I'm trying to come up with something to describe how I understand the system, but it seems that the circuit is intertwined: How heat recovery in E-3 and cooling in E-1 and E-2 behave depends on the relative design duty of those exchangers.
Before we start with the tunings, I suggest that using a converged model at initial condition (100%) flow, run a step change (100 to 50% flow) in Stream 1, and keep all controllers at manual and monitor your streams until it stabilizes.
Having that information will help you see how the the system behaves dynamically without tuning effects and you can use it as a starting point.
Another issue I noticed the pressure of Stream 5 decreased following the reduction in Stream 1 flow rate.
Does V-1 have any pressure control or does it float with MeoH Column?
At face value, you should not lose pressure in Stream 5 as you are reducing your flow -> less hydraulic resistance. Of course you also need to factor in the two-phase behavior of HEx E-1 and the piping in Segment 5.
With a lower pressure entering the flash drum, wouldn’t more volatile components be expected to vaporize, possibly reducing the liquid level instead of increasing it?
Not unless you have more cooling at your exchangers, which pushes Stream 5 to bubble point.
Also, the level controller output reaches 100%, but the PV (level fraction) is still only around 0.6 — well below the high limit of the controller range. Why does the controller saturate even though the level hasn’t hit its upper range?
Aggressive tuning perhaps. Improper range?
For Stream 9 (the syngas stream), steady state was reached approximately 20 minutes after the disturbance, but at a higher temperature. I think this is because the lower flow rate and pressure of Stream 1 lead to a longer residence time in the heat exchanger, allowing more heat recovery.
Higher residence time is a consequence of the HEx operated below its design, which effectively have surplus area (since feed is at turndown), leading to more effective heat transfer.
The heat duty of the reactor also decreased due to the reduced feed. Since the shell side of the reactor is simulated as a flash drum (V3), and we set its duty to zero, less energy is available to generate steam.
If you keep Stream 10 temperature constant.
But the way the model setup only holds if reactor tubes are flooded with BFW. If the tubes are not flooded (which I highly doubt, seeing the insane syngas temperature), then the model will not account for varying surface area.
The amount of steam decreases rather if we set the duty of the drum to 0 excluding the heat from the reactor then heat is utilized to increase the temperature of bfw and generate less generate because its supplied at conditions of 240 C and 48 bar.
I can't I understand it fully, but if my understanding is correct, the main effect of lower R-2 flow is having a built up of V-3 level because you can't fully vaporize the BFW feed rate (still set at 100% flow), until such time the controllers act on the change.
I am not sure why the bfw flow rates is oscillating wildly in response to very small changes in the level fraction.
If you have variation in V-3 pressure, then you need to account for liquid flashing inside the vessel to vapor (which is saturated) without needing heat input, whenever V-3 pressure drops, which leads to more HPS flow, which may lead to pressure backup and increase in vessel pressure, and the cycle continues.
Another thing is you are controlling BFW flow (instead of blowdown, which is fixed in your model), so you'd expect this to change.