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Rod Sampson - School of Marine Science and T echnology - 21st February 2008 ...Open water propeller tests, Standard series model propeller tests and Propeller design diagrams... Resistance & Propulsion (1) MAR 2010

MAR2010 - Standard Series Data

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8/11/2019 MAR2010 - Standard Series Data

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

...Open water propeller tests, Standardseries model propeller tests and Propeller

design diagrams...

Resistance & Propulsion (1)

MAR 2010

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water propeller test

O/W tests performed with the propeller alone inuniform flow to establish:

Basic thrust, torque and propeller efficiency

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water propeller test

Two facilities are commonly used to perform openwater tests:

Towing tank 

Cavitation tunnel

Each facility has its own limitations

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water test - propeller boat

Towing carriageshaft bearing

clearancespropeller boat

boss cap

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water test - cavitation tunnel

Flow direction

shaft bearing

propellerdynamometer

boss cap

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water test - concept

flow direction

Full scale vessel

boss cap

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water test - concept

flow direction

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Undisturbed flow

Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water test - concept

boss cap

Dflow

not less than 1.5D

towing carriage Velocity

• Lenticular shaped “propeller boat” mounted on the towing carriage

• Boat advances through undisturbed flow

• Velocity and shaft rpm are varied

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water test - concept

drive motordynamometer

PROFILE

PLAN

not less than 1.5D

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water test - concept

• measurements taken over a series of runs

• Thrust & Torque are taken at varying J (n usually kept constant)

• Velocity varied from zero speed ( J = 0) to higher values withinthe limitation of the system ( J = 1.0)

note: J = 1.0 is not an upper limit

Tests are performed usually until KT tends to zero

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water test - results

J    =V  

nD

C T    =

ρV  2D2

Test results are presented in the earlier derived coefficients:

C Q   =

Q

ρV  2D3

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water test - results

As CT and CQ  0 as V = 0

CT and CQ are replaced by Aeronautical coefficients

KT and KQ respectively

using:

V    = n2D

2

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water test - results

C T    =

ρV  2D2  K T    =

ρn2D4

C Q   =

Q

ρV  2D3  K Q   =

Q

ρn2D5

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Open water test - results

η0  =P T 

P D=

TV  

Q2πn

η0  =J 

2π×

K T 

K Q

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0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.1 0.2 0.3 0.4 0.5 0.6 0.65 0.7 0.8

KT 10 KQ Eta_0

Advance coefficient

Basic Design - open water tests

Rod Sampson - School of Marine Science and Technology - 21st February 2008

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0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.1 0.2 0.3 0.4 0.5 0.6 0.65 0.7 0.8

KT 10 KQ Eta_0

Advance coefficient

Basic Design - open water tests

φV

2πrn

Thrust

Torque

Vr

φ

V

2πrn

Thrust

Torque

Vr

D

L

D

L

L

Rod Sampson - School of Marine Science and Technology - 21st February 2008

Small V ( J ) = Large T Large V ( J ) = Small T

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Standard series Propeller model test

Tests form the basis for propeller design

Parameters that influence the performance aresystematically varied in the parent design

Rod Sampson - School of Marine Science and Technology - 21st February 2008

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Standard series Propeller model test

Diameter (D)Pitch (P)

Blade area ratio (BAR)Number of blades (Z)

Blade shapeBlade thickness

Usually D is fixed, P/D varied

BAR & Z are varied

Kept constant in line with goodmodern design practice

Rod Sampson - School of Marine Science and Technology - 26th February 2008

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Standard series Propeller model test

Vary P/D

Vary Z

Vary BARParent model P/D

BARZ

3,4,5,6 blades = 4 models

0.4 - 2.0 by 0.2 = 9 models

0.4 - 1.5 by 0.15 = 6 models

216 members

Rod Sampson - School of Marine Science and Technology - 26th February 2008

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Standard series Propeller model test

Rod Sampson - School of Marine Science and Technology - 26th February 2008

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Standard series Propeller model test

From the Parent model a series of 216

propeller models would be generated.

Each member requires testing in open waterconditions

The data from each test is combined intodesign diagrams with varying P/D and fixedBAR & Z

Rod Sampson - School of Marine Science and Technology - 26th February 2008

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Standard series Propeller model test

P/D = 0.4 P/D = 0.8 P/D = 1.0P/D = 0.6

 L ine o f m a x imum e f fic ienc y

K T  P  /  D  =  1 .0 

1 0  K Q  P  /  D  =  1 .0 

η0

1 0  K Q  P / D  =  0 .4 K T  P / D  =  0 .4 

Find optimum diameter to absorb:

a delivered power (kW)

a shaft rotation (N)

an advance speed (VA)

Rod Sampson - School of Marine Science and Technology - 26th February 2008

 J

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Standard series Propeller model test

Rod Sampson - School of Marine Science and Technology - 26th February 2008

Using the above diagram design an propeller(optimum diameter)to absorb:

 

• Delivered Power Pd (kW)

• Rotation N (rpm)• Advance speed J (kn)

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Standard series Propeller model test

First obtain:

n  =N 

60

Q  = 1000P D

2πn

 N.m

Rod Sampson - School of Marine Science and Technology - 26th February 2008

S

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Standard series Propeller model test

Then:

K Q   =

Q

ρn2D5  =

k1

D5

J   =V  A

nD  =

k2

D

Rod Sampson - School of Marine Science and Technology - 26th February 2008

S d d P ll d l

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Standard series Propeller model test

P/D = 0.4 P/D = 0.8 P/D = 1.0P/D = 0.6

 L ine o f m a x imum e f fic ienc y

K T  P  /  D  =  1 .0 

1 0  K Q  P  /  D  =  1 .0 

η0

1 0  K Q  P / D  =  0 .4 K T  P / D  =  0 .4 

Plot 10KQ and J for varying D on the diagram

Intersect with line of maximum efficiency ( )η0

Rod Sampson - School of Marine Science and Technology - 26th February 2008

S d d P ll d l

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Standard series Propeller model test

P/D = 0.4 P/D = 0.8 P/D = 1.0P/D = 0.6

 L ine o f m a x imum e f fic ienc y

K T  P  /  D  =  1 .0 

1 0  K Q  P  /  D  =  1 .0 

η0

1 0  K Q  P / D  =  0 .4 K T  P / D  =  0 .4 

Read off J, hence:   Dopt   =k2

advance coefficient

Interpolate P/D

Rod Sampson - School of Marine Science and Technology - 26th February 2008

P ll D i Di

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  Given data required data

1.2.

3.

4.5.

6.

Propeller Design Diagrams

The representation of systematic open water

diagrams may differ depending upon various designoptions which can be listed as:

P D,N ,V    AP D,D,V    AP D, V  A

T,N,V    AT,D,V    AT, V  A

Dopt

N opt

N opt, Dopt

Dopt

N opt

N opt, Dopt

Rod Sampson - School of Marine Science and Technology - 26th February 2008

P ll D i Di

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Rod Sampson - School of Marine Science and Technology - 26th February 2008

Propeller Design Diagrams

From the previous options the most widely usedcase is option 1 & 4.

Option 1 requires the delivered power and

rotation rate to be known at a specified advancevelocity

The unknown variable is the optimum propeller

diameter

P ll D i Di

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Rod Sampson - School of Marine Science and Technology - 26th February 2008

Propeller Design Diagrams

Considering option 1:

The diameter can be eliminated from the systematicopen water diagrams by replacing the and J

terms as follows:

K Q

K Q  vs  1

P D,N ,V    A  D

opt

K Q

J 5  =

Q

ρN 2D5  ×

1V  anD

5  =

QN 3

ρV  5a

P ll D i Di

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Rod Sampson - School of Marine Science and Technology - 26th February 2008

Propeller Design Diagrams

Since:

P D  = 2π

QN 

K Q

5  =

N 2P D

2πρV  

5  −→

NP 1

2

D

V  

2.5

A

K QJ 5

  = QN 3

ρV  5a

P ll D i Di

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Rod Sampson - School of Marine Science and Technology - 26th February 2008

Propeller Design Diagrams

Let:B p   =

NP 12

D

V  2.5A

andδ  =

1

J =

ND

V  A

P ll D i Di

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Rod Sampson - School of Marine Science and Technology - 26th February 2008

Propeller Design Diagrams

Considering option 4:

A similar analogy can be used by replacing thestandard KT versus J by:

K T 

4  =

ρN 

2

D

4  ×

  1

V  a

nD4

=TN 

2

ρV  

4

a

P ll D i Di

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Rod Sampson - School of Marine Science and Technology - 26th February 2008

Propeller Design Diagrams

Since PT = Va T ( PT = thrust power )

K T 

J 4  =

P T N 2

ρV  5a

−→

NP 1

2

V  5a

= BU 

Let

BU    =

NU 1

2

V  5a

Where U = PT after useful power

P ll D i Di

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Rod Sampson - School of Marine Science and Technology - 26th February 2008

Propeller Design Diagrams

(BP , BU  &  δ )The above coefficients

are known as the D.W. Taylors propeller constants,

most standard series propeller design diagrams aregiven using these constants.

Pr eller Desi n Dia rams

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Rod Sampson - School of Marine Science and Technology - 26th February 2008

Propeller Design Diagrams

BP    =

NP 1

2

DV  2.5A

= 1.158

NP 1

2

DV  2.5A

BU   =NU 

1

2

V  2.5A

= 1.158NU 

1

2

V  2.5A

δ   =ND

V  A= 3.2808

ND

V  A

η0   =P T 

P D

Propeller Design Diagrams

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Rod Sampson - School of Marine Science and Technology - 26th February 2008

Propeller Design Diagrams

Typical diagramBP  − δ 

Basic Design - BP delta diagrams

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Basic Design - BP delta diagrams

Rod Sampson - School of Marine Science and Technology - 26th February 2008

η0

δ 

η0(max)

Line of max.

efficiency

BP Design

P D

BP 

Basic Design - BP delta diagrams

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Basic Design - BP delta diagrams

Rod Sampson - School of Marine Science and Technology - 26th February 2008

η0

δ 

η0(max)

Line of max.

BP Desi

P D

BP 

Calculate BPEnter diagramRead off at max efficiency line

BP  − δ 

δ opt.

Dopt.   = V  aδ opt

N −→ read P/D

Existing standard propeller series

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Existing standard propeller series

Rod Sampson - School of Marine Science and Technology - 26th February 2008

Several key systematic series exist, developed forfixed pitch, controllable pitch propellers, ductedpropellers, etc.

FroudeSchaffranTaylorGawn

WageningenGawn-Burrill (KCA Series)KCn Series

Existing standard propeller series

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Existing standard propeller series

Rod Sampson - School of Marine Science and Technology - 26th February 2008

Existing standard propeller series

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Existing standard propeller series

Rod Sampson - School of Marine Science and Technology - 26th February 2008

One of the most extensive and widely used seriesis the Wageningen B series.

Fixed pitch propeller

Merchant ship style designSlow to medium speed operation

Wageningen B-Series

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Wageningen B Series

Rod Sampson - School of Marine Science and Technology - 21st February 2008

Modern sections Good performance 210 members

Wageningen B-Series Characteristics

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Wageningen B Series Characteristics

Wageningen B-Series Characteristics

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Wageningen B Series Characteristics

• Constant radial pitch distribution

• Small skew

• 15 degrees of backward rake angle

• blade contour with fairly wide tips

• segmental tip blade sections and aerofoil innerradial sections

Wageningen B-Series Characteristics

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Rod Sampson - School of Marine Science and Technology - 21st February 2008

Wageningen B Series Characteristics

B 4. 85

series type = B

blade number = 4

expanded area ratio = 0.85

Wageningen B-Series Characteristics

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Wageningen B Series Characteristics

Wageningen B Series analysed and presented as

polynomial equations

Allows computerisation of the design algorithm

K T  =47n=1

C n  (J )sn

D

tnAe

Ao

un

(Z )vn

K Q  =47n=1

C n  (J )snP 

D

tnAe

Ao

un

(Z )vn