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International Journal of Trend in Scientific Research and Development (IJTSRD)
Volume: 3 | Issue: 4 | May-Jun 2019 Available Online: www.ijtsrd.com e-ISSN: 2456 - 6470
@ IJTSRD | Unique Paper ID - IJTSRD23824 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 521
CFD Simulation of Air Conditioning System of the Classroom
Gaurav Srivastava1, Aman Kumar1, Dipti Chandel1, Harsh Dabas1, Ashish Mishra1, Saurabh2
1B.Tech. Student, 2Assistant Professor Department of Mechanical Engineering
1,2ABES Engineering College, Ghaziabad, Uttar Pradesh, India
How to cite this paper: Gaurav
Srivastava | Aman Kumar | Dipti
Chandel | Harsh Dabas | Ashish Mishra |
Saurabh "CFD Simulation of Air
Conditioning System of the Classroom"
Published in International Journal of
Trend in Scientific Research and
Development
(ijtsrd), ISSN: 2456-
6470, Volume-3 |
Issue-4, June 2019,
pp.521-523, URL:
https://www.ijtsrd.
com/papers/ijtsrd2
3824.pdf
Copyright © 2019 by author(s) and
International Journal of Trend in
Scientific Research and Development
Journal. This is an Open Access article
distributed under
the terms of the
Creative Commons
Attribution License (CC BY 4.0)
(http://creativecommons.org/licenses/
by/4.0)
ABSTRACT
We have focused on the design and modifications of air cooling duct system
using Computational Fluid Dynamics (CFD) considering all air flow patterns
affecting the system efficiency. Necessary tools and methods are applied for
efficient designing. The different load conditions and the layout of the duct
system need to be very accurate because if any deviation will result to problems
like uneven cooling, frictional losses, increased noise & vibrationsand alsomore
power consumption. The above problems highlight the importance for
optimizing the duct design to obtain desired flow conditions. Our work involves
use of theoretical and software tools to get a detailedcomparative analysisof the
costs and benefits involved in selecting a particular shape (rectangular or
circular) for the duct according to theworking conditions. Thefocusof thispaper
rests on using psychrometry chart to calculate the cooling load and other
parameters.
Keywords: classroom, comfort condition
1. INTRODUCTION
Real-life environments such comfort working and living areas can be designed,
analyzed, and built by making comprehensive analyses. These types of analyses
have been done experimentally and/or computationally. As known well,
experimental works areexpensiveand time consuming.Advanced HVAC designin
a room can be achieved by analyzing the data about the air flow requirements of
the room. The necessary data about the flow includes air velocity, Temperature,
cfm, Relative humidity and other specific parameters. All these parameters are
very important for determining human comfort conditions
and inside air quality. In this study, we used parameters of
air velocity and temperature. The design of HVAC system is
decided by empirical formulas and experience. Though
practical approach and formulas provide successful
solutions, but the engineering methodsfailtoaccountforthe
flow patterns that gets affected notonlybythepositioningof
the HVAC system but also by the number of thermalsources.
To study inside airflow patterns, small- scale or full-scale
models are build. Small-scale models are constrained by the
scaling factors of heat transfer and airflow, while full-scale
model for inside evaluations are costly and time taking. The
impact of variables like HVAC positions and thermalsources
can be analyzed via CFD. As reported in the literature, CFD
has been increasingly used as a prediction tool in the design
and assessment of the indoor building.
2. PROBLEM DESCRIPTION
The room on which our study is based is located on 3rd floor
in Ramanujan block, ABES Engineering College. The room is
equipped with the air conditioning system with the
rectangular ducts. The system is designed for the occupancy
of the 60 peoples. The system which is installed is not quick
enough to provide efficient cooling. So we areoptimizingthe
system and doing the simulation of air conditioning system
in order to provide better cooling.
Our main is to propose a different model from which we can
compare which model is best suited for our existing system.
In the existing system we have got rectangular duct so we
want to give model with different duct shape.
3. PARAMETERS IDENTIFICATION
The parameter for our simulation is sizingof theductand air
flow rate. The next parameter are wet bulb temperature,dry
bulb temperature , humidity ratio ,specific enthalpy ,area of
the room and the area of the different different materials.
The other parameters involve all the psychrometeric
parameters. Other parameters are velocity of the air coming
out of the different different ducts.
4. ANALYSIS OF THE PROBLEM
The current condition was fully analyzed in accordance with
the required materials and tools. We followed the deep
thinking process and started gathering data in order to
structure the current problem using the following methods:
A. Market survey
B. Personal questionnaire
C. Research papers
5. SOLUTION APPROACH
5.1 DESIGN PARAMETERS
5.1.1 Design Parameters outside the classroom:
The calculated dry bulb temperature and the wet bulb
temperature outside the classroom is 42°C and 28°C
IJTSRD23824
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID - IJTSRD23824 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 522
5.1.2 Design Parameters inside the classroom:
The desired dry bulb temperature inside the classroom is
24°C and desired relative humidity is 50%.
There are four grill installed in the duct. The velocity of air
from grill obtained is 4m/s.
5.2 CALCULATION
Different types of heat load:
Heat load from different walls ;
1. Exposed Wall, Q = U×A×ΔT
= 3413.608 BTU/hr
2. North and South Wall, Q = 2×( U×A×ΔT)
= 10976.229 BTU/hr
3. West Wall, Q = U×A×ΔT
= 47430882 BTU/hr
Heat load from the walls is 19133.7115 BTU/hr. Heat load
from the roof, Q = U×A×ΔT
= 20189.46 BTU/hr.
Heat load from glass window, Q = U×A×ΔT
= 1384.536 BTU/hr.
Sensible heat load from people, Qs = 245×60
= 14700 BTU/hr
Latent heat load from people, Ql = 155×60
= 9300 BTU/hr.
Total heat load from people is 24000 BTU/hr.
Total lighting load, Q = Watt/ft2 × Area of ft2 × 3.4
= 3935.56 BTU/hr.
5.3 SIMULATION
5.3.1 Establishment of Model:
The dimensions of room are 31x26x7 (all dimensions are in
feet).
The dimensions of installed duct are 77x44x17 (all
dimensions are in cm).
The duct which is rectangular in shape is at the back of the
classroom. There are four grills in the rectangular duct. The
first grill is located at the 40cm from the right side, second
grill is located at 75cm from the first grill, third grill is
located at 1m from the second grill and last grill is located at
the 110cm from the left
5.3.2 Boundary Conditions:
The cubic feet per minute (CFM) at the inlet of the duct is
1.1m/s. The velocity of the air at the first grill is 3.9m/s,
velocity of the air at the second grill is 3.6m/s, velocityofthe
air at the third grill is 4.2m/s and velocity at the last grill is
4m/s.
Outside design conditions include outside dry bulb
temperature at 42°C and wet bulb temperature at 28°C. The
relative humidity of the room is 50%RH.
5.3.3 Model Meshing and Solver Parameter Setting:
This study adopted the method for definingthemeshingsize
function to guarantee the mesh quality of the model.
Meanwhile, mesh quantity was unlikely to be excessively
large. First, the meshes of the significant surveyed surfaces
(e.g., surfaces of the air inlets and exhaust outlets, as well as
the heat flow surfaces with large heat flow) were divided
into small sizes, thereby enabling the mesh densities on
these surfaces to be relatively high. When the mesh function
was defined, the meshes were divided from these critical
surfaces toward the surrounding space at 1.1-fold growth
rate. A total of 4,586,496 meshes and 846,589 nodes were
generated after the calculation.
Fig. 1 Mesh
5.3.4 Simulation Result Analysis
Only the air-conditioning conditions in the summer were
used due to the limited length of this study. The analog CFD
calculation and analysis of the air-conditioning conditions
were conducted at the representative 6:00, 8:00, and 13:00
time frames on the condition thattheairsupplytemperature
difference (9 °C) and air supply volume (111,630 m3/h)
were guaranteed to be unchanged. The temperature field
distributions of the classroom could be obtained based on
the simulation results.
Fig. 2 input of boundary conditions
Fig. 3 Velocity contour
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID - IJTSRD23824 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 523
Fig. 4 Velocity streamline
Fig. 5 Pressure volume rendering 1
Fig. 6 iteration chart
6. Proposed model
We had simulated the classroom with the rectangular duct.
We had seen the results from above simulation. So we have
proposed a new model with circular duct. And also if we
consider the factor of infiltration then the duct with the
rectangular shape is more efficent then the circular one.
Fig. 7 duct with circular duct
7. RESULT DISCUSSION
From this particular studywehad found variousresults. This
particular simulation helps usin determiningvariousfactors
from which we can find efficient cooling. This simulation
provide us that the use of air conditioning between 5-6
tonnes can provide better cooling at the peak conditions.
8. FUTURE ASPECTS
Mathematical modelling of this work can be done with help
of FEM. Various results can be obtained from that
mathematical modelling. Various differential equations can
provide the best results for the discussed work.
9. Conclusion:
The CFD simulation is obtained for the air conditioning
system. Various contours and plot has been obtained. The
plot for the temperatures, velocity, and the streamline is
obtained. These plots are used toobtainvariousconclusions.
References:
[1] Yin Hua, Guo Huafang, Lin Zhenrong, Zeng Bo CFD
simulation of air conditioning system in of a metro
station and research paper on energy saving
operation scheme. Pages 1-6 Guangzhou, China 2017.
[2] Mahmoud Kassas Modelling and simulation of
residential HVAC systems energy consumption. Page
1-10 Dhahran, Saudi Arabia 2015.
[3] Chang Soon Kang, jong-II Park, Mignon Park, Jaeho
Baek, Novel modelling and Control strategies for a
HVAC system including carbon dioxide control,
Suwon, Korea May 2014.
[4] Raad Z. Homod HVAC system modelling types and
the shortcomings of their applications. Page 1-11
Basrah, Iraq may 2013.
[5] Jianmin Sun, Chundong Zahang< Zeyang Zhou
Modelling and Simulation of chilled water system for
central air conditioning , Beijing, China, october
2012.
[6] B. F. Yua, Z. B. Hu, M. Liu, H. L.yang, Q. X.Kong, Y. H.
Liu Air conditioning system and indoor air quality
control for human health. Pages 1-18 Shaanxi, China
October 2007.

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CFD Simulation of Air Conditioning System of the Classroom

  • 1. International Journal of Trend in Scientific Research and Development (IJTSRD) Volume: 3 | Issue: 4 | May-Jun 2019 Available Online: www.ijtsrd.com e-ISSN: 2456 - 6470 @ IJTSRD | Unique Paper ID - IJTSRD23824 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 521 CFD Simulation of Air Conditioning System of the Classroom Gaurav Srivastava1, Aman Kumar1, Dipti Chandel1, Harsh Dabas1, Ashish Mishra1, Saurabh2 1B.Tech. Student, 2Assistant Professor Department of Mechanical Engineering 1,2ABES Engineering College, Ghaziabad, Uttar Pradesh, India How to cite this paper: Gaurav Srivastava | Aman Kumar | Dipti Chandel | Harsh Dabas | Ashish Mishra | Saurabh "CFD Simulation of Air Conditioning System of the Classroom" Published in International Journal of Trend in Scientific Research and Development (ijtsrd), ISSN: 2456- 6470, Volume-3 | Issue-4, June 2019, pp.521-523, URL: https://www.ijtsrd. com/papers/ijtsrd2 3824.pdf Copyright © 2019 by author(s) and International Journal of Trend in Scientific Research and Development Journal. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (CC BY 4.0) (http://creativecommons.org/licenses/ by/4.0) ABSTRACT We have focused on the design and modifications of air cooling duct system using Computational Fluid Dynamics (CFD) considering all air flow patterns affecting the system efficiency. Necessary tools and methods are applied for efficient designing. The different load conditions and the layout of the duct system need to be very accurate because if any deviation will result to problems like uneven cooling, frictional losses, increased noise & vibrationsand alsomore power consumption. The above problems highlight the importance for optimizing the duct design to obtain desired flow conditions. Our work involves use of theoretical and software tools to get a detailedcomparative analysisof the costs and benefits involved in selecting a particular shape (rectangular or circular) for the duct according to theworking conditions. Thefocusof thispaper rests on using psychrometry chart to calculate the cooling load and other parameters. Keywords: classroom, comfort condition 1. INTRODUCTION Real-life environments such comfort working and living areas can be designed, analyzed, and built by making comprehensive analyses. These types of analyses have been done experimentally and/or computationally. As known well, experimental works areexpensiveand time consuming.Advanced HVAC designin a room can be achieved by analyzing the data about the air flow requirements of the room. The necessary data about the flow includes air velocity, Temperature, cfm, Relative humidity and other specific parameters. All these parameters are very important for determining human comfort conditions and inside air quality. In this study, we used parameters of air velocity and temperature. The design of HVAC system is decided by empirical formulas and experience. Though practical approach and formulas provide successful solutions, but the engineering methodsfailtoaccountforthe flow patterns that gets affected notonlybythepositioningof the HVAC system but also by the number of thermalsources. To study inside airflow patterns, small- scale or full-scale models are build. Small-scale models are constrained by the scaling factors of heat transfer and airflow, while full-scale model for inside evaluations are costly and time taking. The impact of variables like HVAC positions and thermalsources can be analyzed via CFD. As reported in the literature, CFD has been increasingly used as a prediction tool in the design and assessment of the indoor building. 2. PROBLEM DESCRIPTION The room on which our study is based is located on 3rd floor in Ramanujan block, ABES Engineering College. The room is equipped with the air conditioning system with the rectangular ducts. The system is designed for the occupancy of the 60 peoples. The system which is installed is not quick enough to provide efficient cooling. So we areoptimizingthe system and doing the simulation of air conditioning system in order to provide better cooling. Our main is to propose a different model from which we can compare which model is best suited for our existing system. In the existing system we have got rectangular duct so we want to give model with different duct shape. 3. PARAMETERS IDENTIFICATION The parameter for our simulation is sizingof theductand air flow rate. The next parameter are wet bulb temperature,dry bulb temperature , humidity ratio ,specific enthalpy ,area of the room and the area of the different different materials. The other parameters involve all the psychrometeric parameters. Other parameters are velocity of the air coming out of the different different ducts. 4. ANALYSIS OF THE PROBLEM The current condition was fully analyzed in accordance with the required materials and tools. We followed the deep thinking process and started gathering data in order to structure the current problem using the following methods: A. Market survey B. Personal questionnaire C. Research papers 5. SOLUTION APPROACH 5.1 DESIGN PARAMETERS 5.1.1 Design Parameters outside the classroom: The calculated dry bulb temperature and the wet bulb temperature outside the classroom is 42°C and 28°C IJTSRD23824
  • 2. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID - IJTSRD23824 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 522 5.1.2 Design Parameters inside the classroom: The desired dry bulb temperature inside the classroom is 24°C and desired relative humidity is 50%. There are four grill installed in the duct. The velocity of air from grill obtained is 4m/s. 5.2 CALCULATION Different types of heat load: Heat load from different walls ; 1. Exposed Wall, Q = U×A×ΔT = 3413.608 BTU/hr 2. North and South Wall, Q = 2×( U×A×ΔT) = 10976.229 BTU/hr 3. West Wall, Q = U×A×ΔT = 47430882 BTU/hr Heat load from the walls is 19133.7115 BTU/hr. Heat load from the roof, Q = U×A×ΔT = 20189.46 BTU/hr. Heat load from glass window, Q = U×A×ΔT = 1384.536 BTU/hr. Sensible heat load from people, Qs = 245×60 = 14700 BTU/hr Latent heat load from people, Ql = 155×60 = 9300 BTU/hr. Total heat load from people is 24000 BTU/hr. Total lighting load, Q = Watt/ft2 × Area of ft2 × 3.4 = 3935.56 BTU/hr. 5.3 SIMULATION 5.3.1 Establishment of Model: The dimensions of room are 31x26x7 (all dimensions are in feet). The dimensions of installed duct are 77x44x17 (all dimensions are in cm). The duct which is rectangular in shape is at the back of the classroom. There are four grills in the rectangular duct. The first grill is located at the 40cm from the right side, second grill is located at 75cm from the first grill, third grill is located at 1m from the second grill and last grill is located at the 110cm from the left 5.3.2 Boundary Conditions: The cubic feet per minute (CFM) at the inlet of the duct is 1.1m/s. The velocity of the air at the first grill is 3.9m/s, velocity of the air at the second grill is 3.6m/s, velocityofthe air at the third grill is 4.2m/s and velocity at the last grill is 4m/s. Outside design conditions include outside dry bulb temperature at 42°C and wet bulb temperature at 28°C. The relative humidity of the room is 50%RH. 5.3.3 Model Meshing and Solver Parameter Setting: This study adopted the method for definingthemeshingsize function to guarantee the mesh quality of the model. Meanwhile, mesh quantity was unlikely to be excessively large. First, the meshes of the significant surveyed surfaces (e.g., surfaces of the air inlets and exhaust outlets, as well as the heat flow surfaces with large heat flow) were divided into small sizes, thereby enabling the mesh densities on these surfaces to be relatively high. When the mesh function was defined, the meshes were divided from these critical surfaces toward the surrounding space at 1.1-fold growth rate. A total of 4,586,496 meshes and 846,589 nodes were generated after the calculation. Fig. 1 Mesh 5.3.4 Simulation Result Analysis Only the air-conditioning conditions in the summer were used due to the limited length of this study. The analog CFD calculation and analysis of the air-conditioning conditions were conducted at the representative 6:00, 8:00, and 13:00 time frames on the condition thattheairsupplytemperature difference (9 °C) and air supply volume (111,630 m3/h) were guaranteed to be unchanged. The temperature field distributions of the classroom could be obtained based on the simulation results. Fig. 2 input of boundary conditions Fig. 3 Velocity contour
  • 3. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID - IJTSRD23824 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 523 Fig. 4 Velocity streamline Fig. 5 Pressure volume rendering 1 Fig. 6 iteration chart 6. Proposed model We had simulated the classroom with the rectangular duct. We had seen the results from above simulation. So we have proposed a new model with circular duct. And also if we consider the factor of infiltration then the duct with the rectangular shape is more efficent then the circular one. Fig. 7 duct with circular duct 7. RESULT DISCUSSION From this particular studywehad found variousresults. This particular simulation helps usin determiningvariousfactors from which we can find efficient cooling. This simulation provide us that the use of air conditioning between 5-6 tonnes can provide better cooling at the peak conditions. 8. FUTURE ASPECTS Mathematical modelling of this work can be done with help of FEM. Various results can be obtained from that mathematical modelling. Various differential equations can provide the best results for the discussed work. 9. Conclusion: The CFD simulation is obtained for the air conditioning system. Various contours and plot has been obtained. The plot for the temperatures, velocity, and the streamline is obtained. These plots are used toobtainvariousconclusions. References: [1] Yin Hua, Guo Huafang, Lin Zhenrong, Zeng Bo CFD simulation of air conditioning system in of a metro station and research paper on energy saving operation scheme. Pages 1-6 Guangzhou, China 2017. [2] Mahmoud Kassas Modelling and simulation of residential HVAC systems energy consumption. Page 1-10 Dhahran, Saudi Arabia 2015. [3] Chang Soon Kang, jong-II Park, Mignon Park, Jaeho Baek, Novel modelling and Control strategies for a HVAC system including carbon dioxide control, Suwon, Korea May 2014. [4] Raad Z. Homod HVAC system modelling types and the shortcomings of their applications. Page 1-11 Basrah, Iraq may 2013. [5] Jianmin Sun, Chundong Zahang< Zeyang Zhou Modelling and Simulation of chilled water system for central air conditioning , Beijing, China, october 2012. [6] B. F. Yua, Z. B. Hu, M. Liu, H. L.yang, Q. X.Kong, Y. H. Liu Air conditioning system and indoor air quality control for human health. Pages 1-18 Shaanxi, China October 2007.