{"id":244476,"date":"2024-10-19T16:03:45","date_gmt":"2024-10-19T16:03:45","guid":{"rendered":"https:\/\/pdfstandards.shop\/product\/uncategorized\/bs-en-61207-62015\/"},"modified":"2024-10-25T11:02:59","modified_gmt":"2024-10-25T11:02:59","slug":"bs-en-61207-62015","status":"publish","type":"product","link":"https:\/\/pdfstandards.shop\/product\/publishers\/bsi\/bs-en-61207-62015\/","title":{"rendered":"BS EN 61207-6:2015"},"content":{"rendered":"

This part of IEC 61207<\/span> <\/span> applies to all aspects of analyzers using photometric techniques for the measurement of concentration of one or more components in a mixture of gases or vapors. It should be used in conjunction with IEC 61207\u20111<\/span> <\/span>.<\/p>\n

For photometric analyzers utilizing tuneable semiconductor laser absorption spectroscopy (TSLAS) for gas measurements, IEC 61207\u20117<\/span> <\/span> should also be referred to.<\/p>\n

This part of IEC 61207<\/span> <\/span> applies to analyzers using non-dispersive and dispersive wavelength selection and using absorption, emission, wavelength derivative or scattering techniques.<\/p>\n

It applies to analyzers which receive either a conditioned or unconditioned sample of gas either under vacuum, at ambient pressure or pressurized.<\/p>\n

It applies to analyzers which measure gas concentrations directly within the sample gas.<\/p>\n

The object of this part is:<\/p>\n