10 years of research on PVT systems at UNSW past, present, and future…
Dr Jose Bilbao, Associate Lecturer SPREE Systems & Policy Group – UNSW Sydney
past, present, and future Dr Jose Bilbao, Associate Lecturer SPREE - - PowerPoint PPT Presentation
10 years of research on PVT systems at UNSW past, present, and future Dr Jose Bilbao, Associate Lecturer SPREE Systems & Policy Group UNSW Sydney 2 Acknowledgments Team leader A/Prof Alistair Sproul PhD graduates Special thanks Dr
Dr Jose Bilbao, Associate Lecturer SPREE Systems & Policy Group – UNSW Sydney
Team leader A/Prof Alistair Sproul PhD graduates Dr Shelley Bambrook (2012 → moved to Germany) Current PhD students Mehrdad Farshchimonfared Simao Lin Jinyi Guo Jianzhou Zhao
2
Special thanks Rob Largent!!! Systems & Policy group! 464 group!
Heat Electricity
PVT
3
Affolter et al. 2006. PVT Roadmap – A European guide for the development and market introduction of PV-Thermal technology, PV Catapult Project.
4
(covered or uncovered)
(covered or uncovered)
5
http://www.vicphysics.org/documents/events/stav2005/spectrum.JPG
Multijunction SQ limit ~ 49% At best ~50% of solar energy is converted to heat, not to electricity
Generally, the efficiency of solar cells decrease with temperature Most of the energy is converted to heat → increases cell/module temperature So, cooling a PV module is a good idea!
6
Dupré, Vaillon, Green, 2015. Physics of the temperature coefficients of solar
Cells, 140, 92-100
1) Decrease the temperature of the cell/module by cooling it with a fluid 2) This increases the efficiency of the cell (more electricity!) 3) We can use the ‘waste’ heat for other purposes (we get heat too!) 4) Profit!*
By the way, PVT is not a new idea, the first publication on the subject was by Wolf in 1976 (40 years ago!).
7
than syde-by-syde systems (PV + SHW)
8
Bergene and Lovvik, 1995 Elswijk et al.2004,
High temperature rise results in low thermal and electrical efficiency (bad) So, it’s better to have a low temperature rise, with high thermal and electrical efficiency (good) But then, how useful is low temperature heat??
9
Bambrook 2011. Thesis: Investigation of photovoltaic / thermal air systems to create a zero energy house in Sydney Efficiency Normalised temp rise
Heat Electricity Efficienc y Temperature rise (Exergy)
10
More useful???
11
A system that could provide electricity and warm water (pre-heating) for houses Criteria:
Important equipment:
12
Remove JB of frameless panel (stored in Bay St)
13
Bond the water channels (collector) Thermocouples
14
Collector with polycarbonate channels Install back insulation and JB
15
Install new frame Mount the PVT collector
16
Mount the header pipe Seal pipe and channels
Water tank 100L 20 W submergible pond pump Thermocouples in inlet, outlet, back of panel, flow sensor, Pyranometer, etc… Standard panel (same model) as control (12% efficiency at STC) System worked 24/7 – daily reset (heating water during the day, cooling water during the night)
17
The PVT system
module, due to higher efficiency (cooling) Except on July (stagnation ‘experiment’, i.e. no flow) What to do when no more hear is needed??
18
Big gap between thermal and electrical
Hence, the application must match the generation profile of PVT systems PVT used only as a solar collector
19
Example of outlet temperature – model vs experiment
20
Bilbao & Sproul 2015. Detailed PVT-water model for transient analysis using RC networks, Solar Energy, 115, 680-693
Example of thermal energy – model vs experiment
21
Bilbao & Sproul 2015. Detailed PVT-water model for transient analysis using RC networks, Solar Energy, 115, 680-693
Example of electrical energy – model vs experiment
22
Bilbao & Sproul 2015. Detailed PVT-water model for transient analysis using RC networks, Solar Energy, 115, 680-693
cover temperature (Type850)
23
Bilbao & Sproul 2015. Detailed PVT-water model for transient analysis using RC networks, Solar Energy, 115, 680-693
24
0% 5% 15 20 25 30 35 40 45 50 55
Tin ( C)
a) UL percentage error (Wv=2m/s, Ta=20 C, N=0)
Type50-C, Ts=Ta Type50, Ts=Ta Type50-C, Ts=Ta-18 Type50, Ts=Ta-18
Bilbao & Sproul 2012. Analysis of flat plate photovoltaic-thermal (PVT) models. World Renewable Energy Forum, Denver.
Difference between PVT models calculating heat loss coefficient (UL) when sky temperature is considered Sky temperature is particularly important in PVT collectors, due to the high emissivity of its surfaces
25
Uncovered Covered
26
Series or parallel (thermal) configuration does matter, but effect is small Covered system provide a higher combined output (but electricity output is greatly reduced) PVT works, but it really depends on the application!
5 10 15 20 25 Jan-12 Feb-12 Mar-12 Apr-12 May-12 Jun-12 Sydney Temperature (°C) Tamb Avg_day (°C) Tsky Avg_day (°C) Tamb Avg_night (°C) Tsky Avg_night (°C) 27
Jan Feb Mar Apr May Jun Average daily Night Radiative Cooling (Wh/m2)
Simulated data from the tuned model Goal was to determined how much cooling was due to radiative losses and convective losses
200 400 600 800 1,000 1,200 1,400 1,600
Total cooling during night periods (W)
a)
Qconv Qrad Qbe 28
Assumptions
(rooftop installation ensures good sky view factor).
(Cfa), and Hamburg (Dfb).
200 400 600 800 1000 1200 1400 Jan Feb Mar Apr May Jun Jul Aug Sep Oct Nov Dec Average Nightly Radiative Cooling Wh/m2 SYDNEY SINGAPORE TUCSON HAMBURG
29
night radiative cooling.
Wh/m2 to 900 Wh/m2 per night.
whole year.
cooling depends on many variables (+10% to 20% can be obtained from convective cooling).
30
200 400 600 800 1000 1200 Sydney Sydney (30 deg Tilt) Singapore Tucson Hamburg Average Nightly Radiative Cooling Wh/m2 Convective Radiative
PVT collectors donated by Solimpeks
PVT roof will provide heating during winter Cooling in summer via desiccant and IEC
34
Guo, Bilbao, Sproul. Ground Coupled Photovoltaic Thermal (PV/T) Driven Desiccant Air Cooling. 2014 Asia-Pacific Solar Research Conference
But…
Yet, BIPVT and high efficiency cells might change this
35
Panasonic Champion SHJ cell
36
Bilbao, Dupre, Johnson. On the effects of high efficiency solar cells and their temperature coefficients on PVT systems. PVSEC-25, Busan, November 2015
Cell Efficiency (%) Module (% / Wp) Temperature Coefficient (Pmpp %/K) Medium 20% 17.6% / 290W
High 30% 26.4% / 435W
Higher 40% 35.2% / 580W
37
Electrical efficiency increases with cell efficiency Thermal efficiency decreases But, total efficiency increases (slightly)
25 35 45 55 65 75 85
38
Similar trend between cover and uncovered systems (compared with previous results) Amount of thermal energy
depending on the application
39
PV performance does not ‘suffer’ as much, because of low temperature coefficients
40
meet load profiles
BIPVT
41
Dr Jose Bilbao – Systems & Energy Policy Group, SPREE j.bilbao@unsw.edu.au
42