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 Page 1


MECHANICAL ENGINEERING – FLUID MECHANICS 
 
Pressure (P):  
? If F be the normal force acting on a surface of area A in contact with liquid, then 
pressure exerted by liquid on this surface is: A F P / ? 
? Units : 
2
/ m N or Pascal (S.I.) and Dyne/cm
2
 (C.G.S.) 
? Dimension :  ] [
] [
] [
] [
] [
] [
2 1
2
2
? ?
?
? ? ? T ML
L
MLT
A
F
P 
? Atmospheric pressure: Its value on the surface of the earth at sea level is nearly 
2 5
/ 10 013 . 1 m N ? or Pascal in S.I. other practical units of pressure are atmosphere, 
bar and torr (mm of Hg) 
?   torr 760 bar 01 . 1 10 01 . 1 1
5
? ? ? ? Pa atm 
? Fluid Pressure at a Point:  
dF
dA
? ?  
Density ( ? ): 
? In a fluid, at a point, density ? is defined as: 
dV
dm
V
m
V
?
?
?
?
? ? 0
lim ? 
? In case of homogenous isotropic substance, it has no directional properties, so is a 
scalar. 
? It has dimensions ] [
3 ?
ML and S.I. unit kg/m
3
 while C.G.S. unit g/cc with 
3 3
/ 10 / 1 m kg cc g ? 
? Density of body = Density of substance 
? Relative density or specific gravity which is defined as : 
of water  Density
of body Density
? RD 
? If 
1
m mass of liquid of density 
1
? and 
2
m mass of density 
2
? are mixed, then as  
     
2 1
m m m ? ? and ) / ( ) / (
2 2 1 1
? ? m m V ? ?    [As ? / m V ? ] 
               
) / ( ) / ( ) / (
2 2 1 1
2 1
i i
i
p m
m
m m
m m
V
m
?
?
?
?
?
? ?
? ?
? 
    If 
2 1
m m ? , ?
?
?
2 1
2 1
2
? ?
? ?
? Harmonic mean 
? If 
1
V volume of liquid of density 
1
? and 
2
V volume of liquid of density 
2
? are 
mixed, then as: 
2 2 1 1
V V m ? ? ? ? and 
2 1
V V V ? ?   [As V m / ? ? ] 
If V V V ? ?
2 1
 2 / ) (
2 1
? ? ? ? ? = Arithmetic Mean 
 
Page 2


MECHANICAL ENGINEERING – FLUID MECHANICS 
 
Pressure (P):  
? If F be the normal force acting on a surface of area A in contact with liquid, then 
pressure exerted by liquid on this surface is: A F P / ? 
? Units : 
2
/ m N or Pascal (S.I.) and Dyne/cm
2
 (C.G.S.) 
? Dimension :  ] [
] [
] [
] [
] [
] [
2 1
2
2
? ?
?
? ? ? T ML
L
MLT
A
F
P 
? Atmospheric pressure: Its value on the surface of the earth at sea level is nearly 
2 5
/ 10 013 . 1 m N ? or Pascal in S.I. other practical units of pressure are atmosphere, 
bar and torr (mm of Hg) 
?   torr 760 bar 01 . 1 10 01 . 1 1
5
? ? ? ? Pa atm 
? Fluid Pressure at a Point:  
dF
dA
? ?  
Density ( ? ): 
? In a fluid, at a point, density ? is defined as: 
dV
dm
V
m
V
?
?
?
?
? ? 0
lim ? 
? In case of homogenous isotropic substance, it has no directional properties, so is a 
scalar. 
? It has dimensions ] [
3 ?
ML and S.I. unit kg/m
3
 while C.G.S. unit g/cc with 
3 3
/ 10 / 1 m kg cc g ? 
? Density of body = Density of substance 
? Relative density or specific gravity which is defined as : 
of water  Density
of body Density
? RD 
? If 
1
m mass of liquid of density 
1
? and 
2
m mass of density 
2
? are mixed, then as  
     
2 1
m m m ? ? and ) / ( ) / (
2 2 1 1
? ? m m V ? ?    [As ? / m V ? ] 
               
) / ( ) / ( ) / (
2 2 1 1
2 1
i i
i
p m
m
m m
m m
V
m
?
?
?
?
?
? ?
? ?
? 
    If 
2 1
m m ? , ?
?
?
2 1
2 1
2
? ?
? ?
? Harmonic mean 
? If 
1
V volume of liquid of density 
1
? and 
2
V volume of liquid of density 
2
? are 
mixed, then as: 
2 2 1 1
V V m ? ? ? ? and 
2 1
V V V ? ?   [As V m / ? ? ] 
If V V V ? ?
2 1
 2 / ) (
2 1
? ? ? ? ? = Arithmetic Mean 
 
MECHANICAL ENGINEERING – FLUID MECHANICS 
 
? With rise in temperature due to thermal expansion of a given body, volume will 
increase while mass will remain unchanged, so density will decrease, i.e., 
    
) 1 ( ) / (
) / (
0
0 0
0 0
? ? ?
?
? ?
? ? ?
V
V
V
V
V m
V m
  [As ) 1 (
0
? ? ? ? ? V V ] 
 or    
) 1 ( –
~
) 1 (
0
0
? ? ?
? ?
?
? ? ?
? ?
? 
? With increase in pressure due to decrease in volume, density will increase, i.e., 
    
V
V
V m
V m
0
0 0
) / (
) / (
? ?
?
?
   [As
V
m
? ? ] 
? By definition of bulk-modulus:
V
p
V B
?
?
? ?
0
 i.e., 
?
?
?
?
?
? ?
? ?
B
p
V V 1
0
 
?
?
?
?
?
? ?
? ? ?
?
?
?
?
? ?
? ?
?
B
p
B
p
1
~
1
0
1
0
? ? ? 
 
Specific Weight ( w ):  
? It is defined as the weight per unit volume. 
? Specific weight 
.
.
Weight m g
g
Volume Volume
? ??? 
 
Specific Gravity or Relative Density (s):  
? It is the ratio of specific weight of fluid to the specific weight of a standard fluid. 
Standard fluid is water in case of liquid and H
2
 or air in case of gas.  
.
.
w w w
g
s
g
? ? ?
? ? ?
? ? ? 
Where, 
w
? ? Specific weight of water, and 
w
? ? Density of water specific. 
  
Specific Volume ( v ): 
? Specific volume of liquid is defined as volume per unit mass. It is also defined as the 
reciprocal of specific density. 
? Specific volume 
1 V
m ?
?? 
Inertial force per unit area = 
A
dt dm v
A
dt dp ) / ( /
? = 
A
Av v ?
 = ?
2
v 
Page 3


MECHANICAL ENGINEERING – FLUID MECHANICS 
 
Pressure (P):  
? If F be the normal force acting on a surface of area A in contact with liquid, then 
pressure exerted by liquid on this surface is: A F P / ? 
? Units : 
2
/ m N or Pascal (S.I.) and Dyne/cm
2
 (C.G.S.) 
? Dimension :  ] [
] [
] [
] [
] [
] [
2 1
2
2
? ?
?
? ? ? T ML
L
MLT
A
F
P 
? Atmospheric pressure: Its value on the surface of the earth at sea level is nearly 
2 5
/ 10 013 . 1 m N ? or Pascal in S.I. other practical units of pressure are atmosphere, 
bar and torr (mm of Hg) 
?   torr 760 bar 01 . 1 10 01 . 1 1
5
? ? ? ? Pa atm 
? Fluid Pressure at a Point:  
dF
dA
? ?  
Density ( ? ): 
? In a fluid, at a point, density ? is defined as: 
dV
dm
V
m
V
?
?
?
?
? ? 0
lim ? 
? In case of homogenous isotropic substance, it has no directional properties, so is a 
scalar. 
? It has dimensions ] [
3 ?
ML and S.I. unit kg/m
3
 while C.G.S. unit g/cc with 
3 3
/ 10 / 1 m kg cc g ? 
? Density of body = Density of substance 
? Relative density or specific gravity which is defined as : 
of water  Density
of body Density
? RD 
? If 
1
m mass of liquid of density 
1
? and 
2
m mass of density 
2
? are mixed, then as  
     
2 1
m m m ? ? and ) / ( ) / (
2 2 1 1
? ? m m V ? ?    [As ? / m V ? ] 
               
) / ( ) / ( ) / (
2 2 1 1
2 1
i i
i
p m
m
m m
m m
V
m
?
?
?
?
?
? ?
? ?
? 
    If 
2 1
m m ? , ?
?
?
2 1
2 1
2
? ?
? ?
? Harmonic mean 
? If 
1
V volume of liquid of density 
1
? and 
2
V volume of liquid of density 
2
? are 
mixed, then as: 
2 2 1 1
V V m ? ? ? ? and 
2 1
V V V ? ?   [As V m / ? ? ] 
If V V V ? ?
2 1
 2 / ) (
2 1
? ? ? ? ? = Arithmetic Mean 
 
MECHANICAL ENGINEERING – FLUID MECHANICS 
 
? With rise in temperature due to thermal expansion of a given body, volume will 
increase while mass will remain unchanged, so density will decrease, i.e., 
    
) 1 ( ) / (
) / (
0
0 0
0 0
? ? ?
?
? ?
? ? ?
V
V
V
V
V m
V m
  [As ) 1 (
0
? ? ? ? ? V V ] 
 or    
) 1 ( –
~
) 1 (
0
0
? ? ?
? ?
?
? ? ?
? ?
? 
? With increase in pressure due to decrease in volume, density will increase, i.e., 
    
V
V
V m
V m
0
0 0
) / (
) / (
? ?
?
?
   [As
V
m
? ? ] 
? By definition of bulk-modulus:
V
p
V B
?
?
? ?
0
 i.e., 
?
?
?
?
?
? ?
? ?
B
p
V V 1
0
 
?
?
?
?
?
? ?
? ? ?
?
?
?
?
? ?
? ?
?
B
p
B
p
1
~
1
0
1
0
? ? ? 
 
Specific Weight ( w ):  
? It is defined as the weight per unit volume. 
? Specific weight 
.
.
Weight m g
g
Volume Volume
? ??? 
 
Specific Gravity or Relative Density (s):  
? It is the ratio of specific weight of fluid to the specific weight of a standard fluid. 
Standard fluid is water in case of liquid and H
2
 or air in case of gas.  
.
.
w w w
g
s
g
? ? ?
? ? ?
? ? ? 
Where, 
w
? ? Specific weight of water, and 
w
? ? Density of water specific. 
  
Specific Volume ( v ): 
? Specific volume of liquid is defined as volume per unit mass. It is also defined as the 
reciprocal of specific density. 
? Specific volume 
1 V
m ?
?? 
Inertial force per unit area = 
A
dt dm v
A
dt dp ) / ( /
? = 
A
Av v ?
 = ?
2
v 
MECHANICAL ENGINEERING – FLUID MECHANICS 
 
Viscous force per unit area: 
r
v
A F
?
? / 
Reynold’s number: 
area unit per force Viscous
area unit per force Inertial 
?
R
N
?
?
?
? r v
r v
v
? ?
/
2
 
Pascal’s Law: 
x y z
p p p ?? ; where, 
x
p ,
y
p and 
z
p are the pressure at point x,y,z respectively. 
 
Hydrostatic Law:  
? 
p
pg
z
?
?
?
or dp pg ? dz 
? 
ph
oo
dp pg dz ?
??
 
? p pgh ? and 
p
h
pg
? ; where, h is known as pressure head.  
 
Pressure Energy Potential energy Kinetic energy 
It is the energy possessed by a 
liquid by virtue of its pressure. It 
is the measure of work done in 
pushing the liquid against 
pressure without imparting any 
velocity to it. 
It is the energy possessed by 
liquid by virtue of its height or 
position above the surface of 
earth or any reference level 
taken as zero level.  
It is the energy possessed by a 
liquid by virtue of its motion or 
velocity. 
Pressure energy of the liquid PV Potential energy of the liquid 
mgh 
Kinetic energy of the liquid 
mv
2
/2 
Pressure energy per unit mass of 
the liquid P/ ? 
Potential energy per unit mass of 
the liquid gh 
Kinetic energy per unit mass of 
the liquid v
2
/2 
Pressure energy per unit volume 
of the liquid P 
Potential energy per unit volume 
of the liquid ?gh 
Kinetic energy per unit volume 
of the liquid ? v
2
/2 
 
 
Quantities that Satisfy a Balance Equation 
Quantit
y 
mass x momentum y momentum z 
momentum 
Energy Species 
? ?
m mu mv mw E + mV
2
/2 m
(K) 
? ?
1 u v w e + V
2
/2 W
(K) 
In this table, u, v, and w are the x, y and z velocity components, E is the total 
thermodynamic internal energy, e is the thermodynamic internal energy per unit mass, 
and m
(K)
 is the mass of a chemical species, K, W
(K)
 is the mass fraction of species K.  
Page 4


MECHANICAL ENGINEERING – FLUID MECHANICS 
 
Pressure (P):  
? If F be the normal force acting on a surface of area A in contact with liquid, then 
pressure exerted by liquid on this surface is: A F P / ? 
? Units : 
2
/ m N or Pascal (S.I.) and Dyne/cm
2
 (C.G.S.) 
? Dimension :  ] [
] [
] [
] [
] [
] [
2 1
2
2
? ?
?
? ? ? T ML
L
MLT
A
F
P 
? Atmospheric pressure: Its value on the surface of the earth at sea level is nearly 
2 5
/ 10 013 . 1 m N ? or Pascal in S.I. other practical units of pressure are atmosphere, 
bar and torr (mm of Hg) 
?   torr 760 bar 01 . 1 10 01 . 1 1
5
? ? ? ? Pa atm 
? Fluid Pressure at a Point:  
dF
dA
? ?  
Density ( ? ): 
? In a fluid, at a point, density ? is defined as: 
dV
dm
V
m
V
?
?
?
?
? ? 0
lim ? 
? In case of homogenous isotropic substance, it has no directional properties, so is a 
scalar. 
? It has dimensions ] [
3 ?
ML and S.I. unit kg/m
3
 while C.G.S. unit g/cc with 
3 3
/ 10 / 1 m kg cc g ? 
? Density of body = Density of substance 
? Relative density or specific gravity which is defined as : 
of water  Density
of body Density
? RD 
? If 
1
m mass of liquid of density 
1
? and 
2
m mass of density 
2
? are mixed, then as  
     
2 1
m m m ? ? and ) / ( ) / (
2 2 1 1
? ? m m V ? ?    [As ? / m V ? ] 
               
) / ( ) / ( ) / (
2 2 1 1
2 1
i i
i
p m
m
m m
m m
V
m
?
?
?
?
?
? ?
? ?
? 
    If 
2 1
m m ? , ?
?
?
2 1
2 1
2
? ?
? ?
? Harmonic mean 
? If 
1
V volume of liquid of density 
1
? and 
2
V volume of liquid of density 
2
? are 
mixed, then as: 
2 2 1 1
V V m ? ? ? ? and 
2 1
V V V ? ?   [As V m / ? ? ] 
If V V V ? ?
2 1
 2 / ) (
2 1
? ? ? ? ? = Arithmetic Mean 
 
MECHANICAL ENGINEERING – FLUID MECHANICS 
 
? With rise in temperature due to thermal expansion of a given body, volume will 
increase while mass will remain unchanged, so density will decrease, i.e., 
    
) 1 ( ) / (
) / (
0
0 0
0 0
? ? ?
?
? ?
? ? ?
V
V
V
V
V m
V m
  [As ) 1 (
0
? ? ? ? ? V V ] 
 or    
) 1 ( –
~
) 1 (
0
0
? ? ?
? ?
?
? ? ?
? ?
? 
? With increase in pressure due to decrease in volume, density will increase, i.e., 
    
V
V
V m
V m
0
0 0
) / (
) / (
? ?
?
?
   [As
V
m
? ? ] 
? By definition of bulk-modulus:
V
p
V B
?
?
? ?
0
 i.e., 
?
?
?
?
?
? ?
? ?
B
p
V V 1
0
 
?
?
?
?
?
? ?
? ? ?
?
?
?
?
? ?
? ?
?
B
p
B
p
1
~
1
0
1
0
? ? ? 
 
Specific Weight ( w ):  
? It is defined as the weight per unit volume. 
? Specific weight 
.
.
Weight m g
g
Volume Volume
? ??? 
 
Specific Gravity or Relative Density (s):  
? It is the ratio of specific weight of fluid to the specific weight of a standard fluid. 
Standard fluid is water in case of liquid and H
2
 or air in case of gas.  
.
.
w w w
g
s
g
? ? ?
? ? ?
? ? ? 
Where, 
w
? ? Specific weight of water, and 
w
? ? Density of water specific. 
  
Specific Volume ( v ): 
? Specific volume of liquid is defined as volume per unit mass. It is also defined as the 
reciprocal of specific density. 
? Specific volume 
1 V
m ?
?? 
Inertial force per unit area = 
A
dt dm v
A
dt dp ) / ( /
? = 
A
Av v ?
 = ?
2
v 
MECHANICAL ENGINEERING – FLUID MECHANICS 
 
Viscous force per unit area: 
r
v
A F
?
? / 
Reynold’s number: 
area unit per force Viscous
area unit per force Inertial 
?
R
N
?
?
?
? r v
r v
v
? ?
/
2
 
Pascal’s Law: 
x y z
p p p ?? ; where, 
x
p ,
y
p and 
z
p are the pressure at point x,y,z respectively. 
 
Hydrostatic Law:  
? 
p
pg
z
?
?
?
or dp pg ? dz 
? 
ph
oo
dp pg dz ?
??
 
? p pgh ? and 
p
h
pg
? ; where, h is known as pressure head.  
 
Pressure Energy Potential energy Kinetic energy 
It is the energy possessed by a 
liquid by virtue of its pressure. It 
is the measure of work done in 
pushing the liquid against 
pressure without imparting any 
velocity to it. 
It is the energy possessed by 
liquid by virtue of its height or 
position above the surface of 
earth or any reference level 
taken as zero level.  
It is the energy possessed by a 
liquid by virtue of its motion or 
velocity. 
Pressure energy of the liquid PV Potential energy of the liquid 
mgh 
Kinetic energy of the liquid 
mv
2
/2 
Pressure energy per unit mass of 
the liquid P/ ? 
Potential energy per unit mass of 
the liquid gh 
Kinetic energy per unit mass of 
the liquid v
2
/2 
Pressure energy per unit volume 
of the liquid P 
Potential energy per unit volume 
of the liquid ?gh 
Kinetic energy per unit volume 
of the liquid ? v
2
/2 
 
 
Quantities that Satisfy a Balance Equation 
Quantit
y 
mass x momentum y momentum z 
momentum 
Energy Species 
? ?
m mu mv mw E + mV
2
/2 m
(K) 
? ?
1 u v w e + V
2
/2 W
(K) 
In this table, u, v, and w are the x, y and z velocity components, E is the total 
thermodynamic internal energy, e is the thermodynamic internal energy per unit mass, 
and m
(K)
 is the mass of a chemical species, K, W
(K)
 is the mass fraction of species K.  
MECHANICAL ENGINEERING – FLUID MECHANICS 
 
The other energy term, mV
2
/2, is the kinetic energy. 
 
? z y x
t t
z y x
t
m
t
Storage ? ? ?
?
?
?
?
? ? ? ?
?
?
?
?
?
? ?
?
) ( ) ( ) ( ?? ? ? ?
  
? x y w z x v z y u Inflow
z y x
? ? ? ? ? ? ? ? ? ? ? ? ? ? ? 
? x y w z x v z y u Outflow
z z y y x x
? ? ? ? ? ? ? ? ?
? ? ? ? ? ?
? ? ? ? ? ? 
? z y x Source ? ? ? ?
?
S 
? 
?
? ? ? ? ? ? ? ?
? ? ? ?
??
S ?
?
?
?
?
?
?
?
?
?
?
?
? ?
? ?
? ?
z
w w
y
v v
x
u u
t
z z z
y y y
x x x
 
? 
*
?
? ? ? ? ? ? ??
S
z
w
y
v
x
u
t
?
?
?
?
?
?
?
?
?
?
?
?
 
? 
? ?
S
z y x
Lim
0
S
*
? ? ? ?
? 
The Mass Balance Equations: 
? 0 ?
?
?
?
?
?
i
i
x
u
t
? ?
 
? 0 ?
?
?
?
?
?
?
?
?
?
?
?
z
w
y
v
x
u
t
? ? ? ?
 
? 0 ?
?
?
?
?
?
?
?
?
i
i
i
i
x
u
x
u
t
?
? ?
 
? 0 ?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
z
w
y
v
x
u
z
w
y
v
x
u
t
? ? ?
?
?
  
? 
i
i
x
u
t Dt
D
or
z
w
y
v
x
u
t Dt
D
?
? ?
?
?
? ?
?
?
?
? ?
?
?
? ?
?
?
? ?
?
?
? ?
?
?
 
? 0 0 0 ? ? ? ?
?
?
? ?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
? ?
?
?
?
?
?
Dt
D
x
u
Dt
D
z
w
y
v
x
u
Dt
D
i
i
 
? 0 0 ?
?
?
? ? ?
?
?
?
?
?
?
?
?
? ?
i
i
x
u
or
z
w
y
v
x
u
 
Page 5


MECHANICAL ENGINEERING – FLUID MECHANICS 
 
Pressure (P):  
? If F be the normal force acting on a surface of area A in contact with liquid, then 
pressure exerted by liquid on this surface is: A F P / ? 
? Units : 
2
/ m N or Pascal (S.I.) and Dyne/cm
2
 (C.G.S.) 
? Dimension :  ] [
] [
] [
] [
] [
] [
2 1
2
2
? ?
?
? ? ? T ML
L
MLT
A
F
P 
? Atmospheric pressure: Its value on the surface of the earth at sea level is nearly 
2 5
/ 10 013 . 1 m N ? or Pascal in S.I. other practical units of pressure are atmosphere, 
bar and torr (mm of Hg) 
?   torr 760 bar 01 . 1 10 01 . 1 1
5
? ? ? ? Pa atm 
? Fluid Pressure at a Point:  
dF
dA
? ?  
Density ( ? ): 
? In a fluid, at a point, density ? is defined as: 
dV
dm
V
m
V
?
?
?
?
? ? 0
lim ? 
? In case of homogenous isotropic substance, it has no directional properties, so is a 
scalar. 
? It has dimensions ] [
3 ?
ML and S.I. unit kg/m
3
 while C.G.S. unit g/cc with 
3 3
/ 10 / 1 m kg cc g ? 
? Density of body = Density of substance 
? Relative density or specific gravity which is defined as : 
of water  Density
of body Density
? RD 
? If 
1
m mass of liquid of density 
1
? and 
2
m mass of density 
2
? are mixed, then as  
     
2 1
m m m ? ? and ) / ( ) / (
2 2 1 1
? ? m m V ? ?    [As ? / m V ? ] 
               
) / ( ) / ( ) / (
2 2 1 1
2 1
i i
i
p m
m
m m
m m
V
m
?
?
?
?
?
? ?
? ?
? 
    If 
2 1
m m ? , ?
?
?
2 1
2 1
2
? ?
? ?
? Harmonic mean 
? If 
1
V volume of liquid of density 
1
? and 
2
V volume of liquid of density 
2
? are 
mixed, then as: 
2 2 1 1
V V m ? ? ? ? and 
2 1
V V V ? ?   [As V m / ? ? ] 
If V V V ? ?
2 1
 2 / ) (
2 1
? ? ? ? ? = Arithmetic Mean 
 
MECHANICAL ENGINEERING – FLUID MECHANICS 
 
? With rise in temperature due to thermal expansion of a given body, volume will 
increase while mass will remain unchanged, so density will decrease, i.e., 
    
) 1 ( ) / (
) / (
0
0 0
0 0
? ? ?
?
? ?
? ? ?
V
V
V
V
V m
V m
  [As ) 1 (
0
? ? ? ? ? V V ] 
 or    
) 1 ( –
~
) 1 (
0
0
? ? ?
? ?
?
? ? ?
? ?
? 
? With increase in pressure due to decrease in volume, density will increase, i.e., 
    
V
V
V m
V m
0
0 0
) / (
) / (
? ?
?
?
   [As
V
m
? ? ] 
? By definition of bulk-modulus:
V
p
V B
?
?
? ?
0
 i.e., 
?
?
?
?
?
? ?
? ?
B
p
V V 1
0
 
?
?
?
?
?
? ?
? ? ?
?
?
?
?
? ?
? ?
?
B
p
B
p
1
~
1
0
1
0
? ? ? 
 
Specific Weight ( w ):  
? It is defined as the weight per unit volume. 
? Specific weight 
.
.
Weight m g
g
Volume Volume
? ??? 
 
Specific Gravity or Relative Density (s):  
? It is the ratio of specific weight of fluid to the specific weight of a standard fluid. 
Standard fluid is water in case of liquid and H
2
 or air in case of gas.  
.
.
w w w
g
s
g
? ? ?
? ? ?
? ? ? 
Where, 
w
? ? Specific weight of water, and 
w
? ? Density of water specific. 
  
Specific Volume ( v ): 
? Specific volume of liquid is defined as volume per unit mass. It is also defined as the 
reciprocal of specific density. 
? Specific volume 
1 V
m ?
?? 
Inertial force per unit area = 
A
dt dm v
A
dt dp ) / ( /
? = 
A
Av v ?
 = ?
2
v 
MECHANICAL ENGINEERING – FLUID MECHANICS 
 
Viscous force per unit area: 
r
v
A F
?
? / 
Reynold’s number: 
area unit per force Viscous
area unit per force Inertial 
?
R
N
?
?
?
? r v
r v
v
? ?
/
2
 
Pascal’s Law: 
x y z
p p p ?? ; where, 
x
p ,
y
p and 
z
p are the pressure at point x,y,z respectively. 
 
Hydrostatic Law:  
? 
p
pg
z
?
?
?
or dp pg ? dz 
? 
ph
oo
dp pg dz ?
??
 
? p pgh ? and 
p
h
pg
? ; where, h is known as pressure head.  
 
Pressure Energy Potential energy Kinetic energy 
It is the energy possessed by a 
liquid by virtue of its pressure. It 
is the measure of work done in 
pushing the liquid against 
pressure without imparting any 
velocity to it. 
It is the energy possessed by 
liquid by virtue of its height or 
position above the surface of 
earth or any reference level 
taken as zero level.  
It is the energy possessed by a 
liquid by virtue of its motion or 
velocity. 
Pressure energy of the liquid PV Potential energy of the liquid 
mgh 
Kinetic energy of the liquid 
mv
2
/2 
Pressure energy per unit mass of 
the liquid P/ ? 
Potential energy per unit mass of 
the liquid gh 
Kinetic energy per unit mass of 
the liquid v
2
/2 
Pressure energy per unit volume 
of the liquid P 
Potential energy per unit volume 
of the liquid ?gh 
Kinetic energy per unit volume 
of the liquid ? v
2
/2 
 
 
Quantities that Satisfy a Balance Equation 
Quantit
y 
mass x momentum y momentum z 
momentum 
Energy Species 
? ?
m mu mv mw E + mV
2
/2 m
(K) 
? ?
1 u v w e + V
2
/2 W
(K) 
In this table, u, v, and w are the x, y and z velocity components, E is the total 
thermodynamic internal energy, e is the thermodynamic internal energy per unit mass, 
and m
(K)
 is the mass of a chemical species, K, W
(K)
 is the mass fraction of species K.  
MECHANICAL ENGINEERING – FLUID MECHANICS 
 
The other energy term, mV
2
/2, is the kinetic energy. 
 
? z y x
t t
z y x
t
m
t
Storage ? ? ?
?
?
?
?
? ? ? ?
?
?
?
?
?
? ?
?
) ( ) ( ) ( ?? ? ? ?
  
? x y w z x v z y u Inflow
z y x
? ? ? ? ? ? ? ? ? ? ? ? ? ? ? 
? x y w z x v z y u Outflow
z z y y x x
? ? ? ? ? ? ? ? ?
? ? ? ? ? ?
? ? ? ? ? ? 
? z y x Source ? ? ? ?
?
S 
? 
?
? ? ? ? ? ? ? ?
? ? ? ?
??
S ?
?
?
?
?
?
?
?
?
?
?
?
? ?
? ?
? ?
z
w w
y
v v
x
u u
t
z z z
y y y
x x x
 
? 
*
?
? ? ? ? ? ? ??
S
z
w
y
v
x
u
t
?
?
?
?
?
?
?
?
?
?
?
?
 
? 
? ?
S
z y x
Lim
0
S
*
? ? ? ?
? 
The Mass Balance Equations: 
? 0 ?
?
?
?
?
?
i
i
x
u
t
? ?
 
? 0 ?
?
?
?
?
?
?
?
?
?
?
?
z
w
y
v
x
u
t
? ? ? ?
 
? 0 ?
?
?
?
?
?
?
?
?
i
i
i
i
x
u
x
u
t
?
? ?
 
? 0 ?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
z
w
y
v
x
u
z
w
y
v
x
u
t
? ? ?
?
?
  
? 
i
i
x
u
t Dt
D
or
z
w
y
v
x
u
t Dt
D
?
? ?
?
?
? ?
?
?
?
? ?
?
?
? ?
?
?
? ?
?
?
? ?
?
?
 
? 0 0 0 ? ? ? ?
?
?
? ?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
? ?
?
?
?
?
?
Dt
D
x
u
Dt
D
z
w
y
v
x
u
Dt
D
i
i
 
? 0 0 ?
?
?
? ? ?
?
?
?
?
?
?
?
?
? ?
i
i
x
u
or
z
w
y
v
x
u
 
MECHANICAL ENGINEERING – FLUID MECHANICS 
 
? 
?
?
?
? ?
?
?
? S ?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
i
i
i
i
x
u
x
u
t t
 
? 
?
?
?
?
? S ?
?
?
?
?
?
i
i
x
u
t
 
Momentum Balance Equation: 
? 
j
i
ij
j
j j j
B
x
B
x x x
term source direction j Net ?
?
?
? ? ?
?
?
?
? ?
?
?
?
?
?
?
?
?
? ?
3
3
2
2
1
1
 
? 3 , 1 ? ? ?
?
?
?
?
?
?
?
?
j B
x x
u u
t
u
j
i
ij
i
j i j
?
? ? ?
 
? For a Newtonian fluid, the stress, s
ij,
 is given by the following equation: 
ij
i
j
j
i
ij ij
x
u
x
u
P ? ? ? ? ? ? ? ? ?
?
?
?
?
?
?
?
?
?
?
?
?
?
? ? ? )
3
2
( 
? 3 , 1 )
3
2
( ? ? ?
?
?
?
?
?
?
?
?
? ? ?
?
?
?
?
?
?
?
?
?
?
?
?
?
? ?
?
?
?
?
?
?
?
?
j B
x
u
x
u
P
x x
u u
t
u
j ij
i
j
j
i
ij
i i
j i j
? ? ? ? ? ?
? ?
 
? 3 , 1 )
3
2
( ? ? ?
?
?
?
?
?
?
? ?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
?
? ?
?
?
?
?
?
j B
x x
u
x
u
x x
P
x
u u
t
u
j
j i
j
j
i
i j i
j i j
? ? ? ?
? ?
  
? 
x
u uu vu wu
B
t x y z
? ? ?
?
? ? ? ?
? ? ? ?
? ? ? ?
 
? 
2
2 ( )
3
P u v u w u
x x x y x y z x z x
? ? ? ? ?
??
???? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ?
? ? ? ? ? ? ? ? ?
?? ? ? ? ? ? ? ??
??
? ? ? ? ? ? ? ? ? ?
? ? ? ? ? ?
?? ??
??
 
Energy Balance Equation: 
? This directional heat flux is given the symbol q
i
: 
i
i
x
T
k q
?
?
? ? 
? 
x
q q
z y
z y x
q q
Volume Unit
heat xDirection Net
x
x
x x
x
x
x
x x
x
?
?
? ? ? ?
? ? ?
?
? ?
? ? ? ?
 
? 
x
q
Volume Unit
source heat xDirection Net
x
Limit
x
?
?
? ?
? ? 0
 
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FAQs on Fluid Mechanics Formulas for GATE ME Exam - Fluid Mechanics for Mechanical Engineering

1. What are some important fluid mechanics formulas that are frequently asked in the GATE ME exam for Mechanical Engineering?
Ans. Some important fluid mechanics formulas that are frequently asked in the GATE ME exam for Mechanical Engineering include: 1. Bernoulli's equation: P + (1/2)ρv^2 + ρgh = constant, where P is the pressure, ρ is the density, v is the velocity, g is the acceleration due to gravity, and h is the height. 2. Reynolds number: Re = (ρvd)/μ, where Re is the Reynolds number, ρ is the density, v is the velocity, d is the characteristic length, and μ is the dynamic viscosity. 3. Poiseuille's law: Q = (πr^4ΔP)/(8μl), where Q is the volumetric flow rate, r is the radius of the tube, ΔP is the pressure difference, μ is the dynamic viscosity, and l is the length of the tube. 4. Torricelli's theorem: v = √(2gh), where v is the velocity of the fluid, g is the acceleration due to gravity, and h is the height of the fluid column. 5. Euler's equation of motion: ∂v/∂t + v.∇v = - (1/ρ)∇P + g, where ∂v/∂t is the acceleration, v is the velocity vector, ∇v is the gradient of the velocity vector, ρ is the density, ∇P is the gradient of the pressure, and g is the acceleration due to gravity.
2. How can I apply Bernoulli's equation in real-life scenarios?
Ans. Bernoulli's equation can be applied in various real-life scenarios, such as: 1. Airplane wings: Bernoulli's equation explains how the difference in air pressure above and below the airplane wings creates lift, allowing the airplane to fly. 2. Venturi meters: Bernoulli's equation is used in venturi meters to measure the flow rate of fluids by calculating the pressure difference between the narrow and wide sections of the pipe. 3. Water supply systems: Bernoulli's equation helps in understanding the flow of water in pipes, determining the pressure at different points, and designing efficient water supply systems. 4. Carburetors: Bernoulli's equation is used in carburetors to mix air and fuel by utilizing the pressure difference to control the flow rates and achieve the desired fuel-air mixture. 5. Sprinkler systems: Bernoulli's equation is employed in designing sprinkler systems to calculate the pressure required to spray water at a certain height and distance.
3. What is the significance of Reynolds number in fluid mechanics?
Ans. The Reynolds number is significant in fluid mechanics because it helps in determining the flow characteristics of a fluid, specifically whether it exhibits laminar or turbulent flow. It is calculated using the formula Re = (ρvd)/μ, where ρ is the density, v is the velocity, d is the characteristic length, and μ is the dynamic viscosity. The significance of Reynolds number can be summarized as follows: 1. Flow regime determination: The Reynolds number helps in identifying the type of flow regime. For low Reynolds numbers, the flow tends to be laminar, whereas for high Reynolds numbers, the flow becomes turbulent. 2. Flow prediction: By calculating the Reynolds number, engineers and researchers can predict the flow behavior, pressure drop, and heat transfer characteristics of a fluid in different applications, such as pipelines, channels, and pumps. 3. Design considerations: Reynolds number plays a crucial role in the design of pipes, ducts, and other fluid flow systems. It helps in determining the appropriate pipe diameter, selecting the right pump, and optimizing the flow conditions for efficient operation. 4. Drag force estimation: Reynolds number is used to estimate the drag force acting on an object moving through a fluid. This is particularly important in aerodynamics and the design of vehicles, airplanes, and submarines. 5. Scale modeling: The Reynolds number is used in scale modeling to ensure that the flow characteristics of a smaller model accurately represent those of a larger prototype. This is essential in fields like hydrodynamics and wind tunnel testing.
4. How is Poiseuille's law applied in medical science and engineering?
Ans. Poiseuille's law, which relates flow rate to pressure difference in a cylindrical tube, finds applications in medical science and engineering in various ways, including: 1. Blood flow in arteries and veins: Poiseuille's law helps in understanding and analyzing the flow of blood in arteries and veins. It provides insights into the factors affecting blood flow rate, such as blood vessel radius, pressure difference, and viscosity, which are crucial in diagnosing and treating cardiovascular diseases. 2. Intravenous (IV) fluid administration: Poiseuille's law is used to calculate the flow rate of IV fluids in medical settings. By considering factors such as the size of the catheter, pressure difference, and fluid viscosity, healthcare professionals can ensure controlled and accurate drug administration. 3. Design of medical devices: Poiseuille's law is applied in the design and optimization of medical devices like catheters, needles, and syringes. It helps in determining the appropriate dimensions, material properties, and flow characteristics to ensure efficient and safe fluid delivery or extraction. 4. Respiratory treatments: Poiseuille's law is relevant in understanding airflow dynamics in the respiratory system and designing devices like inhalers and nebulizers. It aids in determining the appropriate pressure gradients and flow rates for effective drug delivery to the lungs. 5. Microfluidics and lab-on-a-chip systems: Poiseuille's law is utilized in microfluidics and lab-on-a-chip systems for precise control and manipulation of small volumes of fluids. It enables the design of microchannels, valves, and pumps to achieve desired flow rates and mixing capabilities, essential for applications in diagnostics and drug discovery.
5. How is Euler's equation of motion used in analyzing fluid flow problems?
Ans. Euler's equation of motion, given by ∂v/∂t + v.∇v = - (1/ρ)∇P + g, is a fundamental equation used in analyzing fluid flow problems. It combines the principles of conservation of mass and momentum and can be applied in various ways, including: 1. Fluid dynamics analysis: Euler's equation is used to study and analyze the motion of fluids in various scenarios, such as pipe flows, flow around objects, and open channel flows. It helps in understanding the changes in velocity and pressure distribution within the fluid. 2. Pressure distribution calculations: Euler's equation allows engineers and researchers to calculate the pressure distribution in a fluid flow problem. By solving the equation for pressure, one can determine the pressure gradients and variations at different points in the flow. 3. Flow stability analysis: Euler's equation is used to assess the stability of fluid flows. By studying the time-dependent terms (∂v/∂t), researchers can determine the occurrence of instabilities, such as vortex shedding, and analyze their effects on the flow behavior. 4. Turbulence modeling: Euler's equation serves as the basis for turbulence modeling techniques used in computational fluid dynamics (CFD). By applying appropriate turbulence closure models, the equation can be modified to account for the effects of turbulence on the flow. 5. Design optimization: Euler's equation is employed in the design optimization of fluid flow systems. By solving the equation numerically or analytically, engineers can evaluate different design parameters, such as velocity profiles, pressure drops, and flow rates, to optimize the performance and efficiency of systems like pumps, turbines, and heat exchangers.
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