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Newsletter
October 20
2015 [Type the abstract of the document here. The abstract is typically a short
summary of the contents of the document. Type the abstract of the document
here. The abstract is typically a short summary of the contents of the
document.]
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Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
1
INSIDE THIS ISSUE
Newsletter Chair Message………………………………………………………………… 2
Article - CFD Predictions of Pressure Loss in Duct Fittings……………………………… 3
ASHRAE News…………………………………………………………………………… 10
Photos Gallery…………………………………………………………………………….. 11
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Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
2
NEWSLETTER CHAIR MESSAGE
I had the privilege of travelling to Istanbul for the ASHRAE Regional at Large CRC-2015 as the Student
Activities Regional Vice Chair & part of Qatar Oryx Chapter delegation.
The relationship between ASHRAE & Turkey dates back couple of years but our friends in the Turkish
Chapter did their best to provide a successful CRC full with technical presentations and very remarkable
social events at the Bosphorus.
Dear ASHRAE members at Qatar Oryx Chapter, I would like to share with you and to address about the
importance of the CRC.
Members who are attending the Chapter’s Regional Conference (CRC) can get experience where these
conferences provide an excellent opportunity to:
1. Meet with Board Members in the region.
2. Interact and network with other ASHRAE members in the region.
3. Attend seminars and technical presentations presented by ASHRAE distinguished lecturers and
HVAC industry leaders.
4. Communicate and interact with HVAC manufacturers and stakeholders of the country where the
CRC is taking place.
5. Practice and experience the ASHRAE business and election meeting.
6. Attend to share the election of the Region officers and leaders for the next term.
7. Enjoy the special social events and the well planned activities.
8. Practice and explore about the HVAC industries and news at the CRC country.
9. Attend the training session for student activities, CCT, GR, RP & MP.
10. Chance of building the leadership from the CRC program.
These are some of the benefits and many more you should see with your participation in the CRC.
Hassan Sultan
Former President
ASHRAE Qatar Oryx Chapter
ASHRAE RAL SA, RVC
E&IEC Organizing Committee Chair
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Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
3
ARTICLE
Computational Fluid Dynamics (CFD) Predictions of Pressure Loss in Duct Fittings
By: Dr. Ahmad Sleiti, Ph.D., P.E., CEM
INTRODUCTION
This paper reports on a systematic study to establish whether CFD techniques are capable of obtaining
pressure drop predictions in elbows that are accurate to within 15% of experimental loss coefficients. A
test program was initiated to measure the friction factor in a straight duct, and the loss coefficient of both
a single five-gore elbow and two close-coupled five-gore elbows. This paper presents results from tests
conducted on ducts/fittings having a nominal diameter of 203 mm (8 in.). Likewise a comparison of CFD
turbulence models in predicting pressure drop for each of the configurations was performed. This was
achieved by conducting a critical comparison between turbulence models, including k-ε, k-ω and the
Reynolds Stress Model (RSM) to establish their capabilities and limitations in predicting such flows.
TEST PROGRAM
An experimental apparatus was constructed to measure the friction factor in a straight duct, and the loss
coefficient of both a single five-gore elbow and two close-coupled five-gore elbows. The measurements
of pressure drop and volumetric flow rate through the ductwork and fittings were performed in
accordance with ASHRAE Standard 120-2008. The elbow pressure loss experiments were preceded by a
series of tests designed to evaluate the friction factor of straight ducts.
CFD MODELING
Computational fluid dynamics is employed to predict the pressure loss in straight duct, in single elbow
and in close-coupled five gore elbow (Z-configuration and U-configuration). The numerical solution
method used to solve Navier-Stokes equations is the finite volume method. A control-volume-based
technique is used to convert the governing equations to algebraic equations that can be solved
numerically.
Turbulence Models
The Navier-Stokes equations are non-linear partial differential equations that cannot be solved
analytically, except a few special cases. Consequently, for most cases, numerical solution is needed to
solve the NS-equations. Direct Numerical Simulations (DNS’s) and Large Eddy Simulations (LES’s) are
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Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
4
the most accurate but they require large computational resources. Reynolds Averaged Navier Stokes
(RANS) turbulence models although are affected by numerical and physical approximations still they
perform reasonably accurate, require less computational resources and they are widely used for industrial
applications. Thus, in this paper RANS turbulence models are used.
Grid Generation and Boundary Conditions
The performance of turbulence models is evaluated by comparing the CFD predictions of each model to
experimental measurements in straight duct, single elbow, Z-configuration duct and U-configuration duct.
The numerical grid for the studied duct geometries is shown by Figure 1.
CFD RESULTS
1. Straight Duct
Figure 2 shows a comparison between experimental friction factor and 3 CFD k-e turbulence models with
wall roughness. Results in Figure 2 are summarized as follows:
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Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
5
CFD RNG k-e for e/D = 0.009 rough duct: RNG k-e turbulence model was used with 60 x 200 grid size
and standard wall functions to compare friction factor of rough duct to experimental and Moody diagram
friction factor. Results show that the error in friction factor prediction using RNG k-e CFD model ranges
from 6% to more than 17%.
CFD Realizable k-e for e/D = 0.009 rough duct: Realizable k-e turbulence model was used with 60 x
200 grid size and standard wall functions to compare friction factor of rough duct to experimental and
Moody diagram friction factor. Results show that the error in friction factor prediction using Realizable k-
e CFD model ranges from 10% to more than 21%.
Figure 3 shows a comparison between experimental friction factor and 2 CFD k-w turbulence models
with wall roughness. Results in Figure 3 are summarized as follows:
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015
Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
6
CFD Standard k-w for e/D = 0.009 rough duct: Standard k-w turbulence model was used with 60 x 200
grid size and standard wall functions to compare friction factor of rough duct to experimental and Moody
diagram friction factor. Results show that the error in friction factor prediction using Standard k-w CFD
model ranges from 2 % (for high Re) to more than 13% (for low Re).
CFD SST k-w for e/D = 0.009 rough duct: SST k-w turbulence model was used with 60 x 200 grid size
and standard wall functions to compare friction factor of rough duct to experimental and Moody diagram
friction factor. Results show that the error in friction factor prediction using SST k-w CFD model ranges
from 6 % (for high Re) to more than 18% (for low Re).
Figure 4 shows a comparison between experimental friction factor and RSM turbulence model with wall
roughness. Results in Figure 4 are summarized as follows:
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Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
7
CFD RSM for e/D = 0.009 rough duct: RSM turbulence model was used with 60 x 200 grid size and
standard wall functions to compare friction factor of rough duct to experimental and Moody diagram
friction factor. Results show that the error in friction factor prediction using RSM CFD model ranges
from 13 % to more than 22% .
2. Single Elbow
Figure 5 shows a comparison between experimental loss coefficient and CFD k-e turbulence model
predictions for single elbow. Results in Figure 5 are summarized as follows:
CFD Standard k-e for e/D = 0.009 rough duct: A standard k-e turbulence model was used with grid
size of 60 x 200 in the entrance region, 60 x 22 in the curve region and 60 x 160 in the exit region and
with standard wall functions to compare friction factor of rough duct to experimental loss coefficient.
Results show that the error in CFD predictions using Standard k-e ranges from 5% to more than 18%.
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015
Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
8
CFD Standard k-w for e/D = 0.009 rough duct: A standard k-w turbulence model was used with grid
size of 60 x 200 in the entrance region, 60 x 22 in the curve region and 60 x 160 in the exit region and
with standard wall functions to compare friction factor of rough duct to experimental loss coefficient.
Results show that the error in CFD predictions using Standard k-w ranges from 9% to more than 19%.
CFD RSM for e/D = 0.009 rough duct: RSM turbulence model was used with grid size of 60 x 200 in
the entrance region, 60 x 22 in the curve region and 60 x 160 in the exit region and with standard wall
functions to compare friction factor of rough duct to experimental loss coefficient. Results show that the
error in CFD predictions using RSM turbulence model ranges from 4% to 16%, which are more accurate
than k-w and k-e turbulence models
3. Double Elbow Loss Coefficient: Z-Configuration with Lint = 2.52 m (8.28 ft)
Figure 6 shows a comparison between experimental loss coefficient and CFD turbulence model prediction
for the Z-Configuration with Lint = 2.52 m (8.28 ft). Results in Figure 6 are summarized as follows:
CFD Standard k-e for e/D = 0.009 rough duct: A standard k-e turbulence model was used with grid
size of 60 x 200 in the entrance region, 60 x 22 in the curve regions and 60 x 160 in the exit region and
0
10
20
30
40
50
60
70
0 50 100 150 200 250 300 350
Tota
l Pre
ssur
e Los
s (Pa
)
Velocity Pressure (Pa)
ExperimentalData
CFD k-e
CFD k-w
CFD RSM
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015
Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
9
with standard wall functions to compare friction factor of rough duct to experimental loss coefficient.
Results show that the error in CFD predictions using Standard k-e ranges from 0.1% to more than 18%.
CFD Standard k-w for e/D = 0.009 rough duct: A standard k-w turbulence model was used with grid
size of 60 x 200 in the entrance region, 60 x 22 in the curve regions and 60 x 160 in the exit region and
with standard wall functions to compare friction factor of rough duct to experimental loss coefficient.
Results show that the error in CFD predictions using Standard k-w ranges from 7% to more than 24%.
CFD RSM for e/D = 0.009 rough duct: RSM turbulence model was used with grid size of 60 x 200 in
the entrance region, 60 x 22 in the curve regions and 60 x 160 in the exit region and with standard wall
functions to compare friction factor of rough duct to experimental loss coefficient. Results show that the
error in CFD predictions using Standard k-e ranges from 0.4% to more than 15%, which are more
accurate than k-w and k-e turbulence models.
0
20
40
60
80
100
120
140
160
180
0 50 100 150 200 250 300 350 400 450 500
Tota
l Pre
ssur
e Lo
ss (P
a)
Velocity Pressure (Pa)
Experimental Data
CFD k-e
CFD k-w
Experimental Data
CFD k-e
CFD k-w
CFD RSM
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Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
10
ASHRAE NEWS
MANAGE ENERGY EFFECTIVELY Sustained energy management is the quickest,
cheapest, cleanest way to expand the world’s energy supplies and to reduce
greenhouse gas emissions. Learn the strategies for ensuring that energy
management efforts don’t fall short of their potentials. This online course, part of
the 2015 Fall Online Series, will take place October 12, 1:00 – 4:00 EDT. This
course is a part of the ASHRAE Career Enhancement Curriculum Program.
GEOTHERMAL HVAC The 2015 edition of Geothermal Heating and Cooling:
Design of Ground-Source Heat Pump Systems is a complete revision. This is an essential
guide for HVAC design engineers, design-build contractors, GSHP subcontractors, and
energy/construction managers, building owners and architects. The book provides
insights into characteristics of high-quality engineering firms and key information that
should be provided by design firms owners competing for GSHP projects and owners
evaluating them.
HVAC TRAINING IN DUBAI ASHRAE is offering its popular Level I and
Level II HVAC Design training on November 15–19, 2015 in Dubai. Reserve your seat
today to attend both courses to gain real-world knowledge; you can put to immediate
use. HVAC Design: Level I – Essentials provides the fundamental and technical
aspects of HVAC design in commercial buildings. HVAC Design: Level II –
Applications provides advanced instruction on HVAC system designs. Accelerate your
transformation into a more effective member of your design, construction or facilities
maintenance team, whether you are new to the field or an experienced engineer
.
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Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
11
ASHRAE Photos Gallery
Innovative Cooling Solutions with “Indirect Evaporative Cooling”
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Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
12
K 12 Training for Lebanese School
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015
Chapter Officer: Board of Governors: Newsletter Committee: Kinan Fahs – President Ghassan Trabolsi – RP Chair Hassan Sultan - Chair
Fady Abu Jamra – President Elect Mostafa Hariri – SA Chair Kinan Fahs - Member
Salah Nezar – Vice President Ali Ibrahim – CTTC Chair Mostafa Hariri - Member Seenu Pillai – Treasurer Mutassim Al Ghadir – GGAC Chair
Tony Khoury – Secretary Chinna Kannan
Diwakar N. Lal Mohamed El Sayed
13
CRC Turkish (2 - 4.10.2015)