25-Nav-B3 Finite Element Analysis for Ship Structures · May 2016
Question 2 of 7: Stability
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Exams, May 2016 — 98-Nav-B3, 3 hours, closed book, non-communicating calculator permitted (any five of the seven questions constitute a complete paper, all equal value; all seven answered below for full study coverage).
Reference texts: Tupper, Introduction to Naval Architecture, 5th ed.; Lewis (ed.), Principles of Naval Architecture (PNA), 3 vols.; International Code on Intact Stability (IMO IS Code), 2008; Canada Shipping Act / Transport Canada Marine Safety.
Check: this paper, although listed under Finite Element Analysis for Ship Structures, is headed “98-Nav-B3, Small Commercial Ships”; it is a broad small-craft naval-architecture survey paper — propeller open-water performance, ship stability and the inclining experiment, hull/propulsion selection trade-offs, longitudinal shear/bending of a floating body, structural loads and hull materials, fishing-vessel stability regulation, and main-engine selection for a tug — with no finite-element-analysis content whatsoever. It is solved as the exam it actually is.
Find. (a) $GM$, $KG$ from the inclining test, and whether the ship stays upright after the cargo move; (b) the heel angle taken up after the move; (c) the largest weight that can be shifted 14 m without instability.
Approach. Use the small-angle inclining-test formula to get $GM$ (and hence $KG$) in the arrival condition; use the parallel-axis weight-shift rule $\Delta KG=\sum w_id_i/\Delta$ to update $KG$ (and $GM$) after the cargo move; correct the given GZ curve for the resulting rise in $G$ ($GZ'=GZ-\Delta KG\sin\theta$) to read off the new equilibrium heel angle; and set $GM_{new}=0$ to solve for the limiting weight in part (c).
GM from the inclining test. For small angles, $GM=\dfrac{w\,d}{\Delta\tan\theta}=\dfrac{50\times20}{12{,}000\times\tan(6.35^\circ)}=\dfrac{1000}{12{,}000\times0.11128}=\boxed{0.749\ \text{m}}$.
KG in the arrival condition. $KG=KM-GM=10-0.749=\boxed{9.251\ \text{m}}$.
Rise in KG from the cargo move. Moving $w_1=3000$ t up by $d_1=14$ m (mass and hence $\Delta$, $KM$ unchanged) raises the overall centre of gravity by $\Delta KG=\dfrac{w_1d_1}{\Delta}=\dfrac{3000\times14}{12{,}000}=3.5\ \text{m}$, giving $KG_{new}=9.251+3.5=12.751\ \text{m}$.
New GM — stability check. $GM_{new}=KM-KG_{new}=10-12.751=\boxed{-2.751\ \text{m}}$. A negative $GM$ means $G$ has risen above $M$: the ship is initially unstable and will not remain upright — it heels (or lolls) to whatever angle restores a positive righting arm, assuming small-angle wall-sided theory still applies and no free-surface or trim effects complicate the picture (see callout).
Part (b) — correcting the GZ curve for the raised G. Raising $G$ by $\Delta KG=3.5$ m reduces the righting arm at every heel angle by $\Delta KG\sin\theta$: $GZ'(\theta)=GZ(\theta)-3.5\sin\theta$. Tabulating:
$\theta$
GZ (orig.)
$3.5\sin\theta$
GZ′ (corrected)
5°
0.08
0.305
−0.225
10°
0.25
0.608
−0.358
20°
0.34
1.197
−0.857
30°
0.36
1.750
−1.390
40°
0.32
2.250
−1.930
$GZ'$ is negative and becomes steadily more negative from 5° through 40° — there is no angle in the surveyed range where a positive righting arm reappears.
Original GZ curve (blue) versus the curve corrected for the 3.5 m rise in G (red, dashed). The corrected curve stays negative throughout the tabulated 0–40° range: there is no stable heel angle to report within the surveyed data — the ship heels progressively and does not find equilibrium before capsize or downflooding intervenes.
Part (c) — maximum weight for zero margin. Setting $GM_{new}=0$ (the boundary of initial stability) with the same 14 m lift: $0=GM-\dfrac{w_{max}d_1}{\Delta}\ \Rightarrow\ w_{max}=\dfrac{GM\,\Delta}{d_1}=\dfrac{0.749\times12{,}000}{14}=\boxed{642\ \text{tonnes}}$.
Result
Value
Metacentric height, $GM$ (arrival)
0.749 m
Centre of gravity, $KG$ (arrival)
9.251 m
$GM$ after 3000 t / 14 m shift
−2.751 m (unstable — ship does not remain upright)
Heel angle after the shift
No stable angle within 0–40°; GZ′ is negative and worsening throughout — the ship progressively capsizes