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Cen­trifu­gal Water Pump Design

featured_impeller-2

by Johannes Weber

Cen­trifu­gal pumps are commonly used in indus­trial and res­i­den­tial appli­ca­tions due to their rel­a­tively simple design, man­u­fac­tur­ing, and ease-of-main­te­nance. They are also rather effi­cient and easily applic­a­ble in dif­fer­ent sizes. Thus, in the scope of his intern­ship project at FRIEND­SHIP SYSTEMS, Johannes Weber, a BSc student in Trans­port Systems Engi­neer­ing at the Tech­ni­cal Uni­ver­sity of Berlin, was tasked with the imple­men­ta­tion of a design process for a cen­trifu­gal water pump, making full use of the capa­bil­i­ties of CAESES.

Within this over­ar­ch­ing aim, the indi­vid­ual project objec­tives were:

  • Pre­lim­i­nary design para­me­ter cal­cu­la­tion for the radial impeller, based on the selected pump characteristics.
  • Para­met­ric modeling of the impeller.
  • Flow domain modeling for CFD analysis.
  • Dimen­sion­ing and modeling of the spiral casing, includ­ing the volute and the exit diffuser.

STEP 1 | Pump Type and Para­me­ter Selection

A radial type impeller was selected and the B‑NM-50/200A/C pump from Linn-Pumpen GmbH [1] was chosen as a ref­er­ence. The fun­da­men­tal para­me­ters of this pump are pre­sented in the fol­low­ing table.

Data for Q, N and H
Descrip­tionSymbolValue
Vol­u­met­ric FlowQ78 m³/​h
Pressure HeadH55 m
SpeedN2900 rpm

With the help of the Buck­ing­ham-Pi-Theorem, the specific speed is defined as a non-dimen­sional para­me­ter for tur­bo­ma­chines. However, in most cases in the industry the dimen­sional form of the specific speed is used. Con­se­quently, the dimen­sional form was used in this project and cal­cu­lated as Ns= 1091 (US) [2].

STEP 2 | Pre­lim­i­nary Pump Design

While CAESES has an exten­sive set of ded­i­cated modeling func­tion­al­ity for tur­bo­ma­chin­ery, it does not provide pre­lim­i­nary design method­ol­ogy out-of-the-box. However, the so-called feature script­ing func­tion­al­ity provides the user with a complete pro­gram­ming envi­ron­ment that allows them to write their own custom routines. This approach was used here to imple­ment the pre­lim­i­nary dimen­sion­ing of the pump based on selected empir­i­cal formulae and cor­re­la­tion diagrams.

Determining Efficiency from Overall Efficiency – Specific Speed Diagram [2]

The cal­cu­la­tion of the hub diameter was set up using the Overall Effi­ciency – Specific Speed [2] graph and the result­ing shaft torque. The suction diameter, which is highly impor­tant for avoiding cav­i­ta­tion at the leading edge of the blades and accom­mo­dat­ing the minimum-flow require­ment, was deter­mined keeping the cav­i­ta­tion cri­te­rion (NPSHR) in mind. For the cal­cu­la­tion of both suction and impeller diam­e­ters, the Flow Coef­fi­cient – Specific Speed [3] graph was employed and imple­mented in CAESES.

Another impor­tant geo­met­ric design value is the minimum outlet width, which was cal­cu­lated through the graph of Relative Outlet Width — Specific Speed [3] and applied in CAESES. Due to possible cav­i­ta­tion and flow sep­a­ra­tion at the blade, the minimum outlet width should be increased by a certain margin to guar­an­tee the desired vol­u­met­ric flow.

The cal­cu­lated merid­ional dimen­sions of the impeller are given below.

Main Dimen­sions
Descrip­tionSymbolValue
Hub DiameterDh23.66 mm
Suction DiameterD193.28 mm
Impeller DiameterD2224.86 mm
Outlet Widthb220 mm

Further, deter­mi­na­tion of the leading and trailing edge blade angles is impor­tant to achieve the least amount of resis­tance. To cal­cu­late the appro­pri­ate values, the velocity tri­an­gles were used as a basis. The deter­mined angles are pre­sented in the fol­low­ing table, together with the cal­cu­lated minimum number of blades [3, 4]:

Basic Blade Prop­er­ties
Descrip­tionSymbolValue
Angle at leading edge (hub)
\beta_{1B,\mathrm{Hub}}
28.66°
Angle at leading edge (middle)
\beta_{1B,\mathrm{Mid}}
18.49°
Angle at leading edge (shroud)
\beta_{1B,\mathrm{Shroud}}
13.58°
Angle at trailing edge (hub)
\beta_{2B,\mathrm{Hub}}
25°
Number of blades
\mathrm{NOB}

4

STEP 3 | Impeller Modeling

Using the pre­vi­ously deter­mined main dimen­sions and geo­met­ric prop­er­ties as input para­me­ters, a full geo­met­ric model of the impeller was created. Obvi­ously, through­out this process, the def­i­n­i­tion of several addi­tional para­me­ters that describe more detailed attrib­utes of the geometry will be nec­es­sary. These para­me­ters will intro­duce a sizable design space that can later be used to fine-tune and optimize the pump for its specific appli­ca­tion using CFD, depart­ing from the basic pre­lim­i­nary design.

The first step in the modeling process of a radial impeller is to generate the 2D merid­ional contours. For this impeller, this was done by first defining a shroud contour that connects D1 and D2, taking into account the outlet thick­ness. The hub contour was then derived as an offset curve from the shroud with a given width dis­tri­b­u­tion between the inlet and outlet width.

The leading edge, which serves as the stacking curve, was ini­tial­ized as a simple straight con­nec­tion of two points, located on hub and shroud contour, respec­tively. These points were each defined by the inter­sec­tion of a given diameter and the cor­re­spond­ing contour and can be varied by two design vari­ables. Sub­se­quently, the pos­si­bil­ity to create a curved leading edge was intro­duced using an inter­me­di­ate inter­po­la­tion point posi­tioned at a para­me­ter­ized normal distance to the initial straight leading edge.

Meridional Contour Definition

Camber lines at the hub, mid and shroud were created using a so-called Stream Section curve in CAESES, which is offered as pre-defined feature with the option to create the camber curve in dif­fer­ent modes. The blade angle dis­tri­b­u­tions used as an input to the camber line gen­er­a­tion are defined in a separate diagram. Finally, the three camber lines are aligned at the trailing edge by rotating them with the dif­fer­ence between their indi­vid­ual wrap angle and the wrap angle from the hub camber line, result­ing in a per­pen­dic­u­lar trailing edge.

Blade Modeling

Then, the mean camber surface was modeled as a lofted surface inter­po­lat­ing the dif­fer­ent camber lines, followed by the blade surface, which was created by applying thick­ness normal to the camber surface, again using a pre-defined section def­i­n­i­tion provided in CAESES and a spec­i­fied thick­ness distribution.

Finally, the solid blade is the result of inter­sect­ing dif­fer­ent surfaces to the desired closed boundary rep­re­sen­ta­tion (Brep). The solid hub is defined in a similar way, con­nected to the blade with a Boolean oper­a­tion an the root fillet is gen­er­ated at the intersection.

As the pre­lim­i­nary design pro­ce­dure is built directly into the para­met­ric model of the pump, the complete model can simply be updated by changing one or more of the pump’s para­me­ters. The impact of all three fun­da­men­tal para­me­ters (H, Q, and N) on the impeller geometry is visu­al­ized in the ani­ma­tions below, obtained by varying each para­me­ter with a linear increase.

H = [40m , 100m] | With an increasing pressure head, the impeller diameter also increases

Q = [0.015 m3/s , 0.04 m3 m/s] | With the increase of volumetric flow rate, blade wrap and lean angle grow

N = [1200 rpm, 3500 rpm] | When the speed increases, the impeller diameter decreases

STEP 4 | Flow Domain Modeling

The flow domain is the actual geometry that will be exported to an external grid gen­er­a­tor for meshing and can either be modeled manually or using a selec­tion of pre-defined feature def­i­n­i­tions provided in CAESES. In this study, manual modeling was used to generate a periodic single blade passage domain, result­ing in a robust def­i­n­i­tion that conforms to the respec­tive changes of the impeller geometry.

Flow Domain

STEP 5 | Spiral Casing Modeling

The dimen­sions of the volute and the exit velocity were cal­cu­lated by the method and graphs pre­sented in the book Fun­da­men­tals of Tur­bo­ma­chin­ery“ [2].

With these starting values at the volute exit, an algo­rithm can be started, which con­tin­u­ously deter­mines the geo­met­ric values at each cross-sec­tional position. The result was an A/R ratio of ∼16.07 at the exit, whereas the starting A/R from this cal­cu­la­tion was 0. [2]

Due to the dis­ad­van­tages of man­u­fac­tur­ing a volute with a starting A/R ratio of 0, it is common in the industry to maintain a constant A/R ratio in last part of the volute. In this project, a constant A/R ratio with a value of ∼1.49 was applied to the initial 5% of the volute’s total arc length.

After defining the dimen­sions, the volute together with the diffuser and the tongue surface in between the volute and the diffusor could be modeled. This was simply based on the CAESES tutorial Volute Modeling“ and the included Feature Def­i­n­i­tions. The final result of the spiral casing together with the radial impeller can be seen in the fol­low­ing image.

Spiral Casing and Impeller

Con­clu­sion

By using CAESES, the eval­u­a­tion of dif­fer­ent values of the pump’s fun­da­men­tal para­me­ters is fast and prac­ti­cal. The cal­cu­la­tion of pre­lim­i­nary design para­me­ters, as well as empir­i­cal graphs, can be imple­mented directly into CAESES with the help of feature def­i­n­i­tions, auto­mat­i­cally result­ing in a correct dimen­sion­ing of the radial impeller for the current para­me­ter require­ments. This makes it easy to use the project for pre­lim­i­nary design development.

Another aspect is the pos­si­bil­ity to inte­grate a vir­tu­ally unlim­ited — and fully cus­tomized — selec­tion of addi­tional para­me­ters that allows to fine-tune every aspect of the geometry, creating an ideal set up for a quick vari­a­tion of the shape after the pre­lim­i­nary design in order to optimize the pump on the basis of flow analysis.

About the Author

Johannes Weber is a Trans­port Systems Engi­neer­ing student at the Tech­ni­cal Uni­ver­sity of Berlin. He con­ducted his intern­ship at FRIEND­SHIP SYSTEMS in 2022.

Johannes Weber

The process of first getting in touch with CAESES was a great expe­ri­ence due to the range of tuto­ri­als, which made the learning process straight­for­ward and trans­par­ent. Because of the endless capa­bil­i­ties of creating, adjust­ing, and opti­miz­ing geo­met­ric models, it made the process of design­ing the radial pump and imple­ment­ing the cal­cu­la­tions fast, effi­cient, and reliable. In com­bi­na­tion with a modern inter­face, for me, this is a state-of-the-art software, which I am looking forward to use and work with in the future.”

Johannes Weber
BSc Student

Ref­er­ences

[1] LINN PUMPEN, publ., 2015: Close Coupled Cen­trifu­gal Pumps with flanged con­nec­tions. [Last checked on: 30.05.2022]. Avail­able via: https://www.linn-pumpen.de/com/centrifugal-pumps/NM-MNS-DIN-pumps.html

[2] PENG, W. W., 2008: Fun­da­men­tals of Tur­bo­ma­chin­ery. 1st Edition. Hoboken, John Wiley & Sons, ISBN 978 – 94-017‑9627‑9

[3] GÜLICH, J. F., 2020: Kreiselpumpen – Handbuch für Entwick­lung, Anlage­pla­nung und Betrieb., 5th Edition. Berlin, Springer Viewig, ISBN 978 – 3‑662 – 59784

[4] CFturbo, publ., 2021: User manual for CFTurbo Software, Dresden [Last checked on: 30.05.2022]. Avail­able via: https://manual.cfturbo.com/CFturbo_en.pdf

More Infor­ma­tion

See this overview to learn more about the capa­bil­i­ties of CAESES for tur­bo­ma­chin­ery design and contact us to discuss your indi­vid­ual require­ments and our solu­tions in more detail.

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