Effect of Humidity on Charge Decay in Varying Atmospheric Gases
Characterization of surface charge decay for varying materials - PTFE, Acrylic, and metals - of 100 mm diameter, radially symmetric bodies was performed. In a gaseous environment, charged materials will lose their charge depending on gas type, humidity, and other environmental factors. Eventually, t...
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Published in: | 2021 IEEE Pulsed Power Conference (PPC) pp. 1 - 5 |
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IEEE
12-12-2021
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Abstract | Characterization of surface charge decay for varying materials - PTFE, Acrylic, and metals - of 100 mm diameter, radially symmetric bodies was performed. In a gaseous environment, charged materials will lose their charge depending on gas type, humidity, and other environmental factors. Eventually, the charge will be (1) neutralized by ions or electrons in the surrounding gas (2) distributed by conduction on the material surface or in its volume (3) or neutralized by ions or electrons in the material surface and volume. Metal and polymer samples are charged to a known potential in the tens of kilovolts range, and the decaying voltage is monitored with a non-contact probe until the potential reaches near zero. Humidity has an impact on both groups of materials. As a baseline, in air at 42% relative humidity in an enclosed chamber, a positive charge equivalent to 20 kV potential on a metal sphere of 50 mm radius decays to near zero within 25 minutes. In contrast, the same sphere negatively charged decays slightly faster within 20 minutes. Overall, the humidity has a significant effect on the charge decay time, such that an order of magnitude longer times (hours) are observed at low humidity. Effects of chamber size were also studied, drawing a connection to charge carriers in the air available for decay, with chambers of volume(s): 3.3 10 5 cm 3 and 1.4 10 6 cm 3 , respectively. |
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AbstractList | Characterization of surface charge decay for varying materials - PTFE, Acrylic, and metals - of 100 mm diameter, radially symmetric bodies was performed. In a gaseous environment, charged materials will lose their charge depending on gas type, humidity, and other environmental factors. Eventually, the charge will be (1) neutralized by ions or electrons in the surrounding gas (2) distributed by conduction on the material surface or in its volume (3) or neutralized by ions or electrons in the material surface and volume. Metal and polymer samples are charged to a known potential in the tens of kilovolts range, and the decaying voltage is monitored with a non-contact probe until the potential reaches near zero. Humidity has an impact on both groups of materials. As a baseline, in air at 42% relative humidity in an enclosed chamber, a positive charge equivalent to 20 kV potential on a metal sphere of 50 mm radius decays to near zero within 25 minutes. In contrast, the same sphere negatively charged decays slightly faster within 20 minutes. Overall, the humidity has a significant effect on the charge decay time, such that an order of magnitude longer times (hours) are observed at low humidity. Effects of chamber size were also studied, drawing a connection to charge carriers in the air available for decay, with chambers of volume(s): 3.3 10 5 cm 3 and 1.4 10 6 cm 3 , respectively. |
Author | Mankowski, John Neuber, Andreas Dickens, James Stephens, Jacob Friesen, Donald Koone, Neil Cardenas, Zachary Esser, Ben Aponte, Ivan Nelson, Crystal Hattz, David |
Author_xml | – sequence: 1 givenname: Zachary surname: Cardenas fullname: Cardenas, Zachary email: zachary.cardenas@ttu.edu organization: Texas Tech University,Center for Pulsed Power and Power Electronics (P3E),Lubbock,USA – sequence: 2 givenname: Ben surname: Esser fullname: Esser, Ben email: ben.esser@ttu.edu organization: Texas Tech University,Center for Pulsed Power and Power Electronics (P3E),Lubbock,USA – sequence: 3 givenname: Ivan surname: Aponte fullname: Aponte, Ivan email: ivan.aponte@ttu.edu organization: Texas Tech University,Center for Pulsed Power and Power Electronics (P3E),Lubbock,USA – sequence: 4 givenname: James surname: Dickens fullname: Dickens, James email: james.Dickens@ttu.edu organization: Texas Tech University,Center for Pulsed Power and Power Electronics (P3E),Lubbock,USA – sequence: 5 givenname: John surname: Mankowski fullname: Mankowski, John email: john.mankowski@ttu.edu organization: Texas Tech University,Center for Pulsed Power and Power Electronics (P3E),Lubbock,USA – sequence: 6 givenname: Jacob surname: Stephens fullname: Stephens, Jacob email: jacob.c.stephens@ttu.edu organization: Texas Tech University,Center for Pulsed Power and Power Electronics (P3E),Lubbock,USA – sequence: 7 givenname: Donald surname: Friesen fullname: Friesen, Donald email: donald.friesen@cns.doe.gov organization: CNS Pantex,Mission Engineering Development Group,Amarillo,USA – sequence: 8 givenname: Crystal surname: Nelson fullname: Nelson, Crystal email: crystal.nelson@cns.doe.edu organization: CNS Pantex,Facility Engineering Electromagnetics Group,Amarillo,USA – sequence: 9 givenname: Neil surname: Koone fullname: Koone, Neil email: neil.koone@cns.doe.gov organization: CNS Pantex,Facility Engineering Electromagnetics Group,Amarillo,USA – sequence: 10 givenname: David surname: Hattz fullname: Hattz, David email: david.hattz@cns.doe.gov organization: CNS Pantex,Facility Engineering Electromagnetics Group,Amarillo,USA – sequence: 11 givenname: Andreas surname: Neuber fullname: Neuber, Andreas email: Andreas.Neuber@ttu.edu organization: Texas Tech University,Center for Pulsed Power and Power Electronics (P3E),Lubbock,USA |
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Snippet | Characterization of surface charge decay for varying materials - PTFE, Acrylic, and metals - of 100 mm diameter, radially symmetric bodies was performed. In a... |
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SubjectTerms | Charge carriers Charge decay dielectric surface charge Electric potential Humidity Ions Metals Surface resistance Voltage |
Title | Effect of Humidity on Charge Decay in Varying Atmospheric Gases |
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