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25-Nav-A2 Hydrodynamics of Ships (I)_ Resistance and Propulsion · December 2017

Question 2 of 5: Trim from a Longitudinal Weight Shift

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

National Examinations, Dec 2017 — 98-Mar-A2 Fundamentals of Naval Architecture, 3 hours, open book (any non-communicating calculator permitted). Five questions constitute a complete exam paper and each is of equal value.

Reference texts: Tupper, Introduction to Naval Architecture; Lewis (ed.), Principles of Naval Architecture (PNA); IMO, International Code on Intact Stability (IS Code).

Check: this paper, although listed under Hydrodynamics of Ships (I): Resistance and Propulsion, is headed "98-Mar-A2, Fundamentals of Naval Architecture" and its five questions are entirely barge/ship stability and hydrostatics (freeboard, trim, inclining experiment, flooding, GZ curve) with no resistance or propulsion content whatsoever. Solved here as the exam that was actually printed.

Question 2: Trim from a Longitudinal Weight Shift (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. Same barge as Q1 ($L=70$ m, $B=17$ m), at the light-ship draft $d_0=2.2$ m, initially on an even keel. A weight $w=20$ t is shifted $\ell=27$ m towards the bow.

Find. The resulting trim angle.

Approach. A weight shift produces a trimming moment $w\ell$; dividing by the moment-to-change-trim-one-centimetre at the light draft gives the change of trim, which (with $LCF$ at midships for this box form) is split evenly between the ends and converted to an angle through $\tan\theta=\text{trim}/L$.

  1. MCT1cm at the light draft. $\Delta_0=\rho A_W d_0=1.025\times1190\times2.2=2683.45\ \text{t}$ (as in Q1). $BM_{L,0}=L^2/(12d_0)=4900/(12\times2.2)=4900/26.4=185.61\ \text{m}$. $$MCT1cm_0=\dfrac{\Delta_0\,BM_{L,0}}{100L}=\dfrac{2683.45\times185.61}{7000}=71.15\ \text{t}\cdot\text{m/cm}$$ (Interestingly this equals Q1's design-draft value exactly — for a box barge $\Delta\,BM_L=\rho A_W d\times L^2/(12d)=\rho A_W L^2/12$ is independent of draft, so MCT1cm is the same at every waterline.)
  2. Change of trim. $$t=\dfrac{w\ell}{MCT1cm_0}=\dfrac{20\times27}{71.15}=7.59\ \text{cm}=0.0759\ \text{m}$$
  3. Trim angle. With the centre of flotation at midships, this change of trim is the full difference between the forward and aft drafts over the length $L$: $$\boxed{\theta=\tan^{-1}\!\left(\dfrac{t}{L}\right)=\tan^{-1}\!\left(\dfrac{0.0759}{70}\right)=0.062^\circ\ \text{(by the head)}}$$ Equivalently, the forward draft rises by $t/2=3.79\ \text{cm}$ and the aft draft falls by the same amount, since $F$ is at $L/2$.
QuantityResult
MCT1cm at light draft71.15 t·m/cm
Change of trim7.59 cm (0.0759 m), by the head
Draft change at each end±3.79 cm
Trim angle0.062°