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Friday, December 27, 2019

ARCHEMEDIS PRINCIPLES




Archimedes’s Principle and Law of Flotation
Archimedes’s Principle
Consider the diagram below
When piece of wood immersed in fluid then floats due to the buoyant force or upthrust. Where by upthrust force is the upward force enable the object to float or at least seem higher



Archimedes principle also called the law of buoyancy which state that
When a body is partially or totally immersed in a fluid it experiences an upthrust which is equal to the weight of the fluid displaced

U = W
Relationship between Real Weight and Apparent Weight
Consider diagram of the mass (weight) of the object below


Real Weight is the weight of object in air and apparent weight is the weight of object in fluid
Mathematically
U = R - A
Where:
U = Upthrust or Apparent weight loss
A = Apparent weight
R = Real weight
Nb:
i. fluid normally exerts an Upthrust
ii. Upthrust tends to reduce weight of body
iii. 1g of water = 0.01N of water
iv. 1g of water = 1cm3 = 1ml of water

Example,
Given Weight of body in air is 10.10N weight of body when immersed in water is 9.2N. Find the upthrust.
Data given
Real weight, R =10.10N
Apparent weight, A = 9.2N
Upthrust, U = ?
Solution
From: U = R - A
W = 10.10 – 9.2
W =0.9N
Example,
The weight of a body when totally immersed in a liquid is 4.2N if the weight of the liquid displaced is 2.5N. Find the weight of the body in air.
Data given
Apparent weight, A = 4.2N
Upthrust, U = 2.5N
Real weight, R =?
Solution
From: U = R - A - make W1 subject
R = U + A
R = 2.5 + 4.2
R =6.7N
Example,
When an object is totally immersed in water, its weight is recorded as 3.1N if its weight in air is 4.9N. Find upthrust.
Data given
Real weight, R =4.9N
Apparent weight, A = 3.1N
Upthrust, U = ?
Solution
U = 1.8N
Example,
A body immersed in water displaced 1.1N of the liquid if its weight white in the water is 3.3N. Find they weight in air.
Data given
Apparent weight, A = 1.1N
Upthrust, U = 3.3N
Real weight, R =?
Solution
From: U = R - A - make W1 subject
R = U + A
R = 3.3 + 1.1
R = 4.4N
Relative Density by Using Archimedes Principle
Consider the formula below
R.D = msmw (Vw=Vs)
R.D = Ms x gmw x g
Where:
i. mw x g = upthrust = U
ii. Ms x g = real weight = R
iii. R.D = relative density
iv. ms = mass of substance
v. mw (vw = vw) = Mass of an equal volume of water or mass of water displaced

R.D = 𝑅U
But: U = R – A
R.D = 𝑹R−A
Example,
A piece of glass weight in air 1.2N and 0.7N when completely immersed in water calculate it’s.
(a) Relative density
(b) Density of glass

Data given
Weight of body in air, R = 1.2N
Weight of body in water, A = 0.7N
Density of water, ρw = 10000kg/m3
Relative density of glass, R.D = ?
Density of glass, ρg = ?
Solution
(a) Relative density of glass, R.D = ?

From: R.D = R/(R - A) = 1.2/ (1.2 - 0.7) = 2.4
R.D = 2.4
(b) Density of glass, d = ?

From: R.D = ρg/ρw = make ρg subject
ρg = R.D x dw = 2.4 x 1000
ρg = 2400
ρg = 2400 kg/m3
Relative Density of other liquid from water by solid substance in Archimedes Principle
When solid immersed in liquid and water the relative density is given by liquid displaced over water displaced
Mathematically
R.D = weight of liquid displacedWeight of water displaced
R.D = weight of object in air − weight of object in liquidweight of object in air− weight of object in water
R.D = upthrust on liquidupthrust on water = 𝑈𝑙𝑈𝑤
R.D = 𝑅𝐴𝑙𝑅𝐴𝑤
Where:
𝑈𝑙= upthrust on liquid
𝑈𝑤 =upthrust on water
𝐴𝑙= Apparent weight on liquid
𝐴𝑤 = Apparent weight on water
Example,
In an experiment to determine the relative density of a liquid, a solid Q weighted as follows:
Weight Q in air, R = 8.6N
Weight Q in water, AW = 6.0N
Weight Q in liquid, AL = 5.4N
Data given
Weight of body Q in air, R = 8.6 N
Weight of body Q in water, AW = 6.0N
Weight of body Q in liquid, AL = 5.4N
Solution
From:
R.D = 𝑅𝐴𝑙𝑅𝐴𝑤
R.D = 8.6 − 5.4 8.6 – 6.0 = 3.2/2.6 = 1.2
R.D = 1.2
Example,
Using the data shown above and determine the relative density of the liquid
Data given
Weight of body in air, R = 15 N
Weight of body in water, Aw = 11N
Weight of body in liquid, Al = 9N
Relative density, R.D = ?
Solution
From:
R.D = 𝑅𝐴𝑙𝑅𝐴𝑤
R.D = 15 − 9 18 – 11 = 6/7 = 1.5
R.D = 1.5
Example,
A body weights 0.52N in air. Total immersed in water it weighs only 0.32N while its weight when immersed in another liquid is 0.36N. The density of water is 1000 kg/m3. What is the density of the other liquid?
Data given
Weight of body in air, R = 0.52 N
Weight of body in water, Aw = 0.32N
Weight of body in liquid, Al = 0.36N
Density of water ρw = 1000 kg/m3
Relative density, R.D = ?
Density of liquid, ρl = ?
Solution
From:
R.D = 𝑅𝐴𝑙𝑅𝐴𝑤
R.D = 0.52−0.360.52−0.32 = 0.16/0.2 = 0.8
R.D = 0.8
But: R.D = ρl/ ρw – make ρl subject
ρl = R.D x ρw = 0.8 x 1000 = 800
ρl = 800 kg/m3

Sinking
Defn: Sinking is the tendency of an object to fall or drop to lower levels in a fluid

Condition for Sinking
i. Upthrust exerted by fluid is less than weight of object
ii. Object denser than fluid means object has great density than fluid

Floating
Defn: Floating is the tendency of an object to be suspended in (remain) on the surface of a fluid due to the upthrust
Nb:
The ability of an object to float is called Buoyancy
Condition for Floating
i. Upthrust exerted by fluid must be equal or greater to the real weight of the object

Nb: apparent weight approximately equal to zero
A ≈ 0 N
ii. The density of body must lees than that of fluid
iii. Volume of submerged object must be large enough to displace a lot of fluid

Law of Flotation
The law states that
“A floating body displaces its own weight of the fluid in which if floats”
Nb:
The real weight of the body can be expressed in terms of its density

For substance to float, R = U
But: R =mS x g
Since: mS = ρS x vS
Therefore: R = ρS x vS x g
Also: U =mf x g
Since: mf = ρf x vf
Therefore: U = ρf x vf x g
But: vf = %S x vs
Then: %S = (vt/vs) x 100

But: R = U
Then: ρs x vs x g = ρf x vf x g
Ρs x vs x g = ρf x %S x vf x g
Ρs = ρf x %S
Where
R = real weight of substance
U = W = weight of fluid displaced
Ms = mass of substance
Ρs = density of substance
Vs = volume of substance
Mf = mass of fluid displaced
Ρf = density of fluid displaced
Vf = volume of fluid displaced
%S= percentage of substance submerged
Vt = volume submerged

Application of Flotation
Law of flotation is applicant in various substance include
i. Filling Balloons
ii. Filling Hot air balloon
iii. Submarines
iv. Ships
v. Hydrometer

Balloons
Consider the diagram below
Since: mf = ρf x vf
Therefore: U = ρf x vf x g
But: vf = %S x vs
Then: %S = (vt/vs) x 100
But: R = U
Then: ρs x vs x g = ρf x vf x g
Ρs x vs x g = ρf x %S x vf x g
Ρs = ρf x %S
Where
R = real weight of substance
U = W = weight of fluid displaced
Ms = mass of substance
Ρs = density of substance
Vs = volume of substance
Mf = mass of fluid displaced
Ρf = density of fluid displaced
Vf = volume of fluid displaced
%S= percentage of substance submerged
Vt = volume submerged
Application of Flotation
Law of flotation is applicant in various substance include
i. Filling Balloons
ii. Filling Hot air balloon
iii. Submarines
iv. Ships
v. Hydrometer

Balloons
Consider the diagram below
Where:
F = force drift up below
U = upthrust
R = weight of balloon
Mechanism
Balloons is filled with a light gas e.g. Helium which displace volume of air equal to its volume. Since filled gas has the light or has low density that than displaced air so the balloon drifted up by a force
Hot - Air Balloon
Mechanism
When air heated in the envelope is increased and gas inside expand so its volume increase and mass of gas inside envelope remains Constant so its density lowered as if you compare to the external gas (cold air). This different in density drift the balloon and it’s passengers into the air
Consider the diagram below
For substance to float, R = U
But: U = Mt x g
U = (MB + Mc + mh) x g
But: mh = vh x ρh
Then: U = (Mt + vh x ρh) x g - - - - - 1
Also: R = mc x g
But: mc = vc x ρc x g
Then: R = vc x ρc x g - - - - - 2
But: vc = vh = v
Then: equation 1 = equation 2 (U = R)
(Mt + vh x ρh) x g = vc x ρc x g
(Mt + vh x ρh) = vc x ρc
Mt + v x ρh = v x ρc ce: mf = ρf x vf
Mt + v x ρh = v x ρc – make v subject
v = Mt/(ρc - ρh)
v = (ml + mb)/Δρ
Where
Total mass = mt = (MB + Mc + mh)
Volume of hot air = vh
Volume cold air = vc
Mass of hot air = mh
Mass cold air = mc
Mass of balloon = mb
Density hot air = ρh
Density cold air = ρc
Example,
A hot air balloon including the envelope, gondola, burner and fuel and one passenger has a total mass of 450kg. Air outside balloon is at 20℃ and has a density of 1.29kg/m3 the air inside at temperature 120℃ has density of 0.90kg/m3. To what volume must the envelope expand to just lift the balloon into the air?
Data given
Total mass, mt = 450kg
Density at 120℃ , ρ2 = 0.90 kg/m3
Density at 20℃ , ρ1 = 1.29 kg/m3
Volume of air displaced, v1 = ?
Solution
From: v = (ml + mb)/Δρ
v = 450kg /(1.29-0.9)
v = 450kg /(1.29-0.9)
v = 450/0.39 = 1.15
v = 1.15m3
Example,
A balloon has a capacity of 20m3 and it is filled with hydrogen. The balloon fabric and the container have a mass of 2.5kg. What mass of instruments can be lifted by the balloon? (Density of hydrogen = 0.089kg/m3 and density of air is 1.29kg/m3)
Data given
Total mass = mt = ml + mb
Volume capacity, v = 20m3
Volume cold air, v1 =20m3
Mass of balloon, mb = 2.5kg
Density at v2, ρ2 = 0.089kg/m3
Density at v1, ρ1 = 1.29kg/m3
Mass of instrument), ml = ?
Solution
From: v = (ml + mb)/Δρ – make ml subject
Ml = (v x Δρ) – mb)
Ml = (20 x (1.29 – 0.089)) – 2.5
Ml = (20 x 1.201) – 2.5
Ml = 24.02 – 2.5
Ml = 21.52kg
Sub Marine
Consider the diagram above
Mechanism
Submarine made with empty space filled with air called ballast in order to increase its volume in order to devise density of submarine and vice versa
When water filled in the ballast the submarine submerged and when balloon admitted to special tank its due and when ballast is filled with air the sub marine floats like other ship
Nb:
When water quantity increased/ filled in the blast is tend to reduce volume hence increase the density of submarine.
Ship
Ship is made of steel and is expected to sink due to its weight. it contains hollow which increase the volume of ship which help on making less dense that the waters
But when load put on ship it tends to increase the density and mass of ship when overloaded the ship sink completely. To check on over wading ships are marked with line or mark called Plimsoll marks.
Plimsoll line
Plimsoll line on a ship used to show minimum heights (maximum density) above different of water types in different sea as shown in the diagram below

 
Where:
F = for fresh water
S = for sea in summer time
W = for sea in water time
TF = tropical fresh water
WNA = winter in Atlantic
T = Tropical
Hydrometer
Defn: hydrometer is an instrument used for measuring the densities of liquids or hydrometer is an instrument used for determine the relative density of liquids.
Structure of Hydrometer
i. Heavy sinker (bulb): containing mercury or lead shots that keep the hydrometer upright when it floats
ii. Air bulb: it increases volume of displaced liquid and overcomes the weight of the sinker
iii. Stem: stem is thin so that small changes in density (height) give large differences in reading
iv. Scale: inside stem graduated in densities
v. Made up of glass to prevent soaking of the liquid

Nb:
The greater the density of the liquid the shorter the stem of hydrometer immersed
Relative Density of Liquid by Hydrometer
i. When hydrometer floats over water the weight of hydrometer (wg) must equal to the weight of water displaced (ww)

wg = ww
ii. When hydrometer floats over liquid the weight of hydrometer (wg) must equal to the weight of liquid displaced (wl)

wg = wl
iii. since relative density of liquid is given by ratio of density of liquid (ρl) to the density of water (ρw)

R.D = ρl/ρw = wl/vl ÷ ww/vw
Where:
vl = volume of liquid displaced
vw = volume of water displaced
wl = ww
Then: R.D = vw/vl
iv. since cross-section area of the hydrometer is uniform, the volume of water and of liquid displaced are proportional to the lengths immersed in them

R.D = lw/ll
Where:
Lw = length of hydrometer immersed in water
Ll = length of hydrometer immersed in liquid



Consider the Diagram Below
 Where:
Steam volume, v1 = Ah
Bulb volume, v2 = v
Total volume, vt = v1 + v = Ah + v2
But: R = U
Where:
U = upthrust in liquid
ρmn = minimum density
ρmx = maximum density
R = weight of hydrometer
U = vt x ρmn x g
R = v x ρmx x g
But: R = U
Then: vt x ρmn x g = v x ρmx x g
(Ah + v) x ρmn x g = v x ρmx x g
(Ah + v) x ρmn = v x ρmx
Ah x ρmn + v x ρmn = v x ρmx – make v2 subject
v x ρmx - v x ρmn = Ah x ρmn
v x (ρmx - ρmn) = Ah x ρmn
v = (Ah x ρmn)/(ρmx – ρmn
v = (Ah x ρmn)/(ρmx - ρmn)
Example,
Consider the diagram below used to measure density of liquid between 1g/cm3 to 0.81g/cm3 (The area of cross section area of stem is 0.5cm2). Find the volume of hydrometer below 1.0 g/cm3 graduated
Data given
Cross section area of stem, A = 0.5cm2
Height of steam, h = 16 cm
The volume of steam, v1 = Ah = 8 cm3
Total volume, vt = (8 + v2) cm3
Minimum density, ρmn = 0.8 g/cm3
Maximum density, ρmx = 1.0 g/cm3
The volume of bulb, v2 = ?
Solution
The volume of bulb, v2 = ?
From: v2 = (Ah x ρmn)/(ρmx - ρmn)
v2 = (8 x 0.8)/(1 – 0.8)
v2 = 6.4/0.2
v2 = 32 cm3
Example, : NECTA form IV 2012 QN: 4
(a) What does a solid body weight more in air than when immersed in a liquid?
(b) An ordinary hydrometer of mass 27g floats with 4cm of its stem out of water. If cross section area of stem is 0.75cm2 calculate
i. The total volume of stem just under the surface of the liquid
ii. The relative density of the liquid

Data given (b):
Mass of hydrometer, mh = 27g
Mass of water displaced, mw = 27g
Area of stem, A = 0.75cm2
Height of stem, h = 4cm
Density of water, ρw = 1g/cm3
Density of liquid, ρl = ?
Solution
i. Total volume, vt = v1 + v

Volume of stem, v1 = Ah = 3 cm3
Volume of bulb, v = mw x ρw = 27 cm3
vt = v1 + v
vt = Ah + mw x ρw
vt = (3 + 27) cm3
vt = 30 cm3
ii. Relative density, R.D = ?

From: R.D = ρl/ρw
But: ρl = ml/vt = 27/30 = 0.9 g/cm3
Then: R.D = ρl/ρw 0.9/1 = 0.9
R.D = 0.9
Example,
A balloon of volume 2000m3 is filled with hydrogen of density 0.09 kg/m3. If the mass of fabric is 100kg and that of the pilot is 75kg,
i. What will be the greatest mass of equipment that can be carried when operation in air is 1.25kg/m3?
ii. How would this figure change if helium, which has twice the density of hydrogen under the same condition, were to be used?
Solution
i. For hydrogen


Data given
Mt total mass = mt = (ml + mb)
Volume of hydrogen, v2 = 2000m3
Volume surrounding, v1 =20000m3
Mass of balloon, mb = (75+100) = 175kg
Density at v2, ρ2 = 0.09kg/m3
Density at v1, ρ1 = 1.25kg/m3
Density change, Δρ = (ρ2-ρ1) = (1.25 - 0.09) = 1.16kg/m3
Solution
Mass of instrument), ml = ?
From: v = (ml + mb)/Δρ – make ml subject
Ml = (v x Δρ) - mb
Ml = (2000 x 1.16) – 175
Ml = 2320 – 175
Ml = 2145kg
ii. For helium

Data given
Mt total mass = mt = (ml + mb)
Volume of helium, v2 = 2000m3
Volume surrounding, v1 =20000m3
Mass of balloon, mb = (75+100) = 175kg
Density at v2, ρ2 = 0.18kg/m3
Density at v1, ρ1 = 1.25kg/m3
Density change, Δρ = (ρ2-ρ1) = (1.25 - 0.18) = 1.07kg/m3
Solution
Mass of instrument), ml = ?
From:
v = (ml + mb)/Δρ – make ml subject
Ml = (v x Δρ) - mb
Ml = (2000 x 1.07) – 175
Ml = 2140 – 175
Ml = 1965kg
Example,
The mass of a piece of cork (0.25 g/cm3) is 20g. What fraction of the cork is immersed when it floats in water?
Data given
Mass of cork, mc = 20g
Density of cork, ρc = 0.25 g/cm3
Density of water, ρw = 1 g/cm3
Cork Fraction immersed, x = ?
Volume of water displaced, vw = ?
Volume of cork immersed, vc = ?
Solution
From: principle of flotation (vw = vc)
Mc = mass 0f water, mw
20 = vw x 1
Vw = vc = 20 cm3
But: x = vc/vt
Where: Volume of cork, vt = ?
From: ρc = mc/vt
Vt = mc/ ρc = 20/0.25 = 80 cm3
Vt = 80 cm3
X = 20/80 = 1/4
X = 1/4
Example,
The mass of a piece of cork (0.25 g/cm3) is 20g. What fraction of the cork is immersed when it floats in alcohol?(density of alcohol is 0.8 g/cm3)
Data given
Mass of cork, mc = 20g
Density of cork, ρc = 0.25 g/cm3
Density of alcohol, ρa = 0.8 g/cm3
Cork Fraction immersed, x = ?
Volume of alcohol displaced, va = ?
Volume of cork immersed, vc = ?
Solution
From: principle of flotation (va = vc)
Mc = mass 0f water, mw
20 = vw x 0.8
Vw = va = 25 cm3
But: x = vc/vt
Where: Volume of cork, vt = ?
From: ρc = mc/vt
Vt = mc/ ρc = 20/0.25 = 80 cm3
Vt = 80 cm3
X = 25/80 = 5/16
X = 5/16
Example,
A uniform pencil floats upright in water with 8cm of its length immersed. What length is immersed when its floats in glycerol (density of glycerol is 1.3 g/cm3)?
Data given
Length of pencil immersed in water,lw = 8cm
Density of glycerol, ρg = 1.3 g/cm3
Density of water, ρw = 1 g/cm3
Length of pencil immersed in glycerol, lg = ?
Solution
But: R.D of glycerol = lw/lg
Then: lg = lw/R.D = 8/1.3 = 6.2cm
lg = 6.2cm
Example,
A balloon and the gas in it have a mass of 450g and its volume is 500 litres. What is the maximum load it can lift in air of density 1.3 g/cm3?
Data given
Total mass, mt = (ml + mb)
Mass of balloon, mb = 450g
Density of gas, ρg = 1.3 g/cm3
Density change, Δρ = 1.3 g/cm3
Volume of balloon, vb = 500 litres
Maximum load, ml = ?
Solution
Maximum load, ml = ?
From: v = (ml + mb)/Δρ – make ml subject
Ml = (v x Δρ) - mb
Ml = (500 x 1.3) – 450
Ml = 650 – 450
Ml = 200g
Example, : NECTA 2012
The diagram below shows on form of man hydrometer used to me to measure the densities of liquid over the range of 0.8 to 1.00 g/cm3. If the area of cross section of the stem is 0.5 cm2 and the distance between the 0.80 and 100 division is 18cm determine
(a) The volume of hydrometer below 1.00 graduated
(b) The position of the 0.90 graduation

Data given
Cross section area of stem, A = 0.5cm2
Height of steam, h = 18 cm
The volume of steam, v1 = Ah = 9 cm3
Total volume, vt = (9 + v2) cm3
Minimum density, ρmn = 0.8 g/cm3
Maximum density, ρmx = 1.0 g/cm3
The volume of bulb, v2 = ?
Solution
(a) The volume of bulb, v2 = ?

From: v2 = (Ah x ρmn)/(ρmx - ρmn)
v2 = (9 x 0.8)/(1 – 0.8)
v2 = 7.2/0.2
v2 = 36 cm3
(b) What height, h2 of hydrometer when shifted to measure 0.9 g/cm3

But: weight of hydrometer never change
V3 x 0.9 x 0.01N = 0.36N
V3 = 40 3
V3 = Ah2
h2 = 8cm


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