Exhaust Downforce?
#1
Posted 23 August 2005 - 08:11
I was curious whether this effect is in play at all with a modern f1 car and whether or not it was a contributing factor in the move away from the rearfacing exhausts...
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#2
Posted 23 August 2005 - 09:03
#3
Posted 23 August 2005 - 09:18
#4
Posted 23 August 2005 - 09:39
rho*V*revs/2,
where rho is the exhaust density and V the engine capacity. The jet velocity v is the speed by which the exhausts exit the pipe, so the thrust is
rho*V*revs/2*v.
Just to get a rough estimate, use rho = 1.23 kg/^m^3 (density of air, exhaust is heavier, but not by a lot with gas as the fuel), V = 0.003 m^3, revs=300/sec, and v=300 m/s and multiply.
Then you get
1.23*0.003*150*300 = 170 N.
So the peak thrust is on the order of 200 N or so (corresponding to a "20 kg" or "40 lbs" downforce), which is not a lot.
With nitromethane fuel things are a bit different as the mass flow is much larger (the fuel contains extra oxygen for the combustion). Also, the enormous engines increase mass flow as the engine capacity goes up. On the other hand, those engines might not run at 18,000 rpm.
In any case, the claim of "2,000 lbs" downforce seems to be a bit exaggerated. A calculation as rough as the one above would let's say use 5x the density rho (use of compressor and more fuel), 3x engine capacity V, but reduce revs by a factor of 2. I'd be surprised if the downforce vastly exceeded 1-2 kN, which is about "200-400 lbs" of downforce.
#5
Posted 23 August 2005 - 09:50
Originally posted by DOHC
The thrust of a jet is massflow*jet velocity. The massflow is the weight of the exhaust volume produced per time unit:
rho*V*revs/2,
where rho is the exhaust density and V the engine capacity. The jet velocity v is the speed by which the exhausts exit the pipe, so the thrust is
rho*V*revs/2*v.
Just to get a rough estimate, use rho = 1.23 kg/^m^3 (density of air, exhaust is heavier, but not by a lot with gas as the fuel), V = 0.003 m^3, revs=300/sec, and v=300 m/s and multiply.
Then you get
1.23*0.003*150*300 = 170 N.
So the peak thrust is on the order of 200 N or so (corresponding to a "20 kg" or "40 lbs" downforce), which is not a lot.
With nitromethane fuel things are a bit different as the mass flow is much larger (the fuel contains extra oxygen for the combustion). Also, the enormous engines increase mass flow as the engine capacity goes up. On the other hand, those engines might not run at 18,000 rpm.
In any case, the claim of "2,000 lbs" downforce seems to be a bit exaggerated. A calculation as rough as the one above would let's say use 5x the density rho (use of compressor and more fuel), 3x engine capacity V, but reduce revs by a factor of 2. I'd be surprised if the downforce vastly exceeded 1-2 kN, which is about "200-400 lbs" of downforce.
The massflow through a Top Fuel engine is probably around 6 kg/s or so, 2 kN or 250 N/cyl should be a good estimate. Not much when it comes to downforce, but if one cylinder goes out it is enough to affect the balance of the car.
#6
Posted 23 August 2005 - 13:19
#7
Posted 24 August 2005 - 06:53
Exhausts exiting in the diffuser caused problems when the driver lifted for a corner, a substantial amount of downforce was lost and the cars were unsettled.
(I often wondered [in the old days when they could change the car around more] if in a really wet race the exhaust could be configured to blast the standing water from just infront of the rear tyres to aid traction. The reasoning was that in the wet speeds are down, aero is less important so a bulkier exhaust had less effect, and in monsoon conditions it might allow you to out drag other cars from slow corners. Of course if the track dried then you might just melt your tyres...)
#8
Posted 04 September 2005 - 01:04
Nitromethane burns rather slowly so Top Fuel engines typically run less than 9,000rpm and somewhere in the order of 600 total revolutions per race (not including burnout and staging). In order to make the estimated 7-8000hp from their capped V8 displacement of 500 CID, they're consuming tremendous quantities of fuel (roughly 1.5 gallons per second).
The other effect of nitromethane's slow burn is that it's still burning (and expanding) in the exhaust, hence the yellow flame visible in low light conditions (the white flame is burning hydrogen that's been separated from the air by the exhaust gas). The downforce is due to the expansion, not just flow. That said, it's more like 800 lbs. The wing on the other hand produces over 12,000lbs.
If you've never watched one of these cars accellerate past 500km/h in under 5 seconds, you really ought to.
#9
Posted 04 September 2005 - 05:42
#10
Posted 04 September 2005 - 19:12
Originally posted by Canuck
The downforce attributed to Top Fuel engine exhaust has little to do with actual exhaust gas flow.
Nitromethane burns rather slowly so Top Fuel engines typically run less than 9,000rpm and somewhere in the order of 600 total revolutions per race (not including burnout and staging). In order to make the estimated 7-8000hp from their capped V8 displacement of 500 CID, they're consuming tremendous quantities of fuel (roughly 1.5 gallons per second).
The other effect of nitromethane's slow burn is that it's still burning (and expanding) in the exhaust, hence the yellow flame visible in low light conditions (the white flame is burning hydrogen that's been separated from the air by the exhaust gas). The downforce is due to the expansion, not just flow. That said, it's more like 800 lbs. The wing on the other hand produces over 12,000lbs.
If you've never watched one of these cars accellerate past 500km/h in under 5 seconds, you really ought to.
Nitromethane does actually burn faster than gasoline with a laminar flame velocity of 0.5 m/s instead of a typical 0.35 m/s for gasoline. It also burns hotter, with a flame temperature of 2400 degC instead of around 2000 degC.
The reason for the long burns in Top Fuel is because of the rich mixtures used. Since nitromethane can serve as a mono fuel you can basicly increase power by increasing fuel flow alone, that is until the ignition system sets the limit. The fuel pump also reaches the limit at around 1.5 gallons per second at 8000 rpm. Around 5 gallons is used for a run.
The story about burning hydrogen that have been separated is just a myth. Infact, the exhaust gas temperature of a Top Fuel engine is just 500 degF at idle and 1800 degF at the end of the run. The rich mixture of nitromethane has very cood cooling properties.
The truth about the white flames you can probably find if you take a look how nitromethane burn when used as a mono fuel.
4CH3NO2 - > 2N2 + CO2 + 3CO + 3H2O + 3H2
This would create free hydrogen which can then react with the oxygen at the end of the exhaust pipes.
You can't create thrust from expansion. Thrust is created from massflow and velocity. Expansion can only be used to increase the velocity in a nozzle which then create thrust. But unlike a jet engine the velocity of the flow is not as high, and the mass flow is also low in comparison which means you won't get that much thrust as downforce.
My estimate is that the massflow through a Top Fuel engine is somewhere around 6-8 kg/s at 8000 rpm, this means if you want to reach 800 lbs (3530 N) of downforce the exhaust velocity must be 440 m/s (supersonic).
EDIT: Corrected the formula for how nitromethane burn as a mono fuel.
#11
Posted 04 September 2005 - 20:54
#12
Posted 05 September 2005 - 06:17
What I meant to convey was that calculations of exhaust flow that fail to take into account the increased velocity due to still-burning nitromethane in the exhaust were likely to be shy of actual pressures produced.
#13
Posted 05 September 2005 - 08:59
How do teams test the effects of the exhaust flow? Is it trial-by-error, computer modeling or do they actually fire the engines up in the wind tunnel?
They pipe compressed air through the model to simulate exhaust gases.
#14
Posted 05 September 2005 - 13:08
This is the case if you take a toy balloon and release it, or if you take a water-jet propulsion device for a boat, but also if you take a jet engine with or without afterburner, or a rocket motor. This means that thermodynamic expansion per se is not a different or "added" principle, although the added thermal energy may be used to increase nozzle velocity (see J. Edlund's post).
The idea beind chemical/combustion jet propulsion is to produce high pressure, high temperature exhaust through exothermal reactions. Thermodynamic expansion is used to vent the exhaust gasses into a low pressure ambience. With a suitable nozzle shape the exhaust expansion partly converts thermal energy to kinetic energy in the form of momentum carried by the jet. This is what a turbojet engine does. Switch on the afterburner, pump more fuel into the hot exhaust, and you further increase nozzle jet velocity. Still, the thrust cannot exceed the product of nozzle velocity and mass flow (total mass throughput per second).
As for exhaust thrust from internal combustion engines, the mass flow can be fairly accurately estimated. The very large downforce numbers claimed do imply -- as J. Edlund remarks -- that supersonic nozzle velocities are needed. The 2,000 lbs figure seems to require exhaust pipe velocities well above 1,000 m/s. That's quite a rocket motor. If directed to the rear it would offer an added 1G acceleration without requiring traction.
#15
Posted 05 September 2005 - 23:10
http://www.aerospace...ion/q0224.shtml
#16
Posted 06 September 2005 - 18:38
Just as a reference, nitromethane used as a monopropellant in rocket motors has a theoretical exhaust velocity of around 1800 m/s at sea level.
#17
Posted 06 September 2005 - 22:39
#18
Posted 07 September 2005 - 11:22
Originally posted by J. Edlund
The massflow through a Top Fuel engine is probably around 6 kg/s or so, 2 kN or 250 N/cyl should be a good estimate. Not much when it comes to downforce, but if one cylinder goes out it is enough to affect the balance of the car.
That could be a little high even...on paper the ariflow looks like around 4.5 kg/s to me. But I do know the vehicle telemetry indicates the download or "thrust" is in the range of 600-800 lbs so there is something going on there. It's an interesting question. When one candle goes out it will definitely steer the car, that's for sure.
Nitromethane is an interesting substance. If you pour a small puddle of it on the floor and throw a lighted match in it, it will snuff out the match. But if you hit the puddle with a hammer it will go off. In text books its flame speed is supposedly slower than gasoline...but in stoichiometric combustion under pressure it approaches that of dynamite. The extreme spark advance required is simply a result of the very large fuel volume that can be burned per cycle... A/F ratios are in the range of 1.5:1 by weight, which is where all the power comes from. This is not an engine so much as a big old "flame pump" if you will... for lack of a better term. A reciprocating rocket engine.
These engines can do all kinds of crazy things that are hard to validate or even understand. They have been known to "two-stroke" or "diesel" and still make significant power even with the ignition disabled. Often when they are torn down these engines will show "back-siding" on the pistons...the drag racer's term for when there is more detonation and flame damage on the underside of the piston than on the top! It's a different world...and because these engines are too fragile and unstable to run for more than a few seconds, and can't be dyno'ed or quantified in any meaningful way, it will probably remain more of an art than a science. I believe some of the lore is more myth than fact but I am in no position to dispute any of it.
Reminds me of one of my all-time favorite racing quotes... Keith Black was one of the sharpest fuel racers ever, and manufactured most of the blocks and heads used in these engines. A friend down the street phoned him up, said they had reconfigured an enormous old marine dyno, they had a Top Fuel engine all hooked up and ready to go; would he like to come over and watch the first pull? KB said, "Hell no, I'm too close now."
#19
Posted 08 September 2005 - 09:33
If we use the known 0.6 kg/s airflow in an F1 engine, but use 3x the engine capacity and 5x supercharging with 1/2 the revs, we get 3*5*0.6/2 kg/s = 4.5 kg/s.
With an A/F ratio of 1.5:1 by weight, you have 3 kg/s fuel added, for a total massflow of 7.5 kg/s (within Edlund's 6-8 kg/s estimate).
Finally, to have a 9 kN thrust (equiv to the 2000 lbs), you need at least 1,200 m/s (almost Mach 4) nozzle velocity. The more modest 800 lbs claim requires about 500 m/s, still supersonic at M = 1.5.
Whether one would be able to see Mach discs is not clear to me, as the flow through an exhaust pipe is a pulsed flow rather than a steady flow. Would Mach discs be stationary under such circumstances?
But I'm still wondering about why one would use the exhaust pipes as afterburners (unless it's done for the spectacular looks). First, nozzle shape design ususally tries to optimize thrust, which you do by having exhaust pressure = ambient pressure at the nozzle's open end. If you have underexpanded exhaust (higher than ambient pressure), you have less than max possible thrust (you waste energy), and conversely, if it is overexpanded, you waste energy because you have drag in the exhaust's passage through the nozzle.
If one really had the enormous thrust claimed, it would make a lot of sense to put real rocket nozzles at the end of the exhaust pipes, because you'd be able to increase thrust, as well as use that thrust for acceleration.
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#20
Posted 08 September 2005 - 13:14
A crew member was lowering or raising the body on to the chassis when it snagged the throttle causing the car to lurch forwards, slightly injuring 2 crew members.
Now to the point of the post, the crew chief Dick Venerables was standing close to the right side of the car and literally had his pants blown clear off by those exhaust gasses and suffered some slight burns due to the heat and flames coming out of the pipes.
I think that is a good example of the ferocity of the exhaust pulses a 500ci Nitro engine produces.
PS both crewmen where back at the track the next day.
GJ
#21
Posted 08 September 2005 - 13:50
Originally posted by DOHC
But I'm still wondering about why one would use the exhaust pipes as afterburners (unless it's done for the spectacular looks).
This forum cracks me up sometimes.
#22
Posted 09 September 2005 - 11:44
#23
Posted 09 September 2005 - 17:33
#24
Posted 10 September 2005 - 18:05
For the fuel flow we know that the pump sets the limit at around 6 kg/s at 8000 rpm, but maximum fuel flow are probably not used at maximum speed.
Exhaust flow is then air + fuel flow.
As McGuire mentioned nitromethane is also pressure sensitive, infact even a high fuel pressure can cause a certain danger. I assume that this is also the reason why no octane number is given to it. It's also possible to make the mixture even more "explosive" by adding a small amount of hydrazine to the nitromethane. 1% by volume should be enough to give a significant power increase, but the mixture is very unstable.
#25
Posted 11 September 2005 - 09:50
Originally posted by Gear Jammer
pants blown clear off
If we consider skydiving, you reach a maximum velocity of some 50 m/s, which, although a low speed in the present context, is likely to tear your average Armani suit to shreds. This shows that it's difficult to remain properly dressed already at Mach 0.15.
#26
Posted 11 September 2005 - 10:19
Originally posted by Gear Jammer
pants blown clear off
I have heard that if you take a young woman for a quick trip on the back of a motorbike.......Nah, forget it!
PDR
#27
Posted 11 September 2005 - 11:32
#28
Posted 11 September 2005 - 17:04
If we consider skydiving, you reach a maximum velocity of some 50 m/s, which, although a low speed in the present context, is likely to tear your average Armani suit to shreds. This shows that it's difficult to remain properly dressed already at Mach 0.15.
I have heard that if you take a young woman for a quick trip on the back of a motorbike.......Nah, forget it!
PDR
Urban myth, I ride a bike and its never worked for me
;)