In conditions of diminished boost requirement towards the top RPM, the excess exhaust will have to wastegated OUT to prevent from choking the engine on the exhaust side. Choking of any kind increases pumping losses and lowers BSFC. IMHO
Which means that with falling boost, the power would also be falling... and BSFC will be going in wrong direction, getting worse.wuzak wrote:In theory - not necessarily in practice.321apex wrote:The rules allow the following fuel flow:
9500 - 91 kg/h
10000 - 96
10500 - 100 = <<<-------GOLDEN POINT
The higher the engine speed with limited fuel, the higher are the friction losses (FMEP)... and LESS brake POWER. So ideal power peak is at 10500 RPM, however you must factor in the RPM spread for the gearing, which will force you to rev the engine in a zone of DIMINISHING FUEL efficiency [BSFC].
As we have theorised before, in turbo-compound mode the peak power will be moved up the rpm range.
The reason for this that the constant fuel flow from 10,500rpm dictates a constant mass air flow from the turbo and a falling boost requirement.
How do you know that exhaust energy will not be falling as much as boost? Can you prove this without the aid of Cosworth cartoon?wuzak wrote:The exhaust energy doesn't fall as much as the boost, so there is more power to use for the MGU-H. And that the increased MGU-H power more than offsets the increased friction.
This graph is treated as if it was some Gods truth, where it is completely unjustified. This is simply a theoretical study on a very greay area of unknown technology (MGU-H) and it is full of fudge factors.wuzak wrote:The Cosworth graphs seem to confirm a 1000rpm+ shift for peak power to higher rpm.