Interactive study
Verification and forced-response curves for the twin-tank campaign.
Open study →Connected-tank study · U-tube exchange · analytical + CFD
Two tanks joined by a bottom conduit behave as one coupled system. This page resolves the connected exchange (U-tube) mode, the inter-tank mass shift, and the roll moment it produces — from a closed-form model checked against the resolved twin-tank CFD. Geometry is the source-neutral dm1528 reference; no client data appears here.
01 · Why connect the tanks
Roll excites transverse sloshing, but a single tank's first sloshing mode is far faster than the vessel roll period, so on its own it moves almost quasi-statically with the ship. Connecting two tanks through a bottom conduit adds a new, slow mode: water exchanging between the legs, like a U-tube. That exchange mode can be tuned near the roll period, which is exactly what makes connected tanks matter for roll — and it is the mode this page quantifies.
02 · Single tank first
Linear first-mode sloshing, ω² = (πg/L)·tanh(πh/L), on the source-neutral reference. The 1 m free-decay tank reproduces the closed-form target exactly and matches the CFD to ~0.30%, anchoring the method before it is applied to the connected system.
| Case | Direction / length | Analytical | Check |
|---|---|---|---|
| Free-decay 1 m tank | transverse, L = 1 m, h/L = 0.30 | 0.758054 Hz | 0.000% vs closed form; ~0.30% vs CFD |
| Twin leg — longitudinal | L = 20 m | T = 6.25 s | matches CFD framework (6.251 s) |
| Twin leg — transverse | W = 6 m | T = 2.79 s | roll-excited direction |
Both single-tank modes (2.8–6.3 s) sit well above the roll band — confirming a single tank is off-resonance and the useful coupling must come from the connected exchange mode below.
03 · The connected exchange mode
Modelling the two legs joined by the bottom conduit as a U-tube (q = transferred volume; stiffness K = 2ρg/As, inertia M = ρ(ℓc/Ac + 2h/As)) gives the exchange natural period directly. Calibrating the effective conduit length to the CFD response peak was the original approach here; it is superseded. The response peak is loss-controlled and sits well above the natural period, so anchoring an inertia parameter to it is not valid — the calibration is now anchored to the measured natural period instead.
| Conduit length ℓc | Basis | Exchange period | Note |
|---|---|---|---|
| 10.0 m | geometric (centroid-to-centroid) | 19.4 s | uncorrected geometric-path comparison |
| 5.20 m | calibrated to the measured natural period | 14.31 s | 0.520× geometric; 90° phase crossing |
Key finding. The connected exchange natural period is 14.31 s, identified by the 90° phase crossing. The 22–24 s plateau in the 5° forced-roll sweep is the loss-controlled amplitude peak, not the exchange resonance or tuning period; it shifts from 20 s to 40 s across the measured 2.5°–10° roll-amplitude range.
04 · Mass shift & roll moment
For the published 24 s, 5° forcing case, the CFD level-difference amplitude (1.1037 m) fixes the volume exchanged between legs. The 6.66 MN·m redistribution estimate omits two static contributions to the total roll moment: the weight moment of the whole fluid mass about the roll axis and the within-leg free surface.
| Quantity | Analytical | CFD | Agreement |
|---|---|---|---|
| Exchange volume swing | 132.4 m³ | 132.45 m³ | exact |
| Transferred volume (amplitude) | 66.2 m³ | — | = As·Δlevel/2 |
| Inter-tank mass shift (amplitude) | 67.9 tonne | — | ρ · transferred volume |
| Roll moment — hydrostatic | 6.66 MN·m | — | 2ρg·V·arm (arm = 5 m) |
| Roll moment — total | 6.66 MN·m redistribution-only estimate | 9.67 MN·m | ×1.45 static-term residual; resolved in closed form |
These quantities are derived from the CFD-measured level difference (1.1037 m), so this is a derivation cross-check, not an independent prediction: the hydrostatic mass-shift moment captures the static physics, and the ×1.45 factor was previously read as resonant dynamic amplification. It is not: it is present at quasi-static forcing, where inertia cannot contribute, and is now resolved in closed form as two omitted static terms. The page's independent analytical↔CFD validations are the single-tank frequency, the exchange period, and the conduit-area scaling law below.
05 · Conduit-area sensitivity
Three twin-tank CFD runs — recovered from raw post-processing that had never been reduced, and now published in the release — vary the connecting conduit area Ac at a fixed 6.25 s forcing period, well off-resonance for the 14–27 s exchange modes they produce. They give the model an independent test: does it predict how exchange scales with the size of the connection? It does — to ~1–2%, with no per-case calibration.
| Conduit area Ac | Exchange period | CFD exchange amp | Analytical | Scaling ratio, CFD / analytical |
|---|---|---|---|---|
| 3.4 m² | 27.0 s | 7.91 m³ | 5.92 m³ | 1.00 / 1.00 |
| 6.8 m² | 19.4 s | 16.30 m³ | 12.17 m³ | 2.06 / 2.06 |
| 13.5 m² | 14.1 s | 34.60 m³ | 25.58 m³ | 4.38 / 4.32 |
The conduit-area scaling law matches to ~1–2% (ratio columns). The previously applied ×1.34 absolute-magnitude factor must not be interpreted as resonant dynamic amplification; the basis for reconciling absolute exchange magnitude remains unverified — needs owner. Design reading: a larger connection raises both the exchange amplitude and its natural frequency, so Ac is the knob that places the exchange mode relative to roll.
06 · Validation & provenance
dm1528-analytical/0.1 (assumption register A1–A16, results.json). Conduit-area validation: dm1528-ac-validation/0.1 (three off-resonance forced-roll CFD runs, reduced from post-processing and published as cases twin-conduit-a3p4, twin-conduit-a6p8, twin-conduit-a13p5). CFD anchors: immutable release 1034bb4efc5d9b390d51d4d546800c5a25bf6673af824e07ed5265da038ec30b, extending pinned Hugging Face revision 51ba5ddbca8dcfa8faeb6de5c592f342f32cfe2d.