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LCIA Method Data set: Global Warming Potential - fossil fuels (GWP-fossil) (en) en de
Key Data Set Information
Name Global Warming Potential - fossil fuels (GWP-fossil)
Belongs to: Name of LCIA methodology/ies
  • Environmental Footprint
Impact category/ies
  • Climate change
Impact indicator Radiative forcing as Global Warming Potential (GWP100)
General comment Baseline model of the IPCC 2013 + some factors adapted from EF guidance
External documentation / files source
Quantitative reference
Reference quantity
Time representativeness
Reference year 2017
Duration of modelled impact time independent
Geographical representativeness
Intervention location GLO
Impact location GLO
Geographical representativeness description Applicable to world
Impact model
LCIA characterisation model(s) name(s) Baseline model of 100 years of the IPCC
LCIA characterisation model description and included sub-models IPCC model to calculate the relative contribution of different emissions to Global Warming.
Considered environmental or other mechanisms along the impact chain Radiative forcing, including Carbon Feedback
Use advice for data set Timeframe of 100years only.
LCIA method, normalisation, weighting
Type of data set Mid-point indicator
LCIA method principle(s)
  • other
Deviation from LCIA method principle(s) Effective volumes
Normalisation included? No
Weighting included? No
Completeness
Number of basic inventory items covered 217
Commissioner and goal
Commissioner of data set
Project Data set original development within IPCC 5th Assessment Report.
Intended applications Provide globally applicable baseline impact factors for the impact category "Climate change" (midpoint level).
Data generator
Data set generator / modeller
Data entry by
Time stamp (last saved) 2017-01-12T15:25:20.840+01:00
Data set format(s)
Reference to origin of data set
Data entry by
Official recommendation
Recommendation level of LCIA method data set Level III
Publication and ownership
UUID 5f635281-343e-44fb-83df-1971b155e6b6
Date of last revision 2016-12-20T00:00:00
Data set version 01.00.009
Workflow and publication status Data set finalised; entirely published
Owner of data set
Copyright Yes
Access and use restrictions The data set can be used free of charge by anybody to perform LCA studies, to distribute it to third parties, to convert it to other formats, to develop own data sets etc. as long as the ILCD format is mantained. Please note e.g. that reference must be given to the 'Owner of data set' (who may have additional copyright and license requirements on the particular data set that are to be met). Please note also that any modifications/omissions of the data set results in invalidity of any existing 'Official recommendation of data set by governmental body'
Flow Classification Location Exchange direction Mean value Minimum value Maximum value Uncertainty distribution type Relative StdDev in % Data derivation type / status Deviating recommendation Reference to data source(s)
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 0.0961 % Calculated
not available Output 0.0961 % Calculated
not available Output 0.0961 % Calculated
not available Output 0.0961 % Calculated
not available Output 0.0961 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 0.284 % Calculated
not available Output 0.284 % Calculated
not available Output 0.284 % Calculated
not available Output 0.284 % Calculated
not available Output 0.284 % Calculated
not available Output 0.347 % Calculated
not available Output 0.347 % Calculated
not available Output 0.347 % Calculated
not available Output 0.347 % Calculated
not available Output 0.347 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 7370.0 % Unknown derivation
not available Output 7370.0 % Unknown derivation
not available Output 7370.0 % Unknown derivation
not available Output 7370.0 % Unknown derivation
not available Output 3860.0 % Unknown derivation
not available Output 3860.0 % Unknown derivation
not available Output 3860.0 % Unknown derivation
not available Output 3860.0 % Unknown derivation
not available Output 1600.0 % Unknown derivation
not available Output 1600.0 % Unknown derivation
not available Output 1600.0 % Unknown derivation
not available Output 1600.0 % Unknown derivation
not available Output 221.0 % Calculated
not available Output 221.0 % Calculated
not available Output 221.0 % Calculated
not available Output 221.0 % Calculated
not available Output 221.0 % Calculated
not available Output 403.0 % Calculated
not available Output 403.0 % Calculated
not available Output 403.0 % Calculated
not available Output 403.0 % Calculated
not available Output 5510.0 % Calculated
not available Output 5510.0 % Calculated
not available Output 5510.0 % Calculated
not available Output 5510.0 % Calculated
not available Output 1050.0 % Calculated
not available Output 1050.0 % Calculated
not available Output 1050.0 % Calculated
not available Output 1050.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 6590.0 % Calculated
not available Output 6590.0 % Calculated
not available Output 6590.0 % Calculated
not available Output 6590.0 % Calculated
not available Output 1490.0 % Calculated
not available Output 1490.0 % Calculated
not available Output 1490.0 % Calculated
not available Output 1490.0 % Calculated
not available Output 4240.0 % Calculated
not available Output 4240.0 % Calculated
not available Output 4240.0 % Calculated
not available Output 4240.0 % Calculated
not available Output 5250.0 % Calculated
not available Output 5250.0 % Calculated
not available Output 5250.0 % Calculated
not available Output 5250.0 % Calculated
not available Output 5740.0 % Calculated
not available Output 5740.0 % Calculated
not available Output 5740.0 % Calculated
not available Output 5740.0 % Calculated
not available Output 38.0 % Calculated
not available Output 38.0 % Calculated
not available Output 38.0 % Calculated
not available Output 38.0 % Calculated
not available Output 33.0 % Calculated
not available Output 33.0 % Calculated
not available Output 33.0 % Calculated
not available Output 33.0 % Calculated
not available Output 569.0 % Calculated
not available Output 569.0 % Calculated
not available Output 569.0 % Calculated
not available Output 569.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 74.0 % Unknown derivation
not available Output 74.0 % Unknown derivation
not available Output 74.0 % Unknown derivation
not available Output 74.0 % Unknown derivation
not available Output 28.0 % Unknown derivation
not available Output 28.0 % Unknown derivation
not available Output 28.0 % Unknown derivation
not available Output 28.0 % Unknown derivation
not available Output 24.0 % Calculated
not available Output 24.0 % Calculated
not available Output 24.0 % Calculated
not available Output 24.0 % Calculated
not available Output 24.0 % Calculated
not available Output 8.0 % Calculated
not available Output 8.0 % Calculated
not available Output 8.0 % Calculated
not available Output 8.0 % Calculated
not available Output 41.0 % Calculated
not available Output 41.0 % Calculated
not available Output 41.0 % Calculated
not available Output 41.0 % Calculated
not available Output 23.0 % Calculated
not available Output 23.0 % Calculated
not available Output 23.0 % Calculated
not available Output 23.0 % Calculated
not available Output 20.0 % Calculated
not available Output 20.0 % Calculated
not available Output 20.0 % Calculated
not available Output 20.0 % Calculated
not available Output 41.0 % Calculated
not available Output 41.0 % Calculated
not available Output 41.0 % Calculated
not available Output 41.0 % Calculated
not available Output 16.0 % Calculated
not available Output 16.0 % Calculated
not available Output 16.0 % Calculated
not available Output 16.0 % Calculated
not available Output 16.0 % Calculated
not available Output 16.0 % Calculated
not available Output 16.0 % Calculated
not available Output 16.0 % Calculated
not available Output 21.0 % Calculated
not available Output 21.0 % Calculated
not available Output 21.0 % Calculated
not available Output 21.0 % Calculated
not available Output 4.0 % Calculated
not available Output 4.0 % Calculated
not available Output 4.0 % Calculated
not available Output 4.0 % Calculated
not available Output 149.0 % Calculated
not available Output 149.0 % Calculated
not available Output 149.0 % Calculated
not available Output 149.0 % Calculated
not available Output 68.0 % Calculated
not available Output 68.0 % Calculated
not available Output 68.0 % Calculated
not available Output 68.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 0.474 % Calculated
not available Output 0.474 % Calculated
not available Output 0.474 % Calculated
not available Output 0.474 % Calculated
not available Output 0.0131 % Calculated
not available Output 0.0131 % Calculated
not available Output 0.0131 % Calculated
not available Output 0.0131 % Calculated
not available Output 21.0 % Calculated
not available Output 21.0 % Calculated
not available Output 21.0 % Calculated
not available Output 21.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 0.166 % Calculated
not available Output 0.166 % Calculated
not available Output 0.166 % Calculated
not available Output 0.166 % Calculated
not available Output 0.131 % Calculated
not available Output 0.131 % Calculated
not available Output 0.131 % Calculated
not available Output 0.131 % Calculated
not available Output 0.398 % Calculated
not available Output 0.398 % Calculated
not available Output 0.398 % Calculated
not available Output 0.398 % Calculated
not available Output 0.113 % Calculated
not available Output 0.113 % Calculated
not available Output 0.113 % Calculated
not available Output 0.113 % Calculated
not available Output 0.229 % Calculated
not available Output 0.229 % Calculated
not available Output 0.229 % Calculated
not available Output 0.229 % Calculated
not available Output 0.023 % Calculated
not available Output 0.023 % Calculated
not available Output 0.023 % Calculated
not available Output 0.023 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 0.0 % Calculated
not available Output 1.57 % Calculated
not available Output 1.57 % Calculated
not available Output 1.57 % Calculated
not available Output 1.57 % Calculated
not available Output 1.57 % Calculated
not available Output 5350.0 % Calculated
not available Output 5350.0 % Calculated
not available Output 5350.0 % Calculated
not available Output 5350.0 % Calculated
not available Output 5350.0 % Calculated
not available Output 9620.0 % Calculated
not available Output 9620.0 % Calculated
not available Output 9620.0 % Calculated
not available Output 9620.0 % Calculated
not available Output 9620.0 % Calculated
not available Output 8520.0 % Calculated
not available Output 8520.0 % Calculated
not available Output 8520.0 % Calculated
not available Output 8520.0 % Calculated
not available Output 8520.0 % Calculated
not available Output 11500.0 % Calculated
not available Output 11500.0 % Calculated
not available Output 11500.0 % Calculated
not available Output 11500.0 % Calculated
not available Output 11500.0 % Calculated
not available Output 15500.0 % Calculated
not available Output 15500.0 % Calculated
not available Output 15500.0 % Calculated
not available Output 15500.0 % Calculated
not available Output 15500.0 % Calculated
not available Output 20.0 % Calculated
not available Output 20.0 % Calculated
not available Output 20.0 % Calculated
not available Output 20.0 % Calculated
not available Output 20.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 748.0 % Calculated
not available Output 748.0 % Calculated
not available Output 748.0 % Calculated
not available Output 748.0 % Calculated
not available Output 175.0 % Calculated
not available Output 175.0 % Calculated
not available Output 175.0 % Calculated
not available Output 175.0 % Calculated
not available Output 33.0 % Calculated
not available Output 33.0 % Calculated
not available Output 33.0 % Calculated
not available Output 33.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 159.0 % Calculated
not available Output 159.0 % Calculated
not available Output 159.0 % Calculated
not available Output 159.0 % Calculated
not available Output 15.0 % Calculated
not available Output 15.0 % Calculated
not available Output 15.0 % Calculated
not available Output 15.0 % Calculated
not available Output 0.066 % Calculated
not available Output 0.066 % Calculated
not available Output 0.066 % Calculated
not available Output 0.066 % Calculated
not available Output 454.0 % Calculated
not available Output 454.0 % Calculated
not available Output 454.0 % Calculated
not available Output 454.0 % Calculated
not available Output 454.0 % Calculated
not available Output 280.0 % Calculated
not available Output 280.0 % Calculated
not available Output 280.0 % Calculated
not available Output 280.0 % Calculated
not available Output 280.0 % Calculated
not available Output 2070.0 % Calculated
not available Output 2070.0 % Calculated
not available Output 2070.0 % Calculated
not available Output 2070.0 % Calculated
not available Output 2070.0 % Calculated
not available Output 7150.0 % Calculated
not available Output 7150.0 % Calculated
not available Output 7150.0 % Calculated
not available Output 7150.0 % Calculated
not available Output 7150.0 % Calculated
not available Output 210.0 % Calculated
not available Output 210.0 % Calculated
not available Output 210.0 % Calculated
not available Output 210.0 % Calculated
not available Output 210.0 % Calculated
not available Output 50.0 % Calculated
not available Output 50.0 % Calculated
not available Output 50.0 % Calculated
not available Output 50.0 % Calculated
not available Output 50.0 % Calculated
not available Output 223.0 % Calculated
not available Output 223.0 % Calculated
not available Output 223.0 % Calculated
not available Output 223.0 % Calculated
not available Output 223.0 % Calculated
not available Output 1730.0 % Calculated
not available Output 1730.0 % Calculated
not available Output 1730.0 % Calculated
not available Output 1730.0 % Calculated
not available Output 1730.0 % Calculated
not available Output 72.0 % Calculated
not available Output 72.0 % Calculated
not available Output 72.0 % Calculated
not available Output 72.0 % Calculated
not available Output 72.0 % Calculated
not available Output 312.0 % Calculated
not available Output 312.0 % Calculated
not available Output 312.0 % Calculated
not available Output 312.0 % Calculated
not available Output 312.0 % Calculated
not available Output 96.0 % Calculated
not available Output 96.0 % Calculated
not available Output 96.0 % Calculated
not available Output 96.0 % Calculated
not available Output 96.0 % Calculated
not available Output 447.0 % Calculated
not available Output 447.0 % Calculated
not available Output 447.0 % Calculated
not available Output 447.0 % Calculated
not available Output 447.0 % Calculated
not available Output 635.0 % Calculated
not available Output 635.0 % Calculated
not available Output 635.0 % Calculated
not available Output 635.0 % Calculated
not available Output 635.0 % Calculated
not available Output 409.0 % Calculated
not available Output 409.0 % Calculated
not available Output 409.0 % Calculated
not available Output 409.0 % Calculated
not available Output 409.0 % Calculated
not available Output 938.0 % Calculated
not available Output 938.0 % Calculated
not available Output 938.0 % Calculated
not available Output 938.0 % Calculated
not available Output 938.0 % Calculated
not available Output 2350.0 % Calculated
not available Output 2350.0 % Calculated
not available Output 2350.0 % Calculated
not available Output 2350.0 % Calculated
not available Output 179.0 % Calculated
not available Output 179.0 % Calculated
not available Output 179.0 % Calculated
not available Output 179.0 % Calculated
not available Output 179.0 % Calculated
not available Output 2110.0 % Calculated
not available Output 2110.0 % Calculated
not available Output 2110.0 % Calculated
not available Output 2110.0 % Calculated
not available Output 2110.0 % Calculated
not available Output 155.0 % Calculated
not available Output 155.0 % Calculated
not available Output 155.0 % Calculated
not available Output 155.0 % Calculated
not available Output 155.0 % Calculated
not available Output 633.0 % Calculated
not available Output 633.0 % Calculated
not available Output 633.0 % Calculated
not available Output 633.0 % Calculated
not available Output 633.0 % Calculated
not available Output 705.0 % Calculated
not available Output 705.0 % Calculated
not available Output 705.0 % Calculated
not available Output 705.0 % Calculated
not available Output 705.0 % Calculated
not available Output 595.0 % Calculated
not available Output 595.0 % Calculated
not available Output 595.0 % Calculated
not available Output 595.0 % Calculated
not available Output 595.0 % Calculated
not available Output 0.0516 % Calculated
not available Output 0.0516 % Calculated
not available Output 0.0516 % Calculated
not available Output 0.0516 % Calculated
not available Output 0.0516 % Calculated
not available Output 0.0207 % Calculated
not available Output 0.0207 % Calculated
not available Output 0.0207 % Calculated
not available Output 0.0207 % Calculated
not available Output 0.0207 % Calculated
not available Output 0.429 % Calculated
not available Output 0.429 % Calculated
not available Output 0.429 % Calculated
not available Output 0.429 % Calculated
not available Output 0.429 % Calculated
not available Output 0.181 % Calculated
not available Output 0.181 % Calculated
not available Output 0.181 % Calculated
not available Output 0.181 % Calculated
not available Output 0.181 % Calculated
not available Output 3690.0 % Calculated
not available Output 3690.0 % Calculated
not available Output 3690.0 % Calculated
not available Output 3690.0 % Calculated
not available Output 3690.0 % Calculated
not available Output 1340.0 % Calculated
not available Output 1340.0 % Calculated
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not available Output 1340.0 % Calculated
not available Output 1340.0 % Calculated
not available Output 0.154 % Calculated
not available Output 0.154 % Calculated
not available Output 0.154 % Calculated
not available Output 0.154 % Calculated
not available Output 0.154 % Calculated
not available Output 1550.0 % Calculated
not available Output 1550.0 % Calculated
not available Output 1550.0 % Calculated
not available Output 1550.0 % Calculated
not available Output 1550.0 % Calculated
not available Output 397.0 % Calculated
not available Output 397.0 % Calculated
not available Output 397.0 % Calculated
not available Output 397.0 % Calculated
not available Output 397.0 % Calculated
not available Output 20.0 % Calculated
not available Output 20.0 % Calculated
not available Output 20.0 % Calculated
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not available Output 20.0 % Calculated
not available Output 167.0 % Calculated
not available Output 167.0 % Calculated
not available Output 167.0 % Calculated
not available Output 167.0 % Calculated
not available Output 167.0 % Calculated
not available Output 4.0 % Calculated
not available Output 4.0 % Calculated
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not available Output 4.0 % Calculated
not available Output 4.0 % Calculated
not available Output 3080.0 % Calculated
not available Output 3080.0 % Calculated
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not available Output 13900.0 % Calculated
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not available Output 1440.0 % Calculated
not available Output 1440.0 % Calculated
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not available Output 9000.0 % Calculated
not available Output 9000.0 % Calculated
not available Output 9000.0 % Calculated
not available Output 9000.0 % Calculated
not available Output 9000.0 % Calculated
not available Output 863.0 % Calculated
not available Output 863.0 % Calculated
not available Output 863.0 % Calculated
not available Output 863.0 % Calculated
not available Output 863.0 % Calculated
not available Output 5300.0 % Calculated
not available Output 5300.0 % Calculated
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not available Output 285.0 % Calculated
not available Output 285.0 % Calculated
not available Output 285.0 % Calculated
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not available Output 352.0 % Calculated
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not available Output 1030.0 % Calculated
not available Output 1030.0 % Calculated
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not available Output 92.0 % Calculated
not available Output 92.0 % Calculated
not available Output 92.0 % Calculated
not available Output 92.0 % Calculated
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not available Output 175.0 % Calculated
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not available Output 817.0 % Calculated
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not available Output 2740.0 % Calculated
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not available Output 966.0 % Calculated
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not available Output 966.0 % Calculated
not available Output 966.0 % Calculated
not available Output 141.0 % Calculated
not available Output 141.0 % Calculated
not available Output 141.0 % Calculated
not available Output 141.0 % Calculated
not available Output 141.0 % Calculated
not available Output 1950.0 % Calculated
not available Output 1950.0 % Calculated
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not available Output 14000.0 % Calculated
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not available Output 6510.0 % Calculated
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not available Output 632.0 % Calculated
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not available Output 0.255 % Calculated
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not available Output 7380.0 % Calculated
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not available Output 4990.0 % Calculated
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not available Output 6260.0 % Calculated
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not available Output 2140.0 % Calculated
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not available Output 1180.0 % Calculated
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not available Output 790.0 % Calculated
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not available Output 997.0 % Calculated
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not available Output 981.0 % Calculated
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not available Output 365.0 % Calculated
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not available Output 2.0 % Calculated
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not available Output 36.0 % Calculated
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not available Output 3600.0 % Calculated
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not available Output 1120.0 % Calculated
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not available Output 3080.0 % Calculated
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not available Output 3470.0 % Calculated
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not available Output 641.0 % Calculated
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not available Output 1030.0 % Calculated
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not available Output 440.0 % Calculated
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not available Output 1070.0 % Calculated
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not available Output 468.0 % Calculated
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not available Output 20.0 % Calculated
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not available Output 17.0 % Calculated
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not available Output 500.0 % Calculated
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not available Output 867.0 % Calculated
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not available Output 540.0 % Calculated
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not available Output 71.0 % Calculated
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not available Output 71.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 1.0 % Calculated
not available Output 758.0 % Calculated
not available Output 758.0 % Calculated
not available Output 758.0 % Calculated
not available Output 3350.0 % Calculated
not available Output 758.0 % Calculated
not available Output 3350.0 % Calculated
not available Output 3350.0 % Calculated
not available Output 3350.0 % Calculated
not available Output 3350.0 % Calculated
not available Output 69.0 % Unknown derivation
not available Output 69.0 % Unknown derivation
not available Output 69.0 % Unknown derivation
not available Output 69.0 % Unknown derivation
not available Output 509.0 % Unknown derivation
not available Output 509.0 % Unknown derivation
not available Output 509.0 % Unknown derivation
not available Output 509.0 % Unknown derivation
not available Output 509.0 % Unknown derivation
not available Output 3250.0 % Calculated
not available Output 3250.0 % Calculated
not available Output 3250.0 % Calculated
not available Output 3250.0 % Calculated
not available Output 3400.0 % Calculated
not available Output 3400.0 % Calculated
not available Output 3400.0 % Calculated
not available Output 3400.0 % Calculated
not available Output 6200.0 % Calculated
not available Output 6200.0 % Calculated
not available Output 6200.0 % Calculated
not available Output 6200.0 % Calculated
not available Output 4630.0 % Calculated
not available Output 4630.0 % Calculated
not available Output 4630.0 % Calculated
not available Output 4630.0 % Calculated
not available Output 8580.0 % Calculated
not available Output 8580.0 % Calculated
not available Output 8580.0 % Calculated
not available Output 8580.0 % Calculated
not available Output 492.0 % Calculated
not available Output 492.0 % Calculated
not available Output 492.0 % Calculated
not available Output 492.0 % Calculated
not available Output 54.0 % Calculated
not available Output 54.0 % Calculated
not available Output 54.0 % Calculated
not available Output 54.0 % Calculated
not available Output 909.0 % Calculated
not available Output 909.0 % Calculated
not available Output 909.0 % Calculated
not available Output 909.0 % Calculated
not available Output 909.0 % Calculated
not available Output 36.75 % Calculated
not available Output 36.75 % Calculated
not available Output 36.75 % Calculated
not available Output 36.75 % Calculated
not available Output 36.75 % Calculated
not available Output 64.0 % Calculated
not available Output 64.0 % Calculated
not available Output 64.0 % Calculated
not available Output 64.0 % Calculated
not available Output 4.0 % Calculated
not available Output 4.0 % Calculated
not available Output 4.0 % Calculated
not available Output 4.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 116.0 % Calculated
not available Output 116.0 % Calculated
not available Output 116.0 % Calculated
not available Output 116.0 % Calculated
not available Output 193.0 % Calculated
not available Output 193.0 % Calculated
not available Output 193.0 % Calculated
not available Output 193.0 % Calculated
not available Output 712.0 % Calculated
not available Output 712.0 % Calculated
not available Output 712.0 % Calculated
not available Output 712.0 % Calculated
not available Output 712.0 % Calculated
not available Output 11.0 % Calculated
not available Output 11.0 % Calculated
not available Output 11.0 % Calculated
not available Output 11.0 % Calculated
not available Output 587.0 % Unknown derivation
not available Output 587.0 % Unknown derivation
not available Output 587.0 % Unknown derivation
not available Output 587.0 % Unknown derivation
not available Output 587.0 % Unknown derivation
not available Output 79.0 % Unknown derivation
not available Output 79.0 % Unknown derivation
not available Output 79.0 % Unknown derivation
not available Output 79.0 % Unknown derivation
not available Output 17900.0 % Calculated
not available Output 17900.0 % Calculated
not available Output 17900.0 % Calculated
not available Output 17900.0 % Calculated
not available Output 298.0 % Calculated
not available Output 298.0 % Calculated
not available Output 298.0 % Calculated
not available Output 298.0 % Calculated
not available Output 298.0 % Calculated
not available Output 0.121 % Calculated
not available Output 0.121 % Calculated
not available Output 0.121 % Calculated
not available Output 0.121 % Calculated
not available Output 0.111 % Calculated
not available Output 0.111 % Calculated
not available Output 0.111 % Calculated
not available Output 0.111 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 0.00435 % Calculated
not available Output 0.00435 % Calculated
not available Output 0.00435 % Calculated
not available Output 0.00435 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 475.0 % Calculated
not available Output 475.0 % Calculated
not available Output 475.0 % Calculated
not available Output 475.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 8030.0 % Calculated
not available Output 8030.0 % Calculated
not available Output 8030.0 % Calculated
not available Output 8030.0 % Calculated
not available Output 6980.0 % Calculated
not available Output 6980.0 % Calculated
not available Output 6980.0 % Calculated
not available Output 6980.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 703.0 % Calculated
not available Output 703.0 % Calculated
not available Output 703.0 % Calculated
not available Output 703.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 2.0 % Calculated
not available Output 456.0 % Calculated
not available Output 456.0 % Calculated
not available Output 456.0 % Calculated
not available Output 456.0 % Calculated
not available Output 0.00353 % Calculated
not available Output 0.00353 % Calculated
not available Output 0.00353 % Calculated
not available Output 0.00353 % Calculated
not available Output 12300.0 % Calculated
not available Output 12300.0 % Calculated
not available Output 12300.0 % Calculated
not available Output 12300.0 % Calculated
not available Output 0.0853 % Calculated
not available Output 0.0853 % Calculated
not available Output 0.0853 % Calculated
not available Output 0.0853 % Calculated
not available Output 7350.0 % Calculated
not available Output 7350.0 % Calculated
not available Output 7350.0 % Calculated
not available Output 7350.0 % Calculated
not available Output 9880.0 % Calculated
not available Output 9880.0 % Calculated
not available Output 9880.0 % Calculated
not available Output 9880.0 % Calculated
not available Output 10200.0 % Calculated
not available Output 10200.0 % Calculated
not available Output 10200.0 % Calculated
not available Output 10200.0 % Calculated
not available Output 10600.0 % Calculated
not available Output 10600.0 % Calculated
not available Output 10600.0 % Calculated
not available Output 10600.0 % Calculated
not available Output 9480.0 % Calculated
not available Output 9480.0 % Calculated
not available Output 9480.0 % Calculated
not available Output 9480.0 % Calculated
not available Output 8780.0 % Calculated
not available Output 8780.0 % Calculated
not available Output 8780.0 % Calculated
not available Output 8780.0 % Calculated
not available Output 8680.0 % Calculated
not available Output 8680.0 % Calculated
not available Output 8680.0 % Calculated
not available Output 8680.0 % Calculated
not available Output 8460.0 % Calculated
not available Output 8460.0 % Calculated
not available Output 8460.0 % Calculated
not available Output 8460.0 % Calculated
not available Output 7980.0 % Calculated
not available Output 7980.0 % Calculated
not available Output 7980.0 % Calculated
not available Output 7980.0 % Calculated
not available Output 10200.0 % Calculated
not available Output 10200.0 % Calculated
not available Output 10200.0 % Calculated
not available Output 10200.0 % Calculated
not available Output 10800.0 % Calculated
not available Output 10800.0 % Calculated
not available Output 10800.0 % Calculated
not available Output 10800.0 % Calculated
not available Output 262.0 % Calculated
not available Output 262.0 % Calculated
not available Output 262.0 % Calculated
not available Output 262.0 % Calculated
not available Output 262.0 % Calculated
not available Output 26100.0 % Calculated
not available Output 26100.0 % Calculated
not available Output 26100.0 % Calculated
not available Output 26100.0 % Calculated
not available Output 26100.0 % Calculated
not available Output 19400.0 % Calculated
not available Output 19400.0 % Calculated
not available Output 19400.0 % Calculated
not available Output 19400.0 % Calculated
not available Output 17900.0 % Calculated
not available Output 6590.0 % Calculated
not available Output 2350.0 % Calculated
not available Output 3860.0 % Unknown derivation
not available Output 5510.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 15.0 % Calculated
not available Output 15.0 % Calculated
not available Output 2020.0 % Calculated
not available Output 2020.0 % Calculated
not available Output 2020.0 % Calculated
not available Output 2020.0 % Calculated
not available Output 2020.0 % Calculated
not available Output 4.23 % Calculated
not available Output 4.23 % Calculated
not available Output 4.23 % Calculated
not available Output 4.23 % Calculated
not available Output 4.23 % Calculated
not available Output 2020.0 % Calculated
not available Output 2020.0 % Calculated
not available Output 2020.0 % Calculated
not available Output 2020.0 % Calculated
not available Output 2020.0 % Calculated
not available Output 15.0 % Calculated
not available Output 15.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 3.0 % Calculated
not available Output 7350.0 % Calculated
not available Output 36.75 % Calculated
not available Output 1.0 % Calculated
not available Output 1.57 % Calculated