 | turbofan | MiG-31, S-37/Su-47 | 0.716 [6] | 20.3 | 5030 | 49300 | |
Snecma Larzac | turbofan | 1972 | Alpha Jet | 0.716 | 20.3 | 5030 | 49300 |
IHI F3 | turbofan | 1981 | Kawasaki T-4 | 0.7 | 19.8 | 5140 | 50400 |
Saturn AL-31F | turbofan | Su-27 /P/K | 0.666-0.78 [7] [9] | 18.9–22.1 | 4620–5410 | 45300–53000 | |
RR Spey RB.168 | turbofan | AMX | 0.66 [6] | 18.7 | 5450 | 53500 | |
GE F110-GE-129 | turbofan | F-16C/D, F-15 | 0.64 [9] | 18 | 5600 | 55000 | |
GE F110-GE-132 | turbofan | F-16E/F | 0.64 [9] | 18 | 5600 | 55000 | |
Turbo-Union RB.199 | turbofan | Tornado ECR | 0.637 [6] | 18.0 | 5650 | 55400 | |
PW F119-PW-100 | turbofan | 1992 | F-22 | 0.61 [9] | 17.3 | 5900 | 57900 |
Turbo-Union RB.199 | turbofan | Tornado | 0.598 [6] | 16.9 | 6020 | 59000 | |
GE F101-GE-102 | turbofan | 1970s | B-1B | 0.562 | 15.9 | 6410 | 62800 |
PW TF33-P-3 | turbofan | B-52H, NB-52H | 0.52 [6] | 14.7 | 6920 | 67900 | |
RR AE 3007H | turbofan | RQ-4, MQ-4C | 0.39 [6] | 11.0 | 9200 | 91000 | |
GE F118-GE-100 | turbofan | 1980s | B-2 | 0.375 [6] | 10.6 | 9600 | 94000 |
GE F118-GE-101 | turbofan | 1980s | U-2S | 0.375 [6] | 10.6 | 9600 | 94000 |
CFM CF6-50C2 | turbofan | A300, DC-10-30 | 0.371 [6] | 10.5 | 9700 | 95000 | |
GE TF34-GE-100 | turbofan | A-10 | 0.37 [6] | 10.5 | 9700 | 95000 | |
CFM CFM56-2B1 | turbofan | C-135, RC-135 | 0.36 [10] | 10 | 10000 | 98000 | |
Progress D-18T | turbofan | 1980 | An-124, An-225 | 0.345 | 9.8 | 10400 | 102000 |
PW F117-PW-100 | turbofan | C-17 | 0.34 [11] | 9.6 | 10600 | 104000 | |
PW PW2040 | turbofan | Boeing 757 | 0.33 [11] | 9.3 | 10900 | 107000 | |
CFM CFM56-3C1 | turbofan | 737 Classic | 0.33 | 9.3 | 11000 | 110000 | |
GE CF6-80C2 | turbofan | 744, 767, MD-11, A300/310, C-5M | 0.307-0.344 | 8.7–9.7 | 10500–11700 | 103000–115000 | |
EA GP7270 | turbofan | A380-861 | 0.299 [9] | 8.5 | 12000 | 118000 | |
GE GE90-85B | turbofan | 777-200/200ER/300 | 0.298 [9] | 8.44 | 12080 | 118500 | |
GE GE90-94B | turbofan | 777-200/200ER/300 | 0.2974 [9] | 8.42 | 12100 | 118700 | |
RR Trent 970-84 | turbofan | 2003 | A380-841 | 0.295 [9] | 8.36 | 12200 | 119700 |
GE GEnx-1B70 | turbofan | 787-8 | 0.2845 [9] | 8.06 | 12650 | 124100 | |
RR Trent 1000C | turbofan | 2006 | 787-9 | 0.273 [9] | 7.7 | 13200 | 129000 |
Jet engines, cruise | |||||||
---|---|---|---|---|---|---|---|
Model | Type | First run | Application | TSFC | Isp (by weight) | Isp(by weight) | |
lb/lbf·h | g/kN·s | s | m/s | ||||
Ramjet | Mach 1 | 4.5 | 130 | 800 | 7800 | ||
J-58 | turbojet | 1958 | SR-71 at Mach 3.2 (Reheat) | 1.9 [6] | 53.8 | 1895 | 18580 |
RR/Snecma Olympus | turbojet | 1966 | Concorde at Mach 2 | 1.195 [12] | 33.8 | 3010 | 29500 |
PW JT8D-9 | turbofan | 737 Original | 0.8 [13] | 22.7 | 4500 | 44100 | |
Honeywell ALF502R-5 | GTF | BAe 146 | 0.72 [11] | 20.4 | 5000 | 49000 | |
Soloviev D-30KP-2 | turbofan | Il-76, Il-78 | 0.715 | 20.3 | 5030 | 49400 | |
Soloviev D-30KU-154 | turbofan | Tu-154M | 0.705 | 20.0 | 5110 | 50100 | |
RR Tay RB.183 | turbofan | 1984 | Fokker 70, Fokker 100 | 0.69 | 19.5 | 5220 | 51200 |
GE CF34-3 | turbofan | 1982 | Challenger, CRJ100/200 | 0.69 | 19.5 | 5220 | 51200 |
GE CF34-8E | turbofan | E170/175 | 0.68 | 19.3 | 5290 | 51900 | |
Honeywell TFE731-60 | GTF | Falcon 900 | 0.679 [14] | 19.2 | 5300 | 52000 | |
CFM CFM56-2C1 | turbofan | DC-8 Super 70 | 0.671 [11] | 19.0 | 5370 | 52600 | |
GE CF34-8C | turbofan | CRJ700/900/1000 | 0.67-0.68 | 19–19 | 5300–5400 | 52000–53000 | |
CFM CFM56-3C1 | turbofan | 737 Classic | 0.667 | 18.9 | 5400 | 52900 | |
CFM CFM56-2A2 | turbofan | 1974 | E-3, E-6 | 0.66 [10] | 18.7 | 5450 | 53500 |
RR BR725 | turbofan | 2008 | G650/ER | 0.657 | 18.6 | 5480 | 53700 |
CFM CFM56-2B1 | turbofan | C-135, RC-135 | 0.65 [10] | 18.4 | 5540 | 54300 | |
GE CF34-10A | turbofan | ARJ21 | 0.65 | 18.4 | 5540 | 54300 | |
CFE CFE738-1-1B | turbofan | 1990 | Falcon 2000 | 0.645 [11] | 18.3 | 5580 | 54700 |
RR BR710 | turbofan | 1995 | G. V/G550, Global Express | 0.64 | 18 | 5600 | 55000 |
GE CF34-10E | turbofan | E190/195 | 0.64 | 18 | 5600 | 55000 | |
CFM CF6-50C2 | turbofan | A300B2/B4/C4/F4, DC-10-30 | 0.63 [11] | 17.8 | 5710 | 56000 | |
PowerJet SaM146 | turbofan | Superjet LR | 0.629 | 17.8 | 5720 | 56100 | |
CFM CFM56-7B24 | turbofan | 737 NG | 0.627 [11] | 17.8 | 5740 | 56300 | |
RR BR715 | turbofan | 1997 | 717 | 0.62 | 17.6 | 5810 | 56900 |
GE CF6-80C2-B1F | turbofan | 747-400 | 0.605 [12] | 17.1 | 5950 | 58400 | |
CFM CFM56-5A1 | turbofan | A320 | 0.596 | 16.9 | 6040 | 59200 | |
Aviadvigatel PS-90A1 | turbofan | Il-96-400 | 0.595 | 16.9 | 6050 | 59300 | |
PW PW2040 | turbofan | 757-200 | 0.582 [11] | 16.5 | 6190 | 60700 | |
PW PW4098 | turbofan | 777-300 | 0.581 [11] | 16.5 | 6200 | 60800 | |
GE CF6-80C2-B2 | turbofan | 767 | 0.576 [11] | 16.3 | 6250 | 61300 | |
IAE V2525-D5 | turbofan | MD-90 | 0.574 [15] | 16.3 | 6270 | 61500 | |
IAE V2533-A5 | turbofan | A321-231 | 0.574 [15] | 16.3 | 6270 | 61500 | |
RR Trent 700 | turbofan | 1992 | A330 | 0.562 [16] | 15.9 | 6410 | 62800 |
RR Trent 800 | turbofan | 1993 | 777-200/200ER/300 | 0.560 [16] | 15.9 | 6430 | 63000 |
Progress D-18T | turbofan | 1980 | An-124, An-225 | 0.546 | 15.5 | 6590 | 64700 |
CFM CFM56-5B4 | turbofan | A320-214 | 0.545 | 15.4 | 6610 | 64800 | |
CFM CFM56-5C2 | turbofan | A340-211 | 0.545 | 15.4 | 6610 | 64800 | |
RR Trent 500 | turbofan | 1999 | A340-500/600 | 0.542 [16] | 15.4 | 6640 | 65100 |
CFM LEAP-1B | turbofan | 2014 | 737 MAX | 0.53-0.56 | 15–16 | 6400–6800 | 63000–67000 |
Aviadvigatel PD-14 | turbofan | 2014 | MC-21-310 | 0.526 | 14.9 | 6840 | 67100 |
RR Trent 900 | turbofan | 2003 | A380 | 0.522 [16] | 14.8 | 6900 | 67600 |
GE GE90-85B | turbofan | 777-200/200ER | 0.52 [11] [17] | 14.7 | 6920 | 67900 | |
GE GEnx-1B76 | turbofan | 2006 | 787-10 | 0.512 [13] | 14.5 | 7030 | 69000 |
PW PW1400G | GTF | MC-21 | 0.51 [18] | 14.4 | 7100 | 69000 | |
CFM LEAP-1C | turbofan | 2013 | C919 | 0.51 | 14.4 | 7100 | 69000 |
CFM LEAP-1A | turbofan | 2013 | A320neo family | 0.51 [18] | 14.4 | 7100 | 69000 |
RR Trent 7000 | turbofan | 2015 | A330neo | 0.506 [lower-alpha 1] | 14.3 | 7110 | 69800 |
RR Trent 1000 | turbofan | 2006 | 787 | 0.506 [lower-alpha 2] | 14.3 | 7110 | 69800 |
RR Trent XWB-97 | turbofan | 2014 | A350-1000 | 0.478 [lower-alpha 3] | 13.5 | 7530 | 73900 |
PW 1127G | GTF | 2012 | A320neo | 0.463 [13] | 13.1 | 7780 | 76300 |
Civil engines [19] | |||||||||
---|---|---|---|---|---|---|---|---|---|
Model | SL thrust | BPR | OPR | SL SFC | cruise SFC | Weight | Layout | cost ($M) | Introduction |
GE GE90 | 90,000 lbf 400 kN | 8.4 | 39.3 | 0.545 lb/(lbf⋅h) 15.4 g/(kN⋅s) | 16,644 lb 7,550 kg | 1+3LP 10HP 2HP 6LP | 11 | 1995 | |
RR Trent | 71,100–91,300 lbf 316–406 kN | 4.89-5.74 | 36.84-42.7 | 0.557–0.565 lb/(lbf⋅h) 15.8–16.0 g/(kN⋅s) | 10,550–13,133 lb 4,785–5,957 kg | 1LP 8IP 6HP 1HP 1IP 4/5LP | 11-11.7 | 1995 | |
PW4000 | 52,000–84,000 lbf 230–370 kN | 4.85-6.41 | 27.5-34.2 | 0.348–0.359 lb/(lbf⋅h) 9.9–10.2 g/(kN⋅s) | 9,400–14,350 lb 4,260–6,510 kg | 1+4-6LP 11HP 2HP 4-7LP | 6.15-9.44 | 1986-1994 | |
RB211 | 43,100–60,600 lbf 192–270 kN | 4.30 | 25.8-33 | 0.570–0.598 lb/(lbf⋅h) 16.1–16.9 g/(kN⋅s) | 7,264–9,670 lb 3,295–4,386 kg | 1LP 6/7IP 6HP 1HP 1IP 3LP | 5.3-6.8 | 1984-1989 | |
GE CF6 | 52,500–67,500 lbf 234–300 kN | 4.66-5.31 | 27.1-32.4 | 0.32–0.35 lb/(lbf⋅h) 9.1–9.9 g/(kN⋅s) | 0.562–0.623 lb/(lbf⋅h) 15.9–17.6 g/(kN⋅s) | 8,496–10,726 lb 3,854–4,865 kg | 1+3/4LP 14HP 2HP 4/5LP | 5.9-7 | 1981-1987 |
D-18 | 51,660 lbf 229.8 kN | 5.60 | 25.0 | 0.570 lb/(lbf⋅h) 16.1 g/(kN⋅s) | 9,039 lb 4,100 kg | 1LP 7IP 7HP 1HP 1IP 4LP | 1982 | ||
PW2000 | 38,250 lbf 170.1 kN | 6 | 31.8 | 0.33 lb/(lbf⋅h) 9.3 g/(kN⋅s) | 0.582 lb/(lbf⋅h) 16.5 g/(kN⋅s) | 7,160 lb 3,250 kg | 1+4LP 11HP 2HP 5LP | 4 | 1983 |
PS-90 | 35,275 lbf 156.91 kN | 4.60 | 35.5 | 0.595 lb/(lbf⋅h) 16.9 g/(kN⋅s) | 6,503 lb 2,950 kg | 1+2LP 13HP 2 HP 4LP | 1992 | ||
IAE V2500 | 22,000–33,000 lbf 98–147 kN | 4.60-5.40 | 24.9-33.40 | 0.34–0.37 lb/(lbf⋅h) 9.6–10.5 g/(kN⋅s) | 0.574–0.581 lb/(lbf⋅h) 16.3–16.5 g/(kN⋅s) | 5,210–5,252 lb 2,363–2,382 kg | 1+4LP 10HP 2HP 5LP | 1989-1994 | |
CFM56 | 20,600–31,200 lbf 92–139 kN | 4.80-6.40 | 25.70-31.50 | 0.32–0.36 lb/(lbf⋅h) 9.1–10.2 g/(kN⋅s) | 0.545–0.667 lb/(lbf⋅h) 15.4–18.9 g/(kN⋅s) | 4,301–5,700 lb 1,951–2,585 kg | 1+3/4LP 9HP 1HP 4/5LP | 3.20-4.55 | 1986-1997 |
D-30 | 23,850 lbf 106.1 kN | 2.42 | 0.700 lb/(lbf⋅h) 19.8 g/(kN⋅s) | 5,110 lb 2,320 kg | 1+3LP 11HP 2HP 4LP | 1982 | |||
JT8D | 21,700 lbf 97 kN | 1.77 | 19.2 | 0.519 lb/(lbf⋅h) 14.7 g/(kN⋅s) | 0.737 lb/(lbf⋅h) 20.9 g/(kN⋅s) | 4,515 lb 2,048 kg | 1+6LP 7HP 1HP 3LP | 2.99 | 1986 |
BR700 | 14,845–19,883 lbf 66.03–88.44 kN | 4.00-4.70 | 25.7-32.1 | 0.370–0.390 lb/(lbf⋅h) 10.5–11.0 g/(kN⋅s) | 0.620–0.640 lb/(lbf⋅h) 17.6–18.1 g/(kN⋅s) | 3,520–4,545 lb 1,597–2,062 kg | 1+1/2LP 10HP 2HP 2/3LP | 1996 | |
D-436 | 16,865 lbf 75.02 kN | 4.95 | 25.2 | 0.610 lb/(lbf⋅h) 17.3 g/(kN⋅s) | 3,197 lb 1,450 kg | 1+1L 6I 7HP 1HP 1IP 3LP | 1996 | ||
RR Tay | 13,850–15,400 lbf 61.6–68.5 kN | 3.04-3.07 | 15.8-16.6 | 0.43–0.45 lb/(lbf⋅h) 12–13 g/(kN⋅s) | 0.690 lb/(lbf⋅h) 19.5 g/(kN⋅s) | 2,951–3,380 lb 1,339–1,533 kg | 1+3LP 12HP 2HP 3LP | 2.6 | 1988-1992 |
RR Spey | 9,900–11,400 lbf 44–51 kN | 0.64-0.71 | 15.5-18.4 | 0.56 lb/(lbf⋅h) 16 g/(kN⋅s) | 0.800 lb/(lbf⋅h) 22.7 g/(kN⋅s) | 2,287–2,483 lb 1,037–1,126 kg | 4/5LP 12HP 2HP 2LP | 1968-1969 | |
GE CF34 | 9,220 lbf 41.0 kN | 21 | 0.35 lb/(lbf⋅h) 9.9 g/(kN⋅s) | 1,670 lb 760 kg | 1F 14HP 2HP 4LP | 1996 | |||
AE3007 | 7,150 lbf 31.8 kN | 24.0 | 0.390 lb/(lbf⋅h) 11.0 g/(kN⋅s) | 1,581 lb 717 kg | |||||
ALF502/LF507 | 6,970–7,000 lbf 31.0–31.1 kN | 5.60-5.70 | 12.2-13.8 | 0.406–0.408 lb/(lbf⋅h) 11.5–11.6 g/(kN⋅s) | 0.414–0.720 lb/(lbf⋅h) 11.7–20.4 g/(kN⋅s) | 1,336–1,385 lb 606–628 kg | 1+2L 7+1HP 2HP 2LP | 1.66 | 1982-1991 |
CFE738 | 5,918 lbf 26.32 kN | 5.30 | 23.0 | 0.369 lb/(lbf⋅h) 10.5 g/(kN⋅s) | 0.645 lb/(lbf⋅h) 18.3 g/(kN⋅s) | 1,325 lb 601 kg | 1+5LP+1CF 2HP 3LP | 1992 | |
PW300 | 5,266 lbf 23.42 kN | 4.50 | 23.0 | 0.391 lb/(lbf⋅h) 11.1 g/(kN⋅s) | 0.675 lb/(lbf⋅h) 19.1 g/(kN⋅s) | 993 lb 450 kg | 1+4LP+1HP 2HP 3LP | 1990 | |
JT15D | 3,045 lbf 13.54 kN | 3.30 | 13.1 | 0.560 lb/(lbf⋅h) 15.9 g/(kN⋅s) | 0.541 lb/(lbf⋅h) 15.3 g/(kN⋅s) | 632 lb 287 kg | 1+1LP+1CF 1HP 2LP | 1983 | |
WI FJ44-4A | 1,900 lbf 8.5 kN | 0.456 lb/(lbf⋅h) 12.9 g/(kN⋅s) | 445 lb 202 kg | 1+1L 1C 1H 1HP 2LP | 1992 | ||||
WI FJ33-5A | 1,000–1,800 lbf 4.4–8.0 kN | 0.486 lb/(lbf⋅h) 13.8 g/(kN⋅s) | 300 lb 140 kg | 2016 |
The following table gives the efficiency for several engines when running at 80% throttle, which is approximately what is used in cruising, giving a minimum SFC. The efficiency is the amount of power propelling the plane divided by the rate of energy consumption. Since the power equals thrust times speed, the efficiency is given by
where V is speed and h is the energy content per unit mass of fuel (the higher heating value is used here, and at higher speeds the kinetic energy of the fuel or propellant becomes substantial and must be included).
Turbofan | efficiency |
---|---|
GE90 | 36.1% |
PW4000 | 34.8% |
PW2037 | 35.1% (M.87 40K) |
PW2037 | 33.5% (M.80 35K) |
CFM56-2 | 30.5% |
TFE731-2 | 23.4% |
A jet engine is a type of reaction engine, discharging a fast-moving jet of heated gas that generates thrust by jet propulsion. While this broad definition may include rocket, water jet, and hybrid propulsion, the term jet engine typically refers to an internal combustion air-breathing jet engine such as a turbojet, turbofan, ramjet, pulse jet, or scramjet. In general, jet engines are internal combustion engines.
A turboprop is a turbine engine that drives an aircraft propeller.
Specific impulse is a measure of how efficiently a reaction mass engine, such as a rocket using propellant or a jet engine using fuel, generates thrust. For engines like cold gas thrusters whose reaction mass is only the fuel they carry, specific impulse is exactly proportional to the effective exhaust gas velocity.
The turbofan or fanjet is a type of airbreathing jet engine that is widely used in aircraft propulsion. The word "turbofan" is a combination of the preceding generation engine technology of the turbojet, and a reference to the additional fan stage added. It consists of a gas turbine engine which achieves mechanical energy from combustion, and a ducted fan that uses the mechanical energy from the gas turbine to force air rearwards. Thus, whereas all the air taken in by a turbojet passes through the combustion chamber and turbines, in a turbofan some of that air bypasses these components. A turbofan thus can be thought of as a turbojet being used to drive a ducted fan, with both of these contributing to the thrust.
An aircraft engine, often referred to as an aero engine, is the power component of an aircraft propulsion system. Aircraft using power components are referred to as powered flight. Most aircraft engines are either piston engines or gas turbines, although a few have been rocket powered and in recent years many small UAVs have used electric motors.
A jet aircraft is an aircraft propelled by jet engines.
The turbojet is an airbreathing jet engine which is typically used in aircraft. It consists of a gas turbine with a propelling nozzle. The gas turbine has an air inlet which includes inlet guide vanes, a compressor, a combustion chamber, and a turbine. The compressed air from the compressor is heated by burning fuel in the combustion chamber and then allowed to expand through the turbine. The turbine exhaust is then expanded in the propelling nozzle where it is accelerated to high speed to provide thrust. Two engineers, Frank Whittle in the United Kingdom and Hans von Ohain in Germany, developed the concept independently into practical engines during the late 1930s.
An afterburner is an additional combustion component used on some jet engines, mostly those on military supersonic aircraft. Its purpose is to increase thrust, usually for supersonic flight, takeoff, and combat. The afterburning process injects additional fuel into a combustor in the jet pipe behind the turbine, "reheating" the exhaust gas. Afterburning significantly increases thrust as an alternative to using a bigger engine with its attendant weight penalty, but at the cost of increased fuel consumption which limits its use to short periods. This aircraft application of "reheat" contrasts with the meaning and implementation of "reheat" applicable to gas turbines driving electrical generators and which reduces fuel consumption.
The bypass ratio (BPR) of a turbofan engine is the ratio between the mass flow rate of the bypass stream to the mass flow rate entering the core. A 10:1 bypass ratio, for example, means that 10 kg of air passes through the bypass duct for every 1 kg of air passing through the core.
The Rolls-Royce RB.80 Conway was the first turbofan jet engine to enter service. Development started at Rolls-Royce in the 1940s, but the design was used only briefly, in the late 1950s and early 1960s, before other turbofan designs replaced it. The Conway engine was used on versions of the Handley Page Victor, Vickers VC10, Boeing 707-420 and Douglas DC-8-40.
A propelling nozzle is a nozzle that converts the internal energy of a working gas into propulsive force; it is the nozzle, which forms a jet, that separates a gas turbine, or gas generator, from a jet engine.
Jet propulsion is the propulsion of an object in one direction, produced by ejecting a jet of fluid in the opposite direction. By Newton's third law, the moving body is propelled in the opposite direction to the jet. Reaction engines operating on the principle of jet propulsion include the jet engine used for aircraft propulsion, the pump-jet used for marine propulsion, and the rocket engine and plasma thruster used for spacecraft propulsion. Underwater jet propulsion is also used by several marine animals, including cephalopods and salps, with the flying squid even displaying the only known instance of jet-powered aerial flight in the animal kingdom.
A jet engine performs by converting fuel into thrust. How well it performs is an indication of what proportion of its fuel goes to waste. It transfers heat from burning fuel to air passing through the engine. In doing so it produces thrust work when propelling a vehicle but a lot of the fuel is wasted and only appears as heat. Propulsion engineers aim to minimize the degradation of fuel energy into unusable thermal energy. Increased emphasis on performance improvements for commercial airliners came in the 1970s from the rising cost of fuel.
A variable cycle engine (VCE), also referred to as adaptive cycle engine (ACE), is an aircraft jet engine that is designed to operate efficiently under mixed flight conditions, such as subsonic, transonic and supersonic.
Specific thrust is the thrust per unit air mass flowrate of a jet engine and can be calculated by the ratio of net thrust/total intake airflow.
The Rolls-Royce/Snecma Olympus 593 was an Anglo-French turbojet with reheat, which powered the supersonic airliner Concorde. It was initially a joint project between Bristol Siddeley Engines Limited (BSEL) and Snecma, derived from the Bristol Siddeley Olympus 22R engine. Rolls-Royce Limited acquired BSEL in 1966 during development of the engine, making BSEL the Bristol Engine Division of Rolls-Royce.
The Westinghouse J46 is an afterburning turbojet engine developed by the Westinghouse Aviation Gas Turbine Division for the United States Navy in the 1950s. It was primarily employed in powering the Convair F2Y Sea Dart and Vought F7U Cutlass. The engine also powered the land speed-record car known as the Wingfoot Express, designed by Walt Arfons and Tom Green It was intended to power the F3D-3, an improved, swept-wing variant of the Douglas F3D Skyknight, although this airframe was never built.
The Volvo RM8 is a low-bypass afterburning turbofan jet engine developed for the Saab 37 Viggen fighter. An augmented bypass engine was required to give both better fuel consumption at cruise speeds and higher thrust boosting for its short take-off requirement than would be possible using a turbojet. In 1962, the civil Pratt & Whitney JT8D engine, as used for airliners such as the Boeing 727, was chosen as the only engine available which could be modified to meet the Viggen requirements. The RM8 was a licensed-built version of the JT8D, but extensively modified for supersonic speeds, with a Swedish-designed afterburner, and was produced by Svenska Flygmotor.
An airbreathing jet engine is a jet engine in which the exhaust gas which supplies jet propulsion is atmospheric air, which is taken in, compressed, heated, and expanded back to atmospheric pressure through a propelling nozzle. Compression may be provided by a gas turbine, as in the original turbojet and newer turbofan, or arise solely from the ram pressure of the vehicle's velocity, as with the ramjet and pulsejet.
The Boom Symphony is a medium-bypass turbofan engine under development by Boom Technology for use on its Overture supersonic airliner. The engine is designed to produce 35,000 pounds of thrust at takeoff, sustain Overture supercruise at Mach 1.7, and burn sustainable aviation fuel exclusively.