The airbox (and entire tract) on the 2.7t intake is specifically designed for linear results across all intake velocities.
The length of the suction path, from the air flow meter to the turbine impeller, is 1.5 meters.
Y-pipe is asymmetric at the inlet (near the flow meter) and with a large angle of attack of the air flow.
What "linearity" are we talking about? This is pure savings and implementation on one flow meter!
In terms of gas dynamics, a design with a crooked Y-pipe is an engineer's nightmare. It is near the measuring zone of the flow meter that the swirling of the intake air flow occurs, distorting the measured data!
The desire and the idea are clear and real.
Personally, I implemented a signal adder for two flowmeters for atmega 328, two 12-bit spi ADCs and one 12-bit spi DAC. Based on two Bosch flowmeters
0280217814 with a limit of 1560 kg/h and corresponding original linearization curves interpolated to 12 bit resolution.
After working with the code, we got a sampling time of 20 kHz at a resolution of 12 bits.
The addition of values from two flowmeter signals is performed correctly and coincides with the mathematically added values.
The naturally resulting linearization graph(MLHFM) is created mathematically as a sum and put in me7.1.
The official Bosch information about HFM5 indicates the following time parameters for converting air flow into voltage:
1) T1 = 15 ms (In case of sudden increase of the air-mass flow from 10 kg · h–1 auf 0,7 Qm nominal, time required to reach
63% of the final value of the air-mass signal.)
2) T2 = 30 ms ( Period of time in case of a throughflow jump of the air mass | ∆ m/m | ≤ 5%.)
With a conversion time of 15ms, we obtain the maximum frequency of the air mass meter signal change equal to 66.6666 hertz
The available 20kHz ADC/DAC sampling rate is more than sufficient to respond quickly to changing flowmeter signals.
It is important to pay attention to the reference signals Vref, which are twisted into one point by the author of the topic ...)