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Método de EICV-- Datos: Potencial de calentamiento global de los combustibles fósiles (GWP-fossil) (es) en es de
Información general
Nombre Potencial de calentamiento global de los combustibles fósiles (GWP-fossil)
Pertenece a: Nombre de la(s) metodología(s) de EICV
  • Environmental Footprint
Categoría(s) de impacto
  • Climate change
Indicador de impacto Radiative forcing as Global Warming Potential (GWP100)
Comentario general Baseline model of the IPCC 2013 + some factors adapted from EF guidance
Documentación externa/ fuente de archivos
Referencia cuantitativa
Cantidad de referencia
Representatividad temporal
Año de referencia 2017
Duración del impacto modelado time independent
Representatividad geográfica
Ubicación de la intervención GLO
Ubicación del impacto GLO
Descripción de la representatividad geográfica Applicable to world
Modelo de impacto
Nombre(s) del modelo(s) de caracterización de la EICV Baseline model of 100 years of the IPCC
Descripción del modelo de caracterización de la EICV y sub-modelos incluidos IPCC model to calculate the relative contribution of different emissions to Global Warming.
Mecanismos ambientales u otros considerados a lo largo de toda la cadena de impactos Radiative forcing, including Carbon Feedback
Recomendaciones de uso de los datos Timeframe of 100years only.
Método de EICV, normalización, ponderación
Tipo de datos Mid-point indicator
Principio(s) del método de EICV
  • other
Desviación respecto a los principios del método de EICV Effective volumes
Normalización incluida? No
Ponderación incluída? No
Criterios de exclusión
Número de elementos de inventario básico contemplados 217
Propietario y objetivo
Propietario de los datos
Proyecto Data set original development within IPCC 5th Assessment Report.
Aplicaciones previstas Provide globally applicable baseline impact factors for the impact category "Climate change" (midpoint level).
Datos generados por
Generador de datos/modelador
Datos introducidos por
Fecha y hora del último guardado 2022-03-25T13:03:24.640+01:00
Formato(s) de los datos
Referencia al origen de los datos
Datos introducidos por
Recomendación oficial
Nivel recomendado de datos para el método de EICV Level III
Publicación y propiedad
UUID 5f635281-343e-44fb-83df-1971b155e6b6
Fecha de la última revisión 2016-12-20T00:00:00
Versión 01.00.011
Estado del flujo de trabajo y la publicación Data set finalised; entirely published
Propietario de los datos
Copyright Si
Restricciones de acceso y uso 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'
Flujo Clasificación Ubicación Cambiar dirección Valor medio Valor mínimo Valor máximo Tipo de distribución de la incertidumbre Desviación estándar relativa en % Tipo de derivación de datos/estado Recomendación de desviación Referencia a la fuente(s) de datos
not available Output 2.0 % Calculated
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not available Output 0.0961 % Calculated
not available Output 0.0961 % Calculated
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not available Output 1.0 % Calculated
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not available Output 0.284 % Calculated
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not available Output 0.347 % Calculated
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not available Output 2.0 % Calculated
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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
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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
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not available Output 221.0 % Calculated
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not available Output 5740.0 % Calculated
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not available Output 569.0 % Calculated
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not available Output 1.0 % Calculated
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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
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not available Output 149.0 % Calculated
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not available Output 68.0 % Calculated
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not available Output 0.474 % Calculated
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not available Output 0.0131 % Calculated
not available Output 0.0131 % Calculated
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not available Output 21.0 % Calculated
not available Output 21.0 % Calculated
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not available Output 1.0 % Calculated
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not available Output 0.166 % Calculated
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not available Output 0.131 % Calculated
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not available Output 0.398 % Calculated
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not available Output 0.113 % Calculated
not available Output 0.113 % Calculated
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not available Output 0.229 % Calculated
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not available Output 0.023 % Calculated
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not available Output 1.57 % Calculated
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not available Output 5350.0 % Calculated
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not available Output 9620.0 % Calculated
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not available Output 11500.0 % Calculated
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not available Output 748.0 % Calculated
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not available Output 175.0 % Calculated
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not available Output 33.0 % Calculated
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not available Output 159.0 % Calculated
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not available Output 0.066 % Calculated
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not available Output 454.0 % Calculated
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not available Output 280.0 % Calculated
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not available Output 2070.0 % Calculated
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not available Output 7150.0 % Calculated
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not available Output 210.0 % Calculated
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not available Output 50.0 % Calculated
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not available Output 223.0 % Calculated
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not available Output 1730.0 % Calculated
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not available Output 72.0 % Calculated
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not available Output 312.0 % Calculated
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not available Output 96.0 % Calculated
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not available Output 447.0 % Calculated
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not available Output 409.0 % Calculated
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not available Output 2110.0 % Calculated
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not available Output 155.0 % Calculated
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not available Output 633.0 % Calculated
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not available Output 705.0 % Calculated
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not available Output 595.0 % Calculated
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not available Output 0.0516 % Calculated
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not available Output 0.0207 % Calculated
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not available Output 0.429 % Calculated
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not available Output 0.181 % Calculated
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not available Output 0.154 % Calculated
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not available Output 5300.0 % 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 468.0 % 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 17.0 % Calculated
not available Output 17.0 % Calculated
not available Output 17.0 % Calculated
not available Output 17.0 % Calculated
not available Output 500.0 % Calculated
not available Output 500.0 % Calculated
not available Output 500.0 % Calculated
not available Output 500.0 % Calculated
not available Output 867.0 % Calculated
not available Output 867.0 % Calculated
not available Output 867.0 % Calculated
not available Output 867.0 % Calculated
not available Output 540.0 % Calculated
not available Output 540.0 % Calculated
not available Output 540.0 % Calculated
not available Output 540.0 % Calculated
not available Output 540.0 % Calculated
not available Output 71.0 % Calculated
not available Output 71.0 % Calculated
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