Fluid Mach
Fluid Mach
Fluid Mach
ME9
FLUID MACHINERY
CHAPTER 1
1. Pressure head, hP
hv =
, v =
= 32.2
hP, hP =
= weight density
f = weight density of fluid = (S.G.)(water)
Where,
w = 9.81
= 62.4
is the pressure of
a 100 cm
3. Volume flow, Q
4. Power of a jet, P
Figure 1.2
Q = (A
Figure 1.3
P =
v) =
Where, P = Power
= Weight density = g
v = velocity
Q = volume flow rate
5. For bubbles
Where, v =
Cd = coefficient of discharge
Exercise #3: Water is flowing through a cast iron
pipe at the rate of 3500 GPM. The inside diameter of
pipe is 6 in. Find the flow velocity.
Figure 1.4
h + Patm
*absolute P
6.
Bernoullis
Energy
Theorem
neglecting
friction, the total head or total amount of energy
per unit weight, is the same at every point in the
path of flow.
8. Reynolds Number, NR
NR =
(dimensionless)
+ z1 =
+ z2
7. Viscosity,
resistance to flow
property to resist shear deformation.
or
the
or
Kinematic
Viscosity,
absolute
viscosity
hL =
B. Using Darcys Equation:
hL =
L = pipe length
g = 9.81
Q = A1v1 = A2v2
= 32.2
hL
in
A. If venturi-meter is horizontal:
Figure 1.6
=
B. If venturi-meter is vertical
Figure 1.7
=
Figure 1.8
Wo =
- (z1 - z2)
Where,
oVo
Figure 1.9
BF = bouyant force = Wo =
Where, f = density of fluid = SGf
Vd = volume displaced
Ve = volume exposed to air
fVd = oVo
w
Figure 1.9.1
BF =
fVo
Wo =
oVo
R + BF = Wo
Where, R = weight of object in water
Vo = Vd
CHAPTER 2
Hydro-electric Power
Hydraulics - branch of mechanics which deals with the
laws governing the behavior of water and other
liquids in the states of rest and motion.
Hydrostatics - is a branch of hydraulics which deals
on the study of fluids at rest.
- RTK
Ask not what your country can do for you Ask what you can do for your country.
- President John Kennedy
Formulas:
F. Water Power, PW
A. Gross head, hg
PW =
Where,
wQh
= 62.4
H. Generator efficiency, eG
coefficient
of
friction
eG =
or
friction
I. Turbine output, PB
factor
PB = PW
L = length of penstock
g = 9.81
= 32.2
D = inside diameter
eT
eG = (PW
eT)
eG
K. Generator speed, N
C. Net head, h
N =
h = hg - hf
D. Penstock efficiency, e
e =
E. Volume flow of water, Q
Q = Av
Where, N = speed
f = frequency
p = no. of poles (must be even no.)
L. Utilized head, hw
hw = h
eh
, rpm
NS =
*h in feet
, rpm
*h in meters
*N in rpm
Q. Total efficiency, et
et = ehemev
Where, ev = volumetric efficiency
em = mechanical efficiency
R. Turbine type selection based on head, ft.
N. Head of Reaction (Francis and Kaplan) turbines:
NET HEAD
h =
+ z
TYPE OF TURBINE
Up to 70 feet
70 - 110 ft.
Propeller Type
Propeller or Francis
Francis Turbine
Francis or Impulse
Impulse Turbine
CHAPTER 3
Air Compressor
Air Compressor - a machine which is used to increase
the pressure of a gas by decreasing its volume.
eT =
Where, eT - isentropic efficiency, Wa - actual turbine
work, Wi - ideal turbine work
Isentropic efficiency of compressor is the ratio of
the work input required to raise the pressure of a
gas to a specified value in an isentropic manner to
the actual work input.
Figure 3.1
eT =
Where, eT - isentropic efficiency, Wa - actual
compressor work, Wi - ideal compressor work
Formulas:
A. Compression process 1 to 2:
Uses of compressor:
- to drive pneumatic tools
- sand blasting
- industrial cleaning
- spray painting
- starting a diesel engine
- to supply air in mine tunnels
- manufacture of plastic and industrial products
Figure 3.2
P1V1n = P2V2n
= ( )
= ( )
B. Piston displacement, VD
B2SN,
D. Volumetric efficiency, ev
ev =
= 1 + c - c(
E. Compressor power, Wc
Wc =
[( )
Figure 3.3
P2 = discharge pressure
F. Compressor efficiency, ec
ec =
Where, PB = Brake power
G. Piston speed = 2SN
Figure 3.4
Piston rod neglected:
VD = 2(
),
) + * (
+,
Figure 3.5
Formulas:
A. Compressor work, Wc
Wc =
Exercise #2: The initial condition of air in an air
compressor is 98 KPa and 27C and discharges air at
450 KPa. The bore and stroke are 355 mm and 381 mm,
respectively with percent clearance of 8% running at
300 rpm. Find the volume of air at suction.
[( )
B. Intercooler pressure, Px
Px =
Figure 3.6
C. Heat rejected in the intercooler, Q
Q = mcp(Tx - T1)
Where, cp = 1
m =
= ( )
Tx = intercooler temperature
D. Adiabatic compressor efficiency
Figure 3.7
ec =
E. Ideal indicated power, IP
IP = PmiVD
Exercise #3: A two stage air compressor has an
intercooler pressure of 4 kg/cm. What is the
discharge pressure if suction pressure is 1
kg/cm?
Figure 3.8
Formulas:
A. Intercooler pressure, Px
Px =
B. Compressor power, Wc
Wc =
[( )
m =
= ( )
CHAPTER 4
Figure 4.1
D. Air power, Pa
Formulas:
A. Static head, hs
Pa =
hs =
aQh,
KW
E. Fan efficiency, ef
ef =
F. Static power, Ps
Ps =
aQhs
G. Static efficiency, es
hs =
es =
B. Velocity head, hv
H. Fan laws
hv =
velocity
suction
and
discharge
are
Q1 = Q2
Where, = density of air
hv =
C. Total head, h
P = power
h = head
h = hs + hv
= (
= 32.2
at
= (
N = speed
CHAPTER 5
Pumps
Pump - a machine which is used to add energy to a
liquid in order to transfer the liquid from one point
to another point of higher energy level.
- RTK
Types of pumps:
1. Reciprocating pump
Low discharge, high head, self-priming, up to 5 ft.
suction lift, positive displacement pumps:
1. Piston type
2. Plunger type
3. Bellows or diaphragm
2. Centrifugal pump
Figure 5.3
High discharge, low head, not self-priming:
Figure 5.2
This is commonly used as Boiler Feed Pump for steam.
Reciprocating pumps can be single-acting or doubleacting.
They can be simplex, duplex, triplex, etc.
Air chamber - is to smoothen the flow due to the
nature of flow of liquid. This can be placed on the
suction side or discharge side of piping
installation.
Relief valve - this should be installed on the
discharge side between pump and any other valve.
3. Rotary pump
Positive
head:
displacement
pumps,
low
discharge,
low
1. vanes
2. screws
3. lobes
4. gear
Causes of cavitation:
1. Discharge head far below the pump head at peak
efficiency.
1. jet pumps
2. ejector pumps
Pump head:
static
of
discharge
To increase
parallel.
the
discharge,
connect
the
of
discharge
pump
in
Figure 5.7
14. To increase the head of submersible pump,
increase the number of stages of number of impeller.
Figure 5.6
Formulas:
F. Pump efficiency, ep
ep =
G. Head as determined from two pressure readings:
h =
+ z
Figure 5.8
A. Volume flow rate of water, Q
Q = Av
B. Pressure head, hp
hp =
Figure 5.9
C. Velocity head, hv
H. Friction head, hf
hv =
Darcys Equation: hf =
Morse Equation: hf =
I. Specific speed, Ns
Ns =
Ps is negative if it is a vacuum.
E. Water power, PW
Where,
wQh,
KW
Q = discharge, gpm
h = head, ft
J. Similar pumps:
=
K. For the same pump:
Constant impeller diameter, variable speed:
Figure 5.9.1
= (
= (
1. Piston Displacement:
= (
= (
VD = 2 (
)
Piston rod considered: VD =
),
2. Slip = VD - Q
3. %slip =
x 100%
4. volumetric efficiency, ev =
= 1 - Slip