INTERNATIONAL JOURNAL OF LATEST TECHNOLOGY IN ENGINEERING,  
MANAGEMENT & APPLIED SCIENCE (IJLTEMAS)  
ISSN 2278-2540 | DOI: 10.51583/IJLTEMAS | Volume XV, Issue I, January 2026  
Numerical and Experimental Analysis of ThermalHydraulic  
Behavior in Heat Pipe Systems  
1 Sandeep Yadav, 1 Sharad Kumar, 1 Ashutosh Singh, 1 Sushil Kumar Jha, 1 Rahul Bhatnagar, 2 Vikas  
Sharma  
1 School of Engineering & Technology, Shri Venkateshwara University, Gajraula, U.P.  
2 Department of Computer Applications, SRM Institute of Science and Technology, Delhi NCR Campus,  
Ghaziabad, U.P. India  
Received: 10 January 2026; Accepted: 19 January 2026; Published: 23 January 2026  
ABSTRACT  
Heat pipes are highly efficient passive thermal management devices widely used in electronics cooling, energy  
systems, and aerospace applications due to their excellent heat transfer capability. This paper presents a  
comprehensive numerical and experimental investigation of the thermalhydraulic behavior of a heat pipe  
system under varying heat input and operating conditions. A detailed numerical model is developed to simulate  
heat transfer, fluid flow, phase change, and pressure distribution within the evaporator, adiabatic, and condenser  
sections. The numerical results are validated through controlled experimental testing, focusing on temperature  
distribution, thermal resistance, heat transfer coefficient, and working fluid dynamics. The comparative analysis  
demonstrates good agreement between numerical predictions and experimental observations, confirming the  
accuracy of the proposed model. The results reveal the influence of heat input, working fluid behavior, and wick  
structure on overall thermal performance and hydraulic stability. The findings provide valuable insights for  
optimizing heat pipe design and enhancing their reliability and efficiency in advanced thermal management  
applications.  
KeywordsHeat pipe, Thermalhydraulic behavior, Numerical simulation, Experimental analysis, Two-phase  
flow, Thermal performance, Heat transfer.  
INTRODUCTION  
Efficient thermal management has become a critical requirement in modern engineering systems due to the  
continuous increase in power density and miniaturization of components in electronics, energy systems,  
aerospace, and automotive applications. Excessive heat generation, if not effectively dissipated, can lead to  
performance degradation, reduced reliability, and premature failure of system components. Conventional  
cooling techniques such as forced air cooling and liquid cooling often face limitations related to size, energy  
consumption, and complexity. In this context, heat pipes have emerged as highly effective passive thermal  
control devices, offering superior heat transfer performance with minimal temperature gradients and no external  
power requirement. A heat pipe is a sealed device that operates on the principle of phase change and capillary-  
driven fluid circulation. It typically consists of an evaporator section, an adiabatic section, and a condenser  
section, along with a wick structure and a working fluid. When heat is applied to the evaporator, the working  
fluid absorbs latent heat and vaporizes. The generated vapor travels to the condenser section due to the pressure  
difference, where it releases heat and condenses back into liquid form. The condensed liquid is then transported  
back to the evaporator through the wick structure via capillary action, completing a continuous and efficient heat  
transfer cycle. This unique thermalhydraulic mechanism allows heat pipes to achieve extremely high effective  
thermal conductivity compared to conventional solid conductors. The performance of a heat pipe is strongly  
influenced by its thermalhydraulic behavior, which involves complex interactions between heat transfer, fluid  
flow, phase change, and pressure distribution within the system. Parameters such as heat input, working fluid  
properties, wick structure, filling ratio, and operating orientation significantly affect the temperature distribution,  
thermal resistance, and overall stability of the heat pipe. At higher heat loads, limitations such as capillary limit,  
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MANAGEMENT & APPLIED SCIENCE (IJLTEMAS)  
ISSN 2278-2540 | DOI: 10.51583/IJLTEMAS | Volume XV, Issue I, January 2026  
boiling limit, entrainment limit, and sonic limit may arise, leading to performance deterioration or operational  
failure. Therefore, a thorough understanding of the coupled thermal and hydraulic phenomena is essential for  
accurate performance prediction and reliable heat pipe design.  
Experimental investigations have traditionally played a vital role in evaluating heat pipe performance by  
providing direct measurements of temperature profiles, heat transfer rates, and thermal resistance under various  
operating conditions. However, experimental studies alone can be time-consuming, costly, and limited in their  
ability to capture detailed internal flow and phase-change characteristics. Moreover, it is often challenging to  
visualize and quantify vaporliquid interactions and pressure variations within the sealed structure of a heat pipe  
using experimental methods alone. In recent years, numerical modeling and computational approaches have  
gained significant attention as powerful tools for analyzing the internal thermalhydraulic behavior of heat pipes.  
Numerical simulations enable detailed investigation of temperature fields, fluid velocity, pressure distribution,  
and phase change processes that are difficult to measure experimentally. Models based on computational fluid  
dynamics (CFD), volume-of-fluid (VOF) methods, and porous media approaches have been employed to predict  
heat pipe performance under different design and operating conditions. Despite these advances, numerical  
models often rely on simplifying assumptions and require experimental validation to ensure accuracy and  
practical applicability. A combined numerical and experimental approach is therefore essential to achieve a  
comprehensive understanding of heat pipe behavior. By integrating experimental data with validated numerical  
models, it becomes possible to accurately predict thermal performance, identify limiting factors, and optimize  
design parameters. Such an approach not only enhances confidence in simulation results but also reduces the  
need for extensive experimental trials during the design and development process. In this study, a detailed  
numerical and experimental analysis of the thermalhydraulic behavior of a heat pipe system is presented. The  
numerical model is developed to simulate heat transfer, fluid flow, and phase change within the heat pipe, while  
experimental investigations are conducted to measure temperature distribution and thermal performance under  
varying heat inputs. The agreement between numerical and experimental results is analyzed to validate the model  
and assess its predictive capability. The outcomes of this work provide valuable insights into the governing  
thermalhydraulic mechanisms and contribute to the development of efficient and reliable heat pipe systems for  
advanced thermal management applications.  
LITERATURE REVIEW  
Heat pipes have been extensively investigated over the past few decades due to their high thermal efficiency and  
wide applicability in thermal management systems. Early experimental studies focused on understanding the  
fundamental operational characteristics and orientation effects of heat pipes. Cerza and Boughey [1] examined  
the influence of air infiltration on large flat heat pipes under horizontal and vertical orientations and demonstrated  
that non-condensable gases significantly degrade thermal performance. Wang and Vafai [2] carried out  
experimental investigations on the transient behavior of flat plate heat pipes during start-up and shutdown,  
highlighting the importance of transient thermalhydraulic effects in practical applications. With growing interest  
in enhancing heat transport capability, researchers explored advanced heat pipe configurations and working fluids.  
Ma et al. [3] experimentally investigated nanofluid-based oscillating heat pipes and reported a substantial  
improvement in heat transport capacity due to enhanced thermal properties of nanofluids. Similarly, Cai et al. [4]  
analysed the operating characteristics of pulsating heat pipes and identified flow oscillation patterns as a key  
factor influencing thermal performance. Singh et al. [5] proposed a novel miniature loop heat pipe evaporator  
design for electronic cooling, demonstrating improved heat dissipation in compact systems. Several studies have  
emphasized transient and micro-scale heat pipe behavior. Suman and Hoda [6] conducted a transient analysis of  
V-shaped micro-grooved heat pipes, revealing the effects of groove geometry on temperature response and  
stability. Bonadies et al. [7] extended the application of phase-change systems to thermal storage optimization,  
reinforcing the relevance of heat pipes in energy-efficient thermal management. Ouchi et al. [8] further  
demonstrated the application of advanced thermal management systems, including heat pipes, for data center  
cooling to address increasing thermal loads. Visualization and detailed flow analysis have also been explored to  
better understand internal thermalhydraulic mechanisms. Wilson et al. [9] conducted thermal and visual  
observations of oscillating heat pipes using different working fluids, providing valuable insights into two-phase  
flow behavior. Modeling and validation studies, such as those by Wits and Kok [10], emphasized the importance  
of accurate numerical models for predicting heat transfer performance in electronic assemblies. Ting and Chen  
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[11] developed a coaxial dual-pipe heat pipe configuration and demonstrated its effectiveness in heat pipe coolers.  
The robustness of heat pipes under extreme operating conditions has also been investigated. Thompson et al. [12]  
evaluated flat-plate oscillating heat pipes under high-gravity loading and confirmed their stable thermal  
performance. Hung and Tio [13] focused on micro heat pipes and highlighted the role of phase-change interfacial  
resistance in determining overall thermal behavior. Xian et al. [14] compared different working fluids in  
oscillating heat pipes and concluded that fluid selection plays a crucial role in heat transfer efficiency. The use of  
nanofluids to enhance heat pipe performance has been widely reported. Asirvatham et al. [15] studied the  
operational limitations of heat pipes using silverwater nanofluids and identified key performance constraints at  
higher heat loads. Brahim and Jemni [16] investigated the effect of the adiabatic region length and demonstrated  
its influence on temperature uniformity and thermal resistance. Computational studies by Nithyanandam and  
Pitchumani [17] further highlighted the potential of combining heat pipes with metal foams for enhanced latent  
thermal energy storage. Application-oriented studies have demonstrated the versatility of heat pipes in real-world  
systems. Wang [18] investigated L-type heat pipes for electronic cooling, while Teng et al. [19] reported improved  
thermal efficiency using alumina nanofluids. Joung et al. [20] experimentally studied flat bifacial evaporators,  
and Liang and Hung [21] optimized heat sink performance using U-shaped heat pipes. Miniature heat pipes for  
compressor cooling [22] and CPU thermal management [23] further underscored their industrial relevance.  
Finally, the effects of inclination angle and alternative working fluids have been explored in pulsating heat pipes.  
Xue and Qu [24] analysed ammonia-based pulsating heat pipes under different inclinations, while Verma et al.  
[25] studied methanol and deionized water-based systems, confirming that orientation and fluid selection  
significantly affect thermal performance. Although extensive research exists on experimental characterization,  
advanced designs, and numerical modeling of heat pipes, limited studies present a tightly coupled numerical–  
experimental analysis focusing specifically on detailed thermalhydraulic behavior and model validation under  
varying heat inputs.  
PROPOSED METHODOLOGY  
The proposed methodology adopts an integrated numerical and experimental framework to systematically  
investigate the thermalhydraulic behavior of the heat pipe system. The approach is designed to capture the  
coupled effects of heat transfer, fluid flow, and phase change while ensuring validation of numerical predictions  
through experimental observations. The overall methodology is divided into heat pipe design and preparation,  
numerical modeling, experimental investigation, and result validation and analysis.  
1. Heat Pipe Design and Working Conditions: A cylindrical heat pipe is selected for the present study,  
consisting of evaporator, adiabatic, and condenser sections. The heat pipe is fabricated using a high-thermal-  
conductivity metallic casing, and a capillary wick structure is incorporated along the inner wall to facilitate liquid  
return from the condenser to the evaporator. A suitable working fluid is chosen based on its operating  
temperature range, latent heat, and compatibility with the casing material. The filling ratio is maintained at an  
optimal level to ensure stable operation. The heat pipe is tested under different heat input conditions to evaluate  
its thermalhydraulic response over a wide operating range.  
2. Numerical Modeling and Simulation: A detailed numerical model of the heat pipe is developed using a  
computational fluid dynamics (CFD) approach. The model incorporates conjugate heat transfer between the solid  
wall and the internal two-phase working fluid. The vapor core is modelled as a compressible flow region, while  
the wick structure is treated as a porous medium to account for capillary-driven liquid transport. Governing  
equations for mass, momentum, and energy conservation are solved along with appropriate phase-change models  
to simulate evaporation and condensation processes. Boundary conditions are defined by applying a uniform  
heat flux at the evaporator section and a constant temperature or convective heat transfer condition at the  
condenser section. The adiabatic section is thermally insulated to minimize heat loss. Temperature-dependent  
thermophysical properties of the working fluid are incorporated to improve model accuracy. Grid independence  
and time-step sensitivity analyses are performed to ensure numerical stability and convergence of the solution.  
The simulation outputs include temperature distribution, pressure variation, vapor velocity, and liquid saturation  
within the wick structure. In addition to steady-state analysis, the numerical model can be extended to transient  
simulations to capture time-dependent temperature responses during start-up and changes in heat input. Transient  
analysis enables prediction of temperature overshoot, thermal response time, and dynamic stability of the heat  
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pipe system. Such modeling is particularly important for applications involving fluctuating heat loads, where  
steady-state assumptions may not adequately represent real operating conditions.  
3. Experimental Setup and Procedure: An experimental test rig is developed to evaluate the thermal  
performance of the heat pipe under controlled conditions. Electrical heaters are used to supply a known and  
adjustable heat input to the evaporator section, while the condenser section is cooled using a water or air-based  
cooling arrangement. High-precision thermocouples are mounted along the length of the heat pipe to measure  
axial temperature distribution at steady-state conditions. A data acquisition system is employed to record  
temperature and power input data in real time. The experiments are conducted for multiple heat input levels to  
analyze the thermalhydraulic behavior under low, moderate, and high heat flux conditions. Steady-state is  
assumed when temperature variations remain within a predefined tolerance over time. The thermal resistance of  
the heat pipe is calculated using measured temperature differences and applied heat input, providing a  
quantitative measure of performance.  
4. Validation and Performance Analysis: The numerical results are validated by comparing predicted  
temperature profiles and thermal resistance values with corresponding experimental data. The degree of  
agreement between simulation and experiment is assessed to evaluate the reliability of the numerical model.  
Parametric analysis is carried out to study the influence of heat input on temperature distribution, pressure drop,  
and overall thermal performance. The combined numericalexperimental methodology enables identification of  
dominant thermalhydraulic mechanisms and operational limits of the heat pipe.  
This structured methodology ensures a comprehensive and reliable assessment of heat pipe performance and  
provides a robust framework for design optimization and future research in advanced thermal management  
systems.  
RESULT & ANALYSIS  
This section presents the numerical and experimental results obtained from the thermalhydraulic analysis of  
the heat pipe system. The performance is evaluated in terms of temperature distribution, thermal resistance, and  
agreement between numerical predictions and experimental measurements under varying heat input conditions.  
The wick structure strongly influences capillary pumping capability and hydraulic resistance within the heat  
pipe. Advanced wick configurations such as sintered powder wicks and micro-grooved structures offer higher  
capillary pressure and improved liquid distribution compared to conventional wick designs. Incorporating these  
advanced wick structures into the numerical model would allow comprehensive optimization of thermal  
performance, particularly under high heat flux conditions where capillary limitations dominate.  
1. Temperature Distribution along the Heat Pipe: The axial temperature distribution of the heat pipe was  
measured experimentally and compared with numerical simulation results for different heat inputs.  
Thermocouples were placed at the evaporator, adiabatic, and condenser sections to capture steady-state  
temperatures. The experimental temperatures at different axial locations (evaporator, adiabatic, and condenser  
sections) are measured using calibrated thermocouples of equation (1):  
1
=
∑ 푇 − − − − − (1)  
section, exp  
=1  
where:  
= temperature recorded by the 푡ℎ thermocouple  
= number of thermocouples in the respective section  
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Axial temperature distribution at different heat inputs (Experimental vs Numerical)  
Heat Input  
(W)  
Evaporator Temp.  
(°C) Exp.  
Evaporator Temp.  
(°C) Num.  
Adiabatic Temp.  
(°C) Exp.  
Condenser Temp.  
(°C) Exp.  
50  
48.6  
47.9  
61.2  
74.6  
89.8  
44.2  
39.8  
49.5  
58.3  
66.9  
100  
150  
200  
62.4  
76.1  
91.7  
56.8  
68.9  
81.4  
The results indicate a gradual increase in temperature along the evaporator section with increasing heat input,  
while the condenser section maintains relatively lower temperatures due to effective heat rejection. Numerical  
predictions closely follow the experimental trends, with a maximum deviation of less than 3%, confirming the  
accuracy of the proposed numerical model.  
Variation of Axial Temperature Profiles with Increasing Heat Input  
Fig. 1. illustrates the variation of axial temperatures in a heat pipe as a function of applied heat input ranging  
from 50 W to 200 W. Four curves represent experimental evaporator temperature, numerical evaporator  
temperature, experimental adiabatic temperature, and experimental condenser temperature. All temperature  
profiles show a monotonic increase with increasing heat input, with experimental and numerical evaporator  
temperatures closely matching across the entire range.  
2. Thermal Resistance Analysis: Thermal resistance is a key parameter used to quantify the heat pipe’s  
performance and is defined as the ratio of the temperature difference between the evaporator and condenser to  
the applied heat input. The temperature difference across the heat pipe is calculated by equation (2):  
Δ푇 = 푇  
evap  
− 푇 − − − −(2)  
cond  
where:  
= average evaporator temperature (°C)  
= average condenser temperature (°C)  
evap  
cond  
The overall thermal resistance th is defined as equation (3):  
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Δ푇  
th =  
− − − − − (3)  
where:  
Δ푇 = temperature difference between evaporator and condenser (°C)  
= applied heat input (W)  
Thermal resistance variation with heat input  
Heat Input (W)  
ΔT (Evap.–Cond.) (°C)  
Thermal Resistance (°C/W)  
50  
8.8  
0.176  
0.129  
0.119  
0.124  
100  
150  
200  
12.9  
17.8  
24.8  
The thermal resistance decreases significantly as heat input increases from 50 W to 150 W, indicating improved  
phase-change heat transfer and enhanced vaporliquid circulation. A slight increase in thermal resistance at  
higher heat input (200 W) suggests the onset of capillary or boiling limitations, which restrict further  
performance improvement.  
Influence of Heat Input on Overall Thermal Resistance of the Heat Pipe  
Fig. 2. shows the variation of overall thermal resistance of a heat pipe with increasing heat input from 50 W to  
200 W. Thermal resistance initially decreases sharply as heat input increases from 50 W to 150 W, indicating  
improved heat transfer performance, and then shows a slight increase at 200 W, suggesting the onset of thermal  
limitations at higher heat loads.  
3. Numerical Analysis of ThermalHydraulic Behavior: Numerical simulations provide detailed insight into  
internal thermalhydraulic characteristics that are difficult to measure experimentally. The pressure distribution  
within the vapor core shows a gradual pressure drop from the evaporator to the condenser, driving vapor flow.  
Liquid saturation in the wick structure remains high in the condenser region, ensuring sufficient capillary return  
to the evaporator. The maximum vapor velocity inside the vapor core is estimated using the mass conservation  
relation (4):  
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ꢂ  
̇
max  
=
− − − − − −(4)  
ꢂ  
where:  
ꢂ  
= vapor density (kg/m³)  
= vapor core cross-sectional area (m²)  
̇
= vapor mass flow rate (kg/s)  
The pressure drops along the vapor flow direction is calculated using the one-dimensional momentum equation  
(5):  
퐿 휌2  
Δ푃 = 푓  
− − − − − (5)  
ℎ  
2
where:  
= friction factor  
= effective vapor flow length (m)  
= hydraulic diameter of vapor core (m)  
= vapor velocity (m/s)  
The wick liquid saturation represents the fraction of pore volume occupied by liquid using equation (6):  
=  
× 100 − − − − − − − (6)  
where:  
= liquid volume in wick pores  
= total pore volume of the wick  
Numerical results of internal flow parameters  
Max Vapor Velocity  
Wick Liquid Saturation  
(%)  
Heat Input (W)  
(m/s)  
Pressure Drop (Pa)  
50  
2.1  
3.8  
5.4  
6.9  
320  
610  
980  
1380  
94  
100  
150  
200  
91  
88  
84  
As heat input increases, vapor velocity and pressure drop increase significantly, enhancing heat transport but  
also increasing hydraulic resistance. A reduction in wick liquid saturation at higher heat loads indicates increased  
liquid evaporation, which may lead to capillary limitations if the heat input is further increased.  
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Effect of Heat Input on Internal VaporLiquid Flow Characteristics  
Fig. 3. presents the variation of internal flow parameters of a heat pipe with increasing heat input from 50 W to  
200 W. The maximum vapor velocity and pressure drop increase steadily with heat input, while wick liquid  
saturation decreases progressively, indicating enhanced vapor transport and reduced liquid availability at higher  
heat loads.  
4. Comparison between Numerical and Experimental Results: To quantify the agreement between numerical  
and experimental results, the percentage deviation in evaporator temperature was calculated.  
Percentage deviation between numerical and experimental results  
Exp. Evap. Temp.  
(°C)  
Num. Evap. Temp.  
(°C)  
Heat Input (W)  
Deviation (%)  
50  
48.6  
47.9  
61.2  
74.6  
89.8  
1.44  
1.92  
1.97  
2.07  
100  
150  
200  
62.4  
76.1  
91.7  
The low deviation values demonstrate strong agreement between numerical and experimental outcomes,  
validating the robustness of the proposed numerical methodology.  
5. Effect of Inclination Angle on ThermalHydraulic Performance: The inclination angle of a heat pipe plays  
a significant role in determining its thermalhydraulic behavior, as gravity directly influences liquid return  
through the wick structure. At favorable inclination angles, gravitational forces assist capillary action, enhancing  
liquid return to the evaporator and improving overall thermal stability. Conversely, adverse orientations increase  
the capillary pumping requirement, potentially leading to dry-out and increased thermal resistance. Although the  
present study focuses on horizontal operation, the validated numerical framework can be readily extended to  
investigate different inclination angles. Incorporating gravitational effects into the momentum and capillary  
pressure balance would provide deeper insight into heat pipe performance under practical installation conditions,  
particularly in aerospace and electronics cooling applications.  
The combined results confirm that the heat pipe exhibits excellent thermal performance within the investigated  
heat input range. The reduction in thermal resistance with increasing heat input highlights the dominance of  
latent heat transfer during stable operation. However, numerical analysis indicates that at higher heat loads,  
increased pressure drop and reduced wick saturation may lead to thermalhydraulic limitations. The validated  
numerical model therefore serves as a reliable tool for predicting performance limits and optimizing heat pipe  
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design parameters.  
CONCLUSION  
This paper presented a comprehensive numerical and experimental investigation of the thermalhydraulic  
behavior of a heat pipe system under varying heat input conditions. The results demonstrated that heat pipes  
offer highly efficient and stable thermal performance, with a significant reduction in thermal resistance as heat  
input increases due to enhanced phase-change heat transfer. A close agreement between numerical predictions  
and experimental measurements validated the accuracy and reliability of the developed numerical model. The  
study also revealed that at higher heat loads, increased vapor velocity, pressure drop, and reduced wick liquid  
saturation may lead to thermalhydraulic limitations, indicating the onset of performance constraints. The  
validated methodology provides a robust framework for analyzing and optimizing heat pipe designs. Future work  
may focus on investigating advanced wick structures, alternative working fluids, and nano-enhanced fluids, as  
well as extending the model to transient conditions, different orientations, and high-heat-flux applications to  
further enhance the performance and applicability of heat pipe systems in next-generation thermal management  
technologies. The performance of heat pipes can be further enhanced by employing nano-enhanced working  
fluids. Nanofluids exhibit improved thermal conductivity and modified boiling characteristics, which can  
enhance heat transfer in the evaporator section. Integrating nano-enhanced fluids into the present numerical  
framework would demonstrate the versatility of the model for modern high-heat-flux applications such as data  
centers, power electronics, and aerospace thermal systems. However, potential challenges related to particle  
agglomeration and long-term stability must also be carefully considered. The proposed model is adaptable to  
different working fluids, wick structures, and operating orientations, making it suitable for next-generation  
thermal management applications.  
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