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11/6/2010 1 AAiT Chapter 2 Hydrostatics Buoyancy, Floatation and Stability Zerihun Alemayehu Rm. E119B AAiT Hydraulics I By Zerihun Alemayehu Archimedes Principle F B = weight displaced fluid A floating body displaces its own weight of the fluid in which it floats Line of action passes through the centroid of displaced volume Buoyancy Force of buoyancy an upward force exerted by a fluid pressure on fully or partially floating body Gravity

buoyancy, floation, stability and relative equilibrium

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Page 1: buoyancy, floation, stability and relative equilibrium

11/6/2010

1

AAiT

Chapter 2 Hydrostatics

Buoyancy, Floatation and Stability

Zerihun Alemayehu Rm. E119B

AAiT Hydraulics I

By Zerihun Alemayehu

• Archimedes Principle FB = weight displaced fluid

• A floating body displaces its own weight of the fluid in which it floats

• Line of action passes through the centroid of displaced volume

Buoyancy

Force of buoyancy an upward force exerted by a fluid pressure on fully or partially floating body

Gravity

Page 2: buoyancy, floation, stability and relative equilibrium

11/6/2010

2

AAiT Hydraulics I

By Zerihun Alemayehu

C

Fx

Fz

Fx’

Fz’

A

D B

D’ B’

A’

C’

A’

C’

FB = Fz’ – Fz

FB = g Vol (ABCD)

AAiT Hydraulics I

By Zerihun Alemayehu

F1

W

FB1 = 1V

1

F2

W

FB2 = 2V

2

F1 + 1V = W F2 + 2V = W V(1 - 2) = F1 – F2

=W/V

Page 3: buoyancy, floation, stability and relative equilibrium

11/6/2010

3

AAiT Hydraulics I

By Zerihun Alemayehu

• Buoyant force FB = weight of the hydrometer must remain constant

• Hydrometer floats deeper or shallower depending on the specific weight of the fluid

AAiT Hydraulics I

By Zerihun Alemayehu

h

S = 0.821 S = 0.780

A hydrometer weighs 0.0216 N and has a stem at the upper end that is cylindrical and 2.8 mm in diameter. How much deeper will it float in oil of S=0.78 than in alcohol of S=0.821?

1

2

For position 1:

361

1

1068.2

*9810*821.00216.0

mxV

V

WW waterdisplacedhydrometer

For position 2:

mmmh

hx

AhV

WW waterdisplacedhydrometer

2.230232.0

])0028.0(4

1068.2[*9810*780.0

)(*9810*780.00216.0

26

1

Page 4: buoyancy, floation, stability and relative equilibrium

11/6/2010

4

AAiT

STABILITY

AAiT Hydraulics I

By Zerihun Alemayehu

G

W

B

FB

G

W

B

FB

x

Stable Equilibrium: B always above G

G

W

B

FB

G

W

B

FB

x

G, B

Unstable Equilibrium: B always below G

Neutral Equilibrium: B and G

(i) G and B must lie on the same vertical line in the undisturbed position (ii) B must always be above G for stable equilibrium

FB

Page 5: buoyancy, floation, stability and relative equilibrium

11/6/2010

5

AAiT Hydraulics I

By Zerihun Alemayehu

M = Metacenter MG = Metacenteric height

AAiT Hydraulics I

By Zerihun Alemayehu

Page 6: buoyancy, floation, stability and relative equilibrium

11/6/2010

6

AAiT Hydraulics I

By Zerihun Alemayehu

MG = MB - GB

AAiT

RELATIVE EQUILIBRIUM OF LIQUIDS

Page 7: buoyancy, floation, stability and relative equilibrium

11/6/2010

7

AAiT Hydraulics I

By Zerihun Alemayehu

• Constant Velocity Hydrostatics pressure

• Uniform acceleration/Rotation Relative equilibrium

No relative motion between the liquid particles and the container

• Uniform Linear Acceleration • Uniform rotation about a vertical axis

AAiT Hydraulics I

By Zerihun Alemayehu

P xy

g x y z

x

y

z

x

z

y

Considering equilibrium in the vertical direction

Which reduces to

Similarly in the other direction we get

and

𝜕𝑝

𝜕𝑧= −𝜌(𝑎𝑧 + 𝑔)

Page 8: buoyancy, floation, stability and relative equilibrium

11/6/2010

8

AAiT Hydraulics I

By Zerihun Alemayehu

Lines of constant pressure

Hydrostatic pressure Initial level

On lines of constant pressure

x

y

AAiT Hydraulics I

By Zerihun Alemayehu

ax0 and ay =0

Page 9: buoyancy, floation, stability and relative equilibrium

11/6/2010

9

AAiT Hydraulics I

By Zerihun Alemayehu

ax=0 and ay 0 p = -(g + ay)dy

p = -(g + ay)y where h = -y

p = (g + ay)h

AAiT Hydraulics I

By Zerihun Alemayehu

Page 10: buoyancy, floation, stability and relative equilibrium

11/6/2010

10

AAiT Hydraulics I

By Zerihun Alemayehu

AAiT Hydraulics I

By Zerihun Alemayehu

A rectangle block of wood floats in water with 50 mm projecting above the water surface. When placed in glycerine of relative density 1.35, the block projects 75 mm above the surface of glycerine. Determine the relative density of the wood.

Page 11: buoyancy, floation, stability and relative equilibrium

11/6/2010

11

AAiT Hydraulics I

By Zerihun Alemayehu

• Weight of wooden block, W = uptrust in water =

uptrust in glycerine =weight of the fluid displaced

• W = gAh = w g A(h - 50 x 10-3) = GgA (h - 75 x 10-3)

• The relative density of glycerine=

• h = 146.43 x 10-3 m or 146.43 mm

• Hence the relative density of wood,

• /w=(146.43-50)/146.43 = 0.658

AAiT Hydraulics I

By Zerihun Alemayehu

Determine the maximum ratio of a to b for the stability of a rectangular block of mass density b for a small angle of tilt when it floats in a liquid of mass density 1. The dimension a is greater than b.

b

a

Page 12: buoyancy, floation, stability and relative equilibrium

11/6/2010

12

AAiT Hydraulics I

By Zerihun Alemayehu

b

a h

G

B

O

Consider 1 m length of block

Weight of the block = weight of liquid displaced

bg x ab x 1 = 1 g x bh x 1

h = a x (b/1)

OB = h/2 = a x (b/1)/2

BG = OG – OB

= a/2 – (ba)/21 = a(1-b/1)/2 h/2

BM = Moment of inertia of surface area at the water line

Volume of body immersed in liquid

= (1/12 x 1 x b3)/(b x h x 1) = b2/12h BM = (1b2)/(12a b)

For stability BM BG

AAiT Hydraulics I

By Zerihun Alemayehu

A barge 20 m long x 7 m wide has a draft of 2 m when floating in upright position. Its C.G. is 2.25 m above the bottom, (a) what is it’s initial metacenteric height? (b) If a 5 tone weight is shifted 4 m across the barge, to what distance does the water line rise on the side? Find the rightening moment for this lift.

Page 13: buoyancy, floation, stability and relative equilibrium

11/6/2010

13

AAiT Hydraulics I

By Zerihun Alemayehu

A C

(a) BM = I/V

= [1/12 x 20 x 73/(20 x 7 x 2)]

= 2.045 m

OB = ½ x 2 = 1

BG = OG – OB = 2.25 – 1.0 = 1.25 m

MG = BM – BG = 2.045 – 1.25 = 0.795 m

7m

G

B 2.25m 2m

O

AAiT Hydraulics I

By Zerihun Alemayehu

A C

7m

G

B 2.25m 2m

O

M

moment heeling the ship = 5 x 9.81x4 = 196.2 = moment due to the shifting of G to G‘ = W x GG' But GG' = GM sin sin = 196.2/(9.81 x 20 x 7 x 2 x 0.795) = 0.0904 = 5o12’ Rise of water line on one side = 3.5 tan = 3.5 tan 5o12’ = 0.318 m Rightening moment = W x MG tan = 9.81 x 20 x 7 x 2 x 0.795 x tan 5o12’ =197.1 kNm

Page 14: buoyancy, floation, stability and relative equilibrium

11/6/2010

14

AAiT Hydraulics I

By Zerihun Alemayehu

An oil tanker 3 m wide, 2 m deep and 10 m long contains oil of density 900 kg/m3 to a depth of 1 m. Determine the maximum horizontal acceleration that can be given to the tanker such that the oil just reaches its top end.

If this tanker is closed and completely filled with the oil and accelerated horizontally at 3 m/s2 determine that total liquid thrust (i) on the front end, (ii) on the rear end, and (iii) on one of its longitudinal vertical sides.

AAiT Hydraulics I

By Zerihun Alemayehu

2m

10m

1m

ax

maximum possible surface slope = 1/5 = ax/g ax, the maximum horizontal acceleration = 9.81/5 ax = 1.962 m/s2

Page 15: buoyancy, floation, stability and relative equilibrium

11/6/2010

15

AAiT Hydraulics I

By Zerihun Alemayehu

(i) total thrust on front end AB = ½ g x 22 x 3 = 58.86 kN (ii) total thrust on rear end CD: h = 10 x tan = 10 x ax/g = 10 x 3/9.81 = 3.06 m

2m

10m

ax

h

3m/s2

A

B

C

D gh

g(h+2)

= 239 kN

AAiT Hydraulics I

By Zerihun Alemayehu

• A vertical hoist carries a square tank of 2m x 2m containing water to the top of a construction scaffold with a varying speed of 2 m/s per second. If the water depth is 2m, calculate the total hydrostatic trust on the bottom of the tank.

• If this tank of water is lowered with an acceleration equal to that of gravity, what are the thrusts on the floor and sides of the tank?

Page 16: buoyancy, floation, stability and relative equilibrium

11/6/2010

16

AAiT Hydraulics I

By Zerihun Alemayehu

AAiT Hydraulics I

By Zerihun Alemayehu

A 375 mm high open cylinder, 150 mm in diameter, is filled with water and rotated about its vertical axis at an angular speed of 33.5 rad/s. Determine (i) the depth of water in the cylinder when it is brought to rest, and (ii) the volume of water that remains in the cylinder if the speed is doubled.

Page 17: buoyancy, floation, stability and relative equilibrium

11/6/2010

17

AAiT Hydraulics I

By Zerihun Alemayehu

AAiT Hydraulics I

By Zerihun Alemayehu

The free surface assumes the shape shown in the figure