Imagine this block diagram
CAR < — ICE —> K —> ( T -> C -> H ) -> ES. T C H is the turbine, MGU-H, compressor assembly
To charge the ES.
At high speed the K is switched off and the CAR is driven by the ICE alone (say 500 kw) the turbine drives the compressor and the excess goes to the H, the ES gets charged at , say, 50 kw.
1. The K then switches on and the ICE drives the CAR at 380 Kw and the TCH at 120 kw. The H switches to being driven by the K, motoring. The TCH assembly increases speed because it is driven by the excess turbine power plus the 120 kw from the K ( maybe 170 kw) it gains kinetic energy.
2. The K switches off, the H switches from motoring to generating driven by the excess kinetic energy and the the excess turbine power and sends this to the ES. It absorbs the kinetic energy of the TCH which slows.
Repeat 1 and 2 at 20 to 40 hz.
The transmission, tyres and vehicle inertia see power fluctuating between 380 and 500 kw. The K drive train sees a power fluctuation of 0 to 120. The crank sees both, good luck to it.
Earlier in this topic I posted some thoughts on the numbers involved for the THC assembly. I could refine these but the principles hold, and the TCH speed variation will be in the right ballpark. I include that here. The jump will return to the right section for other posts on this topic.
henry wrote: ↑02 Jan 2018, 20:30
Craigy’s posts are very thought provoking.
They reminded me that with the advent of this formula I tried to understand the power requirements for the MGU-H to defeat lag. I think the numbers are also relevant to the “flywheel” discussion
Rotrex advertise an electrically driven centrifugal supercharger, C38-61, which has similar sort of flow/pressure profiles to the F1 numbers. It has a rotational inertia of 9.0E-3 kgm2. I doubled that to allow for the turbine and MGU-H itself giving 1.8E-2 to be accelerated.
In the driving part of the cycle this inertia will be driven by the MGU-K, 120 kw, plus the excess power from the turbine, that is the power in excess of that to drive the compressor. Obviously the latter is very variable, I’ll use 30kw for calcs. So the driving phase is 150 kw. Assuming 20 hz and symmetrical drive and recovery, and a starting speed of 110,000 rpm the speed will go up only 180 rpm. So the fluctuations will be relatively small.
Assuming symmetry the recovery will be 150 x .025 = 3.75 kJ. This gives 75 kJ/sec.
This would mean the MGU-H outputting 150kw in this mode vs the much lower, maybe 60 kw, in sustain mode.
Craigy made the good point that the cycle does not need to be symmetrical. If the MGU-H could generate at 300kw the output per cycle would double.
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