Brochure
3737
2.6 Energy equation for an ideal flow
The energy equation for an ideal flow describes that the sum of pressure
energy, velocity energy and potential energy is constant. Named after
the Swiss physicist Daniel Bernoulli, the equation is known as Bernoulli’s
equation:
[ ]
Pa
ppp
dyn
(2.1)
(2.2)
(2.5)
(2.6)
(2.7)
stattot
+ =
[ ]
PaV
2
1
2
1
2
1
p
2
dyn
⋅ ⋅ =
ρ
[ ]
Papppp
geodynstattot
∆
+
∆
+
∆
p∆
p∆
∆
=
[ ]
Papp
stat, instat, outstat
− =
[ ]
PaVV
2
in
2
outdyn
⋅⋅−⋅ ⋅ =
ρ
ρ
(2.8)
2
1
[
]
Pa
D
1
D
1
4
Q
p
4
in
4
out
2
dyn
− ⋅
⋅ ⋅ =
π
ρΔ
(2.9)
[ ]
Pagzp
geo
⋅ ⋅ ∆ = ∆ ρ
(2.10)
(2.3)
(2.4)
(2.11)
(2.13)
(2.14)
(2.12)
= ⋅ + +
2
22
s
m
Constantzg
2
V
p
ρ
[ ]
Pappp
barrelabs
+ =
[ ]
m
g
p
H
tot
⋅
=
ρ
Δ
[ ]
WQpQgHP
tothyd
⋅
∆ = ⋅⋅ ⋅ = ρ
[ ]
⋅
100
%
[ ]
⋅
100
%
[ ]
⋅
100
%
=
2
hyd
hyd
P
P
η
=
1
hyd
tot
P
P
η
[ ]
WP
2
P
1
P
hyd
> >
(2.15)
(2.16)
(2.17)
(2.17a)
(2.18)
(2.19)
⋅⋅=
hydmotorcontroltot
ηηηη
( )
[ ]
m
g
pp
NPSH
vapourabs,tot,in
A
⋅
−
=
ρ
[ ]
mNPSH = NPSH
3%
NPSH
RA
0.5
+>
NPSH
A
>
[ ]
mNPSH = NPSH
3%
or
R
S
A
.
[ ]
m
g
p
H
g
p
NPSH
p
vapour
suction pipe
,loss
geo
bar
A
⋅
∆
− −
+
⋅ ⋅
=
ρ
ρ
9.81m
23
A
Pa
7375
3500 Pa
m
3
sm992.2kg
101300 Pa
NPSH −−−
⋅ 9.81m
23
sm992.2kg ⋅ 9.81m
23
sm992.2kg ⋅
=
9.81m
23
A
47400
Pa
1
m
3
m
sm973 kg
-27900 Pa + 101000 Pa
+ 500 Pa
NPSH − −+
⋅ 9.81m
23
sm973 kg ⋅
=
6.3mNPSH
A
=
4.7mNPSH
A
=
[ ]
m
g
p
HH
g
pp
NPSH
vapour
loss, pipegeo
barstat,in
A
⋅
−−+
⋅
+ +
=
ρ
ρ
[
( )
0.5
.
ρ
.
V
1
2
Bernoulli’s equation is valid if the following conditions are met:
1. Stationary flow – no changes over time
2. Incompressible flow – true for most liquids
3. Loss-free flow – ignores friction loss
4. Work-free flow – no supply of mechanical energy
Formula (2.10) applies along a stream line or the trajectory of a fluid particle.
For example, the flow through a diusor can be described by formula (2.10),
but not the flow through an impeller since mechancial energy is added.
In most applications, not all the conditions for the energy equation are met. In
spite of this, the equation can be used for making a rough calculation.