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Clocked Speed = 314 mph (506 km/h), Kwinana Race Track, W.A., 2005
Top fuel dragster time: 4.567 s at

Top-Fuel Racing is a class of drag racing in which the cars are run on a maximum of 90% nitromethane and about 10% methanol (also known as racing alcohol), instead of gasoline. The cars are purpose-built race cars, with a layout superficially resembling open-wheel circuit racing vehicles; however, they are much longer, much narrower, and have very thin front tires, to optimize their performance exclusively in a straight line.

Unlike other standing start drag racing classes, these cars compete in a 1,000 foot (304 m) or race (instead of 1,320 feet (402 meters)); the change was made July 2, 2008 by the NHRA in the wake of the fatal crash of driver Scott Kalitta at an NHRA Powerade event at Old Bridge Township Raceway Parkmarker in Englishtown, NJ in June 2008. It seems that 1320 feet is now used again.Some countries such as Australia still run the 1/4 mile in Top Fuel. The FIA used the shorter distance at Mantorp Parkmarker in 2008 due to the limited shutdown area, but the Hockenheimringmarker and Santa Pod Racewaymarker ran the traditional distance at their FIA meet for Top Fuel, as does the IHRA and ANDRA (Australia). They are the fastest such category, with the fastest cars reaching the end of the 1/4 mile in less than 4.0* seconds at speeds up to 337 mph (530 km/h)*Times below 4.0 seconds have not yet been achieved on the 1/4 Mile this time relates to the shorter 1000 feet distance,while the 337 mph is only achieved on the 1/4 mile (all as at Aug 2009). A Top Fuel dragster accelerates from 0 to 100 mph (160 km/h) in as little as .7 seconds, subjecting the driver to a force about 5.7 times their weight. This acceleration takes less than a fifth of the time needed by a production Porsche 911 Turbo to reach the same speed. A top fuel dragster can exceed 280 mph (450 km/h) in just 660 feet (0.2 km). For further information and standards for drag-racing, including safety requirements, see the entry for National Hot Rod Association.

Facts about Top Fuel

Before their run, racers often perform a burnout. This is done for three reasons (water is applied to initially break traction, allowing the tires to spin up). First, it heats the tires up, creating a sticky superficial layer of rubber on the tires. Secondly, it removes debris from the tires. Thirdly, and most importantly, it coats the track surface with rubber which greatly improves traction during the subsequent launch. A Top Fueller's burnout alone can travel one quarter of the way down the track.

At top engine speed, the exhaust gases escaping from the open headers produce about 800-1000 pounds-force (3.6 kilonewtons) of downforce. The massive foil over and behind the rear wheels produces much more downforce, peaking at around 12,000 lbf (53 kN) when the car reaches a speed of about .

Top Fuel dragsters are notorious for the deafening amount of noise their engines create at full throttle (full noise). They generate 120 dB of noise, enough to cause some peoples' eardrums physical pain. This is louder than a Boeing 747 jet airliner at take-off power. The intense levels of sound are not only heard, but also felt as pounding vibrations all over one's body, leading many to compare the experience of watching a Top Fuel dragster make a pass to 'feeling as though the entire drag strip is being bombed'. Prior to the dragsters going down the strip, race announcers usually advise spectators to cover or plug their ears—indeed, ear plugs and even earmuffs are often handed out to fans at the entrance to a Top Fuel event.

The fuel

NHRA regulations limit the composition of the fuel to a maximum of 90% nitromethane (as of 2008); the remainder is largely methanol. However, this mixture is not mandatory, and less nitromethane can be used if desired.

Kenny Bernstein was the first drag racer in NHRA history to break in such a class of car on the 1/4 mile in March, 1992. Bernstein took his dragster over using a mixture of 90-to-100% nitromethane at the time. Despite nitromethane having a much lower energy density (11.2 MJ/kg) than either gasoline (44 MJ/kg) or methanol (22.7 MJ/kg), its addition to the fuel mixture has the net effect of increasing engine output by around 2.3 times compared to gasoline for the same mass of air -- 14.6 kg of air is required to burn one kilogram of gasoline, but only 1.7 kg of air for one kilogram of nitromethane. Since an engine’s cylinder can only contain a limited amount of air on each stroke, 8.7 times more nitromethane than gasoline can be burned in one stroke.

The high temperature of vaporization of nitromethane also means that it will absorb substantial engine heat as it vaporizes, providing an invaluable cooling mechanism. The laminar flame speed and combustion temperature are higher than gasoline at 0.5 m/s and 2400 °C respectively. Power output can be increased by using very rich air fuel mixtures. This is also something that helps prevent pre-ignition, something that is usually a problem when using nitromethane.

Due to the relatively slow burn rate of nitromethane, very rich fuel mixtures are often not fully ignited and some remaining nitromethane can escape from the exhaust pipe and ignite on contact with atmospheric oxygen, burning with a characteristic yellow flame. Additionally, after sufficient fuel has been combusted to consume all available oxygen, nitromethane can combust in the absence of atmospheric oxygen, producing hydrogen, which can often be seen burning from the exhaust pipes at night as a bright white flame. In a typical run the engine can consume as much as 103 litres (22.75 gallons) of fuel during warmup, burnout, staging, and the quarter-mile run.

Top fuel engines

Like many other motor sport formulas originating in the United States, the NHRA favors heavy restrictions on engine configuration, rather than technological development. This restricts the teams to using many decades old technologies* This only relates to basic engine configuration; most other areas are under continuous development e.g. fuel injection,clutch operation,ignition and aero parts.

The engine used to power a Top Fuel drag racing car has its roots in the second generation Chrysler Hemi 426 "Elephant Engine" made 1964-71. Although the Top Fuel engine is built exclusively of specialist parts, it retains the basic configuration with two valves per cylinder activated by pushrods from a centrally-placed camshaft. The engine has hemispherical combustion chambers, a 90 degree V angle; 4.8" bore pitch and a .54" cam lift. The configuration is identical to the overhead valve, single camshaft-in-block "Hemi" V-8 engine which became available for sale to the public in selected Chrysler Corporation (Dodge, DeSoto, and Chrysler) automotive products in 1952.

The NHRA competition rules limit the displacement to 500 cubic inch (8194 cc). A 4.1875" (106.4 mm) bore with a 4.5" (114.3 mm) stroke are customary dimensions. Larger bores have been shown to weaken the cylinder block. Compression ratio is about 6.5:1, as is common on engines with overdriven (the supercharger is driven faster than the crankshaft speed) superchargers.

The block is CNC machined from a piece of forged aluminium. It has press-fitted ductile iron liners. There are no water passages in the block which adds considerable strength and stiffness. Like the original Hemi, the racing cylinder block has a long skirt (to reduce piston "rocking" at the lower limit of piston travel); there are five main bearing caps which are fastened with aircraft-standard-rated steel studs; with additional reinforcing main studs and side bolts. There are three approved suppliers of these custom-made after-market blocks, from which the teams may choose.

The cylinder heads are CNC-machined from aluminum billets. As such, they have no water jackets and rely entirely on the incoming air/fuel mixture for their cooling. The original Chrysler design of two large valves per cylinder is used. The intake valve is made from solid titanium and the exhaust from solid Nimonic 80A or similar. Seats are of ductile iron. Beryllium-copper has been tried but its use is limited due to cost. Valve sizes are around 2.45" (62.2 mm) for the intake and 1.925" (48.9 mm) for the exhaust. In the ports there are integral tubes for the push rods. The heads are sealed to the block by copper gaskets and stainless steel o-rings. Securing the heads to the block is done with aircraft-rated steel studs.

The camshaft is billet steel, made from 8620 carbon steel or similar. It runs in five oil pressure lubricated bearing shells and is driven by gears in the front of the engine. Mechanical roller lifters ride atop the cam lobes and drive the steel push rods up into the steel rockers that actuate the valves. The rockers are of roller type on the intake side, high pressures on the exhaust limits its use to the intake side only. The steel roller rotates on a steel roller bearing and the steel rocker arms rotate on a titanium shaft within bronze bushings. Intake rockers are billet while the exhausts are investment cast. The dual valve springs are of coaxial type and made out of titanium. Valve retainers are also made of titanium, as are the rocker covers.

Billet steel crankshafts are used; they all have a cross plane a.k.a. 90 degree configuration and run in five conventional bearing shells. 180 degree crankshafts have been tried and they can offer increased power, even though the exhaust is of open type. A 180 degree crankshaft is also about 10 kg lighter than 90 degree crankshaft, but they create a lot of vibration. Such is the strength of a top fuel crankshaft that in one incident, the entire engine block was split open and blown off the car during an engine failure, and the crank, with all eight connecting rods and pistons, was left still bolted to the clutch.

Pistons are of forged aluminium, 2618 alloy. They have three ring and aluminium buttons retain the 1.156" x 3.300" steel pin. The piston is anodized and Teflon coated to prevent galling during high temperature operation. The top ring is an L-shaped Dykes ring that provides a good seal during combustion but a second ring must be used to prevent oil from entering the combustion chamber during intake strokes as the Dykes-style ring offers less than optimal combustion gas sealing. The third ring is an oil scraper ring whose function is helped by the second ring.The connecting rods are of forged aluminium and do provide some shock damping, which is why aluminum is used in place of titanium, because titanium connecting rods transmit too much of the combustion impulse to the big-end rod bearings, endangering the bearings and thus the crankshaft and block. Each con rod has two bolts, shell bearings for the big end while the pin runs directly in the rod.

The supercharger is a 14-71 type Roots blower. It has twisted lobes and is driven by a toothed belt. The supercharger is slightly offset to the rear to provide an even distribution of air. Absolute manifold pressure is usually 3.8-4.5 bar (56-66 PSI), but up to 5.0 bar (74 PSI) is possible. The manifold is fitted with a 200 psi burst plate. Air is fed to the compressor from throttle butterflies with a maximum area of 65 sq. in. At maximum pressure, it takes approximately to drive the supercharger.

These superchargers are in fact derivatives of General Motors scavenging-air blowers for their two-cycle diesel engines, which were adapted for automotive use in the early days of the sport. The model name of these superchargers delineates their size; i.e. the once commonly used 6-71 and 4-71 blowers were designed for General Motors diesels having six cylinders of 71 cubic inches each, and four cylinders of 71 cubic inches each, respectively. Thus, the currently used 14-71 design can be seen to be a huge increase in power delivery over the early designs.

Mandatory safety rules require a secured Kevlar-style blanket over the supercharger assembly as "blower explosions" are not uncommon. The absence of a protective blanket exposes the driver, team and spectators to shrapnel in the event that nearly any irregularity in the induction of the air/fuel mixture, the conversion of combustion into rotating crankshaft movements, or in the exhausting of spent gasses is encountered.

The oil system has a wet sump which contains 16 quarts of SAE 70 mineral or synthetic racing oil. The pan is made of titanium or aluminium. Titanium can be used to prevent oil spills in the event of a blown rod. Oil pressure is somewhere around 160–170 lbf/in² during the run, 200 lbf/in² at start up, but actual figures differ between teams.

Fuel is injected by a constant flow injection system. There is an engine driven mechanical fuel pump and about 42 fuel nozzles. The pump can flow 100 gallons per minute at 8000 rpm and 500 PSI fuel pressure. In general 10 injectors are placed in the injector hat above the supercharger, 16 in the intake manifold and two per cylinder in the cylinder head. Usually a race is started with a leaner mixture, then as the clutch begins to tighten as the engine speed builds, the air/fuel mixture is enriched. As engine speed builds pump pressure the mixture is made leaner to maintain a predetermined ratio that is based on many factors, one of which is primary one of race track surface friction. The stoichiometry of both methanol and nitromethane is considerably greater than that of racing gasoline, as they have oxygen atoms attached to their carbon chains and gasoline does not. This means that a "fueler" engine will provide power over a very broad range from very lean to very rich mixtures. Thus, to attain maximum performance, before each race, by varying the level of fuel supplied to the engine, the mechanical crew may select power outputs barely below the limits of tire traction. Power outputs which create tire slippage will "smoke the tires" and the race is often lost.

The air/fuel mixture is ignited by two 14 mm spark plugs per cylinder. These plugs are fired by two 44-ampere magnetos. Normal ignition timing is 58-65 degrees BTDC. (This is dramatically greater spark advance than in a gasoline engine as "nitro" and alcohol burn far slower.) Directly after launch the timing is typically decreased by about 25 degrees for a short time as this gives the tires time to reach their correct shape. The ignition system limits the engine speed to 8400 rpm. The ignition system provides initial 50,000 volts and 1.2 amperes. The long duration spark (up to 26 degrees) provides energy of 950 millijoules. The plugs are placed in such a way that they are cooled by the incoming charge. The ignition system is not allowed to respond to real time information (no computer-based spark lead adjustments), so instead a timer-based retard system is used.

The engine is fitted with open exhaust pipes, 2.75" in diameter and 18" long. These are made of steel and fitted with thermocouples for measuring of the exhaust temperature. They are called "zoomies" and exhaust gases are directed upward and backwards. Exhaust temperature is about 500 °F (260 °C) at idle and 1796 °F (980 °C) by the end of a run. A night run provides visual excitement with slow-burning nitromethane flames many feet above this screaming spectacle of acceleration. A "good run" is over in just 4.5 seconds, the noise ends, and braking parachutes are seen in the distance, after a speed of over has been reached.

The engine is warmed up for about 80 seconds. After the warm up the valve covers are taken off, oil is changed and the car is refueled. The run including tire warming is about 100 seconds which results in a "lap" of about three minutes. After each lap, the entire engine is disassembled and examined, and worn or damaged components are replaced.


Measuring the power output of a top fuel engine directly is not feasible. (Actually this is done on those cars that have a Torque sensor incorporated as part the RacePak data system[Hp=Torque x Rpm/5252]). This is not, as is sometimes stated, because no dynamometer exists that can measure the output of a Top Fuel engine; in reality, dynamometers capable of measuring tens of thousands of horsepower at the appropriate shaft speeds are in widespread use. Rather, it is because a Top Fuel engine cannot be run at its maximum power output for more than about 10 seconds at a time without overheating (or perhaps exploding) as would be necessary to take a reliable power reading. Instead, the power output of the engine is usually calculated based upon the car's weight and its performance. The calculated Power output of these engines is most likely somewhere between 7000 and 8500 horsepower (approximately 4500-6000 kilowatts), with a torque output of 8135 N·m (ca. 6000 lbf·ft) and a brake mean effective pressure of 80–100 bar (8.0-10 MPa).

For the purposes of comparison, a 2008 SSC Ultimate Aero, the world's fastest production automobile at the time, produces horsepower and 1094 lbf·ft (1483 N·m) torque, and the calculated horsepower of a top fuel dragster's supercharged V-8 engine easily surpasses that of the largest aviation piston engine ever conceived, the Lycoming R-7755 , 36-cylinder multibank (nine sets of four cylinders inline in each bank) engine from 1946, which had over fifteen times the displacement of the largest displacement top fuel engine.

Engine weight

  • Block with liners 187 lbs (85 kg)
  • Heads 40 lbs (18 kg) each
  • Crankshaft 81.5 lbs (37 kg)
  • Complete engine 496 lbs (225 kg)

Mandatory safety equipment

Much of organized drag-racing is sanctioned by the National Hot Rod Association. Since 1955, the Association has held regional and national events (typically organized as single elimination tournaments, with the winner of each two car race advancing) and has set rules for safety, with the more powerful cars requiring ever more safety equipment.

Typical safety equipment for contemporary top fuel dragsters: full face helmets with fitted HANS devices; multi-point, quick release safety restraint harness; full body fire suit made of Nomex or similar material, complete with face mask, gloves, socks, shoes, and outer sock-like boots, all made of fire-resistant materials; on board fire extinguishers; kevlar or other synthetic "bullet-proof" blankets around the superchargers and clutch assemblies to contain broken parts in the event of failure or explosion; damage resistant fuel tank, lines, and fittings; externally accessible fuel and ignition shut-offs (built to be accessible to rescue staff); braking parachutes; and a host of other equipment, all built to the very highest standards of manufacturing. Any breakthrough or invention that is likely to contribute to driver, staff, and spectator safety is likely to be adopted as a mandated rule for competition. The 54-year history of NHRA has provided hundreds of examples of safety upgrades.

In 2000, the NHRA mandated the maximum concentration of nitromethane in a car's fuel be no more than 90%. In the wake of a Gateway International Racewaymarker fatality in 2004, involving racer Darrell Russell, the fuel ratio was reduced to 85%. Complaints from teams in regards to cost, however, has resulted in the rule being rescinded starting in 2008, when the fuel mixture returns to 90%, as NHRA team owners, crew chiefs, and suppliers complained about mechanical failures that can result in oildowns or more severe crashes caused by the reduced nitromethane mixture.

The NHRA also mandated that different rear tires be used (in both Top Fuel and Funny Car) to try to prevent them from failing, and that a titanium "shield" be attached around the back-half of the roll-cage in Top Fuel Dragsters (although some Funny Car teams adopted this) to prevent any debris from entering the cockpit. This also was the result of the fatal crash at Gateway International Raceway. The rear tire pressure is also heavily regulated by Goodyear Tire and Rubber on behalf of the NHRA, at 7psi, the absolute minimum pressure allowed. An official is at the starting line who checks tire pressure; if it is lower than 7 psi., the tires are inflated to meet requirements.

The 2008 death of Funny Car driver Scott Kalitta also brought about some new safety precautions, including a sensor that monitors the engine. Should the engine backfire, the fuel pump is automatically shut down, and the parachutes deployed. The idea behind the sensor is to minimize, if not all together eliminate the circumstances that led to Kalitta's death at Old Bridge Township Raceway Parkmarker in Englishtown, New Jerseymarker.

At present, final drive ratios lower than 3.20 (3.2 engine rotations to one rear axle rotation) are prohibited, in an effort to limit top speed potential, thus reducing the perceived level of danger.


  2. NHRA News: Nitro percentage to be raised to 90 in Top Fuel, Funny Car in 2008 (9/15/2007)
  • "The Top Fuel V8", Race Engine Technology, #009, p60-69
  • "Running The Army Motor", Race Engine Technology, #008, p18-30
  • "Top Fuel by the Numbers, By John Kiewicz, Motor Trend, February 2005
  • "Drag Racing: It's Like Plunging Your Toilet with a Claymore Mine, By John Phillips, Car and Driver, August 2002.

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