ABSTRACT:The paper deals with the analysis of the impact of inlet air temperature on the exergy efficiency and exergy of the losing heat flow and determination of the relation between the exergy and thermal efficiency in an exchanger consisting of gravity heat pipes. The assessment of heat processes quality and transformation of energy in the exchanger are also dealt with. a theoretical study (ABTAHI et al. 1988) on the basis of the standard balance of energy flows between the cooled and heated air currents, the coat and working medium of the tube.
KeywordsThe purpose of this paper is to analyze the impact of the inlet air temperatures on exergy efficiency values, exergy values of heat flows and to determine the relation between the exergy efficiency and thermal efficiency in a heat pipe heat exchanger. The paper also deals with evaluating the quality of thermal processes and exergy transformation in the heat exchanger.
METHOD Theoretical analysisThe exergy of the mass flow of 1 kg of gas during its passage through an open thermodynamic system can be determined from the following adiabatic (isoentropic) and isothermal expansion illustrated in Fig. 1.Gas expands from the initial state determined by the pressure p 1 and temperature T 1 to the state of the surrounding environment determined by the pressure p 0 and temperature T 0 . In the case of an adiabatic expansion, the temperature drops to T 2 = T 0 and the pressure p 2 > p 0 is reached. During the subsequent reversible isothermal expansion with a simultaneous heating, the gas pressure drops to p 3 = p 0 .In this case, the maximally utilizable energy (exergy) is equal to the technical work a t1.3 carried out between the initial and final states. The first law of thermodynamics implies that:where: da t -change in specific technical work (J/kg), dq -specific transferred heat (J/kg), dh -change in specific enthalpy (J/kg).Integrating equation (1), we obtain the following result:As 1-2 is dq = 0 in adiabatic expansion, the following applies to transferred heat:Substituting the figure in equation (2), we obtain the following result:This maximum technical work a t1,3 corresponding to the reversible process between the gas state determined by h 1 = h and s 1 = s and the state of the environment determined by h 3 = h 0 and s 3 = s 0 represents the maximum work content of the substance, i.e. exergy e x :The non-utilized specific energy, i.e. anergy a n , is h 0 at T 0 and shared heat at T 0 :According to equation (5), the change in the specific exergy of a heat flow during any process is as follows:In the event of an isobaric heat transfer, the specific enthalpy change dh is equal to the transferred heat dq. The specific entropy change is ds = dq/T in case of a reversible process. The above-mentioned facts indicate that equation (7) can be put as follows:T T Equation (6) can be put as follows:When heat is transferred between cooled air i and heated air e, heat flow dQ transmits exergy flow dE i (10) according to equation (8). Heated air e, however, receives only the ex...