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Abstract— Design of hydraulic turbines involves several stages
of iterative calculations. Furthermore, the selection of the
turbine is unique to each site conditions. This makes the R&D of
the hydraulic turbines a complicated and time consuming work.
Recent advancements in computational tools and processors
have added advantages to the R&D process of hydraulic
turbines. These tools are able not only to compute solutions for
the complex design equations but also provide the user friendly
virtual environment for performance test and design
optimization.
A new program named as “Khoj” has been developed using
Matlab for design optimization of Francis runners. The
optimized design from the program can be further analyzed
using CFD, CAD and FSI tools, which estimate the effect of
design variables on performance of the turbine. For the project
on failure analysis of Khimti runner, the true size runner model
has been developed using SolidWorks. Stress and fatigue
analysis of the runner has been attempted using CosmosWorks.
Study of the general performance behavior of the Pelton runner
and identification of the possible causes of failure of the Khimti
runner at its operating conditions is under progress.
This paper presents the experiences of use of computational
tools for research and development of hydraulic turbines at
Kathmandu University. The research methodology followed and
the computational tools applied, with the recent results for
design optimization of Francis runner, effects of operating
conditions on sediment erosion and failure analysis of Pelton
runner of Khimti Hydropower will be elaborated in-depth.
Effectiveness and limitations of application of computational
tools for R&D of hydraulic turbines will also be discussed.
Index Terms— Computational tools, Design, Hydraulic
turbines, CFD, SolidWorks,
I. INTRODUCTION
EPAL has a huge potential of hydro power. Most of the
surface water in Nepal flows through four major river
basins, Saptakoshi, Narayani, Karnali and Mahakali, extended
Biraj Singh Thapa is a Graduate of Mechanical Engineering from
Kathmandu University. Currently, he is working as a Full time Researcher in Turbine Testing Lab, Kathmandu University. ([email protected]).
Amod Panthee completed his Bacherlor‟s degree in Mechanical
Engineering from Kathmandu University. Currently, he is working as a Research Assistant on RenewableNepal Project at Turbine Testing Lab,
Kathmandu University. (*correspondence email: [email protected]).
Hari Prasad Neopane, PhD. is Associate Professor at Department of Mechanical Engineering, School of Engineering, Kathmandu University. He
works as a program coordinator on EnPe-Master Program in Planning and
Operation of Energy Systems (MPPOES) at Department of Mechanical Engineering, Kathmandu University. ([email protected]).
from east to the west. The total hydropower potential of Nepal
at Q40 is about 53,000 MW [1] as shown in TABLE I.
Despite, having the huge potential, Nepal is still lagging
behind in power generation with total harvested capacity of
650 MW.
Hydraulic turbines
are classified into
different categories
depending upon its
principle and range
of operation [2].
Therefore, the
selection of hydraulic
turbines varies
depending upon the
site criterions. The
installation of
hydropower plants despite having a huge potential becomes
more complex with change in design for a slight variation in
design inputs like Head (H) and Discharge (Q).
Moreover, Nepal is located on the lap of Himalayas. This
increases the sediment concentration in the rivers of Nepal
unlike other countries with igneous mountains. The river
characterized with high sediment concentration is one of the
problems in operation of hydraulic turbines erected at ROR
type or storage type projects [3]. The sediment eroded Francis
runner of Trishuli HEP is shown in Figure I.
The design of
hydraulic turbine
is complex since
it involves a long
iterative process
in design stage.
And it is
necessary to
predict the
behavior of
hydraulic turbines
at various
conditions on real
environment while designing. This makes the design of the
hydraulic turbine more time consuming. But, the use of
computational tools have added advantage in design of
hydraulic turbines and the prediction of behavior at various
Some Applications of Computational Tools for
R&D of Hydraulic Turbines
Biraj Singh Thapa, Amod Panthee*, Hari Prasad Neopane
N
TABLE I
TOTAL HYDROPOWER POTENTIAL
Major Basins Potential (at Q40)
Saptakoshi 17008.3
Narayani 17800.2
Karnali 15661.16
Mahakali 2261.83
Total 52731.83
Figure I: Sediment Eroded Francis Runner
of Trishuli HEP
RENTECH, Dec. 22, 2011 , RenewableNepal, KU, Nepal.
2
operating conditions and complex iterative process can be
done in short period.
II. CHALLENGES IN R&D OF HYDRAULIC TURBINES
There are many challenges in research and development of
hydraulic turbines. The challenges are seen from the initial
design stage after the selection of suitable site for erection of
hydropower station. It is followed by the selection of most
efficient design from a list optimized design to work on real
environment. The challenges continue during operation and
post operation or maintenance stage of the hydraulic turbines.
A. Design of Francis Runner
The design of hydraulic turbines involves many
assumptions. Initial assumptions during design of Francis
turbine are infinite number of thin blades, streamlines are
symmetric about the rotational axis and no frictional losses
are present [4]. But it is difficult to achieve these conditions in
real working conditions. The other assumptions based on the
empirical relation to achieve the desired result with
assumptions stated above are given in TABLE II [4].
TABLE II
INITIAL DESIGN ASSUMPTIONS OF FRANCIS TURBINE
Outlet Peripheral Velocity (U2) Outlet Angle (β2)
35 m/s – 43 m/s 180 - 22
0
The first step in design of a hydraulic turbine is to assume a
streamline. The shape of the streamline is given by equation
(1). The shape of the streamline changes with change in
values of constants „a‟ and „b‟ assumed in the equation from a
circle to an ellipse [5].
(1) (2)
The remaining streamlines on a runner blade of the runner
is obtained using the continuity equation (2) and the
principles of geometry. The geometry of the streamlines is
shown in Figure II where the constants have their usual
meaning. All these assumptions and iterative processes make
the design process a challenging task.
Figure II: Distribution of points along the streamline
B. Operation of a Hydraulic Turbine
Hydraulic Turbines are operated at various conditions. It is
a usual trend to design a hydraulic turbine at Best Efficiency
Point (BEP). But, a hydraulic turbine is operated from part
load to full load depending upon the energy requirement. The
change in operation of hydraulic turbines at different
operating conditions reduces the efficiency and life of the
turbine. Apart from these, it also creates problem in operation
and maintenance of the turbine unit [6].
Depending upon the site of operation, there is a variation in
sediment concentration with different percentage composition
of quartz and mica in rivers of Nepal [3]. So, if we have a list
of optimized design for a specific site to be tested, it would be
a problem to test with a physical model in the lab. The test
becomes more costly and time consuming when tested on a
physical model.
Despite having a
sound hydraulic
design, a hydraulic
turbine fails during
operation. A typical
case of such failure
in Pelton runner of
Khimti HEP is
shown in Figure III.
The reasons for
failure of turbines
during operation may be manufacturing defects, modes of
operation which are steady state and transient state operation
and maintenance procedure applied in the hydraulic turbines.
During the operation of hydraulic turbines, the mode of
operation changes from steady state to transient state upon
variation in load. This produces vibrations and stress on
power
production unit
which might
cause a failure of
the hydraulic
turbines. When
the load is
transferred from
point A to point
B, shown in
Figure IV, the
stress developed in the runner varies which might cause the
untimely failure of the runner when operated on a cycle [7].
C. Maintenance of Hydraulic Turbine
The turbine components are passed through a series of heat
treatment procedure during maintenance. The residual stress
is induced when a large temperature difference has been
created at different sections within the runner components [8].
Also, the improper cooling of the hydraulic turbines forms
weld decay which is a combination of Carbon and Chromium
[9], the ingredients of material used in manufacturing
hydraulic turbines. This induces residual stress in turbine
component and the immediate site of failure [7].
Figure III: Root Crack in Pelton Runner
Figure IV: Pelton Bucket
A B
R1,1; Z1,1
R1,2; Z1,2
Ri+1,1; Zi+1,1
Ri-1,1; Zi-1,1 Ri,1; Zi,1
Ri,2; Zi,2
ri,1
bi,1
Z
R
RENTECH, Dec. 22, 2011 , RenewableNepal, KU, Nepal.
3
III. METHODOLOGY
The Francis runner blade has been developed using general
principles mentioned in Section II and literature [5] for
“Design Optimization of Francis Runner” and “Effects of
Operating Conditions on Sediment Erosion” using the Matlab
program “Khoj” and CAD software. These files are exported
to AnSys CFX for further analysis.
A. Design Optimization of Francis Runner
A range of optimization criterion has been set on outlet
diameter, number of pole pairs in generator, reduced
peripheral velocity at inlet, acceleration of flow through the
runner, height of the runner and blade angle distribution [10].
Several optimized design is then developed using the
optimization criterion. The comparison of the optimized
design is done with the reference design by setting the erosion
factor and erosion tendency as reference indicators.
Erosion Tendency (3) is quantification of tendency of a
specific design of the runner to be eroded in similar sediment
conditions. Erosion Factor (4) is the ratio of erosion tendency
of each new design with respect to reference design.
m3/s
3 (3)
- (4)
The erosion factor for the reference design is set 1 and
compared to the results obtained for optimized design.
B. Effects of Operating Conditions on Sediment Erosion
The factors responsible for sediment erosion are particle
mass, particle velocity, grain shape and size, concentration of
particles and angle of attack at which the collision occurs
between the particle and the surface of the runner blade. The
empirical erosion model, Tabakoff erosion model (5), is used
in analysis which incorporates the factors responsible for
erosion to determine the erosion rate [6].
(5)
Where,
, Vp is the
particle impact velocity, is the impact angle in radians
between the particle path and the wall, is the angle of
maximum erosion. , are the model
constants and depend upon the particle and wall material
combination.
The blade profile is meshed with hexahedral element using
Turbo-Grid. The analysis is done on two modes of operation,
i.e. at best efficiency point with guide vane opening of 160
and at full load point with guide vane opening of 220. The
sediment particles chosen for analysis are of spherical and
non-spherical types. The boundary condition is set as uniform
injection of sand particles of uniform diameter for both modes
of operation [6].
C. Failure Analysis of Pelton Runner
The 3D model of
the Pelton Runner,
shown in Figure V,
has been developed
using the
orthographic
projection of runner
sections provided by
Himal Power Limited
using SolidWorks.
The other model
runner was developed
for stress and fatigue
analysis of the Pelton
runner because of software limitation. The information on
analysis conditions is tabulated in TABLE III.
TABLE III
ANALYSIS CONDITIONS ON COSMOSWORKS
Load
Force 85630 N normal to the reference plane
Distribution Uniform Distribution and Sequential Loading
Restraint
Description On 1 Face (at center)
Study Property
Mesh Type Solid Mesh
Jacobian Check 4 Points
No. of Elements 55709
IV. RESULTS
A. Design Optimization of Francis Runner
The optimized design developed within the defined range of
operation is shown in Figure VII. The optimized design is then
compared with the reference design, shown in Figure VI, of
Jhimruk HEP in Nepal. The result of comparison between the
reference and optimized design is shown in TABLE IV.
Figure VI(a): Streamlines on
Reference Design
Figure VI(b): Sediment Erosion
on Reference Design
Figure VII(a): Streamline on
Optimized Design
Figure VII(b): Sediment
Erosion on Optimized Design
Figure V: 3D Model of Pelton Runner
of Khimti HEP
RENTECH, Dec. 22, 2011 , RenewableNepal, KU, Nepal.
4
TABLE IV
COMPARISON OF EROSION FACTOR
Reference Design Optimized Design
Erosion Factor 1.0 0.481
The design optimization result also showed that the
sediment erosion is reduced significantly with increase in the
runner height [10]. Erosion is also dependent upon the blade
angle distribution. It was found that the erosion rate is
reduced for the optimized design with blade shape 1
compared with the reference design of blade shape 3 [10]
shown in Figure VIII.
B. Effects of Operating Conditions on Sediment Erosion
The effects of operating conditions on sediment erosion
have been analyzed on Francis blade of Cahua Power Plant of
Peru. The result showed that the erosion rate density is higher
at full load operation point than operation at best efficiency
point for both spherical and non-spherical sediments [6],
shown in Figure IX and Figure X.
Figure IX: Erosion due to Spherical Sediment
(a) at BEP (b) at Full Load
Figure X: Erosion due to Non-Spherical Sediment
(a) at BEP (b) at Full Load
This is due to the increase in flow turbulence and higher
relative flow velocities at runner outlet. The increase in
erosion rate is due to the presence of higher rotational motion
which caused more separation of flow. The result suggests
that the operating conditions of hydraulic turbines have
significant effect on erosion of the turbine components.
The analysis was repeated varying the concentration of
sediments at two modes of operation. The results from the
analysis is shown in Figure XI. It can be observed that with an
increase in sediment concentration, the erosion rate density is
increased for both modes of operation. It can be concluded
from the result that the erosion rate in the runner blade is
always higher when operated at full load than at best
efficiency point [6].
Figure XI: Variation of Relative Erosion Rate Density with
mode of Operation
C. Fault Analysis of Pelton Runner at Khimti HEP
The model runner was analyzed using CosmosWorks add-
in in SolidWorks for stress and fatigue analysis. Figure XII
shows the Factor of Safety (FOS) plot of the model runner.
The result shows that the root area of the runner geometry is
critical site for occurrence of failure [7]. The result justifies
the occurrence of crack in the root of pelton bucket shown in
Figure III.
Figure XII: FOS Analysis on a Model Runner
V. CONCLUSION
The use of computational tools in R&D of hydraulic
turbines helps in complex solving the complex mathematical
equations reducing both cost and time. The advantage on
Figure VIII: Blade Angle Distribution
Full Load
BEP
RENTECH, Dec. 22, 2011 , RenewableNepal, KU, Nepal.
5
reduction of cost and time can be justified by the use of the
real environment conditions for virtual testing in lab
repeatedly for different test conditions, which might increase
in cost and time if the problem has to be solved using the real
physical model. In design of hydraulic turbines, it plays an
important role offering flexibility while choosing different
variables that accounts different design result. The effects
due to change of each variable on design can be easily
understood which helps in producing an efficient design. It
also helps in finding the possible causes of failure of
hydraulic turbines during initial design stage.
The use of computational tools can be sometimes
disadvantageous. The assumptions should be carefully taken
to represent the real operating conditions. The results obtained
are dependent upon the accuracy of the input data and
assumptions. Therefore, it is necessary to verify the design
outputs obtained from the computational tool using a physical
model test at lab. Despite significant reduction in erosion
factor of optimized design, Figure VII (a), streamlines in the
optimized design are not uniform as in the reference design,
Figure VI (a). This might cause reduction in efficiency of the
significant design which should be verified with a physical
model test at lab.
The fault analysis of Pelton runner of Khimti HEP is at its
initial research stage. Further works can be done on stress and
fatigue analysis of the real model of runner. The effects due to
the heat treatment procedure on the runner can be analyzed
using appropriate assumptions with the aid of computational
tools. The effect due to different modes of operation on the
turbine component is another prospective area where
computational tools can be used.
REFERENCES
[1] Jha, R. (2007), Total Run-of-River type Hydropower
Potential in Nepal, Hydro Nepal.
[2] Thapa, B. (2004), Sand Erosion in Hydraulic Machinery,
PhD Thesis, Norwegian University of Science and
Technology (NTNU).
[3] Neopane, H. P. (2010), Sediment Erosion in Hydro
Turbines, PhD thesis, Norwegian University of Science
and Technology (NTNU).
[4] Brekke, H. (2001), Hydraulic Turbines: Design, Erection
and Operation, Norwegian University of Science and
Technology (NTNU).
[5] Francke, H. H., et al. (2009), High Pressure Hydraulic
Machinery, Water Power Laboratory, Norwegian
University of Science and Technology (NTNU).
[6] Neopane, H. P. (2011), Relationships between Operating
Conditions of Turbines and Sediment Erosion,
Proceedings in the International Conference of Hydro
2011.
[7] Panthee, A. (2011), Fault Analysis of Pelton Runner of
Khimti Hydropower, Industrial Training Report, Turbine
Testing Lab, Kathmandu University.
[8] Kubota, T., & Tanaka, O. (2010). Fuji Electric Co., Ltd.
Retrieved July 24, 2011, from Fuji Electric:
http://www.fujielectric.com/company/tech_archives/pdf/3
0-04/FER-30-04-151-1984.pdf
[9] Steel Casting Handbook, Supplement 7 Welding of High
Alloy Casting (2004), Steel Founders Society of America.
[10] Thapa, B. S., Eltvik, M., Gjøsæter, K., Dahlhaug, O. G.
(2012), Design Optimization of Francis Runners for
Sediment Handling, Proc. in Int. Conf. on Water
Resources and Renewable Energy Development in Asia,
Thailand.
BIOGRAPHIES
Biraj Singh Thapa is a graduate of Mechanical Engineering from
Kathmandu University. Currently, he is working as a Full time Researcher in RenewableNepal Project at Turbine Testing Lab, School of Engineering,
Kathmandu University.
Amod Panthee completed his Bachelor Degree in Mechanical Engineering
from Kathmandu University. Currently, he is working as a Research Assistant in RenewableNepal project at Turbine Testing Lab, School of Engineering,
Kathmandu University.
Hari Prasad Neopane completed his PhD from NTNU. He is Associate
Professor at Department of Mechanical Engineering, School of Engineering,
Kathmandu University. He works as a program coordinator on EnPe-Master Program in Planning and Operation of Energy Systems (MPPOES) at
Department of Mechanical Engineering, Kathmandu University.
RENTECH, Dec. 22, 2011 , RenewableNepal, KU, Nepal.