DEPARTMENT OF MECHANICAL ENGINEERING NATIONAL UNIVERSITY OF SINGAPORE
Stability of Floating Body ME 2134 - 1
Gao Yifan A0091597N Group 2D1
Objectives
To experimentally determine the center of gravity (C.G.) and metacentric height of a body floating on water. To investigate the effects of placing a weight vertically above the C.G. on the stability of a floating body. To investigate the effects of free surfaces on the stability of a floating body.
Records of Data & Calculation d l=
5.7+6.3+5.5+ 6.5 =6 cm 4
Without the raised mass and free surface,
θ=6.5°
T=
4.40 =0.88 s 5
GM =
mgd ≈ 0.2926 m ( ρg V ¿ ) tanθ
T th =2 π
BM =
(√
K Oy ≈ 1.0757 s g ∙ GM
)
I Oy l b3 = ≈ 0.3472 m V ¿ 12lb d l
1 KB= d l=3 cm 2 KG=KB+ BM −GM ≈ 8.4659 cm With the raised mass,
GM =
mgd ≈ 0.2230 m ( ρg V ¿ ) tanθ
T th =2 π
BM =
(
K Oy ≈ 1.6569 s √ g ∙ GM
)
I Oy l b3 = ≈ 0.3472 m V ¿ 12lb d l
1 KB= d l=3 cm 2 KG=KB+ BM −GM ≈ 15.4184 cm With free surfaces,
θ=7.0 °
T=
5.00 =1.00 s 5
G2 M =
GG2 =
mgd ≈ 0.2715 m ( ρg V ¿ ) tanθ
ρ f Σi =0.9887 cm ρ V¿
GM =G2 M +GG2 =0.2814 m
T th =2 π
(
K Oy ≈ 1.0984 s √ g ∙ G2 M
)
I Oy l b3 BM = = ≈ 0.3472 m V ¿ 12lb d l
1 KB= d l=3 cm 2 KG=KB+ BM −GM ≈ 9.5857 cm
Discussions 3. After putting on the load,
1 KB= ( d l + Δ d l ) 2 where
Δ dl =
mmax ρlb
KG=
KG ' × M +(h+ d)×mmax M +mmax
where
M =ρlb dl
BM =
I Oy l b3 = V ¿ 24 KB× lb
GM =KB+ BM −KG=0 Therefore,
m 1 dl + max + 2 ρlb
(
)
b
(
'
2
12 d l +
mmax ρlb
)
KG × ρlb d l+(h+ d)×mmax = ρlb d l +mmax
mmax ≈ 414.41 tonnes 4. (a). No free surface,
GM =1m
θ=tan −1
( Mgmgd∙GM ) ≈ 1.1458°
(b). 3 ρ l c b c3 ρ l c bc GG2 = = ≈ 0.1708 m ρ 12 V ¿ 12 M
G2 M =GM −G G 2 ≈ 0.8292 m
θ=tan −1
(
mgd ≈ 1.3817° Mg ∙G 2 M
)
(c).
bc 3 2l ( ) ρl b 3 ρ c 2 GG2 = = c c ≈ 0.1708 m ρ 12V ¿ 48 M G2 M=GM −G G2 ≈ 0 .8292 m
θ=tan −1
≈ 1.3817° ( Mgmgd ∙G M ) 2
(d).
lc 3 b 3 ρ 2 c ρ lc b c GG2 = = ≈ 0.0427 m ρ 12 V ¿ 12 M 2
G2 M =GM −G G 2 ≈ 0.9573 m
θ=tan −1
≈ 1.1989° ( Mgmgd ∙G M ) 2
(e).
ρ f l c b c 3 ρf l c b c3 GG2 = = ≈ 0.1667 m ρ 12V ¿ 12 M G2 M =GM −G G 2 ≈ 0.8333 m
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