PERFORMANCE MONITORING OF A HIGH-TEMPERATURE AIR-TO-WATER HEAT PUMP WITH INJECTION CYCLE INSTALLED IN A LOW-INSULATED SINGLE-FAMILY HOUSE IN BELGIUM

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Numbers of Abstract/Session (given by NOC) - 1 - PERFORMANCE MONIORING OF A HIGH-EMPERAURE AIR-O-WAER HEA PUMP WIH INJECION CYCLE INSALLED IN A LOW-INSULAED SINGLE-FAMILY HOUSE IN BELGIUM E. Dumont, Senior Scientist, Energy Research Centre, University of Mons, Mons, Belgium M. Frère, Professor, Energy Research Centre, University of Mons, Mons, Belgium Abstract: his paper deals with the performance monitoring and analysis of a capacity controlled high-temperature air-to-water heat pump with injection cycle. he heat pump has been installed in a low-insulated house in Belgium in March and is used for space heating in combination with panel radiators or for domestic hot water production. Firstly, we present the behavior of the heat pump in space heating mode as well as in domestic hot water production mode. Secondly, the influence of the injection and of the type of heaters on the performance of the heat pump in space heating mode is presented. Finally, the first results for seasonal performance are presented. hese results show that the machine has an efficient control: injection starts for outdoor temperature where it is more efficient than the non injection cycle, defrosting periods are short due to the good management of the speed of the compressor and of the fan of the evaporator. his good behavior allows the heat pump to significantly increase the COP values compared to common air-to-water heat pumps. Key Words: air-to-water heat pump, injection cycle, high-temperature, monitoring 1 INRODUCION Heat pumps are nowadays world-wide recognized as efficient renewable energy systems for space heating and/or domestic hot water production from the viewpoint of primary energy consumption and CO emissions. his efficiency depends on the SPF value which must be higher than.88 for the heat pump to be considered as a renewable energy system, as explained in (Dumont et al. 11). A SPF higher than.88 is easy to obtain nowadays for heat pumps coupled to low-temperature heating systems like heating floors, what is usually not possible for ancient or renovated houses (Dumont et al. a and b, Dumont et al. 7, Dumont et al. 8a and 8b, Duprez et al. 8). he availability of high-spf heat pumps in old or renovated ancient building stock, usually furbished with high-temperature heating systems (radiators), is then of high concern. In order to exhibit a high COP and a high heating capacity, more efficient heat pumps have been developed, which use the socalled injection cycle in combination with efficient control like a variable speed compressor. he purpose of this study is to monitor and analyze the performance of such a heat pump installed in a low-insulated house, firstly to determine its real SPF, and secondly to investigate the possibility of improvements. his paper presents the first experimental results. SYSEM DESCRIPION AND MONIORING.1 System description he dwelling is located near the city of Charleroi (Wallonia, south of Belgium) and is a four sides, single-family house, built in 199. he heating system is composed of 11 radiators (8 at the basement, at the first floor) which have been replaced in May by convector heaters. Details are given in (Dumont et al. 11). he heat pump installed in the house is a

Numbers of Abstract/Session (given by NOC) - - high-temperature air-to-water heat pump. It uses RA as refrigerant in an injection cycle with internal heat exchanger (IHX) and a variable speed compressor control. It is used for space heating or domestic hot water (DHW) production. A tree-way valve sends the hot water either to the radiators or to a coil placed into a hot water tank. he heat pump design is sketched in figure 1. 1 Domestic hot water 1 Water q VW Space heating 1 WAER PUMP Po VALVE B POWER RECEIVER 8 CONDENSER p 1 q VRA p COMPRESSOR p Po p 9 VALVE C BACKUP HEAER indoor Po INERCOOLER RH outdoor outdoor VALVE A EVAPORAOR RA 7 Outdoor air 11 Po Figure 1: Heat pump configuration and sensors position for monitoring he machine is composed of a scroll compressor, a plate condenser, an IHX (power receiver), an intercooler heat exchanger and a finned tubes evaporator (figure 1). In non injection mode, RA vapor at low pressure is superheated (8-1), compressed (1-), condensed (-), expanded (-), condensed (-), expanded (-7) and evaporated (7-8). In injection mode, operations (8-1), (1-), (-), (-), (-), (-7) and (7-8) remain the same. he major part of the liquid at point is subcooled (-) in an intercooler while a small part of the liquid is expanded (-9) and evaporated in the intercooler (9-), then injected in the scroll compressor at point.. System monitoring In order to achieve the heat pump measurements, the system has been equipped with sensors which measure temperatures (), pressures (p), volume flow rates (q VRA, q VW ) and electric power of the outdoor unit (compressor and evaporator fan), of the circulation pump and of the back-up heater (Po). Evaporator surface temperature, indoor temperature, outdoor temperature and humidity (RH) are also monitored (figure 1). Each value is measured every second, averaged over one minute and stored in a data logger, then uploaded every week on a remote computer. Integration of the minute-average values gives daily values, monthly values then annual values. able 1 presents the different sensors. he measurement of temperature and pressure at the same point of the machine allows us to calculate thermodynamic properties like density ρ and specific enthalpy h. hese properties lead to the determination of mass flow rates for RA and water and then to the heat flow rate at the condenser, computed twice: by energy balance on RA (-) and on

Numbers of Abstract/Session (given by NOC) - - water (1-1). Calculation methods are given in (Duprez et al. 8). he monitoring started in March and the results presented here stop on December 1 st. able 1: Sensors used for monitoring Device Range Measurement point Capacity pressure transducer - bar 1,,, RD (Class A) temperature sensor -- C 1,,,,, 8,, 11, 1, 1, 1 RD (Class A) temperature sensor -- C Indoor, outdoor Capacity relative humidity sensor - % Outdoor Vortex volume flow meter (RA) - dm /s Electromagnetic volume flow meter (water) -.88 dm /s 1 Power analyzer -9 kw Outdoor unit, backup heater, Power analyzer - W Water pump RESULS.1 Space heating.1.1 Daily values autumn he results presented in figure were recorded on November 19 th and are typical of a mild weather (autumn-spring). For this day, the outdoor temperature is about 9 C. here are main heating cycles in which cycle # is composed of 1 small heating cycles. Each main cycle begins with a heat flow rate peak which decreases after 1 min and remains constant until the end of the cycle. his decrease seems to limit the condensation temperature at about - C while the evaporation temperature increases from about to C. he indoor temperature increases from 19 to C. he variation of the outdoor unit electric power is similar to the variation of the heat flow rate. he water pump only circulates water during a heating cycle. he COP is high at the beginning of the cycle because the water coming from the radiator is cold. he COP decreases during the heating up of the water due to the thermal inertia of the water and the radiators (1 first minutes of a heating cycle). he COP then increases due to the increase of the evaporation temperature at quasi-constant condensation temperature. he results show the advantage of the speed control of the compressor/evaporator fan to obtain high COP and long cycles even at mild outdoor temperatures. he heat pump runs the whole day without injection, without defrosting and without backup heater..1. Daily values - winter he results presented in figure were recorded on December nd and are typical of a cold winter day. For this day, the outdoor temperature is about -. C. here are main heating cycles interrupted by short defrosting cycles. Each main cycle exhibits the same behavior as the cycles of November 19 th. Several differences are however pointed out. Here, the heat pump works nearly always with injection except for the third cycle around 1:. Injection seems to be used to reach a condensation temperature of about C needed by the low outdoor temperature (- C during the morning). Injection is stopped at noon when the outdoor temperature is about -1 C and a condensation temperature of about C is enough to keep comfortable indoor temperature (like on November 19 th ). Evaporation temperature is around - C and exhibits quick falls due to frost. Defrosting seems efficient since it only occurs 11 times in a day (total of min within 99 min uptime, i.e..%). COP values are rather good because of the efficient control of the outdoor unit speed. hey exhibits small falls before defrosting cycles.

Numbers of Abstract/Session (given by NOC) - - Φ (kw) 18 1 1 1 8 emperature ( C) - : : : : 8: : 1: 1: 1: 18: : : : Heat flow rate indoor cond outdoor evap Po (kw) 8 7 1 1 - emperature ( C) - : : : : 8: : 1: 1: 1: 18: : : : Po OU Po WP outdoor COP (-) 1 emperature ( C) - : : : : 8: : 1: 1: 1: 18: : : : COP OU COP SYS indoor cond outdoor evap Figure : Condenser heat flow rate φ (top), electric powers Po (middle) and COP (bottom) for November 19 th

Numbers of Abstract/Session (given by NOC) - - Φ (kw) 18 1 1 1 8 - - emperature ( C) - : : : : 8: : 1: 1: 1: 18: : : : Heat flow rate indoor cond outdoor evap Po (kw) 8 7 1 1 - emperature ( C) - : : : : 8: : 1: 1: 1: 18: : : : Po OU Po WP outdoor COP (-) 1 emperature ( C) - : : : : 8: : 1: 1: 1: 18: : : : COP OU COP SYS indoor cond outdoor evap Figure : Condenser heat flow rate φ (top), electric powers Po (middle) and COP (bottom) for December nd

-- Numbers of Abstract/Session (given by NOC).1. Injection analysis From the recorded values, it seems that injection can only occur when OUDOOR< C. his criterion is not sufficient and a second criterion related to the temperature of the gas at the compressor outlet seems to be used. Figure presents the measured thermodynamic cycle without or with injection. It shows that injection of cold gas in the compressor at a pressure between the suction and the exhaust pressures allows the system to reduce the temperature of the refrigerant at the outlet of the compressor. 9 7 8 1 7 8 1 Figure : Heat pump cycle without (left) and with injection (right) (experimental data) he main reason for the use of an injection cycle is to boost the heat flow rate delivered by the heat pump. In order to be efficient, this boost must not lead to a decrease of the COP. In order to validate these assumptions, the heat flow rate φ and the COP with and without injection are presented in figures and, respectively (each point is an average measurement over one minute). thiea Heat Pump thconference IEA Heat Pump 11,Conference 1-19 May 11 11, okyo, Japan

Numbers of Abstract/Session (given by NOC) - 7 - Figure : Condenser heat flow rate Φ versus COND - EVAP with ( ) or without injection ( ) Figure : COP OU versus COND - EVAP with ( ) or without injection ( ) Figure shows that when injection occurs, the heat flow rate increases dramatically: it is limited to kw without injection but can reach 1 kw with injection. Figure shows that the injection is efficient because the COP keeps values of about. when injection is used what will not be the case if the injection is not used. hese two figures lead to conclude that the injection process is efficient and well controlled..1. Radiators versus convector heaters As mentioned above, the radiators which were used with the gas boiler in the house were replaced by convector heaters mid-may. Figure 7 compares the monitored daily performance of the heat pump before (radiators) and after the change (convector heaters).

Numbers of Abstract/Session (given by NOC) - 8 -. March - December. COP SYS (-)..... 1. -8 - - - 8 1 1 1 18 OUDOOR ( C) Figure 7: Daily COP SYS versus OUDOOR for heat pump with convector heaters ( ) or radiators ( ). he curves are manufacturer data for different water regimes Figure 7 shows an increase of COP of about. due to the change of the radiators. For mild weather conditions, radiators used a - C water regime while convector heaters use a lower regime (- C). For winter weather conditions, the convector heaters run with a - C water regime. he few measurement points for low outdoor temperature with radiators exhibit what looks like a strange behavior: the water regime seems to remain - C. his oddity is due to the heat pump control which stopped the heating cycle when water was higher than C. Figure 7 shows also a good agreement with the manufacturer data trends.. Domestic hot water production DHW is produced by the same heat pump as the one used for space heating. Both heating modes cannot occur simultaneously. DHW is usually produced at fixed periods of time during the night, and has priority to space heating. he instantaneous behavior is similar to what has been presented for space heating in.1.1 and.1.. he use of injection is similar to what is observed in space heating mode. Figure 8 presents the daily performance of the heat pump for DHW production. Contrary to space heating, DHW is produced over the whole year, i.e. also during summertime. As the outdoor temperature can reach high value during the summer, the COP should also be high. Figure 8 shows that the increase of COP tends to be limited for high outdoor temperatures. his can be explained by the fact that the heat flow rate φ delivered to the water tank is higher for high outdoor temperature (high evaporation temperature), with a quasi-constant condensation temperature. As the evaporator has a fixed UA value, the evaporator LMD increases and the trend in COP increase is flattened. he evaporator LMD versus OUDOOR is presented in figure 9. he heat pump control strategy is not known but it is assumed that it decreases the compressor speed in order to keep the evaporator LMD constant for OUDOOR ranging from - C to about 1 C. When the minimum available speed is reached, the evaporator LMD increases ( OUDOOR higher than 1 C).

Numbers of Abstract/Session (given by NOC) - 9 -. March - December. COP SYS (-).. 1. 1. -8 - - - 8 1 1 1 18 8 OUDOOR ( C) Figure 8: Daily COP SYS versus OUDOOR for heat pump in DHW production mode 18 March - December Evaporator LMD ( C) 1 1 1 8-8 - - - 8 1 1 1 18 8 OUDOOR ( C) Figure 9: Daily average evaporator LMD versus OUDOOR in DHW production mode. Seasonal performance Month performances values for space heating (from March th to December 1 st ) are presented in able where several energy consumption values are presented: E OU (outdoor unit, i.e. compressor and evaporator fan), E WP (condenser water pump), E CH (fans of the convector heaters), E BH (electric backup heater) and E SB (heat pump stand-by energy, that is control electronic and carter resistor consumption). Q is the heat delivered to the water circulating in the radiators. COPM OU includes only E OU while COPM O includes all kinds of energy consumption. We assumed that the stand-by energy is to be included in space heating calculation and not in DHW production. Let s note that the values for March, October

Numbers of Abstract/Session (given by NOC) -- - - and November do not reflect a whole month monitoring (recording began on March th and the heat pump was in stand-by for maintenance from October 19 th to November 8 th ). able : Month performance for space heating Month E OU E WP E CH E BH E SB Q COPM OU (-) COPM O (-) March 98.1 1..1. 1.7 1.8..8 April 1. 1.1.8. 19.8 1.8.7. May.9 9. 1.7.. 9... June 8.7 1.... 1..1.1 July..19. August 9.....97 1.9. 1. September 7.7. 1.7..7 19.7..1 October.9..7. 1. 8..9. November 8. 17. 8.8.77. 17.9.11.9 December 1.9. 17. 1. 9. 899..9.9 able shows that E OU, E WP and Q exhibit an usual profile over the months (high values during winter and low values during summer). E CH is low for March and April because the convector heaters were placed only mid-may. E BH is nearly zero because the injection process is able to deliver the required heat even for low outdoor temperatures (figure ). E SB is quite constant and higher during summer due to the low uptime of the heat pump. COPM OU values are higher in summer due to high evaporation temperatures. COPM O is low during summer due to the integration of E SB in the calculation. he values of E CH for March and April are low because radiators were used (with only one convector heater) and were only replaced mid-may. It is estimated that if convector heaters have been used in March and April, the COPM values would have been. to. higher. Month performances values for DHW production (from March th to December 1 st ) are presented in able. Here, there are no convector heaters or stand-by energy consumption. As mentioned above, COPM OU includes only E OU while COPM O includes all kinds of energy consumption. able : Month performance for DHW production Month E OU E WP E BH Q COPM OU (-) COPM O (-) March. 1.88. 19.79..9 April 78.11...7.9.1 May 79.8...7..9 June 7.1.9. 18.1.9.8 July. 1.9. 19.8.9.88 August 8. 1.. 1.81.9.8 September 8.1.. 19.7.8.7 October.81 1.1. 1.7.7. November 7. 1.. 111.8.7.1 December 89.99.. 18.9. 1.99 able shows that E OU exhibits a profile similar to the space heating profile while E WP and Q exhibit a constant profile over the months (DHW production do not depend of the weather). E BH is zero for the same reason as for space heating. COPM values are higher in summer than in winter for the same reasons as for space heating.

Numbers of Abstract/Session (given by NOC) -- 11 11 - - CONCLUSION A high-temperature heat pump installed in a low-insulated single-family dwelling has been analyzed and its performance monitored since March. he first results presented in this paper show that the use of the injection cycle for low outdoor temperature allow to deliver high heat flow rates while keeping interesting COP values. he efficiency of the injection cycle also allows the heat pump to deliver the required heat without use of the backup heater. he outdoor unit speed control allows the system to heat up the house with the lowest condensation temperature in order to have the best COP and to avoid short heating cycle behavior. he management of defrosting is also good. From the European regulation viewpoint, the target SPF (.88) may be reached for the system investigated. NOMENCLAURE h Specific enthalpy [kj/kg] p Pressure [bar] q VRA RA volume flow rate [dm /s] q VW Water volume flow rate [dm /s] COP Coefficient of performance of a heat pump [-] COP OU Coefficient of performance including only outdoor unit [-] COP SYS Coefficient of performance including only outdoor unit and water pump [-] COPM OU Month COP including only outdoor unit [-] COPM O Month COP including all electric consumptions [-] E BH Seasonal electric consumption of the backup heater [kwh] E CH Seasonal electric consumption of the convector heaters [kwh] E OU Seasonal electric consumption of the outdoor unit [kwh] E SB Seasonal electric consumption during stand-by [kwh] E WP Seasonal electric consumption of the condenser water pump [kwh] LMD Log mean temperature difference [ C] Po Electric power [W] Po OU Electric power of the outdoor unit [W] Po WP Electric power of the condenser water pump [W] Q Seasonal heat delivered to the house [kwh] RH Relative humidity [%] SPF Seasonal performance factor of a heat pump [-] emperature [ C] COND Condensation temperature [ C] EVAP Evaporation temperature [ C] Indoor temperature [ C] INDOOR OUDOOR Outdoor temperature [ C] ρ Density [kg/m ] φ Condenser heat flow rate [W] REFERENCES Dumont E. and Frère M.. Performance of ground source residential heat pumps, Proceedings of the 8 th IEA Heat Pump Conference, Las Vegas, USA, May June, paper p_.

Numbers of Abstract/Session (given by NOC) -- 1 1 - - Dumont E. and Frère M.. Performance measurement and modeling of air source residential heat pumps, Proceedings of the 8 th IEA Heat Pump Conference, Las Vegas, USA, May June, paper p7_7. Dumont E., Duprez M.-E. and Frère M. 7. A simple method for the determination of SPF of heat pumps used in single family dwellings, Proceedings of the nd IIF Congress of Refrigeration, Beijing, China, 1- August 7, paper ICR7-E-1. Dumont E., Duprez M.-E., Lepore R., Nourricier S., Feldheim V. and Frère M. 8. Performance analysis and modeling of a static air-to-water heat pump integrated in a singlefamily dwelling, Proceedings of the 9 th IEA Heat Pump Conference, Zurich, Switzerland, - May 8, paper.1. Dumont E., Lepore R., Nourricier S. and Frère M. 8. Performance monitoring and modeling of a static air-to-water heat pump installed in a single-family dwelling, Proceedings of the 1 st Heat Pump Platform Symposium, Sint-Katelijne-Waver, Belgium, 17 September 8. Dumont E. and Frère M. 11. Performance analysis of high-temperature heat pumps installed in low-insulated dwellings: case of a single-family house in Belgium, Proceedings of the th IEA Heat Pump Conference, okyo, Japan, 1-19 May 11, paper 1. Duprez M.-E., Dumont E. and Frère M. 8. Experimental results of an air-to-water heat pump with a variable speed compressor, Proceedings of the 9 th IEA Heat Pump Conference, Zurich, Switzerland, - May 8, paper..