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Experimental study of a diffusion absorption refrigeration cycle supplied by the exhaust waste heat of a sedan car at low engine speeds

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Abstract

The wasted energy from a car exhaust can be considered as the heat supply for an absorption refrigeration cycle. In practice however, application of such cooling systems in automobiles has been facing a number of technical restrictions one of which is once the car engine runs idle or at low speed. To tackle this matter, the present experimental study has been carried out. A commercial diffusion absorption refrigerator with internal volume of 0.04 cubic meters (Electrolux 27A1) and the exhaust flow from a compact car engine (X100 KIA) are applied. Various engine speeds (1000–2500 rpm) have been tested. First, it was confirmed that the amount of heat transferred to the generator at low engine speeds was not adequate to obtain the low temperature required for the refrigerator compartment. A new generator was therefore designed and built. The experimental results show that by using the modified generator, the heat transfer to the generator improves by more than 19%. The evaporator and refrigerator compartment reached the desirable temperatures of −5.7 °C and 4.2 °C respectively at the engine speed of 2000 rpm. Further improvement of the results was observed at the engine speed of 1000 rpm where the temperatures at the evaporator and the refrigerator compartment were reduced by about 4 °C once the modified generator was applied.

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Abbreviations

\( {\dot{Q}}_{exh} \) :

Heat transfer rate from energy source [W]

\( {\dot{Q}}_{ref} \) :

Cooling capacity [W]

\( {\dot{Q}}_{wall} \) :

Heat transfer through the walls [W]

\( {\dot{Q}}_{ins} \) :

Heat loss through the insulated walls [W]

\( \dot{m} \) :

Mass flow rate [kg s−1]

\( \dot{V} \) :

Volumetric flow rate [m3 s−1]

\( \overline{R} \) :

Universal gas constant [8314 J kmol−1 K−1]

A :

Surface area [m2]

COP :

Coefficient of Performance

c :

Thermal capacity [J kg−1 K−1]

e :

Specific enthalpy [J kg−1]

h :

Heat transfer coefficient [W m−2 K−1]

k f :

Fluid thermal conductivity [W m−1 K−1]

L :

Characteristic length [m]

M air :

Dry air molecular weight [kg kmol−1]

m air :

Dry air mass [kg]

m :

Mass [kg]

P :

Absolute pressure [Pa]

P s :

Water vapor saturation pressure [Pa]

P v :

Water vapor partial pressure [Pa]

P air :

Air partial pressure [Pa]

Pr :

Prandtl number

Ra L :

Rayleigh number

T :

Temperature [K]

T f :

Film temperature [K]

U :

Internal energy [J]

u :

Specific internal energy [J kg−1]

u air :

Dry air specific internal energy [J kg−1]

u v :

Water vapor specific internal energy [J kg−1]

x :

Value of a property

y :

Mass fraction

∆t :

Time interval [s]

∆T :

Temperature difference [K]

ϕ :

Relative humidity [%]

ω :

Specific humidity

ρ :

Density [kg m−3]

ν:

Volume inside the refrigerator [m3]

air :

Air

av :

Average

amb :

Ambient

exh :

Exhaust

ex :

External

ev. body :

Evaporator body and fins

f :

Final

i :

Initial

in :

Internal

ins :

Insulation

inl :

Inlet

outl :

Outlet

sur :

Surface

sh :

Sheet metal of the wall

wall :

Wall

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Correspondence to Majid Bazargan.

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Highlights

• Exhaust waste heat of a car used to run a diffusion absorption refrigeration cycle.

• A new cycle generator designed and built to fit the low engine speed conditions.

• A minimum temperature of 4.2°C obtained at the refrigerator compartment.

• Cooling onset was preceded at low engine speeds by using the modified generator.

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Farzadi, R., Bazargan, M. Experimental study of a diffusion absorption refrigeration cycle supplied by the exhaust waste heat of a sedan car at low engine speeds. Heat Mass Transfer 56, 1353–1363 (2020). https://doi.org/10.1007/s00231-019-02793-w

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  • DOI: https://doi.org/10.1007/s00231-019-02793-w

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