2 2 mitchell lee_am and pwat spectral correction_pvpmc5
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Transcript of 2 2 mitchell lee_am and pwat spectral correction_pvpmc5
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Current State of Spectral Correction
.
Absolute Air Mass (AMa) 3-4
• Sandia Array Performance Model computes spectral shift as a function of air mass:
McSi = a0 + a1·AMa + a2·(AMa)2 + a3·(AMa)
3 + a4·(AMa)4
• Coefficients determined from module testing
0.98
0.99
1
1.01
1.02
1.03
1.04
1.05
1 2 3 4 5
Spe
ctra
l Sh
ift
Absolute Air Mass
Nameplate
Precipitable Water (Pwat) 1-2
• First Solar spectral shift model is calculated using precipitable water:
MCdTe = 1.266 – 0.091exp(1.199(Pwat + 0.5)-0.210)
• Coefficients calculated empirically from 13 TMY locations across the US input into SMARTS
0.95
0.97
0.99
1.01
1.03
1.05
1.07
0 1 2 3 4 5
Spe
ctra
l Sh
ift
Precipitable Water (cm)
Nameplate
1. L. Nelson, M. Frichtl, and A. Panchula, “Changes in cadmium telluride photovoltaic performance due to spectrum,” IEEE Journal of Photovoltaics, vol. 3, No. 1, pp. 488-493, 2013.
2. Mitchell Lee, Lauren Ngan, William Hayes, and Alex F. Panchula, “Comparison of the Effects of Spectrum on Cadmium Telluride and Monocrystalline Silicon Photovoltaic Module
Performance,” 42nd IEEE Photovoltaic Specialists Conference, 2015
3. D. King, W. Boyson, and J. Kratochvill, Photovoltaic Array Performance Model, SAND2004-3535. Albuquerque, New Mexico: Sandia National Laboratories, 2004.
4. D. King, J. Kratochvill, and W. Boyson, “Measuring solar spectral and angle-of-incidence effects on photovoltaic modules and solar irradiance sensors,” in 26th IEEE Photovoltaic
Specialists Conference, 1997, p. 1113 – 1116.
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𝑀 = 𝑏0 + 𝑏1 ∙ 𝐴𝑀𝑎+ 𝑏2 ∙ 𝑝𝑤𝑎𝑡 + 𝑏3 ∙ 𝐴𝑀𝑎 + 𝑏4 ∙ 𝑝𝑤𝑎𝑡 + 𝑏5 ∙
𝐴𝑀𝑎
𝑝𝑤𝑎𝑡
Proposed Two Variable Spectral Correction
2-Variable Correlation
AMa Correlation
Pwat Correlation
(Series 4-2): 𝑀 ≈ 1.266 − 0.091exp(1.199 𝑃𝑤𝑎𝑡 + 0.5−0.210
(Series 4-1 and earlier): 𝑀 ≈ 0.632 + 0.134exp(0.976 𝑃𝑤𝑎𝑡 + 0.050.079)
𝑓1 𝐴𝑀𝑎 = 𝑎0 + 𝑎1 ∙ 𝐴𝑀𝑎 + 𝑎2 ∙ 𝐴𝑀𝑎2 + 𝑎3 ∙ 𝐴𝑀𝑎
3 + 𝑎4 ∙ 𝐴𝑀𝑎4
Where: 𝐴𝑀𝑎 =𝑃
𝑃0∙ 𝐴𝑀
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SMARTS Overview
• Simulated Spectrum with all combinations of AMa and Pwat where:
— 0.1 cm ≤ Pwat ≤ 5 cm
— 1.0 ≤ AMa ≤ 5
• Limit spectral range of simulation to that of CMP11 (280 nm to 2800 nm)
• Kept all other parameters fixed at G173 standard
— Tilt = 37°
— Azimuth = 180°
• Computed spectral shift factor using module specific QE curves (provided by NREL)
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Multi-Si: 2-D Cross Section
Pwat Fixed at G173Multi-Si
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Field Validation: Data Source
Publically Available Data From NREL
• Three locations with distinct climates
• IV characterization and meteorological data at 5 min (or 15 minute) resolution for 13 months
• Several module types (we focused on multi-Si and CdTe)
Golden, CO Eugene, OR Cocoa, FL
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Field Validation: Methodology
𝑀 ≈𝐼𝑠𝑐
𝑃𝑂𝐴∙1000W/m2
𝐼𝑠𝑐0: where 𝐼𝑠𝑐0 tested by Sandia
ISC corrected for:• Temperature using a linear coefficient. • Angle of incidence, AOI, using the Sandia method. • Soiling losses using estimates provided by NREL.
Filtered out data where:• POA ≤ 200 W/m2
• AOI losses ≥ 1 %• Kt <= .70 or Kt >= 1.0• Full days have < 1.5 hours of data
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Golden, Colorado
CdTe
Previous Correlation New Correlation
Multi-Si
𝑀𝑃𝑤𝑎𝑡 = 0.7051 ∙ 𝑀𝑚𝑒𝑎𝑠𝑢𝑟𝑒𝑑 − 0. 28836
𝑅2 = 0.712
𝑀2−𝑃𝑎𝑟𝑎𝑚 = 0.7266 ∙ 𝑀𝑚𝑒𝑎𝑠𝑢𝑟𝑒𝑑 + 0. 258
𝑀𝐴𝑀𝑎 = 0.0360 ∙ 𝑀𝑚𝑒𝑎𝑠𝑢𝑟𝑒𝑑 + 0.956
𝑅2 = 0.001
𝑀2−𝑃𝑎𝑟𝑎𝑚 = 0.561 ∙ 𝑀𝑚𝑒𝑎𝑠𝑢𝑟𝑒𝑑 + 0.424
𝑅2 = 0.356
2-Var has same R2 as Pwat
2-Var improves R2 compared to AMa correlation
𝑅2 = 0.706𝑀𝐴𝐸 = 0.00827; 𝑀𝐴𝐸 = 0.0150;
𝑀𝐴𝐸 = 0.00955; 𝑀𝐴𝐸 = 0.01256;
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Eugene, Oregon
CdTe
Previous Correlation New Correlation
Multi-Si
𝑀𝑝𝑤𝑎𝑡 = 0.536 ∙ 𝑀𝑚𝑒𝑎𝑠𝑢𝑟𝑒𝑑 + 0.476
𝑅2 = 0. 445
𝑀2−𝑃𝑎𝑟𝑎𝑚 = 0.638 ∙ 𝑀𝑚𝑒𝑎𝑠𝑢𝑟𝑒𝑑 + 0.373
𝑅2 = 0.598
𝑀𝐴𝑀𝑎 = 1.00292 ∙ 𝑀𝑚𝑒𝑎𝑠𝑢𝑟𝑒𝑑 − 0.0038
𝑅2 = 0.696
𝑀2−𝑃𝑎𝑟𝑎𝑚 = 0.767 ∙ 𝑀𝑚𝑒𝑎𝑠𝑢𝑟𝑒𝑑 + 0.2303
𝑅2 = 0.817
2-Var improves R2 over Pwat
2-Var improves R2 over AMa
𝑀𝐴𝐸 = 0.0188;
𝑀𝐴𝐸 = 0.00406; 𝑀𝐴𝐸 = 0.00306;
𝑀𝐴𝐸 = 0.0162;
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Cocoa, Florida
CdTe
Previous Correlation New Correlation
Multi-Si
𝑀𝑃𝑤𝑎𝑡 = 0.5420 ∙ 𝑀𝑚𝑒𝑎𝑠𝑢𝑟𝑒𝑑 + 0.476
𝑅2 = 0. 494
𝑀2−𝑃𝑎𝑟𝑎𝑚 = 0.5805 ∙ 𝑀𝑚𝑒𝑎𝑠𝑢𝑟𝑒𝑑 + 0.436
𝑅2 = 0.705
𝑀𝐴𝑀𝑎 = 0.9435 ∙ 𝑀𝑀𝑒𝑎𝑠𝑢𝑟𝑒𝑑 + 0.0439
𝑅2 = 0.428
𝑀2−𝑃𝑎𝑟𝑎𝑚 = 0.9326 ∙ 𝑀𝑚𝑒𝑎𝑠𝑢𝑟𝑒 + 0.0603
𝑅2 = 0. 724
2-Var improves R2 compared to Pwat correlation
2-Var improves R2 compared to AMa correlation
𝑀𝐴𝐸 = 0.0169;
𝑀𝐴𝐸 = 0.0130; 𝑀𝐴𝐸 = 0.00749;
𝑀𝐴𝐸 = 0.0157;
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Precipitable Water Data
United States
Always available
• TMY3
• MERRA
• Empirical derivation
• Meteonorm
Sometimes Available
• Aeronet
• Suominet
World
Always Available
• MERRA
• Empirical derivation
• Meteonorm
Sometimes Available
• Aeronet
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Measured vs Empirical Pwat
Suominet vs Empirical Formula1-2
1. C. Gueymard, “Analysis of Monthly Average Atmospheric Precipitable Water andTurbidity in Canada and Northern United States,” Solar Energy, vol. 53, No.1, pp. 57-71, 1994.
2. C. Gueymard, “Assessment of the Accuracy and Computing speed of SimplifiedSaturation Vapor Equations Using a New Reference Dataset,” Journal of AppliedMeteorology, vol. 32, pp 1294-1300, 1993.
𝑃𝑤𝑎𝑡 = 𝑓(𝑇amb, RH) = 0.1 0.4976 + 1.5265𝑇𝑎𝑚𝑏,𝐾
273.15
+ 𝑒𝑥𝑝 13.6897𝑇𝑎𝑚𝑏,𝐾273.15
− 14.9188𝑇𝑎𝑚𝑏,𝐾273.15
3
× 216.7𝑅𝐻
100𝑇𝑎𝑚𝑏,𝐾𝑒𝑥𝑝 22.33 −
4,914
𝑇𝑎𝑚𝑏,𝐾
−10.922100
𝑇𝑎𝑚𝑏,𝐾
2
−0.39015 𝑇𝑎𝑚𝑏,𝐾
100
MAE = 0.245
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Measured vs Empirical Pwat
Suominet vs Empirical Formula1-2
1. C. Gueymard, “Analysis of Monthly Average Atmospheric Precipitable Water andTurbidity in Canada and Northern United States,” Solar Energy, vol. 53, No.1, pp. 57-71, 1994.
2. C. Gueymard, “Assessment of the Accuracy and Computing speed of SimplifiedSaturation Vapor Equations Using a New Reference Dataset,” Journal of AppliedMeteorology, vol. 32, pp 1294-1300, 1993.
𝑃𝑤𝑎𝑡 = 𝑓(𝑇amb, RH) = 0.1 0.4976 + 1.5265𝑇𝑎𝑚𝑏,𝐾
273.15
+ 𝑒𝑥𝑝 13.6897𝑇𝑎𝑚𝑏,𝐾273.15
− 14.9188𝑇𝑎𝑚𝑏,𝐾273.15
3
× 216.7𝑅𝐻
100𝑇𝑎𝑚𝑏,𝐾𝑒𝑥𝑝 22.33 −
4,914
𝑇𝑎𝑚𝑏,𝐾
−10.922100
𝑇𝑎𝑚𝑏,𝐾
2
−0.39015 𝑇𝑎𝑚𝑏,𝐾
100
MAE = 0.005
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Measured vs Empirical Pwat
Suominet vs Empirical Formula1-2
1. C. Gueymard, “Analysis of Monthly Average Atmospheric Precipitable Water andTurbidity in Canada and Northern United States,” Solar Energy, vol. 53, No.1, pp. 57-71, 1994.
2. C. Gueymard, “Assessment of the Accuracy and Computing speed of SimplifiedSaturation Vapor Equations Using a New Reference Dataset,” Journal of AppliedMeteorology, vol. 32, pp 1294-1300, 1993.
𝑃𝑤𝑎𝑡 = 𝑓(𝑇amb, RH) = 0.1 0.4976 + 1.5265𝑇𝑎𝑚𝑏,𝐾
273.15
+ 𝑒𝑥𝑝 13.6897𝑇𝑎𝑚𝑏,𝐾273.15
− 14.9188𝑇𝑎𝑚𝑏,𝐾273.15
3
× 216.7𝑅𝐻
100𝑇𝑎𝑚𝑏,𝐾𝑒𝑥𝑝 22.33 −
4,914
𝑇𝑎𝑚𝑏,𝐾
−10.922100
𝑇𝑎𝑚𝑏,𝐾
2
−0.39015 𝑇𝑎𝑚𝑏,𝐾
100
MAE = 0.001
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Conclusion
• The proposed two parameter spectral correction was as good, or better than, existing simple corrections in all cases.
• It enables the use of a simple functional form which works for both c-Si and CdTe.
• We recommend that all PV prediction software include this two variable correlation. A preliminary version of our spectral correction is in PVLib.
• High Pwat climates, prediction software is under predicting energy• Empirically based Pwat is sufficient for spectral correction of PV models
𝑀 = 𝑏0 + 𝑏1 ∙ 𝐴𝑀𝑎+ 𝑏2 ∙ 𝑝𝑤𝑎𝑡 + 𝑏3 ∙ 𝐴𝑀𝑎 + 𝑏4 ∙ 𝑝𝑤𝑎𝑡 + 𝑏5 ∙
𝐴𝑀𝑎
𝑝𝑤𝑎𝑡
2-Parameter Correlation
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Acknowledgements
• Sandia
— Cliff Hansen for provide insight into how to improve our spectral model
• NREL
— Bill Marion and others who made field data set possible
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Regression Fit to SMARTS Output
R2 SSE
Model Equation S4-2 Mono-Si S4-2 Mono-Si
Linear 1𝑀 = 𝑏0 + 𝑏1 ∙ 𝐴𝑀𝑎
+ 𝑏2 ∙ 𝑝𝑤𝑎𝑡 + 𝑏3 ∙ 𝐴𝑀𝑎 + 𝑏4 ∙ 𝑝𝑤𝑎𝑡 + 𝑏5 ∙𝐴𝑀𝑎𝑝𝑤𝑎𝑡
0.9965 0.9988 0.0112 0.0011
Linear 2𝑀 = 𝑏0 + 𝑏1 ∙ 𝐴𝑀𝑎
+ 𝑏2 ∙ 𝑝𝑤𝑎𝑡 + 𝑏3 ∙ 𝐴𝑀𝑎 + 𝑏4 ∙ 𝑝𝑤𝑎𝑡 + 𝑏5 ∙𝐴𝑀𝑎𝑝𝑤𝑎𝑡
0.9988 0.9990 0.0038 0.000879
Non-Linear 1𝑀 = 𝑏0 + 𝑏1 ∙ 𝐴𝑀𝑎
+ 𝑏2 ∙ 𝑝𝑤𝑎𝑡 + 𝑏3 ∙ 𝐴𝑀𝑎
𝑏6+ 𝑏4 ∙ 𝑝𝑤𝑎𝑡
𝑏7 + 𝑏5 ∙𝐴𝑀𝑎𝑝𝑤𝑎𝑡
0.9970 0.9989 0.0060 0.0009626
Non-Linear 2𝑀 = 𝑏0 + 𝑏1 ∙ 𝐴𝑀𝑎
+ 𝑏2 ∙ 𝑝𝑤𝑎𝑡 + 𝑏3 ∙ 𝐴𝑀𝑎
𝑏6+ 𝑏4 ∙ 𝑝𝑤𝑎𝑡
𝑏7 + 𝑏5 ∙𝐴𝑀𝑎𝑝𝑤𝑎𝑡
𝑏8 0.9981 0.9995 0.0060 0.000413
Non-Linear 3 𝑀 = 𝑏0 + 𝑏1 ∙ 𝐴𝑀𝑎+ 𝑏2 ∙ 𝑝𝑤𝑎𝑡 + 𝑏3 ∙ 𝐴𝑀𝑎
𝑏7+ 𝑏4 ∙ 𝑝𝑤𝑎𝑡
𝑏8 + 𝑏5 ∙ 𝐴𝑀𝑎
𝑏9∙ 𝑝𝑤𝑎𝑡
𝑏10 0.9992 0.9996 0.0026 0.00036
Non-Linear 4 𝑀 = 𝑏0 + 𝑏1 ∙ 𝐴𝑀𝑎
𝑏4+ 𝑏2 ∙ 𝑝𝑤𝑎𝑡
𝑏5 + 𝑏3 ∙ 𝐴𝑀𝑎
𝑏6∙ 𝑝𝑤𝑎𝑡
𝑏7 0.9981 0.9976 0.0046 0.0021