Experimental investigation of heat transfer enhancement, thermal efficiency, and pressure drop in forced convection of magnetic hybrid nanofluid (Fe3O4/TiO2) under varied magnetic field strengths and waveforms

被引:1
|
作者
Adogbeji, Victor O. [1 ]
Sharifpur, Mohsen [1 ,2 ,3 ]
Meyer, Josua P. [1 ,4 ]
机构
[1] Univ Pretoria, Dept Mech & Aeronaut Engn, Private Bag X20, ZA-0028 Pretoria, South Africa
[2] Univ Witwatersrand, Sch Mech Ind & Aeronaut Engn, Private Bag 3, ZA-2050 Johannesburg, South Africa
[3] China Med Univ, China Med Univ Hosp, Dept Med Res, Taichung, Taiwan
[4] Stellenbosch Univ, Dept Mech & Mechatron Engn, Stellenbosch, South Africa
关键词
Varied magnetic field strengths; Waveforms; Hybrid nanofluid; Heat transfer; Convective flow; Thermal efficiency; Pressure drop; Frequency optimization; Nanoparticle concentration; Turbulent forced convection; FLOW; CONSTANT; WATER;
D O I
10.1016/j.csite.2024.105313
中图分类号
O414.1 [热力学];
学科分类号
摘要
Applying a magnetic field to influence convective flow of ferrofluids has become an efficient method for enhancing heat transfer in thermal systems, particularly in straight tubes. This study investigates the heat transfer properties of Fe3O4/TiO2 nanofluids within a heated copper tube under varied magnetic field strengths and waveforms. Optimal magnetic field conditions were determined at 4 V and 60 Hz across all waveform types, as higher frequencies and voltages increased magnetic field intensity, thereby reducing heat transfer rates. Magnetic waveforms exerted differential influences on pressure drop, indicating varied nanoparticle alignment and turbulence levels, impacting fluid flow dynamics and viscosity. Higher nanoparticle concentration (0.1% vol) correlated with increased pressure drops across sine, square, and triangular waveforms, suggesting heightened flow resistance and potential nanoparticle agglomeration, thus reducing thermal efficiency. Conversely, lower concentrations exhibited enhanced thermal performance due to improved nanoparticle dispersion and reduced thermal resistance. At 0.1% vol, heat transfer enhancement without a magnetic field was 16.5%. The introduction of magnetic field waveforms attenuated this enhancement: 15.3% (sine), 13.26% (square), and 12.59% (triangular). Conversely, at lower volume fractions, heat transfer enhancements with magnetic fields exceeded those without at 0.05% vol, enhancements were 20.92% (sine), 21.3% (square), and 21.34% (triangular); at 0.025% vol, enhancements were 22.07% (sine), 22.3% (square), and 21.32% (triangular); at 0.0125% vol, enhancements were 27.87% (sine), 28.21% (square), and 26.74% (triangular); and at 0.0065% vol, enhancements were 22.24% (sine), 22.3% (square), and 24.49% (triangular).
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页数:23
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