It would be interesting to know what he turbo speed does through the gears. The boost required at 12,000 would be less than that required at 10,500 and the airflow would probably be the same. If they control the boost with turbo speed this would trace a vertical line on the compressor map and the turbo speed would vary significantly (easy to do with the help of the MGUH).Jolle wrote: ↑08 May 2020, 13:42I don’t see much room to use the H as some kind of flywheel to store energy, as there is the limit of 125.000 rpm. The moment you want the K energised again, there is also air demand for the ICE.sosic2121 wrote: ↑08 May 2020, 09:33I'm wondering the same.Jolle wrote: ↑03 May 2020, 16:06Is weight really a problem for the current formula? I mean for the compressor wheel itself. The wheel probably has quite a steady RPM of 125.000 and spun up if asked for by a quite powerful electric motor. A few grams have almost no gain in performance while it becomes more durable.
Having turbo with higher inertia could be an advantage when bypassing 4/2MJ rules.
I was thinking more in line of the 125.000 limit. If ICE designers choose to have a stable fuel/air mix above 10.500 rpm, the turbo should spin on a stable 125.000 rpm trough the whole powerband (of whatever speed the designers choose).
And if something is rotating on a stable speed, weight doesn’t matter.
If you wanted to maintain a constant turbo speed while accelerating it would require throttling at the higher speed which would be less efficient than slowing the turbo with the MGUH and putting some charge in the ES.