TY - JOUR AU - Lazzarin, Renato M AB - Abstract PhotoVoltaic/Thermal cogeneration (PV/T) aims to utilize the same area both for producing electricity and heat. An electric compression heat pump can be coupled to the PV/T panels to contribute to the space heating demand partially using the self-produced electricity. Some Italian climates and economic incentives scenarios are considered with Trnsys simulations to evaluate the energy and economic viability of PV/T-heat pump hybrid technology. Primary energy saving results to be between 35% and 65%, and discounted payback of the investment can be around 10 years in mild climates and southern resorts. 1 INTRODUCTION Not all the wavelengths of the incoming irradiation are usefully converted into electricity in PhotoVoltaic (PV) cells: commercially available single junction PV cells convert between 6% and 25% (under optimum operating conditions and depending on the semiconductor material) into electricity, while the rest is dissipated as heat [1]. This is due to the band-gap energy of the semiconductor material. For example, crystalline silicon PV cells can utilize the entire visible spectrum plus some part of the infrared spectrum, but the energy of all the other wavelengths (the far infrared and the higher energy radiation) is unusable in order to be converted in electricity and instead is dissipated at the cell as thermal energy. The main drawback is that the PV module can reach temperatures as high as 40°C above ambient; this causes an increased intrinsic carrier concentration which tends to increase the dark saturation current of the p–n junction. The main effect is the decreasing of the available maximum electrical power, typically 0.2–0.5% for every 1°C rise in the PV module temperature for crystalline silicon cells. The well-known main idea to face the issues just described is to increase the electrical production of PV by decreasing the normal operating cell temperature by cooling the panel by a liquid (or air) [2]. So PV/Thermal technology (PV/T) aims to utilize the same area both for producing electricity and heat. This also implies to have higher global efficiency with an enhanced use of solar energy [3, 4]. The most common technology is the PV/T flat-plane solar collector where heat extraction from the PV panel is forced by the utilization of a pump for water circulation. Many experimental and theoretical studies have been done in the recent past on the performance of PV/T water cooled plane collectors [5–7]. An experimental study was carried out by the authors as well [8, 9]. From the technical point of view, the performances strongly depend on the channels absorber design, the glazed or unglazed configuration and the flow rate and inlet temperature of thermal fluid. Considering the European Directives constraints on energy efficiency and renewable energy, solar energy is an interesting option in Italy due to the high values of annual solar radiation. Furthermore, different granting systems based on the promotion of electricity from photovoltaics and thermal energy from solar thermal plants have been churned out by the Italian government during last decade. The proposed work aims to sound the energy and economic viability of using PV/T panels for cogeneration purposes for a typical four-bedroom house over different cities in Italy. An electric compression heat pump can be coupled to the PV/T panels to contribute to the space heating (SH) demand partially using the self-produced electricity. The analyses take into account an innovative design useful to mitigate the typical constraints of PV/T flat-plate collectors. These are due to the high operating temperature of the photovoltaic laminate in stagnation conditions (with high risk of damage for the PV, the lower electrical efficiency apart) when considering glazed collectors, and to the lower thermal efficiency when considering unglazed collectors. The analysis here reported takes into account also the present granting system for electricity and thermal energy produced by the PV/T system, evaluating the great energy and economic potential of such technology coupled to an electric compression heat pump for heating, domestic hot water (DWH) and electricity production purposes. 2 THE PV/T PLANT SYSTEM The proposed system is supposed to supply both electrical energy from PV and thermal energy from the liquid cooled thermal collector for a typical two-stage Italian house. The building has a volume of 364 m3, a height of 5.5 m, with a surface of 77 m2 on the ground floor and 58 m2 on the first floor. The proposed PV/T system is depicted in Figure 1: it is intended to supply electrical energy and thermal energy for DHW and low temperature SH, i.e. radiant floor. The whole plant is thought as follows: Liquid cooled PV/T panel with laminate with a surface of 2.0 m2. The panel is thought to be constituted by two glass layers incorporating 60 monocrystalline silicon cells spaced between them, each cell being 156 mm × 156 mm, 3.75 Wp (peak condition). Below the PV layer there is the thermal absorber plate. So, of the total solar radiation incident on the PV/T panel surface, 73% is intercepted by the PV surface ((0.156 × 0.156 × 60)/2 = 0.73), the remaining 27% by the thermal surface (Figure 2). This configuration has been simulated in Trnsys [10] by coupling a PV (type 94a) (with a PV surface of 1.46 m2 and the total solar incident radiation) with a solar thermal collector (type 1) (with a surface of 2 m2 and the 27% of the total solar incident radiation). The liquid is a mixture of water (70%) and glycol (30%) to prevent the liquid from freezing. The plant is constituted by eight PV/T panels in parallel (from the thermal point of view), giving 3.75 × 60 × 8 = 1800 Wp (electrical efficiency at reference conditions = 15.4 %); the DC electrical power produced is converted in AC power by an inverter (efficiency 90%) and so measured by a meter. Another bi-directional meter counts the inlet/outlet energy from/to the grid (net metering); the thermal part of the PV/T panels is connected to a tank internal heat exchanger (type 91) that exchanges heat with water coming from tank-to-tank storage (type 60); the fluid is pumped with one variable speed pump absorbing 60 W; a 500 l tank-to-tank storage (type 60) is used to collect hot water for SH (outer tank) and to pre-heat water for DWH uses (inner tank); and a natural gas fired boiler for DHW and SH integration (seasonal mean efficiency of 85% LHV) (type 6). Figure 1. View largeDownload slide Scheme of the proposed PV/T system for production of electrical energy and thermal energy for DHW and SH. Figure 1. View largeDownload slide Scheme of the proposed PV/T system for production of electrical energy and thermal energy for DHW and SH. Figure 2. View largeDownload slide Scheme of the proposed PV/T panel (drawings not to scale). Figure 2. View largeDownload slide Scheme of the proposed PV/T panel (drawings not to scale). Acontrol system handles the plant from a series of input (dashed line) and output (continuous line) signals (Figure 1). This has been modeled by a type developed by the authors. In particular: DHW: water enters the storage from the network at 12°C and is heated up to 45°C by the hot water stored from the PV/T first and then the boiler. The water is supposed to be delivered to the user at 45°C through a three-way valve; the water consumption is supposed to be 200 l per day. SH: water is drawn from the tank and heated up by the boiler to the water delivery temperature of the SH system (twater). If the storage tank temperature is lower than the water temperature from the radiant floor plant, a three-way valve is supposed to bypass the storage. The set temperature follows a climatic curve with a maximum temperature of 38°C (when ambient temperature tambient is equal to 0°C) and a minimum temperature of 25°C (tambient = 17.33°C):   twater=38−0.75⋅tambient (1) The heating load comes from a dedicated Trnsys model of the house and considering the annual local weather conditions (Test Reference Year (TRY) [11]). Pump in the PV/T modules circuit turns on when outlet temperature from PV/T is 7°C higher than that at the bottom of the storage and irradiance is higher than 300 W/m2. Pump in the PV/T modules circuit turns off when outlet temperature from PV/T is <3°C higher than that at the bottom of the storage and without considering irradiance. Pump is variable speed type (type 3d) allowing the cooling fluid to suitably increase its temperature during winter and low availability of solar energy. The plant considers eight PV/T panels set to the South (0° of azimuth angle) with the optimal tilt angle from the energy point of view (substantially 30° for all the climates): this solution was thought to have an interesting value of the electrical power (1800 Wp) without exceeding in thermal production, considering the low thermal energy uses during summer months. The parallel connection of the panels allows a satisfactory thermal production: other configurations (e.g. four parallels of two panels in series each) are more penalized from the thermal point of view. Furthermore, the here considered PV/T panel configuration (with the thermal plate absorber not directly in contact with the PV layer and the latter substantially unglazed) allows to reduce the risk of damage of the PV layer due to stagnation temperature (~120–140°C). 3 ENERGY ANALYSIS Three different resorts were selected over the Country at three very different latitudes: Venice (45°30′ N), Rome (41°48′ N) and Crotone (39°04′ N). For the sake of brevity, the detailed results are reported for Venice only, the main considerations for the other climates are reported as well. Figure 3 depicts the electrical energy quantities related to PV/T plant: the electrical energy produced is the AC energy, inclusive of pumps consumption. Incident solar radiation is the part, of the total radiation, incident on the PV surface (73%). So electrical efficiency is the ratio between these two quantities. The lower values in summer months (when ambient air temperature and solar radiation are higher) are due to the sensitivity of electrical efficiency of crystalline silicon cells to their temperature. Figure 3. View largeDownload slide Electrical energy produced by PV/T plant, consumed by the pumps, incident solar energy and electrical efficiency (Venice). Figure 3. View largeDownload slide Electrical energy produced by PV/T plant, consumed by the pumps, incident solar energy and electrical efficiency (Venice). Figure 4 shows the thermal energy quantities related to PV/T plant: the thermal energy produced is net of tank losses and referred only to periods when it is useful (that is it is used for DHW or SH aims). Incident solar radiation is the part, of the total radiation, incident on the thermal surface (27%). Again, thermal efficiency is the ratio between these two quantities. In this case, the lower values in summer months are due to the low uses of thermal energy in this period (only for DHW). Figure 4. View largeDownload slide Thermal energy produced by PV/T plant, incident solar energy and thermal efficiency (Venice). Figure 4. View largeDownload slide Thermal energy produced by PV/T plant, incident solar energy and thermal efficiency (Venice). In Figure 5, it is depicted the heat energy used for DHW and SH per month over the year: the total heat is net of the losses at the storage tank which are seen to be around 10% of the total heat produced by the PV/T plant. The contribution to the SH is quite limited (solar ratio is below 10% in winter months), while during summer months thermal production allows to fully satisfy the load. In Southern resorts, such figures are even better, with a solar ratio in winter months varying from 13 to 25% in Rome and from 19 to 37% in Crotone. Figure 5. View largeDownload slide Heat energy produced by the PV/T plant for DHW and SH purposes, DHW and SH demands (Venice). Figure 5. View largeDownload slide Heat energy produced by the PV/T plant for DHW and SH purposes, DHW and SH demands (Venice). Figure 6 resumes the annual electrical and thermal energy production of the PV/T plant for the three climates: the first covers the great part (61.3% in Venice–77% in Crotone) of the annual electrical consumption of an average four-people Italian family, that has been fixed in 3500 kWh. The thermal energy production allows to obtain the solar energy ratio reported in the same figure: in the South of the Country, abundance of sun energy and reduced heat loads lead this figure to be near 50%. Finally, primary energy saving (PES) of the PV/T plant with respect to two different reference scenarios has been calculated: reference scenario A: gas fired boiler both for DHW and SH, seasonal mean efficiency = 85% (LHV); and reference scenario B: electrical air–water heat pump for SH (seasonal mean COP = 3 – 3.2 – 3.3 respectively for Venice, Rome and Crotone) + natural gas boiler for DHW (seasonal mean efficiency = 85% (LHV)). Figure 6. View largeDownload slide Annual thermal and electrical loads covered and thermal/electrical annual energy produced by the PV/T plant among the three resorts in Italy. Figure 6. View largeDownload slide Annual thermal and electrical loads covered and thermal/electrical annual energy produced by the PV/T plant among the three resorts in Italy. In both reference scenarios, electrical uses of the house are supposed to be satisfied by electricity from the grid. In case of reference scenario B, when considering the use of the PV/T plant, the heat integration is obtained by an electric heat pump for SH, and by a natural gas fired boiler for DHW, both with the characteristics just described above. Such hypothesis is taken in order to consider the most diffuse situation. In this case, the PV/T electrical energy production is used to satisfy the needs of heat pump and, if in excess, the other electrical uses of the house (Table 1). Mean efficiency of the electricity from grid (for heat pump and the other electrical uses of the house) is considered to be 46%. This is the energy conversion factor from kWh to toe for the Italian energy efficiency certificates market and it is based on the average efficiency of the Italian electricity system (largely based on natural gas thermoelectric (Rankine and Brayton–Joule) plants) [12]. Table 2 and Figure 7 report (fossil) primary energy consumption (PE) and PES for both the electrical and thermal uses of the house, and the total, following the equations:   PESTH,A=LOADTH,TOT0.85−(AUXDHW0.85+AUXSH0.85)LOADTH,TOT0.85PESEL,A=LOADEL,TOT0.46−(LOADEL,TOT−PVTEL0.46)LOADEL,TOT0.46 (2)  PESTOT,A=(LOADTH,TOT0.85+LOADEL,TOT0.46)−(AUXDHW0.85+AUXSH0.85+LOADEL,TOT−PVTEL0.46)(LOADTH,TOT0.85+LOADEL,TOT0.46) (3)  PESTH,B=(LOADTH,SHCOP⋅0.46+LOADTH,DHW0.85)−(AUXDHW0.85+Θ)(LOADTH,SHCOP⋅0.46+LOADTH,DHW0.85)whereΘ=IFPVTEL