Name: Author Spotlight: Optimization of Airflow Velocities in Battery Cooling Systems for Enhanced Thermal Performance and Reduced Energy Consumption
Uploaded: 2023-11-03T14:40:00
Description: Watch this Scientific Journal Video about Optimization of Airflow Velocities in Battery Cooling Systems for Enhanced Thermal Performance and Reduced Energy Consumption at JoVE.com

Some analysis and optimization software are supported by Tsinghua University, Konkuk University, Chonnam National University, Mokpo University, and Chiba University.

NOTE: The research technology roadmap is shown in Figure 1, where the modeling, simulation, and optimization software are used. The materials required are shown in the Table of Materials.
1. Creating the 3D model
NOTE: We used Solidworks to create the 3D model.
<ol>
	<li>Draw a 252 mm x 175 mm rectangle, click Extrude Boss/Base, and enter 73. Create a new plane 4 mm from the outer surface.</li>
	<li>Draw a rectangle 131 m...

Optimizing Battery Heat Management in Dusty Environments

<ol>
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Y., Qu, Z. G. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Lithium+-+ion+battery+thermal+management+using+heat+pipe+and+phase+change+material+during+discharge+-+charge+cycle:+A+comprehensive+numerical+study.">Lithium - ion battery thermal management using heat pipe and phase change material during discharge - charge cycle: A comprehensive numerical study.</a> Applied Energy. 242, 378-392 (2019).</li><li>Saw, L. 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air-cooled battery thermal management system through designing the flow pattern.</a> Energy. 167, 781-790 (2019).</li><li>Lan, X., Li, X., Ji, S., Gao, C., He, Z. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Design+and+optimization+of+a+novel+reverse+layered+air-cooling+battery+management+system+using+U+and+Z+type+flow+patterns.">Design and optimization of a novel reverse layered air-cooling battery management system using U and Z type flow patterns.</a> International Journal of Energy Research. 46 (10), 14206-14226 (2022).</li><li>Singh, G., Wu, H. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Effect+of+different+inlet/outlet+port+configurations+on+the+thermal+management+of+prismatic+Li-ion+batteries.">Effect of different inlet/outlet port configurations on the thermal management of prismatic Li-ion batteries.</a> Journal of Heat Transfer. 144 (11), 112901 (2022).</li><li>Zhang, J., Wu, X., Chen, K., Zhou, D., Song, M. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Experimental+and+numerical+studies+on+an+efficient+transient+heat+transfer+model+for+air-cooled+battery+thermal+management+systems.">Experimental and numerical studies on an efficient transient heat transfer model for air-cooled battery thermal management systems.</a> Journal of Power Sources. 490, 229539 (2021).</li><li>Qian, X., Xuan, D., Zhao, X., Shi, Z. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Heat+dissipation+optimization+of+lithium-ion+battery+pack+based+on+neural+networks.">Heat dissipation optimization of lithium-ion battery pack based on neural networks.</a> Applied Thermal Engineering. 162, 114289 (2019).</li><li>Chen, K., Wang, S., Song, M., Chen, L. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Structure+optimization+of+parallel+air-cooled+battery+thermal+management+system.">Structure optimization of parallel air-cooled battery thermal management system.</a> International Journal of Heat and Mass Transfer. 111, 943-952 (2017).</li><li>Liu, Y., Zhang, J. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Self-adapting+J-type+air-based+battery+thermal+management+system+via+model+predictive+control.">Self-adapting J-type air-based battery thermal management system via model predictive control.</a> Applied Energy. 263, 114640 (2020).</li><li>Baveja, R., Bhattacharya, J., Panchal, S., Fraser, R., Fowler, M. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Predicting+temperature+distribution+of+passively+balanced+battery+module+under+realistic+driving+conditions+through+coupled+equivalent+circuit+method+and+lumped+heat+dissipation+method.">Predicting temperature distribution of passively balanced battery module under realistic driving conditions through coupled equivalent circuit method and lumped heat dissipation method.</a> Journal of Energy Storage. 70, 107967 (2023).</li><li>Singh, L. K., Kumar, R., Gupta, A. K., Sharma, A. 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A., Petraglia, A. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Global+optimization+using+dimensional+jumping+and+fuzzy+adaptive+simulated+annealing.">Global optimization using dimensional jumping and fuzzy adaptive simulated annealing.</a> Applied Soft Computing. 11 (6), 4175-4182 (2011).</li><li>Ingber, L. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Very+fast+simulated+re-annealing.">Very fast simulated re-annealing.</a> Mathematical and computer modelling. 12 (8), 967-973 (1989).</li><li>Yu, X., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Experimental+study+on+transient+thermal+characteristics+of+stagger-arranged+lithium-ion+battery+pack+with+air+cooling+strategy.">Experimental study on transient thermal characteristics of stagger-arranged lithium-ion battery pack with air cooling strategy.</a> International Journal of Heat and Mass Transfer. 143, 118576 (2019).</li><li>Li, W., Xiao, M., Peng, X., Garg, A., Gao, L. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=A+surrogate+thermal+modeling+and+parametric+optimization+of+battery+pack+with+air+cooling+for+EVs.">A surrogate thermal modeling and parametric optimization of battery pack with air cooling for EVs.</a> Applied Thermal Engineering. 147, 90-100 (2019).</li><li>Chen, K., Zhang, Z., Wu, B., Song, M., Wu, X. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=An+air-cooled+system+with+a+control+strategy+for+efficient+battery+thermal+management.">An air-cooled system with a control strategy for efficient battery thermal management.</a> Applied Thermal Engineering. 236, 121578 (2023).</li><li>Zhao, L., Li, W., Wang, G., Cheng, W., Chen, M. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=A+novel+thermal+management+system+for+lithium-ion+battery+modules+combining+direct+liquid-cooling+with+forced+air-cooling.">A novel thermal management system for lithium-ion battery modules combining direct liquid-cooling with forced air-cooling.</a> Applied Thermal Engineering. 232, 120992 (2023).</li><li>Oyewola, O. M., Awonusi, A. A., Ismail, O. S. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Design+optimization+of+Air-Cooled+Li-ion+battery+thermal+management+system+with+Step-like+divergence+plenum+for+electric+vehicles.">Design optimization of Air-Cooled Li-ion battery thermal management system with Step-like divergence plenum for electric vehicles.</a> Alexandria Engineering Journal. 71, 631-644 (2023).</li><li>Chen, K., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Design+of+parallel+air-cooled+battery+thermal+management+system+through+numerical+study.">Design of parallel air-cooled battery thermal management system through numerical study.</a> Energies. 10 (10), 1677 (2017).</li><li>Lyu, C., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=A+new+structure+optimization+method+for+forced+air-cooling+system+based+on+the+simplified+multi-physics+model.">A new structure optimization method for forced air-cooling system based on the simplified multi-physics model.</a> Applied Thermal Engineering. 198, 117455 (2021).</li><li>Zhang, W. C., Liang, Z. C., Ling, G. Z., Huang, L. S. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Influence+of+phase+change+material+dosage+on+the+heat+dissipation+performance+of+the+battery+thermal+management+system.">Influence of phase change material dosage on the heat dissipation performance of the battery thermal management system.</a> Journal of Energy Storage. 41, 102849 (2021).</li><li>Li, M. L., Zang, M. Y., Li, C. Y., Dai, H. Y. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Optimization+of+structure+of+air+cooling+heat+dissipation+for+Li-ion+batteries.">Optimization of structure of air cooling heat dissipation for Li-ion batteries.</a> Battery Bimonthly. 50 (3), 1001 (2020).</li></ol>

&#160;The BTMS used in this study was established based on the air-cooling system due to its low cost and simplicity of the structure. Because of the low heat transfer capacity, the performance of the air-cooling system is lower than that of the liquid cooling system and phase change material cooling system. However, the liquid cooling system has the disadvantage of refrigerant leakage, and the phase change material cooling system has high mass and low energy density29. These cooling systems have ...

With the rapid development of the automobile industry, traditional fuel vehicles consume a lot of non-renewable resources, resulting in serious environmental pollution and energy shortage. One of the most promising solutions is the development of electric vehicles (EVs)1,2.
The power batteries used for EVs can store electrochemical energy, which is the key to replacing traditional fuel vehicles. Power batteries used in EVs include lithium-ion battery (LIB), nickel-metal hydride battery (NiMH), and electric double-layer capacitor (EDLC)3. Compared to the other batteries, lithium-ion batteries are currently widely used as energy storage units in EVs owing to their advantages such as high energy density, high efficiency, and long life cycle4,5,6,7.
However, due to chemical reaction heat and Joule heat, it is easy to accumulate a large amount of heat and increase the battery temperature during rapid charging and high-intensity discharging. The ideal operating temperature of LIB is 20-40 &#176;C8,9. The maximum temperature difference between the batteries in a battery string should not exceed 5 &#176;C10,11. Otherwise, it may lead to a series of risks such as temperature imbalance between the batteries, accelerated aging, even overheating, fire, explosion, and so on12. Therefore, the critical issue to be resolved is designing and optimizing an efficient battery thermal management system (BTMS) that can control the temperature and temperature difference of the battery pack within a narrow.
Typical BTMS include air cooling, water cooling, and phase change material cooling13. Among these cooling methods, the air cooling type is widely used because of its low cost and simplicity of the structure14. Due to the limited specific heat capacity of air, high temperature and large temperature differences are easy to occur between battery cells in air-cooled systems. In order to improve the cooling performance of air-cooled BTMS, it is necessary to design an efficient system15,16,17. Qian et al.18 collected the battery pack&#39;s maximum temperature and temperature difference to train the corresponding Bayesian neural network model, which is used to optimize cell spacings of the series air-cooled battery pack. Chen et al.19 reported using the Newton method and the flow resistance network model for optimization of the widths of the inlet divergence plenum and the outlet convergence plenum in the Z-type parallel air-cooled system. The results showed a 45% reduction in the temperature difference of the system. Liu et al.20 sampled five groups of the cooling ducts in the J-BTMS and obtained the best combination of cell spacings by the ensemble surrogate-based optimization algorithm. Baveja et al.21 modeled a passively balanced battery module, and the study described the effects of thermal prediction on module-level passive balancing and vice versa. Singh et al.22 investigated a battery thermal management system (BTMS) that used encapsulated phase change material along with forced convective air cooling designed using the coupled electrochemical-thermal modeling. Fan et al.23 proposed a liquid cooling plate comprising a multi-stage Tesla valve configuration to provide a safer temperature range for a prismatic-type lithium-ion battery with high recognition in microfluidic applications. Feng et al. 24 used the coefficient of variation method to evaluate the schemes with different inlet flow rates and battery clearances. Talele et al.25 introduced wall-enhanced pyro lining thermal insulation to store potential generated heating based on optimal placement of heating films.
When one uses air-cooling BTMS, metal dust particles, mineral dust particles, building materials dust particles, and other particles in the external environment will be brought into the air-cooling BTMS by the blower, which can cause the surface of the batteries to be covered with DPM. If there is no heat dissipation plan, it may cause accidents due to the excessively high battery temperature. After simulation, we take the maximum temperature of the battery pack in a specified airflow velocity and dust-free environment as the expected temperature in a dusty environment. First, C-rate refers to the current value required when the battery releases its rated capacity within the specified time, which is equal to a multiple of the battery&#39;s rated capacity in the data value. In this paper, the simulation uses 2C rate discharge. The rated capacity is 10 Ah, and the nominal voltage is 3.2 V. Lithium iron phosphate (LiFePO4) is used as the positive electrode material, and carbon is used as the negative electrode material. The electrolyte has electrolyte lithium salt, a high-purity organic solvent, necessary additives, and other raw materials. The random array representing the different velocity combinations at the inlets was determined through the OLHA, and a 2nd order function between the maximum temperature of the battery pack and the inlet flow velocity combination was set up under the condition of checking the accuracy of the curve fitting. Latin hypercube (LH) designs have been applied in many computer experiments since they were proposed by McKay et al.26. An LH is given by an N x p-matrix L, where each column of L consists of a permutation of the integers 1 to N. In this paper, the optimal Latin hypercube sampling method is used to reduce the computational burden. The method uses stratified sampling to ensure that the sampling points can cover all the sampling internals.
In the following step, the inlet flow velocity combination was optimized to decrease the maximum temperature of the battery pack in a dusty environment based on the ASAM under the condition of considering energy consumption simultaneously. The adaptive simulated annealing algorithm has been extensively developed and widely used in many optimization problems27,28. This algorithm can avoid getting trapped in a local optimum by accepting the worst solution with a certain probability. The global optimum is achieved by defining the acceptance probability and temperature; the calculation speed can also be adjusted by using these two parameters. Finally, for checking the accuracy of the optimization, the optimal result was compared with the analysis result obtained from the simulation software.
In this paper, an optimization method for the inlet flow rate of the battery box is proposed for the battery pack whose temperature rises due to dust cover. The purpose is to reduce the maximum temperature of the dust-covered battery pack to below the maximum temperature of the non-dust-covered battery pack in the case of low energy consumption.

<table border="1" fo:keep-together.within-page="1" fo:keep-with-next.within-page="always">
	<tbody>
		<tr>
			<td>Ansys-Workbench</td>
			<td>ANSYS</td>
			<td>N/A</td>
			<td>Multi-purpose finite element method computer design program software.https://www.ansys.com</td>
		</tr>
		<tr>
			<td>Isight</td>
			<td>Engineous Sogtware</td>
			<td>N/A</td>
			<td>Comprehensive computer-aided engineering software.https://www.3ds.com</td>
		</tr>
		<tr>
			<td>NVIDIA GPU</td>
			<td>NVIDIA</td>
			<td>N/A</td>
			<td>An NVIDIA GPU is needed as some of the software frameworks below will not work otherwise. https://www.nvidia.com</td>
		</tr>
		<tr>
			<td>Software</td>
			<td></td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>SOLIDWORKS</td>
			<td>Dassault Systemes</td>
			<td>N/A</td>
			<td>SolidWorks provides different design solutions, reduces errors in the design process, and improves product quality 
			www.solidworks.com</td>
		</tr>
	</tbody>
</table>

optimization of an air-based heat management system for dusty particulate matter-covered lithium-ion battery packs

This study aims to solve the problem of the cell temperature rise and performance decline caused by dusty particulate matter covering the surface of the cell through the allocation of airflow velocities at the inlets of the battery cooling box under the goal of low energy consumption. We take the maximum temperature of the battery pack at a specified airflow velocity and dust-free environment as the expected temperature in a dusty environment. The maximum temperature of the battery pack in a dusty environment is solved at different inlet airflow velocities, which are the boundary conditions of the analysis model constructed in the simulation software. The arrays representing the different airflow velocity combinations of inlets are generated randomly through the optimal Latin hypercube algorithm (OLHA), where the lower and upper limits of velocities corresponding to the temperatures above the desired temperature are set in the optimization software. We establish an approximate QRSM between the velocity combination and the maximum temperature using the fitting module of the optimization software. The QRSM is optimized based on the ASAM, and the optimal result is in good agreement with the analysis result obtained by the simulation software. After optimization, the flow rate of the middle inlet is changed from 5.5 m/s to 5 m/s, and the total airflow velocity is decreased by 3%. The protocol here presents an optimization method simultaneously considering energy consumption and thermal performance of the battery management system that has been established, and it can be widely used to improve the life cycle of the battery pack with minimum operating cost.

Author Spotlight: Optimization of Airflow Velocities in Battery Cooling Systems for Enhanced Thermal Performance and Reduced Energy Consumption 

Optimization of An Air-Based Heat Management System for Dusty Particulate Matter-Covered Lithium-Ion Battery Packs

This study aims to solve the problem of the cell temperature rise and the performance decline caused by the dusty particulate matter covering the surface of the cell through allocation of airflow velocities at the less of battery cooling box under the goal of low energy consumption. An optimization method simultaneously considering energy consumption and thermal performance of battery management system has been established. And it can be widely used to improve the lifecycle of the battery pack with minimum operating cost.

Following the protocol, the first three parts are the most important, which include modeling, meshing, and simulation, all in order to get the maximum temperature of the battery pack. Then, the airflow velocity is adjusted by sampling, and finally, the optimal flow rate combination is obtained by optimization.
Figure 9&#160;shows the comparison of battery pack temperature distribution in different e...

Watch this Scientific Journal Video about Optimization of Airflow Velocities in Battery Cooling Systems for Enhanced Thermal Performance and Reduced Energy Consumption at JoVE.com

Here, we present the adaptive simulated annealing method (ASAM) to optimize an approximate quadratic response surface model (QRSM) corresponding to a dusty particulate matter-covered battery heat management system and fulfill the temperature drops back by adjusting the airflow velocities combination of system inlets.

This study aims to solve the problem of the cell temperature rise and performance decline caused by dusty particulate matter covering the surface of the ...

optimization-an-air-based-heat-management-system-for-dusty

Research

JoVE Journal

Engineering

Simulation Analysis for Evaluating Temperature and Airflow Dynamics in Battery Packs 

To begin the fluid flow analysis, drag Fluid Flow from the toolbox and Analysis Systems into the project schematic zone. Then hold airFEM mesh, batteryFEM mesh, and dpmFEM mesh fluid flow with the left mouse button and move them to fluid flow setup. Right click on Fluid Flow, then set up and select Update to enter the Setup window.Confirm the validity of the FEM model and check if the mesh has a negative volume. Now, enter the setting interface of the Viscous model and the Radiation model and select the K-epsilon model and the Discrete Ordinates model respectively. Change the fluid type of the numbered battery domains to the solid type.Then on the Solid window, double click each battery domain to change the DPM material to the battery material. Subsequently, choose the source terms item and check the highlighted source terms to add an energy source by assigning the number and the number of energy sources and selecting constant type to input the source value. Change the fluid type of numbered DPM domains to solid type.Next, convert the type of all renamed surfaces, including the inner surfaces of the air domain, all sides of the battery domains, and DPM domains from the default wall to the interface. To generate mesh interfaces, click the Mesh Interfaces and enter the Create and Edit Mesh Interfaces Window. Match the cavity surfaces to all sides, except the upper sides of the battery domains and the lower sides of the DPM domains.Name and number them as interface1 to interface11 respectively. Then match the upper sides of the battery domains and the lower sides of the DPM domains. Name and number them as interface12 to interface22 respectively.To assign the outer border surface as the wall thermal boundary, set the heat transfer coefficient as five in the mixed thermal condition. Then change the material from default aluminum to the previously self-defined battery box material. In the Velocity Inlet window, set airflow velocities of all inlets to five meters per second.Then set the gauge pressure of the outlet to zero in the Pressure Outlet window. Next, set the state of the computing domain with an initial temperature of 300 kelvin and solution initialization type, best standard initialization. Set the number of iterations to 2000 and click Calculate to begin the simulation.To enter the CFD Post window, double click Fluid Flow followed by Results. Then from the toolbox, double click the icon of contour. In the location selector, choose all sides of the batteries and switch from pressure to temperature.Then click Apply to generate the temperature contour of the batteries. Click File, then Export. To select the temperature of the selected variables, then click the dropdown button of the locations to select the battery domains.Click OK followed by the Save button to quit. Battery pack temperature variation at different inlet airflow velocities demonstrated that the maximum battery pack temperature decreases with the increase of inlet airflow velocity. The comparison of the battery pack temperature distribution and the second battery temperature distribution in different environments showed that the temperature of the battery increases under dusty conditions due to the low thermal conductivity of DPM.

Optimization of Latin Hypercube Sampling and Adaptive Simulated Annealing for Temperature Control in Fluid Dynamics

Begin by opening an empty spreadsheet to create a table with rows named inlet1, inlet2, and inlet3 in the first column. Save the file as sampling.xlsx. Run the optimization software and drag the spreadsheet icon onto the single arrow of task one.Then double click the spreadsheet icon to open the Component Editor Excel window. Click the Browse button to import sampling.xlsx. Then click add this mapping to map inlet1, inlet2, and inlet3 to A1, A2, and A3 as parameters.Click OK to return to the initial window. Drag the DOE icon into task one and double click on it to open the Component Editor DOE window. Select Optimal Latin Hypercube.And in the general window, set the number of points to 15. Navigate to the factors window and set 5.5 as the upper limit and five as the lower limit for A1, A2, and A3.Switch to the design matrix window and click generate to produce random sampling points for different inlet velocities. Close the optimization software.Combine the predictor variables x1, x2, and x3 of the velocity arrays and y of the temperature arrays to form a new table. Save the table as sample. txt and import it to fit a response surface model.Rerun the optimization software and drag the approximation icon onto the single arrow of task one. Double click the task one icon to pop up the Component Editor Approximation window to select the response surface model. Navigate to the Data File window and import the sample.txt file containing the prediction variables. Switch to the Parameters window and click Scan to open the parameters in the data file window where the predictor variables of x1, x2, and x3 are defined as input and y as output. Next, go to the Technique Options window and select Quadratic in polynomial order.Switch to the Error Analysis Options window and select cross validation in the error analysis method. Then switch to the View Data window and click Initialize Now to obtain the coefficients of the quadratic linear regression equation, Click the Error Analysis button to open the Approximation Error Analysis window. Check if the errors, meet the acceptable standards for each error type.Close the Approximation Component window. Drag the optimization icon into task one and double click it to open the Component Editor Optimization window. Then select adaptive simulated annealing in the optimization technique.Navigate to the variables window and set 5.5 as the upper limit and five as the lower limit. Switch to the objectives window and select the y parameter before closing the Component Editor Optimization window. Finally, click the run optimization button and wait for the optimization results.Our square analysis showed that the second order polynomial response surface approximation model had a good fitting accuracy. The maximum temperature obtained through optimization was 309.39 kelvin with specific airflow velocities at the inlets. The optimized airflow velocities led to a lower maximum temperature of 309.39 kelvin as compared to the initial case.The sum of airflow velocities of the optimized case is less than the non-optimized cases. However, the maximum temperature does not increase with decreasing airflow velocity. Further, the flow line distribution after optimization becomes wider.Factor x1 has the greatest influence on temperature, while factors x2 and x3 have similar effects.