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PUMPS
and
PIPING
By. Engr. Yuri G. Melliza
PUMPS: It is a steady-state, steady-flow machine in which mechanical
work is added to the fluid in order to transport the liquid from one point to
another point of higher pressure.
Upper
Reservoir

Suction Gauge Discharge Gauge
Lower
Reservoir

Gate Valve
Gate
Valve
CLASSIFICATION OF PUMPS
1. Centrifugal: It consist essentially of an impeller arranged to rotate within
a casing so that the liquid will enter at the center or eye of the impeller and
be thrown outward by centrifugal force to the outer periphery of the impeller
and discharge into the outer case. It operates at high discharge pressure,
low head, high speed and they are not self priming.
 Centrifugal
 Mixed Flow
 single stage
 multi stage
 Propeller or axial flow
 Peripheral
2. Rotary:It is a positive displacement pump consisting of a fixed casing containing gears, cams, screws, vanes, plungers or similar element actuated by
the rotation of the drive shaft. A rotary pump traps a quantity of liquid and
moves it along toward the discharge point. For a gear type rotary pump the
unmeshed gears at the pump provides a space for the liquid to fill as the
gears rotate. The liquid trapped between the teeth and the pump casing is
eventually released at the discharge line. It operates at low heads, low discharge and is used for pumping viscous liquids like oil.
 cam
 gear
 screw
 vane
3. Reciprocating: It is a positive displacement unit wherein the pumping action
is accomplished by the forward and backward movement of a piston or a
plunger inside a cylinder usually provided with valves.
 Piston
 Direct Acting
 single
 duplex
 Crank and Flywheel
 Plunger
 Power Driven
 simplex
 duplex
 triplex
4. Deepwell Pumps: It is used when pumping water from deep wells. The pump
is lowered into the well and operated close to water level. They are usually
motor driven with the motor being at the ground level and connected to the
pump by a long vertical line shaft.
 Turbine
 Ejector or centrifugal
 reciprocating
 Airlift
For a final choice of a pump for a particular operation the following data are needed.
 Number of units required
 Nature of liquid
 Capacity
 Suction conditions
 Discharge conditions
 Intermittent or continuous service
 Total dynamic head
 Position of pump, vertical or horizontal
 Location, geographical, indoor, outdoor, elevation
 Type of power drive
Centrifugal Pump

Reciprocating PUmp
Cylinder

impeller

discharge

eye

Rotary Pump (Gear Type)

Piston
Valves

Gear
Pump principles
Pump principles
Pump principles
FUNDAMENTAL EQUATIONS
1. TOTAL DYNAMIC HEAD
Ht

P2

P1

v2

2

v1

2

2g

γ

Z2

Z1

2. DISCHARGE or CAPACITY
Q = Asvs = Advd m3/sec

3. WATER POWER or FLUID POWER
WP = Q Ht KW
4. BRAKE or SHAFT POWER
BP

2πTN
60,000

KW

HL

meters
5. PUMP EFFICIENCY
ηP

WP
BP

x 100%

6. MOTOR EFFICIENCY
ηm

BP
MP

x 100%

7. COMBINED PUMP-MOTOR EFFICIENCY
ηC
ηC

WP
MP
ηP ηm

x 100%
8. MOTOR POWER
 For Single Phase Motor
MP

EI(cosθ)
1000

KW

 For 3 Phase Motor
MP
where:

3 EI(cosθ)
1000

KW

P - pressure in KPa
v - velocity, m/sec
- specific weight of liquid, KN/m3
Z - elevation, meters
g - gravitational acceleration, m/sec2
HL - total head loss, meters
E - energy, Volts
I - current, amperes
(cos ) - power factor

T - brake torque, N-m
N - no. of RPM
WP - fluid power, KW
BP - brake power, KW
MP - power input to
motor, KW
PIPES and FITTINGS
Nominal Pipe Diameter: Pipe sizes are based on the approximate diameter and
are reported as nominal pipe sizes. Regardless of wall thickness, pipes of the same
nominal diameter have the same outside diameter. This permits interchange of
fittings. Pipe may be manufactured with different and various wall thickness, so
some standardization is necessary. A method of identifying pipe sizes has been
established by ANSI (American National Standard Institute). By convention, pipe
size and fittings are characterized in terms of Nominal Diameter and wall thickness.
For steel pipes, nominal diameter is approximately the same as the inside diameter
for 12" and smaller. For sizes of 14" and larger, the nominal diameter is exactly the
outside diameter.
SCHEDULE NUMBER: The wall thickness of pipe is indicated by a schedule
number, which is a function of internal pressure and allowable stress.
Schedule Number 1000P/S
where P - internal working pressure, KPa
S - allowable stress, KPa
Schedule number in use: 10,20,30, 40,60, 80, 100, 120, 140, and 160.
Schedule 40 "Standard Pipe"
Schedule 80 " Extra Strong Pipe"
FITTING: The term fitting refers to a piece of pipe that can:
1. Join two pieces of pipe
ex. couplings and unions
2. Change pipeline directions
ex. elbows and tees
3. Change pipeline diameters
ex. reducers
4. Terminate a pipeline
ex. plugs and valves
5. Join two streams to form a third
ex. tees, wyes, and crosses
6. Control the flow
ex. valves
VALVES: A valve is also a fitting, but it has more important uses than simply
to connect pipe. Valves are used either to control the flow rate or to shut off
the flow of fluid.
DESIGN OF A PIPING SYSTEM
The following items should be considered by the engineer when he is
developing the design of a piping system.
1. Choice of material and sizes
2. Effects of temperature level and temperature changes.
a. insulation
b. thermal expansion
c. freezing
3. Flexibility of the system for physical and thermal shocks.
4. Adequate support and anchorage
5. Alteration in the system and the service.
6. Maintenance and inspection.
7. Ease of installation
8. Auxiliary and standby pumps and lines
9. Safety
a. Design factors
b. Relief valves and flare systems
HEAD LOSSES
HL = Major loss + Minor losses
Major Loss: Head loss due to friction and turbulence in pipes
Minor Losses: Minor losses includes losses due to valves and fittings,
enlargement, contraction, pipe entrance and pipe exit. Minor losses are most
easily obtained in terms of equivalent length of pipe "Le". the advantage of this
approach is that both pipe and fittings are expressed in terms of
"Equivalent Length" of pipe of the same relative roughness.
Darcy-Weisbach Equation
Considering Major Loss only

f Lv 2
hf
meters
2gD
Considering Major and Minor Losses

hf

f (L

L ) v2
e
meters
2gD
Where; f - friction factor from Moody's Chart
L - length of pipe, m
Le - equivalent length in straight pipe of valves and fittings, m
v - velocity, m/sec
D - pipe inside diameter, m
g - gravitational acceleration, m/sec2

REYNOLD'S NUMBER: Reynold's Number is a non dimensional one which
combines the physical quantities which describes the flow either Laminar
or Turbulent flow. The friction loss in a pipeline is also dependent upon this
dimensionless factor
NR
where;

ρvD

vD

μ

ν

- absolute or dynamic viscosity, Pa-sec
- kinematic viscosity, m2/sec
For a Reynold's Number of less 2100 flow is said to Laminar
For a Reynold's Number of greater than 3000 the flow is Turbulent
Moody’s Chart
f

D

NR

where
- absolute roughness
D - inside diameter
/D - relative roughness
Pump principles
VALUES OF ABSOLUTE ROUGHNESS

FOR NEW PIPES

Type of Material
Drawn tubing, brass, lead, glass
centrifugally spun cement, bituminous
lining, transite
Commercial Steel, Wrought iron
Welded steel pipe
Asphalt-dipped cast iron
Galvanized iron
Cast iron, average
Wood stave

Feet

Millimeter

0.000005
0.00015
0.00015
0.0004
0.0005
0.00085
0.0006 to 0.003

0.0015
0.046
0.046
0.12
0.15
0.25
0.18 to 0.9

Concrete

0.001 to 0.01

0.3 to 3

Riveted steel

0.003 to0.03

0.9 to 9
Pump principles
Pump principles
For Laminar flow:
f

64
NR

Centrifugal Pumps
1. TOTAL HEAD
Ht = nH
where:
n - number of stages
H - head per stage

2. SPECIFIC SPEED: Is the speed in RPM at which a theoretical pump
geometrically similar to the actual pump would run at its best efficiency
if proportion to deliver 1 m3/sec against a total head of 1 m. It serves as
a convenient index of the actual pump type.
NS

where:

N Q

Q - flow in m3/sec for a single suction pump
H - head per stage
N - speed, RPM
NS - specific speed, RPM

3

0.0194 H

4

3. SUCTION SPECIFIC SPEED
S

N Q
3

0.0194 NPSH

4

3

NS

NPSH

S

H

4

where: NPSH - Net Positive Suction Head
4. NET POSITIVE SUCTION HEAD: The amount of pressure in excess
of the vapor pressure of the liquid to prevent cavitation.
NPSH = Hp Hz - Hvp - hfs , meters
where:
Hp - absolute pressure head at liquid surface at suction, m
Hz - elevation of liquid surface at suction, above or below the pump
centerline, m
(+) if above PCL
(-) if below PCL
Hvp - vapor pressure head corresponding the temperature of the
liquid,m
hfs- friction head loss from liquid surface at suction to PCL.

5. CAVITATION: The formation of cavities of water vapor in the suction side
of the pump due to low suction pressure.
CAUSES OF CAVITATION
 Sharp bends.
 High temperature
 High velocity
 Rough surface
 Low atmospheric pressure
EFFECTS OF CAVITATION
 Noise
 Vibration
 Corrosion
 Decreased capacity
6. CAVITATION PARAMETER
4

δ

NPSH

NS

H

S

3
7. IMPELLER DIAMETER
D

60

2gH
πN

meter

where: - peripheral velocity factor whose
value ranges from 0.95 to1.09

8. AFFINITY LAWS OR SIMILARITY LAWS FOR CENTRIFUGAL
MACHINES
a. For Geometrically similar pumps
Q ND3
Power
N3D5
H N2D2
T
N2D5
b. For pumps with Variable Speed and Constant impeller diameter
Q N
Power N3
H N2
c. For pumps at Constant Speed with Variable impeller diameter
Q D
Power D3
H D2
RECIPROCATING PUMPS
Specification: Ds x Dw x L
where: Ds - diameter of steam cylinder
Dw - diameter of water cylinder
L - length of stroke
1. VOLUMETRIC EFFICIENCY
ηV

Q
VD

x 100%

where: Q - discharge , m3/sec
VD - displacement volume, m3/sec
2. DISPLACEMENT VOLUME
 For Single acting
2

VD

L(D W ) Nn' m 3
4(60)

sec

 For Double acting without considering piston rod
2

VD

L(D W ) Nn' m 3
4(60)

sec

 For Double acting considering piston rod
VD

LNn'
4(60)

2

2D W - d

2

m

3

sec

where: N - no. of strokes per minute
L - length of stroke, m
D - diameter of bore, .
d - diameter of piston rod, m
n' - no. of cylinders
n' = 1 (For Simplex)
n' = 2 (For Duplex)
n' = 3 (For Triplex)
3. PERCENT SLIP
% Slip = 100 -

where: hs - enthalpy of supply steam, KJ/kg
he - enthalpy of exhaust steam, KJ/kg
ms - steam flow rate, kg/hr
WP - fluid power, KW

V

4. SLIP
Slip = VD - Q

5. THERMAL EFFICIENCY
e

3600(WP)
m s (h s

he )

x 100%

6. FORCE PRODUCED and ACTING ON THE PISTON ROD
2

Fs

D S (Ps
4

Pe )

KPa

where: Ps - supply steam pressure, KPa
Pe - exhaust steam pressure, KPa
Ds - diameter of steam cylinder, m
(Ps - Pe) - mean effective pressure
7. FORCE TRANSMITTED TO THE LIQUID PISTON
Fw

e m Fs
2

Fw

(Dw) (Pd

Psu )

4

Ds

(Pd

Dw

e m (Ps

where:
em - mechanical efficiency
Psu - suction pressure of water
cylinder, KPa
Pd - discharge pressure of water
cylinder, KPa

KPa

Psu )
Pe )

8. PUMP DUTY: Work done on the water cylinder expressed in
Newton-meter per Million Joules
Pump Duty

9.81m w (H d

H su ) x 10

1000m s (h s - h e )

6

N-m
Million Joules

where: mw - water flow rate, kg/hr
Hd - discharge head of pump, m
Hsu - suction head of pump, m
9. PUMP SPEED
V = 43.64(L)1/2(ft), m/min
2

VD

(D W ) Vn' m
4(60)

where: ft - temperature correction factor
L - length of stroke, m

3

sec

10. TEMPERATURE CORRECTION FACTOR
ft

= 1 For cold water
= 0.85 for 32.2 C water
= 0.71 for 65.5 C water
= 0.55 for 204.4 C water

11. For Indirect Acting pumps
N

907 f t
L
Example no. 1
A mechanical engineer of an industrial plant wishes to install a pump to lift 13
L/sec of water from a sump to a tank on a tower. The water is to be delivered
into a tank 105 KPa. The tank is 18 m above the sump and the pump is 1.5 m
above the water level in the sump.The suction pipe is 100 mm in diameter, 8 m
long and will contain 2 - standard elbows and 1 - Foot valve. The discharge
pipe to the tank is 65 mm in diameter and is 120 m long and contains 5 - 90
elbows, 1 - check valve, and 1 - gate valve. Pipe material is Cast iron.
Determine the KW power required by the pump assuming a pump efficiency of
70% and motor efficiency of 80%.
Other Data
= 0.001569 Pa – sec
= 1000 kg/m3
Pump principles
At Suction

At Discharge
Pump principles
Pump principles
Pump principles
Using point 1 and 2 as reference point
P1 = 0 gage
P2 = 105 Kpa
Z1 = 0
Z2 = 18 m
HL = 0.71+45.634 = 46.34 meters
Pump efficiency = 70%
Motor efficiency = 80%
Overall Efficiency = 0.70(0.80)=0.56
A centrifugal pump design for a 1800 RPM operation and a head of
61 m has a capacity of 190 L/sec with a power input of 132 KW.
What effect will a speed reduction to 1200 RPM have on the head,
capacity and power input of the pump? What will be the change in H,
Q and BP if the impeller diameter is reduced from 305 mm to 254 mm
while the speed is held constant at 1800 RPM. Neglect effects of
fluid viscosity.
Given:
N1 = 1800 RPM
N2 = 1200 RPM
H1 = 61 m
H2 =
Q1 = 190 L/sec
Q2 =
BP1 = 132 KW
BP2 =

For N1 = N2 = 1800 RPM
D1 = 305 mm ; D2 = 254 mm
FROM AFFINITY LAWS OR SIMILARITY LAWS FOR
CENTRIFUGAL MACHINES
a. For Geometrically similar pumps
Q ND3
Power
N3D5
H N2D2
T
N2D5
b. For pumps with Variable Speed and Constant impeller diameter
Q N
Power N3
H N2
c. For pumps at Constant Speed with Variable impeller diameter
Q D
Power D3
H D2
PREPARED BY: ENGR. YURI G. MELLIZA
XAVIER UNIVERSITY
ATENEO DECGAYAN

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Pump principles

  • 2. PUMPS: It is a steady-state, steady-flow machine in which mechanical work is added to the fluid in order to transport the liquid from one point to another point of higher pressure. Upper Reservoir Suction Gauge Discharge Gauge Lower Reservoir Gate Valve Gate Valve
  • 3. CLASSIFICATION OF PUMPS 1. Centrifugal: It consist essentially of an impeller arranged to rotate within a casing so that the liquid will enter at the center or eye of the impeller and be thrown outward by centrifugal force to the outer periphery of the impeller and discharge into the outer case. It operates at high discharge pressure, low head, high speed and they are not self priming.  Centrifugal  Mixed Flow  single stage  multi stage  Propeller or axial flow  Peripheral
  • 4. 2. Rotary:It is a positive displacement pump consisting of a fixed casing containing gears, cams, screws, vanes, plungers or similar element actuated by the rotation of the drive shaft. A rotary pump traps a quantity of liquid and moves it along toward the discharge point. For a gear type rotary pump the unmeshed gears at the pump provides a space for the liquid to fill as the gears rotate. The liquid trapped between the teeth and the pump casing is eventually released at the discharge line. It operates at low heads, low discharge and is used for pumping viscous liquids like oil.  cam  gear  screw  vane
  • 5. 3. Reciprocating: It is a positive displacement unit wherein the pumping action is accomplished by the forward and backward movement of a piston or a plunger inside a cylinder usually provided with valves.  Piston  Direct Acting  single  duplex  Crank and Flywheel  Plunger  Power Driven  simplex  duplex  triplex
  • 6. 4. Deepwell Pumps: It is used when pumping water from deep wells. The pump is lowered into the well and operated close to water level. They are usually motor driven with the motor being at the ground level and connected to the pump by a long vertical line shaft.  Turbine  Ejector or centrifugal  reciprocating  Airlift For a final choice of a pump for a particular operation the following data are needed.  Number of units required  Nature of liquid  Capacity  Suction conditions  Discharge conditions  Intermittent or continuous service  Total dynamic head  Position of pump, vertical or horizontal  Location, geographical, indoor, outdoor, elevation  Type of power drive
  • 11. FUNDAMENTAL EQUATIONS 1. TOTAL DYNAMIC HEAD Ht P2 P1 v2 2 v1 2 2g γ Z2 Z1 2. DISCHARGE or CAPACITY Q = Asvs = Advd m3/sec 3. WATER POWER or FLUID POWER WP = Q Ht KW 4. BRAKE or SHAFT POWER BP 2πTN 60,000 KW HL meters
  • 12. 5. PUMP EFFICIENCY ηP WP BP x 100% 6. MOTOR EFFICIENCY ηm BP MP x 100% 7. COMBINED PUMP-MOTOR EFFICIENCY ηC ηC WP MP ηP ηm x 100%
  • 13. 8. MOTOR POWER  For Single Phase Motor MP EI(cosθ) 1000 KW  For 3 Phase Motor MP where: 3 EI(cosθ) 1000 KW P - pressure in KPa v - velocity, m/sec - specific weight of liquid, KN/m3 Z - elevation, meters g - gravitational acceleration, m/sec2 HL - total head loss, meters E - energy, Volts I - current, amperes (cos ) - power factor T - brake torque, N-m N - no. of RPM WP - fluid power, KW BP - brake power, KW MP - power input to motor, KW
  • 14. PIPES and FITTINGS Nominal Pipe Diameter: Pipe sizes are based on the approximate diameter and are reported as nominal pipe sizes. Regardless of wall thickness, pipes of the same nominal diameter have the same outside diameter. This permits interchange of fittings. Pipe may be manufactured with different and various wall thickness, so some standardization is necessary. A method of identifying pipe sizes has been established by ANSI (American National Standard Institute). By convention, pipe size and fittings are characterized in terms of Nominal Diameter and wall thickness. For steel pipes, nominal diameter is approximately the same as the inside diameter for 12" and smaller. For sizes of 14" and larger, the nominal diameter is exactly the outside diameter. SCHEDULE NUMBER: The wall thickness of pipe is indicated by a schedule number, which is a function of internal pressure and allowable stress. Schedule Number 1000P/S where P - internal working pressure, KPa S - allowable stress, KPa Schedule number in use: 10,20,30, 40,60, 80, 100, 120, 140, and 160. Schedule 40 "Standard Pipe" Schedule 80 " Extra Strong Pipe"
  • 15. FITTING: The term fitting refers to a piece of pipe that can: 1. Join two pieces of pipe ex. couplings and unions 2. Change pipeline directions ex. elbows and tees 3. Change pipeline diameters ex. reducers 4. Terminate a pipeline ex. plugs and valves 5. Join two streams to form a third ex. tees, wyes, and crosses 6. Control the flow ex. valves VALVES: A valve is also a fitting, but it has more important uses than simply to connect pipe. Valves are used either to control the flow rate or to shut off the flow of fluid.
  • 16. DESIGN OF A PIPING SYSTEM The following items should be considered by the engineer when he is developing the design of a piping system. 1. Choice of material and sizes 2. Effects of temperature level and temperature changes. a. insulation b. thermal expansion c. freezing 3. Flexibility of the system for physical and thermal shocks. 4. Adequate support and anchorage 5. Alteration in the system and the service. 6. Maintenance and inspection. 7. Ease of installation 8. Auxiliary and standby pumps and lines 9. Safety a. Design factors b. Relief valves and flare systems
  • 17. HEAD LOSSES HL = Major loss + Minor losses Major Loss: Head loss due to friction and turbulence in pipes Minor Losses: Minor losses includes losses due to valves and fittings, enlargement, contraction, pipe entrance and pipe exit. Minor losses are most easily obtained in terms of equivalent length of pipe "Le". the advantage of this approach is that both pipe and fittings are expressed in terms of "Equivalent Length" of pipe of the same relative roughness. Darcy-Weisbach Equation Considering Major Loss only f Lv 2 hf meters 2gD Considering Major and Minor Losses hf f (L L ) v2 e meters 2gD
  • 18. Where; f - friction factor from Moody's Chart L - length of pipe, m Le - equivalent length in straight pipe of valves and fittings, m v - velocity, m/sec D - pipe inside diameter, m g - gravitational acceleration, m/sec2 REYNOLD'S NUMBER: Reynold's Number is a non dimensional one which combines the physical quantities which describes the flow either Laminar or Turbulent flow. The friction loss in a pipeline is also dependent upon this dimensionless factor NR where; ρvD vD μ ν - absolute or dynamic viscosity, Pa-sec - kinematic viscosity, m2/sec For a Reynold's Number of less 2100 flow is said to Laminar For a Reynold's Number of greater than 3000 the flow is Turbulent
  • 19. Moody’s Chart f D NR where - absolute roughness D - inside diameter /D - relative roughness
  • 21. VALUES OF ABSOLUTE ROUGHNESS FOR NEW PIPES Type of Material Drawn tubing, brass, lead, glass centrifugally spun cement, bituminous lining, transite Commercial Steel, Wrought iron Welded steel pipe Asphalt-dipped cast iron Galvanized iron Cast iron, average Wood stave Feet Millimeter 0.000005 0.00015 0.00015 0.0004 0.0005 0.00085 0.0006 to 0.003 0.0015 0.046 0.046 0.12 0.15 0.25 0.18 to 0.9 Concrete 0.001 to 0.01 0.3 to 3 Riveted steel 0.003 to0.03 0.9 to 9
  • 24. For Laminar flow: f 64 NR Centrifugal Pumps 1. TOTAL HEAD Ht = nH where: n - number of stages H - head per stage 2. SPECIFIC SPEED: Is the speed in RPM at which a theoretical pump geometrically similar to the actual pump would run at its best efficiency if proportion to deliver 1 m3/sec against a total head of 1 m. It serves as a convenient index of the actual pump type.
  • 25. NS where: N Q Q - flow in m3/sec for a single suction pump H - head per stage N - speed, RPM NS - specific speed, RPM 3 0.0194 H 4 3. SUCTION SPECIFIC SPEED S N Q 3 0.0194 NPSH 4 3 NS NPSH S H 4 where: NPSH - Net Positive Suction Head
  • 26. 4. NET POSITIVE SUCTION HEAD: The amount of pressure in excess of the vapor pressure of the liquid to prevent cavitation. NPSH = Hp Hz - Hvp - hfs , meters where: Hp - absolute pressure head at liquid surface at suction, m Hz - elevation of liquid surface at suction, above or below the pump centerline, m (+) if above PCL (-) if below PCL Hvp - vapor pressure head corresponding the temperature of the liquid,m hfs- friction head loss from liquid surface at suction to PCL. 5. CAVITATION: The formation of cavities of water vapor in the suction side of the pump due to low suction pressure.
  • 27. CAUSES OF CAVITATION  Sharp bends.  High temperature  High velocity  Rough surface  Low atmospheric pressure EFFECTS OF CAVITATION  Noise  Vibration  Corrosion  Decreased capacity 6. CAVITATION PARAMETER 4 δ NPSH NS H S 3
  • 28. 7. IMPELLER DIAMETER D 60 2gH πN meter where: - peripheral velocity factor whose value ranges from 0.95 to1.09 8. AFFINITY LAWS OR SIMILARITY LAWS FOR CENTRIFUGAL MACHINES a. For Geometrically similar pumps Q ND3 Power N3D5 H N2D2 T N2D5 b. For pumps with Variable Speed and Constant impeller diameter Q N Power N3 H N2 c. For pumps at Constant Speed with Variable impeller diameter Q D Power D3 H D2
  • 29. RECIPROCATING PUMPS Specification: Ds x Dw x L where: Ds - diameter of steam cylinder Dw - diameter of water cylinder L - length of stroke 1. VOLUMETRIC EFFICIENCY ηV Q VD x 100% where: Q - discharge , m3/sec VD - displacement volume, m3/sec
  • 30. 2. DISPLACEMENT VOLUME  For Single acting 2 VD L(D W ) Nn' m 3 4(60) sec  For Double acting without considering piston rod 2 VD L(D W ) Nn' m 3 4(60) sec  For Double acting considering piston rod VD LNn' 4(60) 2 2D W - d 2 m 3 sec where: N - no. of strokes per minute L - length of stroke, m D - diameter of bore, . d - diameter of piston rod, m n' - no. of cylinders n' = 1 (For Simplex) n' = 2 (For Duplex) n' = 3 (For Triplex)
  • 31. 3. PERCENT SLIP % Slip = 100 - where: hs - enthalpy of supply steam, KJ/kg he - enthalpy of exhaust steam, KJ/kg ms - steam flow rate, kg/hr WP - fluid power, KW V 4. SLIP Slip = VD - Q 5. THERMAL EFFICIENCY e 3600(WP) m s (h s he ) x 100% 6. FORCE PRODUCED and ACTING ON THE PISTON ROD 2 Fs D S (Ps 4 Pe ) KPa where: Ps - supply steam pressure, KPa Pe - exhaust steam pressure, KPa Ds - diameter of steam cylinder, m (Ps - Pe) - mean effective pressure
  • 32. 7. FORCE TRANSMITTED TO THE LIQUID PISTON Fw e m Fs 2 Fw (Dw) (Pd Psu ) 4 Ds (Pd Dw e m (Ps where: em - mechanical efficiency Psu - suction pressure of water cylinder, KPa Pd - discharge pressure of water cylinder, KPa KPa Psu ) Pe ) 8. PUMP DUTY: Work done on the water cylinder expressed in Newton-meter per Million Joules Pump Duty 9.81m w (H d H su ) x 10 1000m s (h s - h e ) 6 N-m Million Joules where: mw - water flow rate, kg/hr Hd - discharge head of pump, m Hsu - suction head of pump, m
  • 33. 9. PUMP SPEED V = 43.64(L)1/2(ft), m/min 2 VD (D W ) Vn' m 4(60) where: ft - temperature correction factor L - length of stroke, m 3 sec 10. TEMPERATURE CORRECTION FACTOR ft = 1 For cold water = 0.85 for 32.2 C water = 0.71 for 65.5 C water = 0.55 for 204.4 C water 11. For Indirect Acting pumps N 907 f t L
  • 34. Example no. 1 A mechanical engineer of an industrial plant wishes to install a pump to lift 13 L/sec of water from a sump to a tank on a tower. The water is to be delivered into a tank 105 KPa. The tank is 18 m above the sump and the pump is 1.5 m above the water level in the sump.The suction pipe is 100 mm in diameter, 8 m long and will contain 2 - standard elbows and 1 - Foot valve. The discharge pipe to the tank is 65 mm in diameter and is 120 m long and contains 5 - 90 elbows, 1 - check valve, and 1 - gate valve. Pipe material is Cast iron. Determine the KW power required by the pump assuming a pump efficiency of 70% and motor efficiency of 80%. Other Data = 0.001569 Pa – sec = 1000 kg/m3
  • 40. Using point 1 and 2 as reference point P1 = 0 gage P2 = 105 Kpa Z1 = 0 Z2 = 18 m HL = 0.71+45.634 = 46.34 meters Pump efficiency = 70% Motor efficiency = 80% Overall Efficiency = 0.70(0.80)=0.56
  • 41. A centrifugal pump design for a 1800 RPM operation and a head of 61 m has a capacity of 190 L/sec with a power input of 132 KW. What effect will a speed reduction to 1200 RPM have on the head, capacity and power input of the pump? What will be the change in H, Q and BP if the impeller diameter is reduced from 305 mm to 254 mm while the speed is held constant at 1800 RPM. Neglect effects of fluid viscosity. Given: N1 = 1800 RPM N2 = 1200 RPM H1 = 61 m H2 = Q1 = 190 L/sec Q2 = BP1 = 132 KW BP2 = For N1 = N2 = 1800 RPM D1 = 305 mm ; D2 = 254 mm
  • 42. FROM AFFINITY LAWS OR SIMILARITY LAWS FOR CENTRIFUGAL MACHINES a. For Geometrically similar pumps Q ND3 Power N3D5 H N2D2 T N2D5 b. For pumps with Variable Speed and Constant impeller diameter Q N Power N3 H N2 c. For pumps at Constant Speed with Variable impeller diameter Q D Power D3 H D2
  • 43. PREPARED BY: ENGR. YURI G. MELLIZA XAVIER UNIVERSITY ATENEO DECGAYAN