Download presentation
Presentation is loading. Please wait.
1
Centrifugal pumps
3
Impellers
4
Multistage impellers
5
Cross section of high speed water injection pump
Source:
6
Water injection unit 4 MW Source:
7
Specific speed that is used to classify pumps
nq is the specific speed for a unit machine that is geometric similar to a machine with the head Hq = 1 m and flow rate Q = 1 m3/s
9
Affinity laws Assumptions: Geometrical similarity
Velocity triangles are the same
10
Exercise Find the flow rate, head and power for a centrifugal pump that has increased its speed Given data: hh = 80 % P1 = 123 kW n1 = 1000 rpm H1 = 100 m n2 = 1100 rpm Q1 = 1 m3/s
11
Exercise Find the flow rate, head and power for a centrifugal pump impeller that has reduced its diameter Given data: hh = 80 % P1 = 123 kW D1 = 0,5 m H1 = 100 m D2 = 0,45 m Q1 = 1 m3/s
12
Velocity triangles
14
Reduced cu2 Slip angle Friction loss Slip angle Impulse loss Slip Best efficiency point
15
Power Where: M = torque [Nm] w = angular velocity [rad/s]
16
In order to get a better understanding of the different velocities that represent the head we rewrite the Euler’s pump equation
17
Euler’s pump equation Pressure head due to change of peripheral velocity Pressure head due to change of absolute velocity Pressure head due to change of relative velocity
18
Rothalpy Using the Bernoulli’s equation upstream and downstream a pump one can express the theoretical head: The theoretical head can also be expressed as: Setting these two expression for the theoretical head together we can rewrite the equation:
19
Rothalpy The rothalpy can be written as:
This equation is called the Bernoulli’s equation for incompressible flow in a rotating coordinate system, or the rothalpy equation.
20
Stepanoff We will show how a centrifugal pump is designed using Stepanoff’s empirical coefficients. Example: H = 100 m Q = 0,5 m3/s n = 1000 rpm b2 = 22,5 o
21
Specific speed: This is a radial pump
22
We choose:
23
w2 c2 cm2 u2 cu2
24
Thickness of the blade Until now, we have not considered the thickness of the blade. The meridonial velocity will change because of this thickness. We choose: s2 = 0,005 m z = 5
25
w1 c1= cm1 u1
26
Dhub We choose: Without thickness
27
Thickness of the blade at the inlet
w1 Cm1=6,4 m/s b1 u1
28
w2 c2 cm2=4,87m/s b2=22,5o u2=44,3 m/s cu2
29
w2 c2 cm2=4,87m/s u2=44,3 m/s cu2
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.