The reason why you want the H to be able to generate at >120kW is for the condition where it's offloading inertia and turbine power into the ES, and isn't being driven by the K.wuzak wrote: ↑04 Jan 2018, 13:37The H could only ever receive 120kW (plus a small efficiency factor) from the K, as the K is limited to 120kW in either motor or generator mode.
Quite why you would want the H to be able to generate 240kW is beyond me, unless that is the power required for spooling the turbo. Which I doubt.
But the spooling power requirement is likely to be the sizing factor for the H, not the recovery power.
You want the inertial energy out of the H to the ES to happen as fast as possible so that once it's depleted the flywheel down to the lower rpm limit, you can get back to receiving energy from the K at the regulated maximum 120kW rate.
Some examples:
If the H receives energy from the K at 120kW and dumps it to the ES at 60kW, it spends 2/3rds of its time unavailable to receive energy from the K, and can spend only 1/3rd of the time spooling up off energy from the K.
If the H receives energy from the K at 120kW and dumps it to the ES at 120kW, it spends 50% of its time unavailable to receive energy from the K, so spends half the time charging and half discharging energy from the K.
If the H receives energy from the K at 120kW and dumps it to the ES at 240kW, it spends 1/3rd of its time unavailable to receive energy from the K and can spend 2/3rds of the time spooling up off energy from the K.
You want the H spending as little time as possible dumping flywheel energy into the ES, because the faster it does that, the more time it's available to store from the K, and the more energy you can collect outwith the 2MJ K->ES rule.
To show a ridiculously extreme, non-real-world example, if you could transfer from the H to the ES at 1200kW, you could spend 91% of the MGU-H time collecting energy from the K at 120kW and only 9% of the time forwarding it to the ES at 1200kW.
Obviously, if you're talking about energy transfers of over 4MJ a lap from the ES to the K using the H as a go-between the same logic applies: the more time you are transferring energy from ES to H, the less time the H can be driving the K.