Efficiency improvement in solar cells MSc_TI | Winter Term 2015 - - PowerPoint PPT Presentation
Efficiency improvement in solar cells MSc_TI | Winter Term 2015 - - PowerPoint PPT Presentation
Efficiency improvement in solar cells MSc_TI | Winter Term 2015 Klaus Naumann Agenda Introduction Physical Basics Function of Solar Cells Cell Technologies Efficiency Improvement Outlook 2 MSc TI | Seminar |
MSc TI | Seminar | 2015
Agenda
- Introduction
- Physical Basics
- Function of Solar Cells
- Cell Technologies
- Efficiency Improvement
- Outlook
2
MSc TI | Seminar | 2015
Agenda
- Introduction
- Physical Basics
- Function of Solar Cells
- Cell Technologies
- Efficiency Improvement
- Outlook
3
MSc TI | Seminar | 2015
Introduction | Application Examples
4
MSc TI | Seminar | 2015
Introduction | Sun, Radiation and the Sahara Miracle
5
Source: Konrad Mertens, Photovoltaics β Fundamentals, Technology and Practice, Wiley 2014
- Radiation power of sun:
π
ππ£π = 3.845 β 1026 π
- Solar constant:
- utside Earthβs atmosphere:
πΉ0 = 1367 π π2
- Global radiation:
Inside the atmosphere:
πΉπ» β 1000 π π2
βSun sends us more than 7000 time the energy than we use in a yearβ
π
πΉππ π’β = 1.119 β 1018 ππβ
π
πππ ππ = 1.454 β 1014 ππβ
MSc TI | Seminar | 2015
Introduction | Air Mass
6
- AM 0 (Air Mass 0): outside the atmosphere
- AM 1 (Air Mass 1): inside the atmosphere (vertical path through atmosphere)
- AM 1.5 (Air Mass 1.5): light travelled 1.5 times the distance compared to AM 1
Source: http://www.greenrhinoenergy.com/solar/radiation/spectra.php
MSc TI | Seminar | 2015
Introduction | Solar Spectrum and Radiation Types
7 Losses:
- Reflection at atmosphere
- Absorption of light
- Scattering
ο¨ Two types of radiation:
- Direct
- Diffuse
ο πΉπ» = πΉπΈππ πππ’ + πΉπΈππππ£π‘π
Source: Konrad Mertens, Photovoltaics β Fundamentals, Technology and Practice, Wiley 2014
MSc TI | Seminar | 2015
Agenda
- Introduction
- Physical Basics
- Function of Solar Cells
- Cell Technologies
- Efficiency Improvement
- Outlook
8
MSc TI | Seminar | 2015
Physical Basics | Bohrβs Atomic Model and Band Model
9
- Ionizing energy:
separate electron from the atom
- Photon:
light packet of particular wavelength
- Absorption of light:
light particle hits electron and is
- absorbed. Released energy lifts
electron from Valence band to Conduction band
βπ
π» = π π β π π = β β π
π = π0 π
h = Planckβs constant Source: Konrad Mertens, Photovoltaics β Fundamentals, Technology and Practice, Wiley 2014
MSc TI | Seminar | 2015
Physical Basics | Semiconductor Band Gap
10
Source: Konrad Mertens, Photovoltaics β Fundamentals, Technology and Practice, Wiley 2014
MSc TI | Seminar | 2015
Agenda
- Introduction
- Physical Basics
- Function of Solar Cells
- Cell Technologies
- Efficiency improvement
- Outlook
11
MSc TI | Seminar | 2015
Function of Solar Cells | p-n junction
12
Source: http://wanda.fiu.edu/teaching/courses/Modern_ lab_manual/_images/pn-junction_energy.png
MSc TI | Seminar | 2015
Function of Solar Cells | Method of Function
13
Source: Konrad Mertens, Photovoltaics β Fundamentals, Technology and Practice, Wiley 2014
MSc TI | Seminar | 2015
Function of Solar Cells | Solar Panel Construction
14
Source: http://www.dupont.com/content/en_us/home/products- and-services/solar-photovoltaic-materials/what-makes- up-solar- panel/_jcr_content/thumbnail.img.jpg/1435680366722.jpg
Multiple Solar Cells in one Solar Panel
MSc TI | Seminar | 2015
Function of Solar Cells | Characteristic Curve
16
Source:
http://www.alternative-energy- tutorials.com/energy-articles/solar-cell-i-v- characteristic.html
- Load Resistance determines
- perating point:
- R = 0
ο π½ππ·
- R = β
ο π
ππ·
- Maximum Power Point (MPP):
ππππ = π½πππ β π
πππ
- Fill Factor (FF):
πΊπΊ =
ππππ β π½πππ πππ· β π½ππ·
=
ππππ πππ· β π½ππ·
- Si-Cells: 0.75 β 0.85
- Thin Film: 0.6 β 0.75
- Measure for Quality
MSc TI | Seminar | 2015
Agenda
- Introduction
- Physical Basics
- Function of Solar Cells
- Cell Technologies
- Efficiency Improvement
- Outlook
17
MSc TI | Seminar | 2015
Cell Technologies | Cell Types
18
- Thick Film (150 β 250 Β΅m)
Ξ·max
- Monocrystalline
(1st Gen Cells) ~ 20 %
- Polycrystalline
(1st Gen Cells) ~ 16 %
- Thin Film (< 10 Β΅m)
- Amorphous Silicon
(2nd Gen Cells) ~ 10 %
- Cadmium-Telluride
(2nd Gen Cells) ~ 10 %
- CIGS (CuInxGa(1-x)Se2)* (2nd Gen Cells)
~ 15 %
- Emerging: Perovskite(3rd Gen Cells)
- Multi-Layer
*Copper-Indium-Gallium-Selenide
MSc TI | Seminar | 2015
Cell Technologies | Comparison of Cell Types
19
Mono Poly Thin CIGS Generation 1st Gen 2nd Gen Efficiency 14 β 20 % 12 β 16 % 6 β 10 % 13 β 15 % Low light performance Losses (diffuse) Low losses Thermal behavior High temperature losses Low losses Cost (1 = lowest) 3 2 1 4 Long-term test Very high Performance, stable High Performance, stable Average Performance Low Performance (in winter higher) Durability High High Lower Not tested yet Weight β β Failure vulnerability ββ β β = High, β = Low, ββ = Very low
Source: http://www.solaranlagen-portal.com/solarmodule/systeme/vergleich
MSc TI | Seminar | 2015
Agenda
- Introduction
- Physical Basics
- Function of Solar Cells
- Cell Technologies
- Efficiency Improvement
- Outlook
20
MSc TI | Seminar | 2015
Efficiency Improvement | AR Coating
21 Anti-Reflection Coating
- Reduction of reflection
increases efficiency
- With certain coatings and
specific wavelengths: Reflection ο 0
Source: Konrad Mertens, Photovoltaics β Fundamentals, Technology and Practice, Wiley 2014
MSc TI | Seminar | 2015
Efficiency Improvement | Radiation Bundling
22
- Reduction of solar cell area
- Cell curve moves up
ο higher efficiency
- Efficiency increase not continuously!
ο Electrical losses increase as well
- Resistance rise with square of
- perating current
ο Heat sink needed
- Record: 43.5 % efficiency
(concentration factor: 418(!)) Radiation Bundling
Source: Mertens, Konrad: Photovoltaics β Fundamentals, Technology and Practice, Wiley 2014 King, Richard R.: Raising the Efficiency Ceiling in Multijunction Solar Cells, Spectrolab, Inc., 2009
MSc TI | Seminar | 2015
Efficiency Improvement | Multi-Layer Cells
23 Multi-Layer Cells
Source: http://www.solarpowerworldonline.com/2011/10/solar-cells- without-the-silicon/ http://www.sj-solar.com/technology/
MSc TI | Seminar | 2015
Efficiency Improvement | Perovskite
24 New Materials: Perovskite
- Thin film cells (stand-alone or in multi-layer cells)
- Very fast efficiency improvement
(2006: 2.2 % ο 2014: 20.1 %)
- CH3NH3PbX3 where
X = π½β π½πππππ , πΆπ β πΆπ πππππ ππ π·πβ (π·βπππ πππ)
- Anode/Cathode material defines bandgap
ο not tuned to one wavelength ο higher efficiency
- Low energy input in processing compared to Si
ο Low material/manufacturing costs
- Flexible | Light-weight | Semi-Transparent
Source: Dyakonov, Prof. Dr. Vladimir, Perowskit- Halbleiter erobern die (DΓΌnnschicht-) Photovoltaik, ZAE Bayern, 2014
MSc TI | Seminar | 2015
Agenda
- Introduction
- Physical Basics
- Function of Solar Cells
- Cell Technologies
- Efficiency Improvement
- Outlook
25
MSc TI | Seminar | 2015
Outlook | Smart Grids
26
- Decentralisation of energy supply
- Efficiency of high importance (decrease of required place and costs)
- Photovoltaics is a big and important part in future concepts (smart grid)
Source: http://www.tonex.com/training-courses/smart-grid-training-for-non-engineers/
MSc TI | Seminar | 2015
Outlook | Innovations
27
MSc TI | Seminar | 2015
Outlook | Innovations
28
Source: http://www.scientificamerican.com/article/farming
- solar-energy-in-space/
MSc TI | Seminar | 2015
Thank You
29 Questions?