Removal of 2-Heptanone by Dielectric Barrier Discharges - The Effect of a Catalyst Support
2‐heptanone is representative of a class of odorous molecules. Recent studies have shown that by adding a catalyst to a dielectric barrier discharge (DBD) plasma, the elimination of 90% of this molecule can be achieved with low consumption of electric energy, at room temperature, for concentrations...
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Veröffentlicht in: | Plasma processes and polymers 2005-03, Vol.2 (3), p.256-262 |
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description | 2‐heptanone is representative of a class of odorous molecules. Recent studies have shown that by adding a catalyst to a dielectric barrier discharge (DBD) plasma, the elimination of 90% of this molecule can be achieved with low consumption of electric energy, at room temperature, for concentrations below 1 000 ppm. In the presented work, the removal of the ketone by DBD, both in dry air and within a slice of a honeycomb monolith of cordierite without a catalyst, was studied. In both experiments, the discharge was operated in a plane‐to‐plane geometry with a discharge volume of 10 cm3. A high voltage, bipolar pulse generator (40 kV max, 1–140 Hz frequency range) was used. In dry air, it was found that 2‐heptanone is almost totally removed (>95%) for a specific deposited energy of about 500 J · l−1, but this elimination is less effective in the porous cordierite reactor (80%) for the same energy. This effect is explained by the very different spatial distribution of the plasma within the discharge volume, as seen using a CCD camera. Moreover, the adsorption‐desorption equilibrium of the molecule at the surface of the material is greatly influenced by the discharge.
2‐Heptanone removal as a function of the specific energy for the DBD both in dry air and in the cordierite catalyst support. |
doi_str_mv | 10.1002/ppap.200400088 |
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2‐Heptanone removal as a function of the specific energy for the DBD both in dry air and in the cordierite catalyst support.</description><subject>2-heptanone</subject><subject>catalysts support</subject><subject>dielectric barrier discharges (DBD)</subject><subject>nonthermal plasma</subject><subject>volatile organic compounds (VOC)</subject><issn>1612-8850</issn><issn>1612-8869</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNqFkDFPwzAQRiMEEqWwMntiSzk7ceyMpYUWqSoVFFVisRznQgNpE-wUyL8nVVDFxvSdTu-dTp_nXVIYUAB2XVW6GjCAEACkPPJ6NKLMlzKKjw8zh1PvzLk3gAC4hJ738oib8lMXpMwI86dY1XpbbpEkDRnnWKCpbW7IjbY2R9uunFlr-4qO-GS5RnKbZS2ylzUZ6VoXjavJ066qSlufeyeZLhxe_Gbfe767XY6m_uxhcj8aznwTslD6aBgkkaQmFCmwgIosSSPKKUIbEYQyZSFQMEkaJpqJNOYcQTM0Is4SCkHQ9666u5UtP3boarVp38Si0Fssd06xmAopgrAFBx1obOmcxUxVNt9o2ygKal-h2leoDhW2QtwJX3mBzT-0WiyGi7-u37m5q_H74Gr7riIRCK5W84kar-azxZxzJYMfuiiDiA</recordid><startdate>20050331</startdate><enddate>20050331</enddate><creator>Blin-Simiand, Nicole</creator><creator>Tardiveau, Pierre</creator><creator>Risacher, Aurore</creator><creator>Jorand, François</creator><creator>Pasquiers, Stéphane</creator><general>WILEY-VCH Verlag</general><general>WILEY‐VCH Verlag</general><scope>BSCLL</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20050331</creationdate><title>Removal of 2-Heptanone by Dielectric Barrier Discharges - The Effect of a Catalyst Support</title><author>Blin-Simiand, Nicole ; Tardiveau, Pierre ; Risacher, Aurore ; Jorand, François ; Pasquiers, Stéphane</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4248-ec20b681c47d02317fbd6151e0d616048d24010cbd4ba27d955e0a2ec79fb1033</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2005</creationdate><topic>2-heptanone</topic><topic>catalysts support</topic><topic>dielectric barrier discharges (DBD)</topic><topic>nonthermal plasma</topic><topic>volatile organic compounds (VOC)</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Blin-Simiand, Nicole</creatorcontrib><creatorcontrib>Tardiveau, Pierre</creatorcontrib><creatorcontrib>Risacher, Aurore</creatorcontrib><creatorcontrib>Jorand, François</creatorcontrib><creatorcontrib>Pasquiers, Stéphane</creatorcontrib><collection>Istex</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Plasma processes and polymers</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Blin-Simiand, Nicole</au><au>Tardiveau, Pierre</au><au>Risacher, Aurore</au><au>Jorand, François</au><au>Pasquiers, Stéphane</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Removal of 2-Heptanone by Dielectric Barrier Discharges - The Effect of a Catalyst Support</atitle><jtitle>Plasma processes and polymers</jtitle><addtitle>Plasma Processes Polym</addtitle><date>2005-03-31</date><risdate>2005</risdate><volume>2</volume><issue>3</issue><spage>256</spage><epage>262</epage><pages>256-262</pages><issn>1612-8850</issn><eissn>1612-8869</eissn><abstract>2‐heptanone is representative of a class of odorous molecules. Recent studies have shown that by adding a catalyst to a dielectric barrier discharge (DBD) plasma, the elimination of 90% of this molecule can be achieved with low consumption of electric energy, at room temperature, for concentrations below 1 000 ppm. In the presented work, the removal of the ketone by DBD, both in dry air and within a slice of a honeycomb monolith of cordierite without a catalyst, was studied. In both experiments, the discharge was operated in a plane‐to‐plane geometry with a discharge volume of 10 cm3. A high voltage, bipolar pulse generator (40 kV max, 1–140 Hz frequency range) was used. In dry air, it was found that 2‐heptanone is almost totally removed (>95%) for a specific deposited energy of about 500 J · l−1, but this elimination is less effective in the porous cordierite reactor (80%) for the same energy. This effect is explained by the very different spatial distribution of the plasma within the discharge volume, as seen using a CCD camera. Moreover, the adsorption‐desorption equilibrium of the molecule at the surface of the material is greatly influenced by the discharge.
2‐Heptanone removal as a function of the specific energy for the DBD both in dry air and in the cordierite catalyst support.</abstract><cop>Weinheim</cop><pub>WILEY-VCH Verlag</pub><doi>10.1002/ppap.200400088</doi><tpages>7</tpages></addata></record> |
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subjects | 2-heptanone catalysts support dielectric barrier discharges (DBD) nonthermal plasma volatile organic compounds (VOC) |
title | Removal of 2-Heptanone by Dielectric Barrier Discharges - The Effect of a Catalyst Support |
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