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Modeling Performance of WECS Installed in Residential Towers

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Present a computer model for WECS confined ... k- model of turbulence ... 1/2 ln(y/yo) k= s/( C 1/2 ) =( s/ )3/2/ y September, 2002. PHOENICS Conf Moscow. 8 ... – PowerPoint PPT presentation

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Title: Modeling Performance of WECS Installed in Residential Towers


1
Modeling Performance of WECS Installed in
Residential Towers
  • M.A. Serag-Eldin
  • American University in Cairo

2
INTRODUCTION-I
  • It has been
  • proposed to
  • exploit high
  • building
  • structures in
  • windy areas to
  • install WECS

3
INTRODUCTION-II
  • Advantages
  • Saving in WECS tower cost
  • Saving of land required for wind-farms
  • Saving of energy transmission costs
  • Possibility of increasing wind speed due to
    funneling effect

4
OBJECTIVES
  • Present a computer model for WECS confined amidst
    building blocks.
  • Reveal how the model is implemented in PHOENICS
  • Demonstrate the application of the model , and
    reveal its use as a design tool

5
Modeling Wind Flow
  • Domain assumed entirely in constant stress layer,
    with neutral stability
  • k-? model of turbulence
  • governing equations expressing mass conservation,
    momentum balance in 3D, transport of k and ?
  • eqns of form ? . ( ? V ? ) ? . ( ?? ?? )
    S?
  • where ? any dependent variable , V u i v j
    w k
  • ?? and S? are the diffusion coefficient and
    source term, respectively , for ?

6
Source term expressions
  • ? S?
  • u - ?p/?x?(?e?u/?x)/?x?(?e?v/?x)/?y?(?e?w/?x)/?
    z
  • v - ?p/?y?(?e?u/?y)/?x?(?e?v/?y)/?y?(?e?w/?y)/?
    z
  • w - ?p/?z?(?e?u/?z)/?x?(?e?v/?z)/?y?(?e?w/?z)/?
    z
  • k Gk - ? ?
  • ? C1 ?/k.Gk - C2 ? ?2/k
  • Gk ?t 2(?u/?x)2 (?v/?y)2 (?w/?z)2
    (?u/?y?v/?x)2
  • ( ?u/?z?w/?x)2 (?v/?z?w/?y)2 ,
    ?t ? ? C? k2 /?
  • standard (k-?) model coefficients

7
WECS model BCs
  • WECS characteristics displayed as power/thrust
    .vs.w
  • thrust effect introduced implicitly through w
    source-term
  • Inflow B.C.s
  • Undisturbed Atmospheric Flow, i.e.
  • u v 0
  • w 1 / ?. (?s/?)1/2 ln(y/yo)
  • k ?s/(? C?1/2 )
  • ?(?s/?)3/2/?y

8
Boundary-Conditions-II
  • Top boundary undisturbed atmospheric flow.
  • Outflow boundary constant press, zero gradients
  • Ground boundary
  • us vs ws 0
  • ?s ? ?/ln(y/yo)2 (w2 u2)
  • k ?s/(?C?1/2)
  • ? (?s/?)3/2 / ?y
  • Side boundaries symmetry boundary and
    undisturbed atmospheric flow

9
CASE I Rectangular Blocks w/o Bottom Pass
10
TOP VIEW OF BUILDING
Wind direction
11
Cross-sectional elevation
12
Grid at WECS k-plane
13
Grid Enlargement
14
Grid at Cowl Entrance
15
Grid in Hub j-plane
Wind
direction
16
Grid in Symmetry Plane
Wind
direction
17
Flow in Symmetry Plane
18
Enlargement of Flow
19
Pressure in symmetry plane
20
Flow in Hub1 j-plane
21
Pressure in Hub Plane
22
Case II Open Pass
23
Flow in Symmetry Plane
24
Pressure in symmetry plane
25
Case III convergent-divergent blocks
26
Flow in Hub 1 j-plane
27
Flow in Hub 3 j-plane
28
Flow in symmetry plane
29
Pressure in Hub1 j-plane
30
Case IV Turbine 2 out of service
31
Pressure distribution
32
Case V Roof Turbine
33
Flow in symmetry plane
34
Pressure in symmetry plane
35
Pressure in Turbines plane
36
Summary of Results for 5 Cases
37
Summary Conclusion
  • The predictions revealed that there is a gain in
    speed for all cases which varied from case to
    case, albeit not very spectacular best results
    require careful design of building shape,
    however this must be developed in conjunction
    with architectural requirements
  • the number of variables that need to be
    investigated are enormous, including various
    building shapes and dimensions, HAWT
    character-istics and location, wind speed and
    direction, upstream wind profile and presence of
    nearby flow obstacles all of which may be
    readily investigated with the aid of the present
    model .
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