SlideShare a Scribd company logo
1 of 68
FINAL EXAM. 2017 - 2018
By: DR. EZZAT EL-SAYED G. SALEH
Question No. 1 β€œ6 Marks”
The figure shows a bearing, in which a vertical shaft is rotating. An oil film
between the bottom surface of the shaft and a bearing is provided to
rotate. The viscous resistance is offered by the oil to the shaft. Let:
N = speed of the shaft, & R = radius of the shaft,
y = thickness of oil film & the area of the elementary ring = 2 r. dr
Estimate:
a) Total torque required to overcome
the viscous resistance,
a) The power β€œP” absorbed.
Solution: (6 Marks)
 Total torque required to overcome the viscouse resistance
𝑇 =
0
𝑇
𝑑𝑇 =
0
𝑅
πœ‡ Γ—
𝑉
𝑦
. 𝑑𝐴 . π‘Ÿ =
0
𝑅
πœ‡ Γ—
πœ” . π‘Ÿ
𝑦
. 2 πœ‹ π‘Ÿ π‘‘π‘Ÿ . π‘Ÿ
=
πœ‡ βˆ™ πœ‹2
βˆ™ 𝑁
15 𝑦 0
𝑅
π‘Ÿ3 βˆ™ π‘‘π‘Ÿ =
πœ‡ βˆ™ πœ‹2
βˆ™ 𝑁
15 𝑦
π‘Ÿ4
4 0
𝑅
=
πœ‡ βˆ™ πœ‹2
βˆ™ 𝑁
15 𝑦
Γ—
𝑅4
4
=
πœ‡ βˆ™ πœ‹2
βˆ™ 𝑁
60 𝑦
βˆ™ 𝑅4
 The power absorbed β€œP”= 𝐹 Γ— 𝑉 = 𝑇 Γ— πœ”
=
πœ‡βˆ™πœ‹2βˆ™ 𝑁
60 𝑦
βˆ™ 𝑅4 Γ—
2 πœ‹ 𝑁
60
𝑃 =
πœ‡ βˆ™ πœ‹3 βˆ™ 𝑁2
1800 𝑦
βˆ™ 𝑅4
Question No. 2 β€œ16 Marks”
Water is pumped at a rate of 20 cfs through the system shown in the figure.
a) What differential pressure will occur across the orifice?
b) What power must the pump supply to the flow for the given conditions?
c) Also, draw the HGL and the EGL for the system. Assume f = 0.015 for the
pipe.
Solution:
𝑄 = 𝐢𝑑 βˆ™ π‘Žπ‘›
2 𝑃𝑖 βˆ’ 𝑃𝐿
𝜌𝐿 1 βˆ’ 𝛽4 = 𝐢𝑑 βˆ™ π‘Žπ‘›
2 βˆ†π‘ƒ
𝜌𝐿. 1 βˆ’ 𝛽4
where:
𝑑𝑛 = 1 𝑓𝑑 & π‘Žπ‘› = πœ‹ βˆ™ 12 4 = 3.14 4 = 0.785 𝑓𝑑2 and
𝛽 = 𝑑𝑛 𝐷𝑃 = 1 2 = 0.5
 Substituting for 𝑄 = 20 𝑐𝑓𝑠 π‘–π‘›π‘‘π‘œ π‘‘β„Žπ‘’ π‘Žπ‘π‘œπ‘£π‘’ π‘’π‘žπ‘’π‘Žπ‘‘π‘–π‘œπ‘›, 𝑀𝑒 β„Žπ‘Žπ‘£π‘’
20 = 0.62 Γ— 0.785
2 βˆ†π‘ƒ
1.94 Γ— 1 βˆ’ 0.54
1688.64 =
2 βˆ†π‘ƒ
1.94 Γ— 1 βˆ’ 0.54
Or the pressure drop across the orifice plate is:
βˆ†π‘ƒ = 1535.61 𝐼𝑏 𝑓𝑑2 = 24.58 𝑓𝑑 π‘œπ‘“ π‘€π‘Žπ‘‘π‘’π‘Ÿ (6 Marks)
 The average velocity of flow through the pipe is
𝑉 = 𝑄 𝐴 = 𝑄 𝐴 = 20 πœ‹ βˆ™ 22
4 = 6.37 𝑓𝑑 𝑠𝑒𝑐
 The head loss through the pipe only
β„ŽπΏ =
8 π‘“βˆ™πΏ
𝑔 βˆ™ πœ‹2βˆ™ 𝐷𝑃
5 Γ— 𝑄2 =
8 Γ—0.015Γ—300
𝑔 βˆ™ πœ‹2βˆ™ 25 Γ— 202 = 3.54 𝑓𝑑
 Applying Bernoulli’s equation between points β€œ1” and β€œ2”
1
2
𝑍 +
𝑃
𝜌 𝑔
+
𝑉2
2 𝑔 1
+ β„Žπ‘ = 𝑍 +
𝑃
𝜌 𝑔
+
𝑉2
2 𝑔 2
+ β„ŽπΏ 1 β†’2
10 0 0 5 0 0
24.58 + 3.54
10 + β„Žπ‘ = 5 + 24.58 + 3.54
∴ β„Žπ‘= 23.12 𝑓𝑑 π‘Žπ‘›π‘‘
ο‚΅ Power must the pump supply to the flow for the given conditions,
π‘ƒπ‘œπ‘€π‘’π‘Ÿ = 𝜌 𝑔 Γ— 𝑄 Γ— 𝐻𝑝=
1.94Γ—32.2Γ—20Γ—23.12
550
β‰… 53 𝐻𝑝 (8 Marks)
H.G.L
E.G.L
HP
(2 Marks)
Question No. 3 β€œ10 Marks”
The counterweight pivot gate shown in the figure, controls the flow from a
tank. The gate is rectangular and is 3m x 2 m.
Determine the value of the counterweight β€œW” such that the upstream
water can be 1.5 m.
1.5 m
w
Pivot
ο‚΅ The hydrostatic force on the gate
𝐹𝐺 = 𝜌 𝑔 β„Žtβˆ™ 𝐴 = 1000 Γ— 9.81 Γ— 1.50 2 Γ— 3 Γ— 2 =
44145 𝑁 =044145 𝑁 103 = 44.145 π‘˜π‘
ο‚΅ tIt acts at β„Žπ‘.𝑝
= β„Ž +
𝐼𝑐.𝑔
𝐴 βˆ™ β„Ž
=
2
3
Γ— 3.0 = 2.0 π‘š π‘Žπ‘π‘œπ‘£π‘’ π‘‘β„Žπ‘’ β„Žπ‘–π‘›π‘”π‘’ π‘œπ‘› π‘‘β„Žπ‘’ 𝑖𝑛𝑐𝑙𝑖𝑛𝑒𝑑 π‘”π‘Žπ‘‘π‘’
w
1.5 m
πœƒ = π‘π‘œπ‘ βˆ’1
1.5
3
= 60π‘œ
πœƒ
hinge
W sin 60
ο‚΅ Taking moments about the hinge
𝐹𝐺 Γ— 3 βˆ’ β„Žπ‘.𝑝 = π‘Š sin 60π‘œ Γ— 0.60
∴ π‘Š =
𝐹𝐺 Γ— 3 βˆ’ β„Žπ‘.𝑝
sin 60π‘œ Γ— 0.60
=
44.145 Γ— 3 βˆ’ 2
sin 60π‘œ Γ— 0.60
= 84.96 𝐾𝑁
ο‚΅ The value of the counterweight β€œW” such that the upstream water can
be 1.5 m is 84.96 KN. (10 Marks)
Question No. 4 β€œ12 Marks”
A pump is used to deliver water from a well to a tank. The bottom of the tank is
2 m above the water surface in the well. The pipe is commercial steel 2.5 m
long with a diameter of 5 cm and f = 0.02. The pump develops a head of 20 m.
A triangular weir with an included angle of 60Β° β€œCd = 0.58” is located in a wall
of the tank with the bottom of the weir 1 m above the tank floor. Find the level
of the water in the tank above the floor of the tank.
Solution:
ο‚΅ The discharge through a triangular
Weir is expressed as
ο‚΅ 𝑄𝑀=
8
15
𝐢𝑑 2 𝑔 tan
πœƒ
2
βˆ™ 𝐻𝑀
5 2
∴ For πœƒ = 60π‘œ & 𝐢𝑑 = 0.58
𝑄𝑀 =
8
15
Γ— 0.58 Γ— 2 Γ— 9.81 Γ— tan
60
2
βˆ™ 𝐻𝑀
5 2
= 0.79 𝐻𝑀
5 2
ο‚΅ From the given data
𝑄𝑀 = 0.79 βˆ™ β„Ž βˆ’ 1 5 2
ο‚΅ To have a constant water level,
π‘„π‘π‘’π‘šπ‘ = π‘„π‘€π‘’π‘–π‘Ÿ
1
2
ο‚΅ Applying Bernoulli equation between points β€œ1” and β€œ2” gives,
𝑍 +
𝑃
𝜌 𝑔
+
𝑉2
2 𝑔 1
+ β„Žπ‘ = 𝑍 +
𝑃
𝜌 𝑔
+
𝑉2
2 𝑔 2
+ β„ŽπΏ 1 β†’2
ο‚΅ Taking water surface at the lower tank as a reference datum
𝑍 +
𝑃
𝜌 𝑔
+
𝑉2
2 𝑔 1
+ β„Žπ‘ = 𝑍 +
𝑃
𝜌 𝑔
+
𝑉2
2 𝑔 2
+ β„ŽπΏ 1 β†’2
ο‚΅ The head loss in the given system β„ŽπΏ 1 β†’2 =
8 𝑓 𝐿
𝑔 πœ‹2 𝐷5 Γ— 𝑄2
=
8Γ—0.02Γ—2.5
9.81Γ— πœ‹2 Γ—0.055 Γ— 𝑄2
= 13220.3 𝑄2
0 0 0 2 + h 0 0
20 m
∴ 20 = (2 + β„Ž) + 13220.3 𝑄2
or
18 = β„Ž + 13220.3 𝑄2
ο‚΅ But, π‘„π‘π‘’π‘šπ‘ = 0.79 βˆ™ β„Ž βˆ’ 1 5 2
∴ 18 = β„Ž + 13220.3 Γ— 0.79 βˆ™ β„Ž βˆ’ 1 5 2 2
𝑖. 𝑒. 18 = β„Ž + 8250 βˆ™ β„Ž βˆ’ 1 5
∴ 𝐡𝑦 π‘‘π‘Ÿπ‘–π‘Žπ‘™ π‘Žπ‘›π‘‘ π‘’π‘Ÿπ‘Ÿπ‘œπ‘Ÿ "β„Ž" = 1.28 π‘š
ο‚΅ The level of the water in the tank above the floor of the tank = 1.28 π‘š.
(12 Marks)
Question No. 5 β€œ16 Marks”
i. For a hydraulic machine shown in the figure, the following data are available:
Flow : From β€œA” to β€œB”
Discharge: 200 L/s of water
Diameters: at β€œA” 20 cm, and at β€œB” 30 cm
Elevation (m): at β€œA” 105 m, and at β€œB” 100 m
Pressures : at β€œA” 100 kpa, and at β€œB” 200 kpa.
a) Is this machine a pump or a turbine?
b) Calculate the power input or output depending on whether it is pump or a
turbine.
For a hydraulic machine shown in the figure, the following data are available:
Flow : From β€œA” to β€œB”
Discharge : 200 L/s of water
Diameters : at β€œA” 20 cm, and at β€œB” 30 cm
Elevation (m) : at β€œA” 105 m, and at β€œB” 100 m
Pressures : at β€œA” 100 KPa, and at β€œB” 200 KPa.
a) Is this machine a pump or a turbine?
b) Calculate the power input or output depending on whether it is pump or a
turbine.
Solution:
Using the continuity equation
𝑉1 = 𝑄 𝐴1 =
(200 1000)
1000 Γ— πœ‹ .0.20 2 4
= 6.37π‘š 𝑠
and 𝑉2 = 𝑄 𝐴2 =
(200 1000)
1000Γ— πœ‹ .0.30 2 4
= 2.83 π‘š 𝑠
Applying Bernoulli’s equation to point β€œA”, gives the (TEL)A
𝑍 +
𝑃
𝜌 𝑔
+
𝑉2
2 𝑔 𝐴
= 105 +
100Γ—103
103Γ—9.81
+
6.372
2Γ—9.81
= 117.26π‘š
and that at point β€œB”, (TEL)B
𝑍 +
𝑃
𝜌 𝑔
+
𝑉2
2 𝑔 𝐡
= 100 +
200 Γ— 103
103 Γ— 9.81
+
2.832
2 Γ— 9.81
= 120.80π‘š
ο‚΅ Since the TEL at β€œB” is larger than that at β€œA” (the friction losses is
assumed to be zero), this machine a pump with a head = 120.8 βˆ’
117.26 = 3.54 π‘š
ο‚΅ To estimate the power
π‘ƒπ‘œπ‘€π‘’π‘Ÿ = 𝜌 𝑔 Γ— 𝑄 Γ— β„Žπ‘=
103Γ—9.81Γ—(200 103)Γ—3.54
103 = 6.95 π‘˜π‘. π‘š 𝑠 = 6.95 π‘˜π‘€
(8 Marks)
19
ii- A vertical circular tank of 600mm
diameter and 2.5m height is full of
water. It contains two orifices each of
1300 mm2 area, one at the bottom of
the tank and the other at a height of
1.25m above the bottom as shown in
figure.
 Determine the time required to empty
the tank. Take coefficient of discharge
for both of the orifices as 0.62.
20
Given:
β€’ Diameter of the tank =600 = 0.60 m
β€’ Height of the tank = 2.50 m
β€’ Area of each orifice = 1300 mm2 = 1300x 10-6 m2
β€’ C
d
= 0.60
 For the sake of simplicity, let use divide the tank into two parts, i.e.,
 first up to the center of the top orifice, and the to the bottom orifice.
 First of all, consider first part of the example. In this case, the water
is flowing through both orifices.
 Now consider an instant, when the height of water above center of
the top orifice be β€œh” meters and the height of the water above the
bottom orifice will be β€œh +1.25”.
21
The surface area of the tank is constant, 𝐴 =
πœ‹Γ—0.62
4
= 0.283 π‘š2
ο‚£ Now let us use the general equation for the time to empty the tank,
𝑑𝑑 = βˆ’
π΄βˆ™π‘‘β„Ž
πΆπ‘‘βˆ™ π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 β„Ž
β†’ (1)
or for this case (two identical orifices)
𝑑𝑑 = βˆ’
𝐴 βˆ™ π‘‘β„Ž
𝐢𝑑 βˆ™ π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 β„Ž + 𝐢𝑑 βˆ™ π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 β„Ž + 1.25
=βˆ’
π΄βˆ™π‘‘β„Ž
2. 𝐢𝑑 Γ— π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 β„Ž+ β„Ž+1.25
22
For the given data;
𝑇1= βˆ’ 0
1.25 𝐴 βˆ™π‘‘β„Ž
2 . 𝐢𝑑 Γ—π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’βˆ™ 2𝑔 β„Ž+ β„Ž+1.25
= βˆ’
𝐴
2 πΆπ‘‘βˆ™ π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 0
1.25 π‘‘β„Ž
β„Ž+ β„Ž+1.25
Multiplying both numerator and denominator by:
β„Ž βˆ’ β„Ž + 1.25
𝑇1 = βˆ’
𝐴
2 πΆπ‘‘βˆ™ π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 0
1.25
β„Ž βˆ’ β„Ž + 1.25 . π‘‘β„Ž
1.25
= βˆ’
0.283
2 Γ— 0.60 Γ— 0.0013 2 Γ— 9.81 Γ— 1.25 0
1.25
β„Ž βˆ’ β„Ž + 1.25 . π‘‘β„Ž
β‰… 55.82 𝑠𝑒𝑐.
23
Now consider the flow of water below the center of the top orifice. A
little consideration will show that now the water will be flowing through
the bottom orifice only. We know that the time required to empty the
tank,
𝑇2 =
2 𝐴 β„Ž
πΆπ‘‘βˆ™ π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔
=
2 Γ— 0.283 Γ— 1.25
0.6 Γ— 0.0013 Γ— 2 Γ— 9.81
= 183.16 sec
The total time,
𝑇1+ 𝑇2= 55.82 + 183.16 = 239 sec β‰… 4 min
(8 Marks)
24
Question No. 6 β€œ10 Marks”
A sluice gate is used to control the water flow rate over a dam. The
gate is 20 ft wide, and the depth of the water above the bottom of the
sluice gate is 16 ft. The depth of the water upstream of the gate is 20 ft,
and the depth downstream is 3 ft.
i. Estimate the flow rate under the gate and the force on the gate.
𝐹π‘₯
Applying Bernoulli’s equation to point β€œ1” and point β€œ1”, gives,
(Neglecting minor losses and taking the bed of the channel as a
reference datum)
𝑍 +
𝑃
𝜌 𝑔
+
𝑉2
2 𝑔 1
= 𝑍 +
𝑃
𝜌 𝑔
+
𝑉2
2 𝑔 2
For unit discharge
𝑍 +
𝑃
𝜌 𝑔
+
𝑉2
2 𝑔 1
= 𝑍 +
𝑃
𝜌 𝑔
+
𝑉2
2 𝑔 2
=2
0
 0 π‘ž2
2 𝑔 𝑦2
= 3  0 π‘ž2
2 𝑔 𝑦2
20 + 0 +
π‘ž2
2 𝑔 𝑦1
2 = = 3 + 0 +
π‘ž2
2 𝑔 𝑦1
2
∴ 20 βˆ’ 3 ) Γ— 2 Γ— 32.2 = π‘ž2 βˆ™
1
32
βˆ’
1
202
 The flow rate under the gate "π‘ž" β‰… 100 𝑓𝑑3 𝑠/𝑓𝑑 (5 Marks)
 Applying momentum equation between point β€œ1” and point β€œ1”, gives,
𝐹π‘₯,1 βˆ’ 𝐹π‘₯,2 βˆ’ 𝐹π‘₯ = ρ 𝑄 𝑉2 βˆ’ 𝑉1 ……… Eq. (1)
or
𝐹π‘₯,1 βˆ’ 𝐹π‘₯,2 βˆ’ 𝐹π‘₯ = ρ π‘ž2
1
𝑦2
βˆ’
1
𝑦1
 To obtain 𝐹π‘₯,1 βˆ’ 𝐹π‘₯,2 ,
𝐹π‘₯,1 βˆ’ 𝐹π‘₯,2 = 0.5 𝜌 𝑔 𝑦1
2
βˆ’ 𝑦2
2
= 0.50 Γ— 1.94 Γ— 32.2 Γ— 202 βˆ’ 32
= 12212.50 𝐼𝑏 𝑓𝑑 ⇉
π‘Žπ‘›π‘‘ ρ π‘ž2
1
𝑦2
βˆ’
1
𝑦1
= 1.94 Γ— 1002
1
3
βˆ’
1
20
= 5496 𝐼𝑏 𝑓𝑑 ⇉
Eq. (1) gives,
12212.50 βˆ’ 𝐹π‘₯ = 5496
or
𝐹π‘₯ = 12212.50 βˆ’ 5496 = 6716.5 𝐼𝑏 𝑓𝑑 ⇇
 The total force on the gate.
 𝐹π‘₯Γ— 20 = 6716.5 Γ— 20 = 134330 𝐼𝑏 ⇇ … (5 Marks)
 State the assumptions upon which simple tank drainage problems
are based.
 Water flows at a steady rate of 350 m3/ h into a vertical – sided
tank of area 10 m2. The water discharges continuously from a
sluice gate of area 0.0564 m2.
If the initial level in the tank is 2.50 m above the sluice, determine:
The final depth after 5 minutes assuming a discharge coefficient of
0.60 for the sluice.
( Ans. 0.60 m)
A long pipe is installed to carry water from one large reservoir to another (see the
attached figure). The total length of the pipe is of 10 km, its diameter is 0.5 m and
its roughness factor = 0.018. It must climb over a hill, so that the altitude changes
along with distance. The pump must be powerful to push 1 m3/s of water.
What is the pressure drop generated by the water flow?
What is the pumping power required to meet the design requirement,
What would be the power required for the same volume flow if the pipe is
doubled?
Layout of the water pipe (the vertical scale is greatly exaggerated). The
diameter of the pipe is also exaggerated.
25 ft
L = 600 ft, D = ?? , f = 0.02
Main
A
B
Reference datum
The figure shows a pipe delivering water to the putting green on a golf
course. The pressure in the main is 80 p.s.i and it is necessary to
maintain a minimum of 60 p.s.i at point B to adequately supply a
sprinkler system. Specify the required size of steel pipe ( f = 0.02) to
supply 0.50 ft3/s.
Q = 0.5 ft3/s
Pipe Flow and Pipe Systems
Solution: Given:
Diameter of the circular disc 𝐷 = 200/1000 =0.20 m
∴ 𝑅 = D/2 =0.10 m
𝑦 = 0.0004 m
𝑁 = 1000 r.p.m
πœ‡ = 1.05 poise = 1.05/10 = 0.105 N.s/m2
Then
The power required to rotate the disc is given as
𝑃 =
πœ‡ πœ‹2βˆ™π‘2𝑅2βˆ™
1800 ×𝑦
=
0.105Γ— πœ‹2Γ—10002Γ—0.12βˆ™
18000Γ—0.0004
= 452.1 𝑀
Find the power required to rotate a circular disc of diameter 200 mm at
1000 r.p.m. The circular disc has a clearness of 0.4 mm from the bottom
flat plate and the clearness contains oil of viscosity 1.05 poise.
For the system shown in figure, calculate the height β€œH” of oil
at which the rectangular hinged gate will just begin to rotate
counterclockwise.
Gate 1.5x 0.6 m
Oil
S.G.= 0.80
Air
H
1.5 m
30 KPa
Hinge
F1
F2
Oil
Pressure
Air Pressure
1.5 m
(a)
(b)
Deep sump catch basin 2
nonproprietary settling
β„ŽπΏ = π‘˜ .
𝑉2
2 𝑔
where: k =
𝐷𝑝𝑖𝑝𝑒
2
𝐢𝑑. π·π‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’
2 βˆ’ 1
2
∴ β„ŽπΏ=
𝐷𝑝𝑖𝑝𝑒
2
𝐢𝑑. π·π‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’
2 βˆ’ 1
2
.Γ—
8 𝑄2
𝑔 πœ‹2 𝐷𝑝𝑖𝑝𝑒
4
β„ŽπΏ =
22
0.62 Γ— 12
βˆ’ 1
2
.
8 Γ— 202
32.2 Γ— πœ‹2 Γ— 24
= 18.70 ft
𝑸𝑽 =
π…πŸ
πŸ’
Γ— π’…πŸ Γ—
𝟐 βˆ†π‘·
𝝆 𝟏 βˆ’
π’…πŸ’
π‘«πŸ’
Flow
Internal Flow
Pipe Flow
Open Channel Flow
External Flow
Storm water flowing into pond from concrete sewage discharge pipe
The Bernoulli’s equation can be considered to be a statement of the
conservation of energy principle appropriate for flowing fluids.
A vertical circular tank of 600mm diameter and 2.5m height is full of
water. It contains two orifices each of 1300 mm2 area, one at the bottom
of the tank and the other at a height of 1.25m above the bottom as shown
in figure.
Determine the time required to empty the tank. Take coefficient of
discharge for both of the orifices as 0.62..
1.25 m
2.50 m
600 mm
Given,
 Diameter of the tank = 600 mm = 0.6 m & H = 2.5 m
Area of each orifice, a = 1300 mm2 & Cd = 0.62
For the sake of simplicity, let us divide the problem into two parts, i.e.,
first up to the center of the top orifice, and then up to the bottom orifice.
 First of all, consider the first part of the problem. In that case, the water
is flowing through both the orifices.
 Now consider an instant, when the height of water above the center of
the top orifice be h meters. At that instant, the height of water above
the bottom orifice will be (h + 1.25) meters.
 We know that the surface area of the tank,
∴ 𝐴𝑇=
πœ‹
4
Γ— 𝐷𝑇
2
=
πœ‹
4
Γ— 0.602 = 0.283 π‘š2
 Now let us use the general equation for the time to empty a tank,
𝑑𝑑 =
βˆ’ 𝐴 π‘‘β„Ž
𝐢𝑑 βˆ™ π‘Ž βˆ™ 2 𝑔 β„Ž
=
βˆ’ 𝐴 π‘‘β„Ž
𝐢𝑑 βˆ™ π‘Ž βˆ™ 2 𝑔 β„Ž + 1.25 + 𝐢𝑑 βˆ™ π‘Ž βˆ™ 2 𝑔 β„Ž
=
βˆ’ 𝐴 π‘‘β„Ž
𝐢𝑑 βˆ™ 2 π‘Ž βˆ™ 2 𝑔 β„Ž + 1.25 + β„Ž
 The time β€œT1” required to bring the water level up to the center of the
top orifice may be found by integrating the above equation between the
limits 1.25m and 0. Therefore
𝑇1 =
1.25
0
βˆ’ 𝐴 π‘‘β„Ž
𝐢𝑑 βˆ™ 2π‘Ž βˆ™ 2 𝑔 β„Ž + 1.25 + β„Ž
or 𝑇1 =
βˆ’ 𝐴
𝐢𝑑 βˆ™2π‘Ž βˆ™ 2 𝑔 1.25
0 π‘‘β„Ž
β„Ž+1.25 + β„Ž
Multiplying the numerator and denominator by
β„Ž + 1.25 βˆ’ β„Ž
𝑇1 =
0.283
0.62 Γ— 2 Γ— 0.0013 Γ— 2 Γ— 9.81 0
1.25
β„Ž + 1.25 βˆ’ β„Ž
1.25
𝑇1 = 39.58 Γ— 1.05πŸ“ = 61.35 𝑆
 Now consider the flow of water below the center of the top orifice. A
little consideration will show that now the water will be flowing through
the bottom orifice only. We know that the time required to empty the
tank,
𝑇2 =
2 𝐴 𝐻1
𝐢𝑑 βˆ™ 2π‘Ž βˆ™ 2 𝑔
=
2 Γ— 0.283 Γ— 1.25
0.62 Γ— 0.0013 Γ— 2 Γ— 9.81
= 177.25 𝑆
Total time,
𝑇 = 𝑇1 + 𝑇2 = 61.35 + 177.25 β‰… 239 𝑆
‫االبعاد‬
:
120
*
45
*
40
Dimensions 122 x 67
5 shelf's
Name of Presentation
Company Name
Slide Master
β€’ Your Text here
β€’ Lorem ipsum dolor sit amet, consectetuer adipiscing elit, sed
diam nonummy nibh euismod tincidunt ut laoreet dolore
magna aliquam erat volutpat. Ut wisi enim ad minim veniam
β€’ Duis autem vel eum iriure dolor in hendrerit in vulputate velit
esse molestie consequat, vel illum dolore eu feugiat nulla
facilisis at vero eros et accumsan et iusto odio dignissim qui
blandit praesent luptatum zzril delenit augue duis dolore te
feugait nulla facilisi.
FINAL EXAM QUESTIONS ON BEARINGS AND FLUID MECHANICS

More Related Content

What's hot

Full Report.pdf
Full Report.pdfFull Report.pdf
Full Report.pdfgoat17
Β 
Ψ­Ω„ΩˆΩ„ Ω…Ψ³Ψ§ΩŠΩ”Ω„ Ω‚Ω†ΩˆΨ§Ψͺ مفΨͺΩˆΨ­Ω‡ 100 Ψ΅
Ψ­Ω„ΩˆΩ„ Ω…Ψ³Ψ§ΩŠΩ”Ω„ Ω‚Ω†ΩˆΨ§Ψͺ مفΨͺΩˆΨ­Ω‡ 100 Ψ΅Ψ­Ω„ΩˆΩ„ Ω…Ψ³Ψ§ΩŠΩ”Ω„ Ω‚Ω†ΩˆΨ§Ψͺ مفΨͺΩˆΨ­Ω‡ 100 Ψ΅
Ψ­Ω„ΩˆΩ„ Ω…Ψ³Ψ§ΩŠΩ”Ω„ Ω‚Ω†ΩˆΨ§Ψͺ مفΨͺΩˆΨ­Ω‡ 100 Ψ΅shaymaa17
Β 
Examples solutions in open channel flow
Examples solutions in open channel flowExamples solutions in open channel flow
Examples solutions in open channel flowDr. Ezzat Elsayed Gomaa
Β 
(Part iii)- open channels
(Part iii)- open channels(Part iii)- open channels
(Part iii)- open channelsMohsin Siddique
Β 
Open channel design
Open channel designOpen channel design
Open channel designMohsin Siddique
Β 
Pipe network analysis with examples
Pipe network analysis with examplesPipe network analysis with examples
Pipe network analysis with examplesMohsin Siddique
Β 
energy dissipator in hydraulic structure
energy dissipator  in  hydraulic structure energy dissipator  in  hydraulic structure
energy dissipator in hydraulic structure Kiran Jadhav
Β 
Notches and weir
Notches and weirNotches and weir
Notches and weirDewang Agrawal
Β 
(Part ii)- open channels
(Part ii)- open channels(Part ii)- open channels
(Part ii)- open channelsMohsin Siddique
Β 
Open Channel Flows (Lecture notes 04)
Open Channel Flows (Lecture notes 04)Open Channel Flows (Lecture notes 04)
Open Channel Flows (Lecture notes 04)Shekh Muhsen Uddin Ahmed
Β 
LECTURE 5 FLUID FLOW MEASUREMENT.pptx
LECTURE 5 FLUID FLOW MEASUREMENT.pptxLECTURE 5 FLUID FLOW MEASUREMENT.pptx
LECTURE 5 FLUID FLOW MEASUREMENT.pptxVanJasperCastillo
Β 
Geo Technical Engineering (computing lateral earth pressure)
Geo Technical Engineering (computing lateral earth pressure)Geo Technical Engineering (computing lateral earth pressure)
Geo Technical Engineering (computing lateral earth pressure)Latif Hyder Wadho
Β 
Examples on seepage
Examples on seepageExamples on seepage
Examples on seepageMalika khalil
Β 
Ce533 ch1
Ce533 ch1Ce533 ch1
Ce533 ch1sam4111
Β 
Dymanics of open channel flow
Dymanics of open channel flowDymanics of open channel flow
Dymanics of open channel flowMohsin Siddique
Β 

What's hot (20)

Full Report.pdf
Full Report.pdfFull Report.pdf
Full Report.pdf
Β 
Ψ­Ω„ΩˆΩ„ Ω…Ψ³Ψ§ΩŠΩ”Ω„ Ω‚Ω†ΩˆΨ§Ψͺ مفΨͺΩˆΨ­Ω‡ 100 Ψ΅
Ψ­Ω„ΩˆΩ„ Ω…Ψ³Ψ§ΩŠΩ”Ω„ Ω‚Ω†ΩˆΨ§Ψͺ مفΨͺΩˆΨ­Ω‡ 100 Ψ΅Ψ­Ω„ΩˆΩ„ Ω…Ψ³Ψ§ΩŠΩ”Ω„ Ω‚Ω†ΩˆΨ§Ψͺ مفΨͺΩˆΨ­Ω‡ 100 Ψ΅
Ψ­Ω„ΩˆΩ„ Ω…Ψ³Ψ§ΩŠΩ”Ω„ Ω‚Ω†ΩˆΨ§Ψͺ مفΨͺΩˆΨ­Ω‡ 100 Ψ΅
Β 
Examples solutions in open channel flow
Examples solutions in open channel flowExamples solutions in open channel flow
Examples solutions in open channel flow
Β 
Specific Energy (Lecture notes 05)
Specific Energy (Lecture notes 05)Specific Energy (Lecture notes 05)
Specific Energy (Lecture notes 05)
Β 
(Part iii)- open channels
(Part iii)- open channels(Part iii)- open channels
(Part iii)- open channels
Β 
Open channel design
Open channel designOpen channel design
Open channel design
Β 
Pipe network analysis with examples
Pipe network analysis with examplesPipe network analysis with examples
Pipe network analysis with examples
Β 
energy dissipator in hydraulic structure
energy dissipator  in  hydraulic structure energy dissipator  in  hydraulic structure
energy dissipator in hydraulic structure
Β 
SLUICE GATE
SLUICE GATESLUICE GATE
SLUICE GATE
Β 
Notches and weir
Notches and weirNotches and weir
Notches and weir
Β 
(Part ii)- open channels
(Part ii)- open channels(Part ii)- open channels
(Part ii)- open channels
Β 
Open Channel Flows (Lecture notes 04)
Open Channel Flows (Lecture notes 04)Open Channel Flows (Lecture notes 04)
Open Channel Flows (Lecture notes 04)
Β 
LECTURE 5 FLUID FLOW MEASUREMENT.pptx
LECTURE 5 FLUID FLOW MEASUREMENT.pptxLECTURE 5 FLUID FLOW MEASUREMENT.pptx
LECTURE 5 FLUID FLOW MEASUREMENT.pptx
Β 
Weirs and flumes with broad
Weirs and flumes  with broad Weirs and flumes  with broad
Weirs and flumes with broad
Β 
Geo Technical Engineering (computing lateral earth pressure)
Geo Technical Engineering (computing lateral earth pressure)Geo Technical Engineering (computing lateral earth pressure)
Geo Technical Engineering (computing lateral earth pressure)
Β 
Orifice and mouthpieces
Orifice and mouthpieces Orifice and mouthpieces
Orifice and mouthpieces
Β 
Examples on seepage
Examples on seepageExamples on seepage
Examples on seepage
Β 
Open Channel Flow
Open Channel FlowOpen Channel Flow
Open Channel Flow
Β 
Ce533 ch1
Ce533 ch1Ce533 ch1
Ce533 ch1
Β 
Dymanics of open channel flow
Dymanics of open channel flowDymanics of open channel flow
Dymanics of open channel flow
Β 

Similar to FINAL EXAM QUESTIONS ON BEARINGS AND FLUID MECHANICS

UNIT-II FMM
UNIT-II FMMUNIT-II FMM
UNIT-II FMMAravind Ra
Β 
Ψ£Ψ³Ψ¦Ω„Ψ© 1
Ψ£Ψ³Ψ¦Ω„Ψ© 1Ψ£Ψ³Ψ¦Ω„Ψ© 1
Ψ£Ψ³Ψ¦Ω„Ψ© 1Lama K Banna
Β 
Hidraulica ejercicios
Hidraulica ejercicios Hidraulica ejercicios
Hidraulica ejercicios FiorbelaGutierrez
Β 
Problem solving in fluid mechanics
Problem solving in fluid mechanicsProblem solving in fluid mechanics
Problem solving in fluid mechanicsDr. Ezzat Elsayed Gomaa
Β 
Water flow from plastic bottles through pin hole t, engineering math 2 project
Water flow  from plastic bottles through pin hole t, engineering math 2 projectWater flow  from plastic bottles through pin hole t, engineering math 2 project
Water flow from plastic bottles through pin hole t, engineering math 2 projectMubarek Kurt
Β 
pipe lines lec 2.pptx
pipe lines lec 2.pptxpipe lines lec 2.pptx
pipe lines lec 2.pptxamirashraf61
Β 
Midterm f09 solution
Midterm f09 solutionMidterm f09 solution
Midterm f09 solutionmohan sc
Β 
Heat Transfer Final Project, Peden
Heat Transfer Final Project, PedenHeat Transfer Final Project, Peden
Heat Transfer Final Project, PedenDrew Peden
Β 
Design of isolated footing by ACI code
Design of isolated footing by ACI codeDesign of isolated footing by ACI code
Design of isolated footing by ACI codeMahmoud Al-Sharawi
Β 
Rhodes solutions-ch4
Rhodes solutions-ch4Rhodes solutions-ch4
Rhodes solutions-ch4sbjhbsbd
Β 
Pipe project daniel
Pipe project danielPipe project daniel
Pipe project danielDaniel Jalili
Β 
Ejercicios sobre flujo permanente no uniforme
Ejercicios sobre flujo permanente no uniformeEjercicios sobre flujo permanente no uniforme
Ejercicios sobre flujo permanente no uniformeFiorbelaGutierrez
Β 
Tarea 5 hidraulica iii-cabrera arias roberto alejandro
Tarea 5 hidraulica iii-cabrera arias roberto alejandroTarea 5 hidraulica iii-cabrera arias roberto alejandro
Tarea 5 hidraulica iii-cabrera arias roberto alejandroAlejandro Cabrera
Β 
Practica fΓ­sica II EstΓ‘tica de fluidos
Practica fΓ­sica II EstΓ‘tica de fluidosPractica fΓ­sica II EstΓ‘tica de fluidos
Practica fΓ­sica II EstΓ‘tica de fluidosjoseluis1261
Β 
Fluid kinemtics by basnayake mis
Fluid kinemtics by basnayake misFluid kinemtics by basnayake mis
Fluid kinemtics by basnayake misEngMyKer
Β 
pipe lines lec 2.pptx
pipe lines lec 2.pptxpipe lines lec 2.pptx
pipe lines lec 2.pptxamirashraf61
Β 

Similar to FINAL EXAM QUESTIONS ON BEARINGS AND FLUID MECHANICS (20)

UNIT-II FMM
UNIT-II FMMUNIT-II FMM
UNIT-II FMM
Β 
Ψ£Ψ³Ψ¦Ω„Ψ© 1
Ψ£Ψ³Ψ¦Ω„Ψ© 1Ψ£Ψ³Ψ¦Ω„Ψ© 1
Ψ£Ψ³Ψ¦Ω„Ψ© 1
Β 
solved problems in hydrostatic
solved problems in hydrostatic solved problems in hydrostatic
solved problems in hydrostatic
Β 
Hidraulica ejercicios
Hidraulica ejercicios Hidraulica ejercicios
Hidraulica ejercicios
Β 
Problem solving in fluid mechanics
Problem solving in fluid mechanicsProblem solving in fluid mechanics
Problem solving in fluid mechanics
Β 
Ejercicios hidraulica
Ejercicios hidraulicaEjercicios hidraulica
Ejercicios hidraulica
Β 
Water flow from plastic bottles through pin hole t, engineering math 2 project
Water flow  from plastic bottles through pin hole t, engineering math 2 projectWater flow  from plastic bottles through pin hole t, engineering math 2 project
Water flow from plastic bottles through pin hole t, engineering math 2 project
Β 
Flow in Pipes
Flow in PipesFlow in Pipes
Flow in Pipes
Β 
pipe lines lec 2.pptx
pipe lines lec 2.pptxpipe lines lec 2.pptx
pipe lines lec 2.pptx
Β 
Midterm f09 solution
Midterm f09 solutionMidterm f09 solution
Midterm f09 solution
Β 
Heat Transfer Final Project, Peden
Heat Transfer Final Project, PedenHeat Transfer Final Project, Peden
Heat Transfer Final Project, Peden
Β 
MF 10 TuberΓ­as en paralelo y ramificadas
MF 10 TuberΓ­as en paralelo y ramificadasMF 10 TuberΓ­as en paralelo y ramificadas
MF 10 TuberΓ­as en paralelo y ramificadas
Β 
Design of isolated footing by ACI code
Design of isolated footing by ACI codeDesign of isolated footing by ACI code
Design of isolated footing by ACI code
Β 
Rhodes solutions-ch4
Rhodes solutions-ch4Rhodes solutions-ch4
Rhodes solutions-ch4
Β 
Pipe project daniel
Pipe project danielPipe project daniel
Pipe project daniel
Β 
Ejercicios sobre flujo permanente no uniforme
Ejercicios sobre flujo permanente no uniformeEjercicios sobre flujo permanente no uniforme
Ejercicios sobre flujo permanente no uniforme
Β 
Tarea 5 hidraulica iii-cabrera arias roberto alejandro
Tarea 5 hidraulica iii-cabrera arias roberto alejandroTarea 5 hidraulica iii-cabrera arias roberto alejandro
Tarea 5 hidraulica iii-cabrera arias roberto alejandro
Β 
Practica fΓ­sica II EstΓ‘tica de fluidos
Practica fΓ­sica II EstΓ‘tica de fluidosPractica fΓ­sica II EstΓ‘tica de fluidos
Practica fΓ­sica II EstΓ‘tica de fluidos
Β 
Fluid kinemtics by basnayake mis
Fluid kinemtics by basnayake misFluid kinemtics by basnayake mis
Fluid kinemtics by basnayake mis
Β 
pipe lines lec 2.pptx
pipe lines lec 2.pptxpipe lines lec 2.pptx
pipe lines lec 2.pptx
Β 

More from Dr. Ezzat Elsayed Gomaa

Seven edition in fluid mechanics White
Seven edition in fluid mechanics WhiteSeven edition in fluid mechanics White
Seven edition in fluid mechanics WhiteDr. Ezzat Elsayed Gomaa
Β 
Manometers, Pitot tube and Pumps & Turbines Final.
Manometers,  Pitot tube  and Pumps & Turbines Final.Manometers,  Pitot tube  and Pumps & Turbines Final.
Manometers, Pitot tube and Pumps & Turbines Final.Dr. Ezzat Elsayed Gomaa
Β 
Solved Examples in fluid mechanics final
Solved Examples in fluid mechanics finalSolved Examples in fluid mechanics final
Solved Examples in fluid mechanics finalDr. Ezzat Elsayed Gomaa
Β 
Solved Examples in fluid mechanics
Solved Examples in fluid mechanics Solved Examples in fluid mechanics
Solved Examples in fluid mechanics Dr. Ezzat Elsayed Gomaa
Β 
Problem solving in fluid mechanics
Problem solving in fluid mechanicsProblem solving in fluid mechanics
Problem solving in fluid mechanicsDr. Ezzat Elsayed Gomaa
Β 
Sheetproblems in open channel flow
Sheetproblems in open channel flowSheetproblems in open channel flow
Sheetproblems in open channel flowDr. Ezzat Elsayed Gomaa
Β 
Introduction to Hydraulics "Engineering is your job"
Introduction to Hydraulics "Engineering is your job"Introduction to Hydraulics "Engineering is your job"
Introduction to Hydraulics "Engineering is your job"Dr. Ezzat Elsayed Gomaa
Β 

More from Dr. Ezzat Elsayed Gomaa (20)

Summer training
Summer  trainingSummer  training
Summer training
Β 
notes in fluid mechanics
notes in fluid mechanicsnotes in fluid mechanics
notes in fluid mechanics
Β 
Worked examples
  Worked examples  Worked examples
Worked examples
Β 
Seven edition in fluid mechanics White
Seven edition in fluid mechanics WhiteSeven edition in fluid mechanics White
Seven edition in fluid mechanics White
Β 
Manometers, Pitot tube and Pumps & Turbines Final.
Manometers,  Pitot tube  and Pumps & Turbines Final.Manometers,  Pitot tube  and Pumps & Turbines Final.
Manometers, Pitot tube and Pumps & Turbines Final.
Β 
clarifier-calculations
clarifier-calculationsclarifier-calculations
clarifier-calculations
Β 
worked examples
worked examples worked examples
worked examples
Β 
Solved Examples in fluid mechanics final
Solved Examples in fluid mechanics finalSolved Examples in fluid mechanics final
Solved Examples in fluid mechanics final
Β 
Solved Examples in fluid mechanics
Solved Examples in fluid mechanics Solved Examples in fluid mechanics
Solved Examples in fluid mechanics
Β 
Problem solving in fluid mechanics
Problem solving in fluid mechanicsProblem solving in fluid mechanics
Problem solving in fluid mechanics
Β 
sheet of pipe flow
sheet of pipe flowsheet of pipe flow
sheet of pipe flow
Β 
Sheetproblems in open channel flow
Sheetproblems in open channel flowSheetproblems in open channel flow
Sheetproblems in open channel flow
Β 
Introduction to Hydraulics "Engineering is your job"
Introduction to Hydraulics "Engineering is your job"Introduction to Hydraulics "Engineering is your job"
Introduction to Hydraulics "Engineering is your job"
Β 
pelton wheel
pelton wheel pelton wheel
pelton wheel
Β 
Quasi steady and un steady flow
Quasi steady and un steady flowQuasi steady and un steady flow
Quasi steady and un steady flow
Β 
Presentation on MCQ on fluid
Presentation on MCQ on fluidPresentation on MCQ on fluid
Presentation on MCQ on fluid
Β 
MCQ Ex in Fluid mechanics
MCQ Ex in Fluid mechanicsMCQ Ex in Fluid mechanics
MCQ Ex in Fluid mechanics
Β 
How to draw EGL&HGL
 How to draw EGL&HGL How to draw EGL&HGL
How to draw EGL&HGL
Β 
MCQ on fluid & Hydraulics
MCQ on fluid & HydraulicsMCQ on fluid & Hydraulics
MCQ on fluid & Hydraulics
Β 
Fountains&pumps&turbines
 Fountains&pumps&turbines Fountains&pumps&turbines
Fountains&pumps&turbines
Β 

Recently uploaded

(MEERA) Dapodi Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Escorts
(MEERA) Dapodi Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Escorts(MEERA) Dapodi Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Escorts
(MEERA) Dapodi Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Escortsranjana rawat
Β 
College Call Girls Nashik Nehal 7001305949 Independent Escort Service Nashik
College Call Girls Nashik Nehal 7001305949 Independent Escort Service NashikCollege Call Girls Nashik Nehal 7001305949 Independent Escort Service Nashik
College Call Girls Nashik Nehal 7001305949 Independent Escort Service NashikCall Girls in Nagpur High Profile
Β 
SPICE PARK APR2024 ( 6,793 SPICE Models )
SPICE PARK APR2024 ( 6,793 SPICE Models )SPICE PARK APR2024 ( 6,793 SPICE Models )
SPICE PARK APR2024 ( 6,793 SPICE Models )Tsuyoshi Horigome
Β 
Coefficient of Thermal Expansion and their Importance.pptx
Coefficient of Thermal Expansion and their Importance.pptxCoefficient of Thermal Expansion and their Importance.pptx
Coefficient of Thermal Expansion and their Importance.pptxAsutosh Ranjan
Β 
Microscopic Analysis of Ceramic Materials.pptx
Microscopic Analysis of Ceramic Materials.pptxMicroscopic Analysis of Ceramic Materials.pptx
Microscopic Analysis of Ceramic Materials.pptxpurnimasatapathy1234
Β 
Call Girls Service Nagpur Tanvi Call 7001035870 Meet With Nagpur Escorts
Call Girls Service Nagpur Tanvi Call 7001035870 Meet With Nagpur EscortsCall Girls Service Nagpur Tanvi Call 7001035870 Meet With Nagpur Escorts
Call Girls Service Nagpur Tanvi Call 7001035870 Meet With Nagpur EscortsCall Girls in Nagpur High Profile
Β 
Model Call Girl in Narela Delhi reach out to us at πŸ”8264348440πŸ”
Model Call Girl in Narela Delhi reach out to us at πŸ”8264348440πŸ”Model Call Girl in Narela Delhi reach out to us at πŸ”8264348440πŸ”
Model Call Girl in Narela Delhi reach out to us at πŸ”8264348440πŸ”soniya singh
Β 
(ANJALI) Dange Chowk Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...
(ANJALI) Dange Chowk Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...(ANJALI) Dange Chowk Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...
(ANJALI) Dange Chowk Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...ranjana rawat
Β 
Structural Analysis and Design of Foundations: A Comprehensive Handbook for S...
Structural Analysis and Design of Foundations: A Comprehensive Handbook for S...Structural Analysis and Design of Foundations: A Comprehensive Handbook for S...
Structural Analysis and Design of Foundations: A Comprehensive Handbook for S...Dr.Costas Sachpazis
Β 
(PRIYA) Rajgurunagar Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...
(PRIYA) Rajgurunagar Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...(PRIYA) Rajgurunagar Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...
(PRIYA) Rajgurunagar Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...ranjana rawat
Β 
DJARUM4D - SLOT GACOR ONLINE | SLOT DEMO ONLINE
DJARUM4D - SLOT GACOR ONLINE | SLOT DEMO ONLINEDJARUM4D - SLOT GACOR ONLINE | SLOT DEMO ONLINE
DJARUM4D - SLOT GACOR ONLINE | SLOT DEMO ONLINEslot gacor bisa pakai pulsa
Β 
Software Development Life Cycle By Team Orange (Dept. of Pharmacy)
Software Development Life Cycle By  Team Orange (Dept. of Pharmacy)Software Development Life Cycle By  Team Orange (Dept. of Pharmacy)
Software Development Life Cycle By Team Orange (Dept. of Pharmacy)Suman Mia
Β 
HARDNESS, FRACTURE TOUGHNESS AND STRENGTH OF CERAMICS
HARDNESS, FRACTURE TOUGHNESS AND STRENGTH OF CERAMICSHARDNESS, FRACTURE TOUGHNESS AND STRENGTH OF CERAMICS
HARDNESS, FRACTURE TOUGHNESS AND STRENGTH OF CERAMICSRajkumarAkumalla
Β 
VIP Call Girls Service Hitech City Hyderabad Call +91-8250192130
VIP Call Girls Service Hitech City Hyderabad Call +91-8250192130VIP Call Girls Service Hitech City Hyderabad Call +91-8250192130
VIP Call Girls Service Hitech City Hyderabad Call +91-8250192130Suhani Kapoor
Β 
(SHREYA) Chakan Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Esc...
(SHREYA) Chakan Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Esc...(SHREYA) Chakan Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Esc...
(SHREYA) Chakan Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Esc...ranjana rawat
Β 
Call Girls Service Nashik Vaishnavi 7001305949 Independent Escort Service Nashik
Call Girls Service Nashik Vaishnavi 7001305949 Independent Escort Service NashikCall Girls Service Nashik Vaishnavi 7001305949 Independent Escort Service Nashik
Call Girls Service Nashik Vaishnavi 7001305949 Independent Escort Service NashikCall Girls in Nagpur High Profile
Β 
High Profile Call Girls Nagpur Meera Call 7001035870 Meet With Nagpur Escorts
High Profile Call Girls Nagpur Meera Call 7001035870 Meet With Nagpur EscortsHigh Profile Call Girls Nagpur Meera Call 7001035870 Meet With Nagpur Escorts
High Profile Call Girls Nagpur Meera Call 7001035870 Meet With Nagpur EscortsCall Girls in Nagpur High Profile
Β 
Introduction and different types of Ethernet.pptx
Introduction and different types of Ethernet.pptxIntroduction and different types of Ethernet.pptx
Introduction and different types of Ethernet.pptxupamatechverse
Β 

Recently uploaded (20)

(MEERA) Dapodi Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Escorts
(MEERA) Dapodi Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Escorts(MEERA) Dapodi Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Escorts
(MEERA) Dapodi Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Escorts
Β 
College Call Girls Nashik Nehal 7001305949 Independent Escort Service Nashik
College Call Girls Nashik Nehal 7001305949 Independent Escort Service NashikCollege Call Girls Nashik Nehal 7001305949 Independent Escort Service Nashik
College Call Girls Nashik Nehal 7001305949 Independent Escort Service Nashik
Β 
SPICE PARK APR2024 ( 6,793 SPICE Models )
SPICE PARK APR2024 ( 6,793 SPICE Models )SPICE PARK APR2024 ( 6,793 SPICE Models )
SPICE PARK APR2024 ( 6,793 SPICE Models )
Β 
Coefficient of Thermal Expansion and their Importance.pptx
Coefficient of Thermal Expansion and their Importance.pptxCoefficient of Thermal Expansion and their Importance.pptx
Coefficient of Thermal Expansion and their Importance.pptx
Β 
Microscopic Analysis of Ceramic Materials.pptx
Microscopic Analysis of Ceramic Materials.pptxMicroscopic Analysis of Ceramic Materials.pptx
Microscopic Analysis of Ceramic Materials.pptx
Β 
Call Girls Service Nagpur Tanvi Call 7001035870 Meet With Nagpur Escorts
Call Girls Service Nagpur Tanvi Call 7001035870 Meet With Nagpur EscortsCall Girls Service Nagpur Tanvi Call 7001035870 Meet With Nagpur Escorts
Call Girls Service Nagpur Tanvi Call 7001035870 Meet With Nagpur Escorts
Β 
Roadmap to Membership of RICS - Pathways and Routes
Roadmap to Membership of RICS - Pathways and RoutesRoadmap to Membership of RICS - Pathways and Routes
Roadmap to Membership of RICS - Pathways and Routes
Β 
Model Call Girl in Narela Delhi reach out to us at πŸ”8264348440πŸ”
Model Call Girl in Narela Delhi reach out to us at πŸ”8264348440πŸ”Model Call Girl in Narela Delhi reach out to us at πŸ”8264348440πŸ”
Model Call Girl in Narela Delhi reach out to us at πŸ”8264348440πŸ”
Β 
(ANJALI) Dange Chowk Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...
(ANJALI) Dange Chowk Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...(ANJALI) Dange Chowk Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...
(ANJALI) Dange Chowk Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...
Β 
Structural Analysis and Design of Foundations: A Comprehensive Handbook for S...
Structural Analysis and Design of Foundations: A Comprehensive Handbook for S...Structural Analysis and Design of Foundations: A Comprehensive Handbook for S...
Structural Analysis and Design of Foundations: A Comprehensive Handbook for S...
Β 
(PRIYA) Rajgurunagar Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...
(PRIYA) Rajgurunagar Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...(PRIYA) Rajgurunagar Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...
(PRIYA) Rajgurunagar Call Girls Just Call 7001035870 [ Cash on Delivery ] Pun...
Β 
DJARUM4D - SLOT GACOR ONLINE | SLOT DEMO ONLINE
DJARUM4D - SLOT GACOR ONLINE | SLOT DEMO ONLINEDJARUM4D - SLOT GACOR ONLINE | SLOT DEMO ONLINE
DJARUM4D - SLOT GACOR ONLINE | SLOT DEMO ONLINE
Β 
Software Development Life Cycle By Team Orange (Dept. of Pharmacy)
Software Development Life Cycle By  Team Orange (Dept. of Pharmacy)Software Development Life Cycle By  Team Orange (Dept. of Pharmacy)
Software Development Life Cycle By Team Orange (Dept. of Pharmacy)
Β 
HARDNESS, FRACTURE TOUGHNESS AND STRENGTH OF CERAMICS
HARDNESS, FRACTURE TOUGHNESS AND STRENGTH OF CERAMICSHARDNESS, FRACTURE TOUGHNESS AND STRENGTH OF CERAMICS
HARDNESS, FRACTURE TOUGHNESS AND STRENGTH OF CERAMICS
Β 
VIP Call Girls Service Hitech City Hyderabad Call +91-8250192130
VIP Call Girls Service Hitech City Hyderabad Call +91-8250192130VIP Call Girls Service Hitech City Hyderabad Call +91-8250192130
VIP Call Girls Service Hitech City Hyderabad Call +91-8250192130
Β 
(SHREYA) Chakan Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Esc...
(SHREYA) Chakan Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Esc...(SHREYA) Chakan Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Esc...
(SHREYA) Chakan Call Girls Just Call 7001035870 [ Cash on Delivery ] Pune Esc...
Β 
Call Us -/9953056974- Call Girls In Vikaspuri-/- Delhi NCR
Call Us -/9953056974- Call Girls In Vikaspuri-/- Delhi NCRCall Us -/9953056974- Call Girls In Vikaspuri-/- Delhi NCR
Call Us -/9953056974- Call Girls In Vikaspuri-/- Delhi NCR
Β 
Call Girls Service Nashik Vaishnavi 7001305949 Independent Escort Service Nashik
Call Girls Service Nashik Vaishnavi 7001305949 Independent Escort Service NashikCall Girls Service Nashik Vaishnavi 7001305949 Independent Escort Service Nashik
Call Girls Service Nashik Vaishnavi 7001305949 Independent Escort Service Nashik
Β 
High Profile Call Girls Nagpur Meera Call 7001035870 Meet With Nagpur Escorts
High Profile Call Girls Nagpur Meera Call 7001035870 Meet With Nagpur EscortsHigh Profile Call Girls Nagpur Meera Call 7001035870 Meet With Nagpur Escorts
High Profile Call Girls Nagpur Meera Call 7001035870 Meet With Nagpur Escorts
Β 
Introduction and different types of Ethernet.pptx
Introduction and different types of Ethernet.pptxIntroduction and different types of Ethernet.pptx
Introduction and different types of Ethernet.pptx
Β 

FINAL EXAM QUESTIONS ON BEARINGS AND FLUID MECHANICS

  • 1. FINAL EXAM. 2017 - 2018 By: DR. EZZAT EL-SAYED G. SALEH
  • 2. Question No. 1 β€œ6 Marks” The figure shows a bearing, in which a vertical shaft is rotating. An oil film between the bottom surface of the shaft and a bearing is provided to rotate. The viscous resistance is offered by the oil to the shaft. Let: N = speed of the shaft, & R = radius of the shaft, y = thickness of oil film & the area of the elementary ring = 2 r. dr Estimate: a) Total torque required to overcome the viscous resistance, a) The power β€œP” absorbed.
  • 3. Solution: (6 Marks)  Total torque required to overcome the viscouse resistance 𝑇 = 0 𝑇 𝑑𝑇 = 0 𝑅 πœ‡ Γ— 𝑉 𝑦 . 𝑑𝐴 . π‘Ÿ = 0 𝑅 πœ‡ Γ— πœ” . π‘Ÿ 𝑦 . 2 πœ‹ π‘Ÿ π‘‘π‘Ÿ . π‘Ÿ = πœ‡ βˆ™ πœ‹2 βˆ™ 𝑁 15 𝑦 0 𝑅 π‘Ÿ3 βˆ™ π‘‘π‘Ÿ = πœ‡ βˆ™ πœ‹2 βˆ™ 𝑁 15 𝑦 π‘Ÿ4 4 0 𝑅 = πœ‡ βˆ™ πœ‹2 βˆ™ 𝑁 15 𝑦 Γ— 𝑅4 4 = πœ‡ βˆ™ πœ‹2 βˆ™ 𝑁 60 𝑦 βˆ™ 𝑅4  The power absorbed β€œP”= 𝐹 Γ— 𝑉 = 𝑇 Γ— πœ” = πœ‡βˆ™πœ‹2βˆ™ 𝑁 60 𝑦 βˆ™ 𝑅4 Γ— 2 πœ‹ 𝑁 60 𝑃 = πœ‡ βˆ™ πœ‹3 βˆ™ 𝑁2 1800 𝑦 βˆ™ 𝑅4
  • 4. Question No. 2 β€œ16 Marks” Water is pumped at a rate of 20 cfs through the system shown in the figure. a) What differential pressure will occur across the orifice? b) What power must the pump supply to the flow for the given conditions? c) Also, draw the HGL and the EGL for the system. Assume f = 0.015 for the pipe.
  • 5. Solution: 𝑄 = 𝐢𝑑 βˆ™ π‘Žπ‘› 2 𝑃𝑖 βˆ’ 𝑃𝐿 𝜌𝐿 1 βˆ’ 𝛽4 = 𝐢𝑑 βˆ™ π‘Žπ‘› 2 βˆ†π‘ƒ 𝜌𝐿. 1 βˆ’ 𝛽4 where: 𝑑𝑛 = 1 𝑓𝑑 & π‘Žπ‘› = πœ‹ βˆ™ 12 4 = 3.14 4 = 0.785 𝑓𝑑2 and 𝛽 = 𝑑𝑛 𝐷𝑃 = 1 2 = 0.5  Substituting for 𝑄 = 20 𝑐𝑓𝑠 π‘–π‘›π‘‘π‘œ π‘‘β„Žπ‘’ π‘Žπ‘π‘œπ‘£π‘’ π‘’π‘žπ‘’π‘Žπ‘‘π‘–π‘œπ‘›, 𝑀𝑒 β„Žπ‘Žπ‘£π‘’ 20 = 0.62 Γ— 0.785 2 βˆ†π‘ƒ 1.94 Γ— 1 βˆ’ 0.54 1688.64 = 2 βˆ†π‘ƒ 1.94 Γ— 1 βˆ’ 0.54 Or the pressure drop across the orifice plate is: βˆ†π‘ƒ = 1535.61 𝐼𝑏 𝑓𝑑2 = 24.58 𝑓𝑑 π‘œπ‘“ π‘€π‘Žπ‘‘π‘’π‘Ÿ (6 Marks)
  • 6.  The average velocity of flow through the pipe is 𝑉 = 𝑄 𝐴 = 𝑄 𝐴 = 20 πœ‹ βˆ™ 22 4 = 6.37 𝑓𝑑 𝑠𝑒𝑐  The head loss through the pipe only β„ŽπΏ = 8 π‘“βˆ™πΏ 𝑔 βˆ™ πœ‹2βˆ™ 𝐷𝑃 5 Γ— 𝑄2 = 8 Γ—0.015Γ—300 𝑔 βˆ™ πœ‹2βˆ™ 25 Γ— 202 = 3.54 𝑓𝑑  Applying Bernoulli’s equation between points β€œ1” and β€œ2” 1 2
  • 7. 𝑍 + 𝑃 𝜌 𝑔 + 𝑉2 2 𝑔 1 + β„Žπ‘ = 𝑍 + 𝑃 𝜌 𝑔 + 𝑉2 2 𝑔 2 + β„ŽπΏ 1 β†’2 10 0 0 5 0 0 24.58 + 3.54 10 + β„Žπ‘ = 5 + 24.58 + 3.54 ∴ β„Žπ‘= 23.12 𝑓𝑑 π‘Žπ‘›π‘‘ ο‚΅ Power must the pump supply to the flow for the given conditions, π‘ƒπ‘œπ‘€π‘’π‘Ÿ = 𝜌 𝑔 Γ— 𝑄 Γ— 𝐻𝑝= 1.94Γ—32.2Γ—20Γ—23.12 550 β‰… 53 𝐻𝑝 (8 Marks)
  • 9. Question No. 3 β€œ10 Marks” The counterweight pivot gate shown in the figure, controls the flow from a tank. The gate is rectangular and is 3m x 2 m. Determine the value of the counterweight β€œW” such that the upstream water can be 1.5 m. 1.5 m w Pivot
  • 10. ο‚΅ The hydrostatic force on the gate 𝐹𝐺 = 𝜌 𝑔 β„Žtβˆ™ 𝐴 = 1000 Γ— 9.81 Γ— 1.50 2 Γ— 3 Γ— 2 = 44145 𝑁 =044145 𝑁 103 = 44.145 π‘˜π‘ ο‚΅ tIt acts at β„Žπ‘.𝑝 = β„Ž + 𝐼𝑐.𝑔 𝐴 βˆ™ β„Ž = 2 3 Γ— 3.0 = 2.0 π‘š π‘Žπ‘π‘œπ‘£π‘’ π‘‘β„Žπ‘’ β„Žπ‘–π‘›π‘”π‘’ π‘œπ‘› π‘‘β„Žπ‘’ 𝑖𝑛𝑐𝑙𝑖𝑛𝑒𝑑 π‘”π‘Žπ‘‘π‘’ w 1.5 m πœƒ = π‘π‘œπ‘ βˆ’1 1.5 3 = 60π‘œ πœƒ hinge W sin 60
  • 11. ο‚΅ Taking moments about the hinge 𝐹𝐺 Γ— 3 βˆ’ β„Žπ‘.𝑝 = π‘Š sin 60π‘œ Γ— 0.60 ∴ π‘Š = 𝐹𝐺 Γ— 3 βˆ’ β„Žπ‘.𝑝 sin 60π‘œ Γ— 0.60 = 44.145 Γ— 3 βˆ’ 2 sin 60π‘œ Γ— 0.60 = 84.96 𝐾𝑁 ο‚΅ The value of the counterweight β€œW” such that the upstream water can be 1.5 m is 84.96 KN. (10 Marks)
  • 12. Question No. 4 β€œ12 Marks” A pump is used to deliver water from a well to a tank. The bottom of the tank is 2 m above the water surface in the well. The pipe is commercial steel 2.5 m long with a diameter of 5 cm and f = 0.02. The pump develops a head of 20 m. A triangular weir with an included angle of 60Β° β€œCd = 0.58” is located in a wall of the tank with the bottom of the weir 1 m above the tank floor. Find the level of the water in the tank above the floor of the tank.
  • 13. Solution: ο‚΅ The discharge through a triangular Weir is expressed as ο‚΅ 𝑄𝑀= 8 15 𝐢𝑑 2 𝑔 tan πœƒ 2 βˆ™ 𝐻𝑀 5 2 ∴ For πœƒ = 60π‘œ & 𝐢𝑑 = 0.58 𝑄𝑀 = 8 15 Γ— 0.58 Γ— 2 Γ— 9.81 Γ— tan 60 2 βˆ™ 𝐻𝑀 5 2 = 0.79 𝐻𝑀 5 2 ο‚΅ From the given data 𝑄𝑀 = 0.79 βˆ™ β„Ž βˆ’ 1 5 2 ο‚΅ To have a constant water level, π‘„π‘π‘’π‘šπ‘ = π‘„π‘€π‘’π‘–π‘Ÿ 1 2
  • 14. ο‚΅ Applying Bernoulli equation between points β€œ1” and β€œ2” gives, 𝑍 + 𝑃 𝜌 𝑔 + 𝑉2 2 𝑔 1 + β„Žπ‘ = 𝑍 + 𝑃 𝜌 𝑔 + 𝑉2 2 𝑔 2 + β„ŽπΏ 1 β†’2 ο‚΅ Taking water surface at the lower tank as a reference datum 𝑍 + 𝑃 𝜌 𝑔 + 𝑉2 2 𝑔 1 + β„Žπ‘ = 𝑍 + 𝑃 𝜌 𝑔 + 𝑉2 2 𝑔 2 + β„ŽπΏ 1 β†’2 ο‚΅ The head loss in the given system β„ŽπΏ 1 β†’2 = 8 𝑓 𝐿 𝑔 πœ‹2 𝐷5 Γ— 𝑄2 = 8Γ—0.02Γ—2.5 9.81Γ— πœ‹2 Γ—0.055 Γ— 𝑄2 = 13220.3 𝑄2 0 0 0 2 + h 0 0 20 m
  • 15. ∴ 20 = (2 + β„Ž) + 13220.3 𝑄2 or 18 = β„Ž + 13220.3 𝑄2 ο‚΅ But, π‘„π‘π‘’π‘šπ‘ = 0.79 βˆ™ β„Ž βˆ’ 1 5 2 ∴ 18 = β„Ž + 13220.3 Γ— 0.79 βˆ™ β„Ž βˆ’ 1 5 2 2 𝑖. 𝑒. 18 = β„Ž + 8250 βˆ™ β„Ž βˆ’ 1 5 ∴ 𝐡𝑦 π‘‘π‘Ÿπ‘–π‘Žπ‘™ π‘Žπ‘›π‘‘ π‘’π‘Ÿπ‘Ÿπ‘œπ‘Ÿ "β„Ž" = 1.28 π‘š ο‚΅ The level of the water in the tank above the floor of the tank = 1.28 π‘š. (12 Marks)
  • 16. Question No. 5 β€œ16 Marks” i. For a hydraulic machine shown in the figure, the following data are available: Flow : From β€œA” to β€œB” Discharge: 200 L/s of water Diameters: at β€œA” 20 cm, and at β€œB” 30 cm Elevation (m): at β€œA” 105 m, and at β€œB” 100 m Pressures : at β€œA” 100 kpa, and at β€œB” 200 kpa. a) Is this machine a pump or a turbine? b) Calculate the power input or output depending on whether it is pump or a turbine.
  • 17. For a hydraulic machine shown in the figure, the following data are available: Flow : From β€œA” to β€œB” Discharge : 200 L/s of water Diameters : at β€œA” 20 cm, and at β€œB” 30 cm Elevation (m) : at β€œA” 105 m, and at β€œB” 100 m Pressures : at β€œA” 100 KPa, and at β€œB” 200 KPa. a) Is this machine a pump or a turbine? b) Calculate the power input or output depending on whether it is pump or a turbine. Solution: Using the continuity equation 𝑉1 = 𝑄 𝐴1 = (200 1000) 1000 Γ— πœ‹ .0.20 2 4 = 6.37π‘š 𝑠 and 𝑉2 = 𝑄 𝐴2 = (200 1000) 1000Γ— πœ‹ .0.30 2 4 = 2.83 π‘š 𝑠
  • 18. Applying Bernoulli’s equation to point β€œA”, gives the (TEL)A 𝑍 + 𝑃 𝜌 𝑔 + 𝑉2 2 𝑔 𝐴 = 105 + 100Γ—103 103Γ—9.81 + 6.372 2Γ—9.81 = 117.26π‘š and that at point β€œB”, (TEL)B 𝑍 + 𝑃 𝜌 𝑔 + 𝑉2 2 𝑔 𝐡 = 100 + 200 Γ— 103 103 Γ— 9.81 + 2.832 2 Γ— 9.81 = 120.80π‘š ο‚΅ Since the TEL at β€œB” is larger than that at β€œA” (the friction losses is assumed to be zero), this machine a pump with a head = 120.8 βˆ’ 117.26 = 3.54 π‘š ο‚΅ To estimate the power π‘ƒπ‘œπ‘€π‘’π‘Ÿ = 𝜌 𝑔 Γ— 𝑄 Γ— β„Žπ‘= 103Γ—9.81Γ—(200 103)Γ—3.54 103 = 6.95 π‘˜π‘. π‘š 𝑠 = 6.95 π‘˜π‘€ (8 Marks)
  • 19. 19 ii- A vertical circular tank of 600mm diameter and 2.5m height is full of water. It contains two orifices each of 1300 mm2 area, one at the bottom of the tank and the other at a height of 1.25m above the bottom as shown in figure.  Determine the time required to empty the tank. Take coefficient of discharge for both of the orifices as 0.62.
  • 20. 20 Given: β€’ Diameter of the tank =600 = 0.60 m β€’ Height of the tank = 2.50 m β€’ Area of each orifice = 1300 mm2 = 1300x 10-6 m2 β€’ C d = 0.60  For the sake of simplicity, let use divide the tank into two parts, i.e.,  first up to the center of the top orifice, and the to the bottom orifice.  First of all, consider first part of the example. In this case, the water is flowing through both orifices.  Now consider an instant, when the height of water above center of the top orifice be β€œh” meters and the height of the water above the bottom orifice will be β€œh +1.25”.
  • 21. 21 The surface area of the tank is constant, 𝐴 = πœ‹Γ—0.62 4 = 0.283 π‘š2 ο‚£ Now let us use the general equation for the time to empty the tank, 𝑑𝑑 = βˆ’ π΄βˆ™π‘‘β„Ž πΆπ‘‘βˆ™ π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 β„Ž β†’ (1) or for this case (two identical orifices) 𝑑𝑑 = βˆ’ 𝐴 βˆ™ π‘‘β„Ž 𝐢𝑑 βˆ™ π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 β„Ž + 𝐢𝑑 βˆ™ π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 β„Ž + 1.25 =βˆ’ π΄βˆ™π‘‘β„Ž 2. 𝐢𝑑 Γ— π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 β„Ž+ β„Ž+1.25
  • 22. 22 For the given data; 𝑇1= βˆ’ 0 1.25 𝐴 βˆ™π‘‘β„Ž 2 . 𝐢𝑑 Γ—π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’βˆ™ 2𝑔 β„Ž+ β„Ž+1.25 = βˆ’ 𝐴 2 πΆπ‘‘βˆ™ π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 0 1.25 π‘‘β„Ž β„Ž+ β„Ž+1.25 Multiplying both numerator and denominator by: β„Ž βˆ’ β„Ž + 1.25 𝑇1 = βˆ’ 𝐴 2 πΆπ‘‘βˆ™ π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 0 1.25 β„Ž βˆ’ β„Ž + 1.25 . π‘‘β„Ž 1.25 = βˆ’ 0.283 2 Γ— 0.60 Γ— 0.0013 2 Γ— 9.81 Γ— 1.25 0 1.25 β„Ž βˆ’ β„Ž + 1.25 . π‘‘β„Ž β‰… 55.82 𝑠𝑒𝑐.
  • 23. 23 Now consider the flow of water below the center of the top orifice. A little consideration will show that now the water will be flowing through the bottom orifice only. We know that the time required to empty the tank, 𝑇2 = 2 𝐴 β„Ž πΆπ‘‘βˆ™ π‘Žπ‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2𝑔 = 2 Γ— 0.283 Γ— 1.25 0.6 Γ— 0.0013 Γ— 2 Γ— 9.81 = 183.16 sec The total time, 𝑇1+ 𝑇2= 55.82 + 183.16 = 239 sec β‰… 4 min (8 Marks)
  • 24. 24 Question No. 6 β€œ10 Marks” A sluice gate is used to control the water flow rate over a dam. The gate is 20 ft wide, and the depth of the water above the bottom of the sluice gate is 16 ft. The depth of the water upstream of the gate is 20 ft, and the depth downstream is 3 ft. i. Estimate the flow rate under the gate and the force on the gate. 𝐹π‘₯
  • 25. Applying Bernoulli’s equation to point β€œ1” and point β€œ1”, gives, (Neglecting minor losses and taking the bed of the channel as a reference datum) 𝑍 + 𝑃 𝜌 𝑔 + 𝑉2 2 𝑔 1 = 𝑍 + 𝑃 𝜌 𝑔 + 𝑉2 2 𝑔 2 For unit discharge 𝑍 + 𝑃 𝜌 𝑔 + 𝑉2 2 𝑔 1 = 𝑍 + 𝑃 𝜌 𝑔 + 𝑉2 2 𝑔 2 =2 0  0 π‘ž2 2 𝑔 𝑦2 = 3  0 π‘ž2 2 𝑔 𝑦2 20 + 0 + π‘ž2 2 𝑔 𝑦1 2 = = 3 + 0 + π‘ž2 2 𝑔 𝑦1 2
  • 26. ∴ 20 βˆ’ 3 ) Γ— 2 Γ— 32.2 = π‘ž2 βˆ™ 1 32 βˆ’ 1 202  The flow rate under the gate "π‘ž" β‰… 100 𝑓𝑑3 𝑠/𝑓𝑑 (5 Marks)  Applying momentum equation between point β€œ1” and point β€œ1”, gives, 𝐹π‘₯,1 βˆ’ 𝐹π‘₯,2 βˆ’ 𝐹π‘₯ = ρ 𝑄 𝑉2 βˆ’ 𝑉1 ……… Eq. (1) or 𝐹π‘₯,1 βˆ’ 𝐹π‘₯,2 βˆ’ 𝐹π‘₯ = ρ π‘ž2 1 𝑦2 βˆ’ 1 𝑦1  To obtain 𝐹π‘₯,1 βˆ’ 𝐹π‘₯,2 , 𝐹π‘₯,1 βˆ’ 𝐹π‘₯,2 = 0.5 𝜌 𝑔 𝑦1 2 βˆ’ 𝑦2 2 = 0.50 Γ— 1.94 Γ— 32.2 Γ— 202 βˆ’ 32 = 12212.50 𝐼𝑏 𝑓𝑑 ⇉
  • 27. π‘Žπ‘›π‘‘ ρ π‘ž2 1 𝑦2 βˆ’ 1 𝑦1 = 1.94 Γ— 1002 1 3 βˆ’ 1 20 = 5496 𝐼𝑏 𝑓𝑑 ⇉ Eq. (1) gives, 12212.50 βˆ’ 𝐹π‘₯ = 5496 or 𝐹π‘₯ = 12212.50 βˆ’ 5496 = 6716.5 𝐼𝑏 𝑓𝑑 ⇇  The total force on the gate.  𝐹π‘₯Γ— 20 = 6716.5 Γ— 20 = 134330 𝐼𝑏 ⇇ … (5 Marks)
  • 28.
  • 29.  State the assumptions upon which simple tank drainage problems are based.  Water flows at a steady rate of 350 m3/ h into a vertical – sided tank of area 10 m2. The water discharges continuously from a sluice gate of area 0.0564 m2. If the initial level in the tank is 2.50 m above the sluice, determine: The final depth after 5 minutes assuming a discharge coefficient of 0.60 for the sluice. ( Ans. 0.60 m)
  • 30. A long pipe is installed to carry water from one large reservoir to another (see the attached figure). The total length of the pipe is of 10 km, its diameter is 0.5 m and its roughness factor = 0.018. It must climb over a hill, so that the altitude changes along with distance. The pump must be powerful to push 1 m3/s of water. What is the pressure drop generated by the water flow? What is the pumping power required to meet the design requirement, What would be the power required for the same volume flow if the pipe is doubled? Layout of the water pipe (the vertical scale is greatly exaggerated). The diameter of the pipe is also exaggerated.
  • 31. 25 ft L = 600 ft, D = ?? , f = 0.02 Main A B Reference datum The figure shows a pipe delivering water to the putting green on a golf course. The pressure in the main is 80 p.s.i and it is necessary to maintain a minimum of 60 p.s.i at point B to adequately supply a sprinkler system. Specify the required size of steel pipe ( f = 0.02) to supply 0.50 ft3/s. Q = 0.5 ft3/s Pipe Flow and Pipe Systems
  • 32. Solution: Given: Diameter of the circular disc 𝐷 = 200/1000 =0.20 m ∴ 𝑅 = D/2 =0.10 m 𝑦 = 0.0004 m 𝑁 = 1000 r.p.m πœ‡ = 1.05 poise = 1.05/10 = 0.105 N.s/m2 Then The power required to rotate the disc is given as 𝑃 = πœ‡ πœ‹2βˆ™π‘2𝑅2βˆ™ 1800 ×𝑦 = 0.105Γ— πœ‹2Γ—10002Γ—0.12βˆ™ 18000Γ—0.0004 = 452.1 𝑀 Find the power required to rotate a circular disc of diameter 200 mm at 1000 r.p.m. The circular disc has a clearness of 0.4 mm from the bottom flat plate and the clearness contains oil of viscosity 1.05 poise.
  • 33. For the system shown in figure, calculate the height β€œH” of oil at which the rectangular hinged gate will just begin to rotate counterclockwise. Gate 1.5x 0.6 m Oil S.G.= 0.80 Air H 1.5 m 30 KPa Hinge F1 F2 Oil Pressure Air Pressure 1.5 m (a) (b)
  • 34.
  • 35.
  • 36.
  • 37.
  • 38. Deep sump catch basin 2 nonproprietary settling
  • 39.
  • 40.
  • 41.
  • 42.
  • 43. β„ŽπΏ = π‘˜ . 𝑉2 2 𝑔 where: k = 𝐷𝑝𝑖𝑝𝑒 2 𝐢𝑑. π·π‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2 βˆ’ 1 2 ∴ β„ŽπΏ= 𝐷𝑝𝑖𝑝𝑒 2 𝐢𝑑. π·π‘œπ‘Ÿπ‘–π‘“π‘–π‘π‘’ 2 βˆ’ 1 2 .Γ— 8 𝑄2 𝑔 πœ‹2 𝐷𝑝𝑖𝑝𝑒 4 β„ŽπΏ = 22 0.62 Γ— 12 βˆ’ 1 2 . 8 Γ— 202 32.2 Γ— πœ‹2 Γ— 24 = 18.70 ft
  • 44. 𝑸𝑽 = π…πŸ πŸ’ Γ— π’…πŸ Γ— 𝟐 βˆ†π‘· 𝝆 𝟏 βˆ’ π’…πŸ’ π‘«πŸ’
  • 45.
  • 46. Flow Internal Flow Pipe Flow Open Channel Flow External Flow
  • 47.
  • 48. Storm water flowing into pond from concrete sewage discharge pipe
  • 49. The Bernoulli’s equation can be considered to be a statement of the conservation of energy principle appropriate for flowing fluids.
  • 50.
  • 51.
  • 52.
  • 53.
  • 54.
  • 55.
  • 56.
  • 57. A vertical circular tank of 600mm diameter and 2.5m height is full of water. It contains two orifices each of 1300 mm2 area, one at the bottom of the tank and the other at a height of 1.25m above the bottom as shown in figure. Determine the time required to empty the tank. Take coefficient of discharge for both of the orifices as 0.62.. 1.25 m 2.50 m 600 mm
  • 58. Given,  Diameter of the tank = 600 mm = 0.6 m & H = 2.5 m Area of each orifice, a = 1300 mm2 & Cd = 0.62 For the sake of simplicity, let us divide the problem into two parts, i.e., first up to the center of the top orifice, and then up to the bottom orifice.  First of all, consider the first part of the problem. In that case, the water is flowing through both the orifices.  Now consider an instant, when the height of water above the center of the top orifice be h meters. At that instant, the height of water above the bottom orifice will be (h + 1.25) meters.  We know that the surface area of the tank,
  • 59. ∴ 𝐴𝑇= πœ‹ 4 Γ— 𝐷𝑇 2 = πœ‹ 4 Γ— 0.602 = 0.283 π‘š2  Now let us use the general equation for the time to empty a tank, 𝑑𝑑 = βˆ’ 𝐴 π‘‘β„Ž 𝐢𝑑 βˆ™ π‘Ž βˆ™ 2 𝑔 β„Ž = βˆ’ 𝐴 π‘‘β„Ž 𝐢𝑑 βˆ™ π‘Ž βˆ™ 2 𝑔 β„Ž + 1.25 + 𝐢𝑑 βˆ™ π‘Ž βˆ™ 2 𝑔 β„Ž = βˆ’ 𝐴 π‘‘β„Ž 𝐢𝑑 βˆ™ 2 π‘Ž βˆ™ 2 𝑔 β„Ž + 1.25 + β„Ž  The time β€œT1” required to bring the water level up to the center of the top orifice may be found by integrating the above equation between the limits 1.25m and 0. Therefore
  • 60. 𝑇1 = 1.25 0 βˆ’ 𝐴 π‘‘β„Ž 𝐢𝑑 βˆ™ 2π‘Ž βˆ™ 2 𝑔 β„Ž + 1.25 + β„Ž or 𝑇1 = βˆ’ 𝐴 𝐢𝑑 βˆ™2π‘Ž βˆ™ 2 𝑔 1.25 0 π‘‘β„Ž β„Ž+1.25 + β„Ž Multiplying the numerator and denominator by β„Ž + 1.25 βˆ’ β„Ž 𝑇1 = 0.283 0.62 Γ— 2 Γ— 0.0013 Γ— 2 Γ— 9.81 0 1.25 β„Ž + 1.25 βˆ’ β„Ž 1.25 𝑇1 = 39.58 Γ— 1.05πŸ“ = 61.35 𝑆  Now consider the flow of water below the center of the top orifice. A little consideration will show that now the water will be flowing through the bottom orifice only. We know that the time required to empty the tank,
  • 61. 𝑇2 = 2 𝐴 𝐻1 𝐢𝑑 βˆ™ 2π‘Ž βˆ™ 2 𝑔 = 2 Γ— 0.283 Γ— 1.25 0.62 Γ— 0.0013 Γ— 2 Γ— 9.81 = 177.25 𝑆 Total time, 𝑇 = 𝑇1 + 𝑇2 = 61.35 + 177.25 β‰… 239 𝑆
  • 63. Dimensions 122 x 67 5 shelf's
  • 64.
  • 65.
  • 67. Slide Master β€’ Your Text here β€’ Lorem ipsum dolor sit amet, consectetuer adipiscing elit, sed diam nonummy nibh euismod tincidunt ut laoreet dolore magna aliquam erat volutpat. Ut wisi enim ad minim veniam β€’ Duis autem vel eum iriure dolor in hendrerit in vulputate velit esse molestie consequat, vel illum dolore eu feugiat nulla facilisis at vero eros et accumsan et iusto odio dignissim qui blandit praesent luptatum zzril delenit augue duis dolore te feugait nulla facilisi.