Dyno sheets

or it can be rewritten as HP=T*(RPM/5252)
so when RPM=5252, the equation becomes HP=T*(5252/5252)
Since (5252/5252)=1, the equation becomes HP=T, but this is only true for RPM=5252. The two numbers have to be equal at 5252 RPM as dictated by the equation or it is a bogus dyno graph.
The 5252 constant comes from the conversion of the units of T*RPM to HP. If we have 400 ft-lb of torque at 5000 RPM, running through the equation gives us 380.8 HP. Without the equation, we have the power (not the unit horsepower) of the engine as P=T*RPM
or P=400 ft-lb*5000 RPM
so P=2000000 ft-lb-rev/min, since there are 60 seconds in a minute
P=2000000 ft-lb-rev/min(1 min/60 sec), the min terms cancel giving
P=33333.333 ft-lb-rev/sec, now to convert from rotational motion to linear motion, there are 2*pi (or 2*3.1416=6.2832) units in one revolution
so P=33333.33 ft-lb-rev/sec(6.2832/rev), the rev terms cancel giving
P=209439.5 ft-lb/sec, finally, 1 HP=550 ft-lb/sec or 1=sec-HP/550 ft-lb
so P=209439.5 ft-lb/sec(sec-HP/550 ft-lb) the sec, ft, and lb terms cancel
This leaves P=380.8 HP which checks
Written out, the conversion is (1 min/60 sec)(6.2832/rev)(sec-HP/550 ft-lb) or (1*6.2832)/(60*550)(min-sec-HP)/(sec-rev) or 1/5252.1131 (min-sec-HP)/(sec-rev). As you can see, it's not exactly 5252.
or it can be rewritten as HP=T*(RPM/5252)
so when RPM=5252, the equation becomes HP=T*(5252/5252)
Since (5252/5252)=1, the equation becomes HP=T, but this is only true for RPM=5252. The two numbers have to be equal at 5252 RPM as dictated by the equation or it is a bogus dyno graph.
The 5252 constant comes from the conversion of the units of T*RPM to HP. If we have 400 ft-lb of torque at 5000 RPM, running through the equation gives us 380.8 HP. Without the equation, we have the power (not the unit horsepower) of the engine as P=T*RPM
or P=400 ft-lb*5000 RPM
so P=2000000 ft-lb-rev/min, since there are 60 seconds in a minute
P=2000000 ft-lb-rev/min(1 min/60 sec), the min terms cancel giving
P=33333.333 ft-lb-rev/sec, now to convert from rotational motion to linear motion, there are 2*pi (or 2*3.1416=6.2832) units in one revolution
so P=33333.33 ft-lb-rev/sec(6.2832/rev), the rev terms cancel giving
P=209439.5 ft-lb/sec, finally, 1 HP=550 ft-lb/sec or 1=sec-HP/550 ft-lb
so P=209439.5 ft-lb/sec(sec-HP/550 ft-lb) the sec, ft, and lb terms cancel
This leaves P=380.8 HP which checks
Written out, the conversion is (1 min/60 sec)(6.2832/rev)(sec-HP/550 ft-lb) or (1*6.2832)/(60*550)(min-sec-HP)/(sec-rev) or 1/5252.1131 (min-sec-HP)/(sec-rev). As you can see, it's not exactly 5252.

or it can be rewritten as HP=T*(RPM/5252)
so when RPM=5252, the equation becomes HP=T*(5252/5252)
Since (5252/5252)=1, the equation becomes HP=T, but this is only true for RPM=5252. The two numbers have to be equal at 5252 RPM as dictated by the equation or it is a bogus dyno graph.
The 5252 constant comes from the conversion of the units of T*RPM to HP. If we have 400 ft-lb of torque at 5000 RPM, running through the equation gives us 380.8 HP. Without the equation, we have the power (not the unit horsepower) of the engine as P=T*RPM
or P=400 ft-lb*5000 RPM
so P=2000000 ft-lb-rev/min, since there are 60 seconds in a minute
P=2000000 ft-lb-rev/min(1 min/60 sec), the min terms cancel giving
P=33333.333 ft-lb-rev/sec, now to convert from rotational motion to linear motion, there are 2*pi (or 2*3.1416=6.2832) units in one revolution
so P=33333.33 ft-lb-rev/sec(6.2832/rev), the rev terms cancel giving
P=209439.5 ft-lb/sec, finally, 1 HP=550 ft-lb/sec or 1=sec-HP/550 ft-lb
so P=209439.5 ft-lb/sec(sec-HP/550 ft-lb) the sec, ft, and lb terms cancel
This leaves P=380.8 HP which checks
Written out, the conversion is (1 min/60 sec)(6.2832/rev)(sec-HP/550 ft-lb) or (1*6.2832)/(60*550)(min-sec-HP)/(sec-rev) or 1/5252.1131 (min-sec-HP)/(sec-rev). As you can see, it's not exactly 5252.

graphs a loss when actual torque is actually more ?
Ed
Ed
The Best of Corvette for Corvette Enthusiasts
Ed
Ed
that peaks Torque at 412 @ 4800 rpm I can see the torque dropping off dramatically after 5200 rpm. That might explain where the 4.10
gears just make it happen that much faster. It runs now about like
a c6 zo6 stocker with the GEARS & the FAST
that peaks Torque at 412 @ 4800 rpm I can see the torque dropping off dramatically after 5200 rpm. That might explain where the 4.10
gears just make it happen that much faster. It runs now about like
a c6 zo6 stocker with the GEARS & the FAST
Ed
Ed
little more for me . Leon
little more for me . Leon
Ed
http://forums.corvetteforum.com/show...&postcount=421
You can see the length of the dyno run was used to calculate HP, so it's intuitive that a shorter dyno run would increase the HP required to overcome inertia of all rotating components from the harmonic dampener to the tires and everything in between. Most of the "indicated" HP loss with 4.10s on an inertia type dyno goes to overcome inertia in the rotating engine/drivetrain components.
There's another part of the HP loss that's a real loss and that has to do with the gears themselves. When going from 3.42s to 4.10s on the same diameter ring gear, the ring gear has to gain teeth. The only way to do that is to increase the pitch/angle of the gear teeth. The rear end gears are called hypoid gears as opposed to spur, helical, worm, etc. Spur gears are the most efficient with a good quality involute spur gear having pure rolling motion at the pitch line giving less than 1% HP loss. Worm gears are the worst with pure sliding action defining the motion between the two gear teeth and very high HP loss associated with low efficiency. Hypoid gears have a combination of rolling and sliding and are in between spur gears and worm gears in efficiency. As the pitch increases, sliding action increases resulting in less efficiency. It's not a lot but it represents a real loss on the road vs the "measured" loss due to inertia on the dyno.
If you were to run your car with 4.10s against one just like it except for 3.42s in a roll race from 45 MPH to let's say 130 MPH, the two cars would be dead even at the end...or very close to it. The 4.10 car will be in 2nd gear while the 3.42 car is still in 1st meaning the 3.42 car has the best overall gearing and will jump out to a lead. But when the 3.42 car shifts to 2nd, the 4.10 car now has the best overall gearing and begins to pull back ahead until it has to make the 2-3 shift and the advantage goes back to the 3.42 car. The two cars see-saw back and forth to 130 MPH where they should be about even because the average HP put to the road is about equal. The advantage to the 4.10s is better acceleration from a dead stop because it multiplies torque at the lower RPM and allows the engine to get up on the HP curve sooner. 1st gear is the only gear where you're very low in RPM and substantially off the HP curve...all of the other gears drop to 4400 RPM or more after the shift making the average HP put to the ground the same. The 4.10s increase the average HP put to the ground in a 1/4 mile run by getting up on the HP curve quicker in 1st gear and running out close to redline in 4th at the end to capture almost all of the area under the HP curve in that gear. While 4.10s help in the 1/4 mile to run with stock Z06s, don't do a roll race against one from 45+ MPH or you'll get walked badly.
http://forums.corvetteforum.com/show...&postcount=421
You can see the length of the dyno run was used to calculate HP, so it's intuitive that a shorter dyno run would increase the HP required to overcome inertia of all rotating components from the harmonic dampener to the tires and everything in between. Most of the "indicated" HP loss with 4.10s on an inertia type dyno goes to overcome inertia in the rotating engine/drivetrain components.
About the dyno, an inertia machines formula is based off of rate of acceleration, but it's not the only determing factor. Believe me the dyno takes gearing into account whether it's making plain to see or not. It knows if the car is turning the drum at 70mph @ 2200 rpm with the 3.42 or 55mph @2200 rpm with the 4.10s. So yes you're going to accelerate faster from whatever mph with 4.10's but you're not going hit the same top speed either. If you are losing top end speed because of the gears, you're losing power on the dyno. You're not getting curve necessary to give you an accurate hp reading. I don't really care to get into an argument with you, my dyno has an absorber and a strain gauge and the gearing is out in the open and there is no fudge factor, so I don't have to worry about things like that. You've got what you got 4.10 gearing or 3.42 gearing I'll get the same number and that's the way I want it. You can't put a fast accelerating 2 stroke dirtbike on the dyno and run it and come up with 400 hp. On the street though that bike might be faster from 0-30. Just because it can turn the drum fast for a short time doesn't equal a lot of hp.
It doesn't matter though I'm more interested in how his stock LS2 cam makes power up to 6300 rpm.
Ed
About the dyno, an inertia machines formula is based off of rate of acceleration, but it's not the only determing factor. Believe me the dyno takes gearing into account whether it's making plain to see or not. It knows if the car is turning the drum at 70mph @ 2200 rpm with the 3.42 or 55mph @2200 rpm with the 4.10s. So yes you're going to accelerate faster from whatever mph with 4.10's but you're not going hit the same top speed either. If you are losing top end speed because of the gears, you're losing power on the dyno. You're not getting curve necessary to give you an accurate hp reading. I don't really care to get into an argument with you, my dyno has an absorber and a strain gauge and the gearing is out in the open and there is no fudge factor, so I don't have to worry about things like that. You've got what you got 4.10 gearing or 3.42 gearing I'll get the same number and that's the way I want it. You can't put a fast accelerating 2 stroke dirtbike on the dyno and run it and come up with 400 hp. On the street though that bike might be faster from 0-30. Just because it can turn the drum fast for a short time doesn't equal a lot of hp.
It doesn't matter though I'm more interested in how his stock LS2 cam makes power up to 6300 rpm.
Ed
to 6500 rpm. I dont know where you got the idea that a stock cam
will stop making power at 5700 rpm. Most that do make the 400+ are boltons with ported FAST, TB , LGLT's and of course the tuner involved.
on a bone stocker I can believe it. BTW the dirtbike on the dyno is not a very good analogy.
to 6500 rpm. I dont know where you got the idea that a stock cam
will stop making power at 5700 rpm. Most that do make the 400+ are boltons with ported FAST, TB , LGLT's and of course the tuner involved.
on a bone stocker I can believe it. BTW the dirtbike on the dyno is not a very good analogy.
Ed
It doesn't matter though I'm more interested in how his stock LS2 cam makes power up to 6300 rpm.
Ed
Work is done ON the wheel/tire by the engine to increase their KE with the amount of work done (KE added) given by the KE (after) minus the KE (before). KE=1/2Iw^2 (where w is the angular velocity) from the link I gave above and presented here again. http://hyperphysics.phy-astr.gsu.edu/hbase/mi.html
The rate at which work is being done on the wheel/tire is equal to the rate at which the KE is increasing. HP is the rate at which work is being done so we're left with finding the KE added and dividing by the time it took to add the KE to the wheel/tire to find the average HP required to accelerate it from one RPM to another. (This is from my old Physics book which I tried to scan in but my scanner stopped working.)
We'll use more realistic numbers for the C6Z06:
Tires- 36 LBs @ 24" average diameter
Wheels- 20 LBs @ 15" average diameter
I for the tire is I=(16.33 KG)(.3048m)^2=1.517 kg-m^2
I for the wheel is I=(9.07 KG)(.1905m)^2=.3292 kg-m^2
Tire+wheel I=1.517+.3292=1.846 kg-m^2
We'll use the video from the following link:
http://www.livernoismotorsports.com/....phtml?t=video
The 15th one down is a stock LMB C6Z06 with the engine running from ~1700 RPM to ~6900 RPM during the run which took 18 seconds total.
1700 RPM @ the crank=(1700/3.42/60)(2)(pi)=52.05 rad/sec at the wheel.
KE (before)=1/2(1.846)(52.05)^2=2501 Joules
6900 RPM @ the crank=(6900/3.42/60)(2)(pi)=211.3 rad/sec at the wheel.
KE (after)=1/2(1.846)(211.3)^2=41201 Joules
KE (after)-KE (before)=41201-2501=38700 Joules
1 Joule=.738 ft-lb
38700(.738)=28560.6 ft-lb which is the total work done to increase the RPM from 1700 to 6900.
To get the rate at which work was done, divide by the 18 sec dyno run giving: 28560.6 ft-lb/18 sec= 1586.7 ft-lb/sec
1 HP=550 ft-lb/sec, so we have 1586.7/550=2.885 HP for one tire/wheel or 5.77 HP for both tires/wheels.
If you replace the wheel/tire in the example above with a drum from an inertia dyno, it's basically the same thing. The engine is doing work on the drum by adding kinetic energy (work/kinetic energy in FT-LB, not to be confused with torque which is LB-FT) to it. The time required to add the kinetic energy is the rate the engine is doing work (FT-LB/sec) which is the definition of HP. The lower "top speed" with 4.10s has absolutely nothing to do with the rate at which kinetic energy is added to the dyno drum. You've got a good dog in the race but I think he's just barking up the wrong tree.
As far as the LS2 making HP above 6000 RPM with the stock cam, you do realize you can shift the peak HP RPM several hundred RPM with bolt ons such as intake and exhaust that "tunes" the engine either up or down in the RPM range. Kind of like the difference between a dual-plane and single-plane intake manifold on a carbureted engine. Or a long tube/small primary diameter header vs a short tube/large primary diameter header. The cam will indeed set the RPM range but the intake/exhaust tuning determines the exact RPM within that range.
Again, this is just a discussion.

















