See discussions, stats, and author profiles for this publication at: https://www.researchgate.net/publication/282604680 REFRIGERANT CHARGE AMOUNT IN HEAT PUMP SYSTEMS AND EVALUATING OPTIMAL AMOUNT OF GAS Conference Paper · September 2015 CITATIONS READS 0 7,354 4 authors, including: Faraz Afshari Nesrin Adıgüzel Erzurum Technical University Ataturk University 95 PUBLICATIONS 1,181 CITATIONS 12 PUBLICATIONS 69 CITATIONS SEE PROFILE All content following this page was uploaded by Faraz Afshari on 06 October 2015. The user has requested enhancement of the downloaded file. SEE PROFILE ULIBTK’15 20. Ulusal Isı Bilimi ve Tekniği Kongresi 02-5 Eylül 2015, BALIKESİR REFRIGERANT CHARGE AMOUNT IN HEAT PUMP SYSTEMS AND EVALUATING OPTIMAL AMOUNT OF GAS Faraz AFSHARĠ*, Ömer ÇOMAKLI**, Nesrin ADIGÜZEL***, ġendoğan KARAGÖZ**** * Atatürk Üniversitesi, Mühendislik Fakültesi, Makine Mühendisliği Bölümü faraz.afshari@atauni.edu.tr ** Atatürk Üniversitesi, Mühendislik Fakültesi, Makine Mühendisliği Bölümü ocomakli@atauni.edu.tr ***Kafkas Üniversitesi, Mühendislik Fakültesi, Makine Mühendisliği Bölümü nesrin_ozdemir25@yahoo.com **** Atatürk Üniversitesi, Mühendislik Fakültesi, Makine Mühendisliği Bölümü skaragoz@atauni.edu.tr Abstract: The refrigerant charge amount is one of very important factors in heat pumps and cooling systems that generally affect condensing pressure. Heating and cooling capacity of these systems could increase with gas charge amount. However, there is an ideal charge amount for the best coefficient of performance (COP). On the other side, compressor power varies with the refrigerant amount in a system. This study has focused on optimization of the charge amount in a heat pump using several refrigerant as R134a, R404a and R22, also stepwise gas rising have been observed in concerned outcomes as p-h, T-s and COP diagrams. Compressor consumption (w), coefficient of performance and condenser outlet heat (Qh) has been measured in different levels of gas amount. Keywords: Refrigerant gas, Heat pumps, Charge amount, COP, P-h and T-s diagrams. ISI POMPA SĠSTEMLERĠNDE SOĞUTUCU GAZIN ġARJ MĠKTARI VE GAZIN OPTĠMUM TUTARININ DEĞERLENDĠRMESĠ Özet: Isı pompası düşük sıcaklıktaki bir ortamda bulunan ekonomik değeri olmayan ısıyı, kullanılmak üzere daha yüksek sıcaklıktaki bir ortama pompalayan ve bu işi yapmak için pompalandığı ısıya daha az mekanik iş harcayan bir sistemdir. Soğutucu akışkan miktarı ısı pompalar ve soğutma sistemlerinde çok önemli faktörlerden biridir ve bu sistemlerin Isıtma ve soğutma kapasitesi gaz şarj miktarı ile artabilir, Ancak, performans katsayısı için (COP) ideal bir şarj miktarı bulunmalıdır. Sistemde kompresör gücü (w), alınan ve atılan ısı (Q h,L) soğutucu gaz miktarı ile değişmesi hesaplanmıştır. Bu çalışmada R134a, R404a ve R22 soğutucu gazları kullanarak şarj tutarının optimizasyonu araştırılmıştır. Ayrıca, gaz miktarının artışıyla pH, Ts ve COP diyagramları ve ilgili sonuçlar gözlemlenmiştir. Anahtar Kelimler: Isı pompası, Soğutucu gaz, Şarj miktarı, COP, P-h ve T-s. which has the maximum COP (coefficient of performance) value is water to air type with 3.94 and followed by water to water type with 3.73, air to air type with 3.54 and air to water type with 3.40. In order to investigate the performance of the solar-ground source heat pump system in the province of Erzurum having cold climate, an experimental set-up was constructed. In this study, the performance of the system was experimentally investigated. The experimentally obtained results are used to calculate the heat pump coefficient of performance (COP) and the system performance (COPS). The coefficient of performance of 1. introducion In recent years, the use of clean and renewable energy sources such as solar, wind, geothermal and biomass energy has received considerable attention for industrial and domestic applications (Çomaklı Ö., et al, 1996). Fast urbanization caused by industry revolution made to emerge the idea finding a remedy to human needs from a centre in addition to the social services like water supply, sewer system, public transportation and district heating system. In a study, results show that the heat pump unit 1 ULIBTK’15 20. Ulusal Isı Bilimi ve Tekniği Kongresi 02-5 Eylül 2015, BALIKESİR the heat pump and system were found to be in the range of 3.0-3.4 and 2.7-3.0, respectively. This study also shows that this system could be used for residential heating in the province of Erzurum being a cold climate region of Turkey (Çakır U., 2013, Bakirci K., et al, 2011). In some studies, the aim of the study is to select working fluids which have excellent performance and are environment friendly for moderately high temperature heat pump (Pan L., et al, 2011). A domestic heating system has been designed, constructed and tested. The evacuated tubular solar collector has been used to achieve higher collector efficiencies. The effects of evaporation temperature on the heating capacity and performance of the system have been investigated (Çağlar A, ve Yamalı C., 2012,). Thermal performance analysis of a direct expansion solar assisted heat pump was investigated by Kong X. and friends (Kong X., et al, 2011). Many studies aimed at minimizing the charge in a refrigerating machine were thus developed. On a global level, reduction of refrigerant charges must not affect energy aspects while respecting environmental constraints. Independently of the choice of refrigerant, environmental and or safety issues can be minimised by reducing the amount of refrigerant charge per heat pump or refrigeration system (Fernando P., et al, 2004, Choi H., et al, 2012). The system refrigerant charge are believed to have a great effect on the cycling thermal performance. In CO2 heat pump, the CO2 system shows a large variation of the performance according to refrigerant charge. In a study has been reported that, the performance of the CO2 heat pump was measured and analyzed by varying the refrigerant charge amount at standard cooling condition. In addition, the performance sensitivity of the CO2 system as a function of refrigerant charge was compared to those for the R22, R410A, and R407C systems (Zhang D., et al, 2014, Cho H., et al, 2005). The refrigerant charge amount is a key factor for heat pump system optimization, and normally determines the condensing pressure, which affects the subcooling at the exit of the condenser. Heating capacity increases as subcooling increases, however, there is an optimum charge amount for the best coefficient of performance (COP) (Corberan J., et al, 2008). Charge optimisation study of a propane heat pump, optimal refrigerant charge of a water-to-water heat pump, Refrigeration systems with minimum charge of refrigerant, analysis of gas mixtures are some the studies that show the importance of the charge amount in the heat pump system (Corberan J., et al, 2011, Kim D., et al, 2014, Çomaklı Ö., et al). aluminum fins air source evaporator, an expansion valve, and a water-cooled copper pipe body type condenser. The condenser and evaporator were used to transfer heat from the refrigerant to water and air to refrigerant respectively and so air was as a heat source and water was sink for the constructed heat pump. Temperatures in the test setup were monitored at the selected locations using T-types thermocouples, and refrigerant pressures were also measured in the locations as shown in figure. Compressor power consumption calculated by using voltage and amperage measured by a digital amperemeter. A volumetrical flow meter was set up to obtain flow rate of the condenser cooling water. all sensors was calibrated to decrease uncertainties during experimantal tests (Karagöz Ş., 2002).At first level 2000 gr refrigerant, and then in a 200-300 gr increments of the gas was added into the system to find out maximum COP respect to the gas amount. A total of 7 Tests performed in each stage (4 tests for different condenser water flow and 3 tests for different evaporator air temperature). Fig 1. Schematic diagram of the air-to-water heat pump experimental setup. Based on the tests, it was found that the full charge of R134a,R404a and R22 refrigerants for the heat pump unit was 5800 gr, 5200 gr, 6200 gr respectively. Heating capacity was calculated using condenser water flow rate and temperature difference between inlet and outlet. To confirm the calculation, the capacity was also determined by refrigerant flow rate and enthalpy difference between condenser inlet and outlet. 3. Results and discussion 2. Experimental setup and test procedure Fig. 2,3. shows the variations of the R134a refrigerant heating capacity and COP as a function of refrigerant charge at the four different water flow. Gas amount has increased from 2000 gr upto 7000 gr and in every stage water supply has been increased in four levels. For overcharged conditions, the COP was reduced due to a decrease of the temperature difference between the refrigerant and the water and compressor power consumption with increasing gas amount. For designed heat pump was to measure the performance and effeciency of AWHP system to investigate different types of refrigerants under various operating conditions. Fig. 1 is shown a schematic of the heat pump unit have been use in this experimental study. In the system several fluids were used including R134a, R404a and R22. As shown in the figure, designed heat pump consists of a reciprocating compressor, copper pipe with 2 ULIBTK’15 20. Ulusal Isı Bilimi ve Tekniği Kongresi 02-5 Eylül 2015, BALIKESİR undercharge conditions, the capacity dropped due to a reduction of refrigerant flow rate and compressor efficiency. 3 7000 6000 2,5 5000 2 2000 gram 2000 gram Qh (watt) 3000 COP 3400 1,5 3800 4200 3000 4000 3400 3800 3000 4200 4600 4600 5000 1 5000 2000 5400 5400 5800 5800 6100 0,5 6100 1000 6400 6400 0 0 water flow rate kg/s water flow rate kg/s Fig 2. The effect of the refrigerant charge and water flow rate Fig 3. The effect of the refrigerant charge and water flow rate on the COP. on the heating capacity. 3 2,5 COP 2 0,049281 kg/s 1,5 0,065708 kg/s 1 0,09857 kg/s 0,131433 kg/s 0,5 0 2000 2500 3000 3400 3800 4200 4600 5000 5400 5800 6400 7000 Gas amount (gr) Fig 4. COP increasing due to gas amount in different water flow rate for 134a refrigerant. flow rate for 134a refrigerant. 3 3 7000 2,5 6000 5000 COP 2 4000 1,5 3000 1 2000 0,5 Qh - Compressor power (watt) ULIBTK’15 20. Ulusal Isı Bilimi ve Tekniği Kongresi 02-5 Eylül 2015, BALIKESİR 1000 0 0 1800 2800 3800 4800 5800 6800 Gas amount (gr) cop compressor consumption kompresör güçpower masrafı Qh (ısıtma kapasitesi) Fig 5. Heating capacity, compressor power and COP diagram for increasing R134a refrigerant flow rate for 134a refrigerant. 3 2,5 COP 2 1,5 COP R134a COP R404a COP R22 1 0,5 0 2000 2400 2800 3200 3600 4000 4400 4800 5200 5600 6000 6400 6800 7200 gas amount (gr) Fig 6. COP increasing due to gas amount for three different gases in 0,131433 kg/s water flow rate 4 7600 ULIBTK’15 20. Ulusal Isı Bilimi ve Tekniği Kongresi 02-5 Eylül 2015, BALIKESİR 8000 7000 Qh (watt) 6000 5000 4000 R134 3000 R404 2000 R22 1000 0 2000 3000 4000 5000 6000 7000 8000 gas amount (gr) Fig 7. heating capacity increasing due to gas amount for three different gases in 0,131433 kg/s water flow rate It was presented that compressor worked in very different condition for various refrigerants and charge levels. input and discharge pressures and temperatures was compared and it was revealed that R22 caused higher temperature than others in the discharge line. On the other hand R404a preduced most pressure between gasses in the output of the compressor. Fig. 8 and 9 are shown differences between input and output temperature and pressure respect to the gas charge amount in constant test condition. (ΔT and ΔP are differences between compressor inlet and discharge temperatures and pressures.) as shown in the fig. 8, R22 resulted more temperature difference following by R404a and R134a. in the other diagram R404a revealed more pressure change inside Compressor compartment which is related to the properties of refrigerant such as specific volume, liquid density and vaporization latent heat. 1000 900 R134a 800 R404a ΔP (kpa) 700 R22 600 500 400 300 200 100 0 2000 3000 4000 5000 6000 7000 gas amount (gr) Fig 9. Pressure difference between compressor input and discharge line for three gases with increasing charge amount 100 R134a 90 R404a 80 R22 ΔT °C 70 60 50 40 30 20 10 2000 3000 4000 5000 6000 7000 gas amount (gr) Fig.8. Temperature difference between compressor input and discharge line for three gases with increasing charge amount 5 ULIBTK’15 20. Ulusal Isı Bilimi ve Tekniği Kongresi 02-5 Eylül 2015, BALIKESİR Fig 10. Heat pump cycle in Enthalpy-Pressure diagram for three gases when charge quantity is 5400 gr (water flow rate was constant equal to 0,131433 kg/s). 4. Conclusions References The amount of refrigerant gas in the heat pump unit is very important parameter influencing system performance. In this study the experiments were conducted by varying refrigerant charge amount and effect of the water flow rate and evaporator air temperature on the system capacity. Undercharge or overcharge of refrigerant decrease performance and deteriorated system reliability. The COP quantity improved significantly with the rise of refrigerant charge up to optimal charge, but it slowly decreased as the refrigerant charge increased beyond optimal charge. In this study, every three gases have different COP in every stage. Also R22 refrigerant has more heating capacity than two others. Compressor in the heat pump unit worked in different conditions due to several parameters, the refrigerant charge and gas type is two important parameters that cause to change in inlet and discharge temperature and pressure. Bakirci K., Et al, 2011, Energy Analysis of a SolarGround Source Heat Pump System with Vertical ClosedLoop for Heating Applications, Int. J. Energy, 36, 3224 3232 Björk E, and Palm B., 2006, Refrigerant Mass Charge Distribution in a Domestic Refrigerator. Part I: Transient Conditions, Int. J. Applied Thermal Engineering, 26, 829 – 837 Cho H., Et al, 2005, Effects of Refrigerant Charge Amount on the Performance of a Transcritical CO2 Heat Pump, Int. J. Refrigeration, 28, 1266 - 1273 Choi H., Et al, 2012, Refrigerant Amount Detection Algorithm for a Ground Source Heat Pump Unit, Int. J. Renewable Energy, 42, 111-117 Choia j, and Kim Y., 2004, Influence of the Expansion Device on the Performance of a Heat Pump Using R407C under a Range of Charging Conditions, Int. J. 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