Keywords

1 Introduction

Nanofluids were first proposed as a revolutionary heat transfer medium by Choi et al. [1]. Nanofluids are created colloids of host fluids and nanoparticles. Researchers have recently considered using energy-efficient nanoparticles into lubricants and refrigerants. There are two categories of nanorefrigerants: direct refrigerants and lubricants-based refrigerants. Although in the latter, nanolubricants are combined with the refrigerants, the former directly disperses the required amount of small nanoparticles in the host refrigerant [2]. The thermophysical and heat transport capacities notably increase when nanoparticles are introduced to refrigerants, which increases efficiency and reliability [3, 4]. The scientific community on nanofluids has published very few experimental studies about the behaviour of boiling in nanorefrigerants [5]. Most research, many of which are also inconsistent [6], have demonstrated both advantages and disadvantages of flow boiling heat transfer [7]. The current study [8] employs an experimental methodology to investigate the effects of incorporating TiO2 nanoparticles into R134a refrigerant, with a focus on flow boiling regime studies.

2 Experimental Methodology

2.1 Flow Boiling Heat Transfer Studies on R134a/TiO2 Nanorefrigerant

To validate the experimental design, the estimated heat transfer coefficient for pure R134a from the literature is compared with the experimental value. Studies utilizing TiO2-nano refrigerant were the next to investigate the impact of nanoparticles on the heat transfer coefficient. It was decided to use particle concentrations of 0.1, 0.4, and 0.8 vol%. The effects of particle concentration, heat flow, mass flux, and vapour quality are investigated concerning the heat transfer coefficient (HTC).

2.1.1 Experimental Test Rig

ASTM D7863-17 standard is followed to conduct the convective heat transfer experiments [9]. Figure 1 shows the schematic diagram of the experimental set-up.

Fig. 1
A schematic diagram of set up of test section with the preheater and flow meter on one side and expansion device on other side. Lubricant charging line is connected to gas pump, refrigerant tank, and condenser.

Schematic diagram of the experimental set-up

The test evaporator is a horizontal copper tube that is smooth, 10.2 mm in diameter, and 1 m long. The refrigerant is cycled through using a gear pump, which also makes up for pressure loss. To guarantee sub-cooled liquid at the pump's inlet, the temperature of the condensing medium is controlled concerning the saturation temperature of the refrigerant matching the pressure. It is anticipated that there will be no heat loss and that the heat input into the test portion will remain constant. T-type thermocouples are used at six different points along the test section to measure the outer tube wall temperature with an accuracy of 0.50 °C. The heat transfer coefficients acquired from various sources are compared using the correlation for R134a given by Panek et al.

2.2 Performance Evaluation of Vapour Compression Refrigeration System (VCRS)

Experimental research has been done to explain how nanorefrigerant affects VCRS performance. For the performance tests, an in-house test rig is created. In the refrigerant compressor, tests are carried out using R134a+ pure PAG (poly alkylene glycol) lubricant and R134a+ TiO2-PAG nanolubricants. The experimental study's assumed particle concentration is 0.1 vol%. To establish repeatability, the experiments are repeated in identical environmental settings, and it is discovered that the results roughly match. For the purpose of calculating the performance characteristics, average values are used.

3 Results and Discussion

3.1 Flow Boiling Heat Transfer of R134a/PAG Oil and R134a/TiO2/PAG Oil

The heat transfer coefficients at various mass fluxes and volume fractions are compared in Fig. 2. It is evident that the flow boiling heat transfer properties are significantly influenced by the nanorefrigerant. The graph unequivocally demonstrates that, for all mass fluxes, the presence of nanoparticles in the refrigerant resulted in a higher heat transfer coefficient than the mixture of pure lubricant and refrigerant. The outcomes also demonstrate that the mass flux is accompanied by an increase in the heat transfer coefficient. The reasons for the rise in HTC are a change in flow regimes and higher liquid velocities at higher mass fluxes. The maximum HTC for nanolubricants is 196.13, 211.28, and 205.28 W/m2 K, respectively, for concentrations of 0.1, 0.4, and 0.8 vol%. With a volume fraction of 0.4%, nanolubricant exhibits the highest.

Fig. 2
Two plot graphs of comparison of heat transfer coefficient versus vapour quality for R 134 a with pure oil, and with T i O 2 nano lubricants of 3 different volume percentages.

Comparison of heat transfer coefficient versus vapour quality at a mass flux of 34 kg/m2 s, b mass flux of 47 kg/ms

3.2 Power Consumption and COP of the VCRS

With pure lubricant and nanolubricant, the hermetic refrigerant compressor's power consumption is assessed. The comparison of the power used by the refrigerant compressor and COP in both scenarios is shown in Fig. 3. By substituting nanolubricants for pure lubricant, the power used by the refrigerant compressor is decreased. TiO2 nanoparticles added to the lubricant have a notable impact on power usage. Compared with pure lubricant, there is an 8.33% decrease in power usage. The image makes it evident that adding nano-sized TiO2 particles to the refrigerant greatly increases the COP of the VCRS. In comparison with pure lubricant-refrigerant mixture nanorefrigerant, R134a-TiO2 exhibits a 19.4% increase in COP.

Fig. 3
Two vertical bar graphs of power consumption and C O P of R 134 a P A G and R 134 a T i O 2. Power consumption of R 134 a P A G is maximum, 0.5, and C O P of R 134 a T i O 2 is maximum, approx 1.8.

Comparison of power consumption and COP

4 Conclusions

The current study examines the usage of nanorefrigerant in a VCRS from the perspective of energy conservation, as well as the experimental determination of the flow boiling heat transfer parameters of R134a/TiO2. The main conclusions are that (i) the flow boiling heat transfer properties of R134a-TiO2 nanolubricant outperform those of pure refrigerant at all particle concentrations, and (ii) at a volume fraction of 0.4%, the greatest flow boiling heat transfer coefficient is observed. Also, the performance coefficient of the vapour compression refrigeration system is raised by 19.4%, while the power consumption of the hermetic reciprocating compressor is reduced by 8.33%. The use of a revolutionary nanolubricant could result in the creation of HVAC systems that use less energy.