buoyancy and flotation dr. mohamed tarek shamaa · dr. mohamed tarek shamaa buoyancy and flotation....
TRANSCRIPT
Dr. Mohamed Tarek Shamaa
BUOYANCY AND FLOTATION
The Archimedes' principle states, "Whenever a bodyis immersed wholly or partially in a fluid, it isbuoyed up (i.e., lifted up) by a force equal to theweight of fluid displaced by the body (the force ofbuoyancy or simply buoyancy). Or in other words,whenever a body is immersed wholly or partially ina fluid, the resultant force acting on it, is equal to thedifference between the upward pressure of the fluidon its bottom, and the downward force due togravity.
A stone weigh 105Ib in air. When submerged in water, it weight 67.0 Ib. Find the volume and specific gravity of the stone.
Solution
Buoyant force Fb = weight of water displaced by stone = Win air - Win
water
Fb = 105 – 67 = 38 Ib
weight of water displaced = 38 = water V = 62.4 V
V = V stone = 0.609 ft3
W in air = stone Vstone = (SG) water Vstone = (SG) Fb ,
SG = weight of stone in air / weight of equal volume of water
SG = 105 / [(0.609)(62.4)] = 2.76
Archimedes, when asked by King Hiero if the new crown was pure gold (SG = 19.3), found the crown weight in air to be 11.8 N and in water to be 10.9 N. Was it gold?
Solution: The buoyancy is the difference between air weight and underwater weight:
Fb = Wc air-Wc water = 11.8 - 10.9 = 0.9 N = water Vcrown
But also Wair = crown Vcrown = (SG) water Vcrown = (SG) Fb ,
Wc water = Wc air- Fb = (SG) Fb - Fb
so Wc in water= Fb(SG-1)
Solve for SGcrown = 1+ Wc in water /Fb = 1 + 10.9/0.9 = 13.1
(not pure gold)
The centre of buoyancy is the point, through
which the force of buoyancy is supposed to act. It
is always the centre of gravity of the volume of
the liquid displaced. In other words, the centre of
buoyancy is the centre of area of the immersed
section.
A completely submerged body, such as a submarine, will remain in
equilibrium at rest only, if (i) the buoyant force is equal to the
weight W and (ii) the centre of buoyancy (B) lies directly above
the center of gravity(G). Submarines are required to use
balancing tanks, to makes FB = W and trimming tanks to brink the
centre of buoyancy above the centre of gravity.
if the center of gravity of the completely submerged body is above
the center of buoyancy, the resulting couple formed by the weight and
the buoyant force will cause the body to overturn and move to a new
equilibrium position. Thus, a completely submerged body with its
center of gravity above its center of buoyancy is in an unstable
equilibrium position.
Whenever a body, floating in a liquid, is given a small angulardisplacement, it starts oscillating about some point. This point,about which the body starts oscillating, is called metacentre.
the distance between the centre of
gravity G and the metacentre is
known as the metacentric height. This
height will be positive when M lies
above G, and represents the condition
for stable equilibrium of the vessel.
If, however, the metacentre M lies
below G (in between B and G), the
metacentric height is negative
signifying unstable equilibrium.
The metacentric height will be positive when M lies above G, and
represents the condition for stable equilibrium of the vessel. If,
however, the metacenter M lies below G (in between B and G), the
metacentric height is negative signifying unstable equilibrium.
DETERMINATION OF METACENTRIC HEIGHT
The buoyant force acting through B'
F'b = W + df - df = W = Fb
By moments about B,
F'b × BB' = df × gg
BB' = df × gg / F'b = df × gg/W
BB' = df × gg / ρ g V (1)
Where V is the volume of the displaced
fluid.
df = ρg×(1/2) AA'×(1/2)b×L
AA' = (1/2) b θ and gg =( 2/3) (1/2)b + 2/3(1/2)b = 2/3b
Substitute in (1)
BB' = MB θ = (ρg ×(1/4)b θ × (1/2)b ×L ×(2/3)b)/ ρgV
Or MB = (1/12) Lb3/V = I/V
Where I is the second moment of the plan area of the body at water
level about its longitudinal axis. Hence, the metacentric height:
MG = MB – GB
MG = I/V – GB
MB = I/V = MG + GB
If the centre of gravity G is below B, then the metacentricheight is given by:
MG = I/V + GB
MB = I/V = MG - GB
The distance MB = I/V is known as the metacentric radius
A rectangular barge is 20 m long, 7 m wide and 3 m deep. it has a
draft of 2 m when fully loaded. The C.G. of barge is on the axis of
symmetry at the water surface. Determine the stability condition of
the barge and the metacentric height.
Sol. A floating body remains in stable equilibrium so long as it has a
positive metacentric height i.e.,
MG = MB – GB = I/V - GB
I = L × d3/12 = 20 × (7)3/12
V = L × d × depth of draft = 20 × 7 × 2
BG = 2 – 1 = 1 m
Making substitutions, the metacentric height is determined as:
MG = [20 × (7)3/12] / (20 × 7 × 2 ) - 1 =1.0417 m
Under the given conditions, the barge is stable and its metacentric
height is 1.0417
Example
A rectangular pontoon is 7m long and 3m wide the weight of the
pontoon is 30 ton. Determine the position of center of gravity
above the base of the pontoon such that it does not overturn in
seawater take the specific weight of water as 0.98 ton/ m3.
Example
Sol. Wtotal= Wdis = Fb = water V dis
30 = 7*3*h*0.98
h=1.45m
I = 7× 33 /12 = 15.75m4
V= 7 × 3 × 1.45 =
MB = I/V = 15.75/30.45 = 0.517m
OM = OB + MB
OB = h/2 = 1.45/2 = 0.725m
OM = 0.725 + 0.517 = 1.242m
OG = OM = 1.242m (Neutral case)
0.725 OG 1.242
O
Determine the volume and density of an object that weight 4 N in water and 5 N in an alcohol of SG 0.8.
Example
Solution:
Fb = Weight of displaced fluid
[(9790)(V object) = W object - 4
[(0.8)(9790)(V object) = W object - 5
subtracting the second equation from the first gives
9790 V object - 7832 V object = 1 , 1958 V object =1
V object = 0.0005107m3
[(9.79)×(1000) ×(0.0005107) = W object - 4 ,
W object = 9.0 N
= W object / V object = 9.0/0.0005107 = 17623 N/m3
= / g = 17623/9.81= 1796 kg/m3 ,
Solution:
Fb rod = 9790(π/4)(0.04)2(8) = 98.42 N,
W rod = rod V rod = (SG) water V rod = (SG) Fb
W rod - Fb rod = (SG) Fb rod - Fb rod = (SG -1 ) Fb rod
W lead =2(9.81) = 19.62 N,
F b lead = water V lead = (water / lead ) ×w lead = W lead / SGlead =
F b lead = 19.62/11.4 = 1.72 N.
Sum moments about B:
MB = 0 = (SG-1)(98.42)(4 cos30o ) - (19.62- 1.72)(8cos30o ) = 0
Solve for SGrod = 0.636
ExampleThe uniform rod in the figure is hinged at B
and in static equilibrium when 2 kg of lead (SG
= 11.4) are attached at its end. What is the
specific gravity of the rod material?
Example
A cylinder made of wood (SG = 0.6) and circular in cross section is
required to float in oil (SG = 0.9), if d = the diameter of the cylinder
and L = height. Prove that L cannot exceed 0.75d for the cylinder to
floating with its longitudinal axis vertical.
Sol. OG = 0.5 L
OB = 0.5h'
W = Fb = Wdis
(d2/4) ×L×0.6 × water = (d2/4) ×h'×0.9 × water
h'=0.67×L OB=0.5h'=0.34×L
BG = OG – OB = 0.5L - 0.34L = 0.16 L
MB = I/V = [(π/4)×(d/2)4 ]/ [(π/4)×(d)2 ×h'] = 0.0933 × (d2/L)
BG = MB
0.16 L = 0.0933 × (d2/L)
d = 1.3L
L = 0.75d