Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion
Molecular communication (MC) is a method where the transmission of information involves the use of chemicals or molecules instead of electromagnetic waves. The study of MC to date has mostly focused on the nano (nm) to micro (μm) scale and there have been only a few experimental studies on the subje...
Ausführliche Beschreibung
Autor*in: |
Daniel Tunc McGuiness [verfasserIn] Stamatios Giannoukos [verfasserIn] Alan Marshall [verfasserIn] Stephen Taylor [verfasserIn] |
---|
Format: |
E-Artikel |
---|---|
Sprache: |
Englisch |
Erschienen: |
2018 |
---|
Schlagwörter: |
---|
Übergeordnetes Werk: |
In: IEEE Access - IEEE, 2014, 6(2018), Seite 46706-46717 |
---|---|
Übergeordnetes Werk: |
volume:6 ; year:2018 ; pages:46706-46717 |
Links: |
---|
DOI / URN: |
10.1109/ACCESS.2018.2866679 |
---|
Katalog-ID: |
DOAJ057813779 |
---|
LEADER | 01000caa a22002652 4500 | ||
---|---|---|---|
001 | DOAJ057813779 | ||
003 | DE-627 | ||
005 | 20230308220621.0 | ||
007 | cr uuu---uuuuu | ||
008 | 230227s2018 xx |||||o 00| ||eng c | ||
024 | 7 | |a 10.1109/ACCESS.2018.2866679 |2 doi | |
035 | |a (DE-627)DOAJ057813779 | ||
035 | |a (DE-599)DOAJ7999bd5b71144f90a11d8edc3de19d26 | ||
040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
041 | |a eng | ||
050 | 0 | |a TK1-9971 | |
100 | 0 | |a Daniel Tunc McGuiness |e verfasserin |4 aut | |
245 | 1 | 0 | |a Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion |
264 | 1 | |c 2018 | |
336 | |a Text |b txt |2 rdacontent | ||
337 | |a Computermedien |b c |2 rdamedia | ||
338 | |a Online-Ressource |b cr |2 rdacarrier | ||
520 | |a Molecular communication (MC) is a method where the transmission of information involves the use of chemicals or molecules instead of electromagnetic waves. The study of MC to date has mostly focused on the nano (nm) to micro (μm) scale and there have been only a few experimental studies on the subject of macro-scale. In this paper properties of macro-scale MC are experimented and studied. These are signal flow (<i<q</i<), carrier flow (<i<Q</i<), and bit duration (<i<T</i<). A mass spectrometer with a quadrupole mass analyzer is used as the detector and an in-house-built odor generator is used as the chemical pulse generator. This paper has shown that the signal energy has a quadratic relation to signal flow whereas the carrier flow has a non-linear relation to both the signal amplitude and the signal energy. The bit duration has shown that the system reaches a saturation point as the bit duration is increased and this effect also occurs in the leftover chemical signal after bit transmission. Finally, a mathematical model is developed for the first time to explain the molecular transmission on the macro-scale using advection-diffusion equation. | ||
650 | 4 | |a Molecular communication | |
650 | 4 | |a mass spectrometry | |
650 | 4 | |a macro-scale | |
653 | 0 | |a Electrical engineering. Electronics. Nuclear engineering | |
700 | 0 | |a Stamatios Giannoukos |e verfasserin |4 aut | |
700 | 0 | |a Alan Marshall |e verfasserin |4 aut | |
700 | 0 | |a Stephen Taylor |e verfasserin |4 aut | |
773 | 0 | 8 | |i In |t IEEE Access |d IEEE, 2014 |g 6(2018), Seite 46706-46717 |w (DE-627)728440385 |w (DE-600)2687964-5 |x 21693536 |7 nnns |
773 | 1 | 8 | |g volume:6 |g year:2018 |g pages:46706-46717 |
856 | 4 | 0 | |u https://doi.org/10.1109/ACCESS.2018.2866679 |z kostenfrei |
856 | 4 | 0 | |u https://doaj.org/article/7999bd5b71144f90a11d8edc3de19d26 |z kostenfrei |
856 | 4 | 0 | |u https://ieeexplore.ieee.org/document/8445572/ |z kostenfrei |
856 | 4 | 2 | |u https://doaj.org/toc/2169-3536 |y Journal toc |z kostenfrei |
912 | |a GBV_USEFLAG_A | ||
912 | |a SYSFLAG_A | ||
912 | |a GBV_DOAJ | ||
912 | |a GBV_ILN_11 | ||
912 | |a GBV_ILN_20 | ||
912 | |a GBV_ILN_22 | ||
912 | |a GBV_ILN_23 | ||
912 | |a GBV_ILN_24 | ||
912 | |a GBV_ILN_31 | ||
912 | |a GBV_ILN_39 | ||
912 | |a GBV_ILN_40 | ||
912 | |a GBV_ILN_60 | ||
912 | |a GBV_ILN_62 | ||
912 | |a GBV_ILN_63 | ||
912 | |a GBV_ILN_65 | ||
912 | |a GBV_ILN_69 | ||
912 | |a GBV_ILN_70 | ||
912 | |a GBV_ILN_73 | ||
912 | |a GBV_ILN_95 | ||
912 | |a GBV_ILN_105 | ||
912 | |a GBV_ILN_110 | ||
912 | |a GBV_ILN_151 | ||
912 | |a GBV_ILN_161 | ||
912 | |a GBV_ILN_170 | ||
912 | |a GBV_ILN_213 | ||
912 | |a GBV_ILN_230 | ||
912 | |a GBV_ILN_285 | ||
912 | |a GBV_ILN_293 | ||
912 | |a GBV_ILN_370 | ||
912 | |a GBV_ILN_602 | ||
912 | |a GBV_ILN_2014 | ||
912 | |a GBV_ILN_4012 | ||
912 | |a GBV_ILN_4037 | ||
912 | |a GBV_ILN_4112 | ||
912 | |a GBV_ILN_4125 | ||
912 | |a GBV_ILN_4126 | ||
912 | |a GBV_ILN_4249 | ||
912 | |a GBV_ILN_4305 | ||
912 | |a GBV_ILN_4306 | ||
912 | |a GBV_ILN_4307 | ||
912 | |a GBV_ILN_4313 | ||
912 | |a GBV_ILN_4322 | ||
912 | |a GBV_ILN_4323 | ||
912 | |a GBV_ILN_4324 | ||
912 | |a GBV_ILN_4325 | ||
912 | |a GBV_ILN_4335 | ||
912 | |a GBV_ILN_4338 | ||
912 | |a GBV_ILN_4367 | ||
912 | |a GBV_ILN_4700 | ||
951 | |a AR | ||
952 | |d 6 |j 2018 |h 46706-46717 |
author_variant |
d t m dtm s g sg a m am s t st |
---|---|
matchkey_str |
article:21693536:2018----::aaeeaayiimcoclmlclromnctoss |
hierarchy_sort_str |
2018 |
callnumber-subject-code |
TK |
publishDate |
2018 |
allfields |
10.1109/ACCESS.2018.2866679 doi (DE-627)DOAJ057813779 (DE-599)DOAJ7999bd5b71144f90a11d8edc3de19d26 DE-627 ger DE-627 rakwb eng TK1-9971 Daniel Tunc McGuiness verfasserin aut Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Molecular communication (MC) is a method where the transmission of information involves the use of chemicals or molecules instead of electromagnetic waves. The study of MC to date has mostly focused on the nano (nm) to micro (μm) scale and there have been only a few experimental studies on the subject of macro-scale. In this paper properties of macro-scale MC are experimented and studied. These are signal flow (<i<q</i<), carrier flow (<i<Q</i<), and bit duration (<i<T</i<). A mass spectrometer with a quadrupole mass analyzer is used as the detector and an in-house-built odor generator is used as the chemical pulse generator. This paper has shown that the signal energy has a quadratic relation to signal flow whereas the carrier flow has a non-linear relation to both the signal amplitude and the signal energy. The bit duration has shown that the system reaches a saturation point as the bit duration is increased and this effect also occurs in the leftover chemical signal after bit transmission. Finally, a mathematical model is developed for the first time to explain the molecular transmission on the macro-scale using advection-diffusion equation. Molecular communication mass spectrometry macro-scale Electrical engineering. Electronics. Nuclear engineering Stamatios Giannoukos verfasserin aut Alan Marshall verfasserin aut Stephen Taylor verfasserin aut In IEEE Access IEEE, 2014 6(2018), Seite 46706-46717 (DE-627)728440385 (DE-600)2687964-5 21693536 nnns volume:6 year:2018 pages:46706-46717 https://doi.org/10.1109/ACCESS.2018.2866679 kostenfrei https://doaj.org/article/7999bd5b71144f90a11d8edc3de19d26 kostenfrei https://ieeexplore.ieee.org/document/8445572/ kostenfrei https://doaj.org/toc/2169-3536 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 6 2018 46706-46717 |
spelling |
10.1109/ACCESS.2018.2866679 doi (DE-627)DOAJ057813779 (DE-599)DOAJ7999bd5b71144f90a11d8edc3de19d26 DE-627 ger DE-627 rakwb eng TK1-9971 Daniel Tunc McGuiness verfasserin aut Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Molecular communication (MC) is a method where the transmission of information involves the use of chemicals or molecules instead of electromagnetic waves. The study of MC to date has mostly focused on the nano (nm) to micro (μm) scale and there have been only a few experimental studies on the subject of macro-scale. In this paper properties of macro-scale MC are experimented and studied. These are signal flow (<i<q</i<), carrier flow (<i<Q</i<), and bit duration (<i<T</i<). A mass spectrometer with a quadrupole mass analyzer is used as the detector and an in-house-built odor generator is used as the chemical pulse generator. This paper has shown that the signal energy has a quadratic relation to signal flow whereas the carrier flow has a non-linear relation to both the signal amplitude and the signal energy. The bit duration has shown that the system reaches a saturation point as the bit duration is increased and this effect also occurs in the leftover chemical signal after bit transmission. Finally, a mathematical model is developed for the first time to explain the molecular transmission on the macro-scale using advection-diffusion equation. Molecular communication mass spectrometry macro-scale Electrical engineering. Electronics. Nuclear engineering Stamatios Giannoukos verfasserin aut Alan Marshall verfasserin aut Stephen Taylor verfasserin aut In IEEE Access IEEE, 2014 6(2018), Seite 46706-46717 (DE-627)728440385 (DE-600)2687964-5 21693536 nnns volume:6 year:2018 pages:46706-46717 https://doi.org/10.1109/ACCESS.2018.2866679 kostenfrei https://doaj.org/article/7999bd5b71144f90a11d8edc3de19d26 kostenfrei https://ieeexplore.ieee.org/document/8445572/ kostenfrei https://doaj.org/toc/2169-3536 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 6 2018 46706-46717 |
allfields_unstemmed |
10.1109/ACCESS.2018.2866679 doi (DE-627)DOAJ057813779 (DE-599)DOAJ7999bd5b71144f90a11d8edc3de19d26 DE-627 ger DE-627 rakwb eng TK1-9971 Daniel Tunc McGuiness verfasserin aut Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Molecular communication (MC) is a method where the transmission of information involves the use of chemicals or molecules instead of electromagnetic waves. The study of MC to date has mostly focused on the nano (nm) to micro (μm) scale and there have been only a few experimental studies on the subject of macro-scale. In this paper properties of macro-scale MC are experimented and studied. These are signal flow (<i<q</i<), carrier flow (<i<Q</i<), and bit duration (<i<T</i<). A mass spectrometer with a quadrupole mass analyzer is used as the detector and an in-house-built odor generator is used as the chemical pulse generator. This paper has shown that the signal energy has a quadratic relation to signal flow whereas the carrier flow has a non-linear relation to both the signal amplitude and the signal energy. The bit duration has shown that the system reaches a saturation point as the bit duration is increased and this effect also occurs in the leftover chemical signal after bit transmission. Finally, a mathematical model is developed for the first time to explain the molecular transmission on the macro-scale using advection-diffusion equation. Molecular communication mass spectrometry macro-scale Electrical engineering. Electronics. Nuclear engineering Stamatios Giannoukos verfasserin aut Alan Marshall verfasserin aut Stephen Taylor verfasserin aut In IEEE Access IEEE, 2014 6(2018), Seite 46706-46717 (DE-627)728440385 (DE-600)2687964-5 21693536 nnns volume:6 year:2018 pages:46706-46717 https://doi.org/10.1109/ACCESS.2018.2866679 kostenfrei https://doaj.org/article/7999bd5b71144f90a11d8edc3de19d26 kostenfrei https://ieeexplore.ieee.org/document/8445572/ kostenfrei https://doaj.org/toc/2169-3536 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 6 2018 46706-46717 |
allfieldsGer |
10.1109/ACCESS.2018.2866679 doi (DE-627)DOAJ057813779 (DE-599)DOAJ7999bd5b71144f90a11d8edc3de19d26 DE-627 ger DE-627 rakwb eng TK1-9971 Daniel Tunc McGuiness verfasserin aut Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Molecular communication (MC) is a method where the transmission of information involves the use of chemicals or molecules instead of electromagnetic waves. The study of MC to date has mostly focused on the nano (nm) to micro (μm) scale and there have been only a few experimental studies on the subject of macro-scale. In this paper properties of macro-scale MC are experimented and studied. These are signal flow (<i<q</i<), carrier flow (<i<Q</i<), and bit duration (<i<T</i<). A mass spectrometer with a quadrupole mass analyzer is used as the detector and an in-house-built odor generator is used as the chemical pulse generator. This paper has shown that the signal energy has a quadratic relation to signal flow whereas the carrier flow has a non-linear relation to both the signal amplitude and the signal energy. The bit duration has shown that the system reaches a saturation point as the bit duration is increased and this effect also occurs in the leftover chemical signal after bit transmission. Finally, a mathematical model is developed for the first time to explain the molecular transmission on the macro-scale using advection-diffusion equation. Molecular communication mass spectrometry macro-scale Electrical engineering. Electronics. Nuclear engineering Stamatios Giannoukos verfasserin aut Alan Marshall verfasserin aut Stephen Taylor verfasserin aut In IEEE Access IEEE, 2014 6(2018), Seite 46706-46717 (DE-627)728440385 (DE-600)2687964-5 21693536 nnns volume:6 year:2018 pages:46706-46717 https://doi.org/10.1109/ACCESS.2018.2866679 kostenfrei https://doaj.org/article/7999bd5b71144f90a11d8edc3de19d26 kostenfrei https://ieeexplore.ieee.org/document/8445572/ kostenfrei https://doaj.org/toc/2169-3536 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 6 2018 46706-46717 |
allfieldsSound |
10.1109/ACCESS.2018.2866679 doi (DE-627)DOAJ057813779 (DE-599)DOAJ7999bd5b71144f90a11d8edc3de19d26 DE-627 ger DE-627 rakwb eng TK1-9971 Daniel Tunc McGuiness verfasserin aut Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Molecular communication (MC) is a method where the transmission of information involves the use of chemicals or molecules instead of electromagnetic waves. The study of MC to date has mostly focused on the nano (nm) to micro (μm) scale and there have been only a few experimental studies on the subject of macro-scale. In this paper properties of macro-scale MC are experimented and studied. These are signal flow (<i<q</i<), carrier flow (<i<Q</i<), and bit duration (<i<T</i<). A mass spectrometer with a quadrupole mass analyzer is used as the detector and an in-house-built odor generator is used as the chemical pulse generator. This paper has shown that the signal energy has a quadratic relation to signal flow whereas the carrier flow has a non-linear relation to both the signal amplitude and the signal energy. The bit duration has shown that the system reaches a saturation point as the bit duration is increased and this effect also occurs in the leftover chemical signal after bit transmission. Finally, a mathematical model is developed for the first time to explain the molecular transmission on the macro-scale using advection-diffusion equation. Molecular communication mass spectrometry macro-scale Electrical engineering. Electronics. Nuclear engineering Stamatios Giannoukos verfasserin aut Alan Marshall verfasserin aut Stephen Taylor verfasserin aut In IEEE Access IEEE, 2014 6(2018), Seite 46706-46717 (DE-627)728440385 (DE-600)2687964-5 21693536 nnns volume:6 year:2018 pages:46706-46717 https://doi.org/10.1109/ACCESS.2018.2866679 kostenfrei https://doaj.org/article/7999bd5b71144f90a11d8edc3de19d26 kostenfrei https://ieeexplore.ieee.org/document/8445572/ kostenfrei https://doaj.org/toc/2169-3536 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 6 2018 46706-46717 |
language |
English |
source |
In IEEE Access 6(2018), Seite 46706-46717 volume:6 year:2018 pages:46706-46717 |
sourceStr |
In IEEE Access 6(2018), Seite 46706-46717 volume:6 year:2018 pages:46706-46717 |
format_phy_str_mv |
Article |
institution |
findex.gbv.de |
topic_facet |
Molecular communication mass spectrometry macro-scale Electrical engineering. Electronics. Nuclear engineering |
isfreeaccess_bool |
true |
container_title |
IEEE Access |
authorswithroles_txt_mv |
Daniel Tunc McGuiness @@aut@@ Stamatios Giannoukos @@aut@@ Alan Marshall @@aut@@ Stephen Taylor @@aut@@ |
publishDateDaySort_date |
2018-01-01T00:00:00Z |
hierarchy_top_id |
728440385 |
id |
DOAJ057813779 |
language_de |
englisch |
fullrecord |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">DOAJ057813779</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230308220621.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230227s2018 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1109/ACCESS.2018.2866679</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)DOAJ057813779</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)DOAJ7999bd5b71144f90a11d8edc3de19d26</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="050" ind1=" " ind2="0"><subfield code="a">TK1-9971</subfield></datafield><datafield tag="100" ind1="0" ind2=" "><subfield code="a">Daniel Tunc McGuiness</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2018</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Molecular communication (MC) is a method where the transmission of information involves the use of chemicals or molecules instead of electromagnetic waves. The study of MC to date has mostly focused on the nano (nm) to micro (μm) scale and there have been only a few experimental studies on the subject of macro-scale. In this paper properties of macro-scale MC are experimented and studied. These are signal flow (<i<q</i<), carrier flow (<i<Q</i<), and bit duration (<i<T</i<). A mass spectrometer with a quadrupole mass analyzer is used as the detector and an in-house-built odor generator is used as the chemical pulse generator. This paper has shown that the signal energy has a quadratic relation to signal flow whereas the carrier flow has a non-linear relation to both the signal amplitude and the signal energy. The bit duration has shown that the system reaches a saturation point as the bit duration is increased and this effect also occurs in the leftover chemical signal after bit transmission. Finally, a mathematical model is developed for the first time to explain the molecular transmission on the macro-scale using advection-diffusion equation.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Molecular communication</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">mass spectrometry</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">macro-scale</subfield></datafield><datafield tag="653" ind1=" " ind2="0"><subfield code="a">Electrical engineering. Electronics. Nuclear engineering</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Stamatios Giannoukos</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Alan Marshall</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Stephen Taylor</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">In</subfield><subfield code="t">IEEE Access</subfield><subfield code="d">IEEE, 2014</subfield><subfield code="g">6(2018), Seite 46706-46717</subfield><subfield code="w">(DE-627)728440385</subfield><subfield code="w">(DE-600)2687964-5</subfield><subfield code="x">21693536</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:6</subfield><subfield code="g">year:2018</subfield><subfield code="g">pages:46706-46717</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doi.org/10.1109/ACCESS.2018.2866679</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doaj.org/article/7999bd5b71144f90a11d8edc3de19d26</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://ieeexplore.ieee.org/document/8445572/</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">https://doaj.org/toc/2169-3536</subfield><subfield code="y">Journal toc</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_DOAJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_213</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_230</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4249</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4306</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4307</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4322</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4367</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">6</subfield><subfield code="j">2018</subfield><subfield code="h">46706-46717</subfield></datafield></record></collection>
|
callnumber-first |
T - Technology |
author |
Daniel Tunc McGuiness |
spellingShingle |
Daniel Tunc McGuiness misc TK1-9971 misc Molecular communication misc mass spectrometry misc macro-scale misc Electrical engineering. Electronics. Nuclear engineering Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion |
authorStr |
Daniel Tunc McGuiness |
ppnlink_with_tag_str_mv |
@@773@@(DE-627)728440385 |
format |
electronic Article |
delete_txt_mv |
keep |
author_role |
aut aut aut aut |
collection |
DOAJ |
remote_str |
true |
callnumber-label |
TK1-9971 |
illustrated |
Not Illustrated |
issn |
21693536 |
topic_title |
TK1-9971 Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion Molecular communication mass spectrometry macro-scale |
topic |
misc TK1-9971 misc Molecular communication misc mass spectrometry misc macro-scale misc Electrical engineering. Electronics. Nuclear engineering |
topic_unstemmed |
misc TK1-9971 misc Molecular communication misc mass spectrometry misc macro-scale misc Electrical engineering. Electronics. Nuclear engineering |
topic_browse |
misc TK1-9971 misc Molecular communication misc mass spectrometry misc macro-scale misc Electrical engineering. Electronics. Nuclear engineering |
format_facet |
Elektronische Aufsätze Aufsätze Elektronische Ressource |
format_main_str_mv |
Text Zeitschrift/Artikel |
carriertype_str_mv |
cr |
hierarchy_parent_title |
IEEE Access |
hierarchy_parent_id |
728440385 |
hierarchy_top_title |
IEEE Access |
isfreeaccess_txt |
true |
familylinks_str_mv |
(DE-627)728440385 (DE-600)2687964-5 |
title |
Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion |
ctrlnum |
(DE-627)DOAJ057813779 (DE-599)DOAJ7999bd5b71144f90a11d8edc3de19d26 |
title_full |
Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion |
author_sort |
Daniel Tunc McGuiness |
journal |
IEEE Access |
journalStr |
IEEE Access |
callnumber-first-code |
T |
lang_code |
eng |
isOA_bool |
true |
recordtype |
marc |
publishDateSort |
2018 |
contenttype_str_mv |
txt |
container_start_page |
46706 |
author_browse |
Daniel Tunc McGuiness Stamatios Giannoukos Alan Marshall Stephen Taylor |
container_volume |
6 |
class |
TK1-9971 |
format_se |
Elektronische Aufsätze |
author-letter |
Daniel Tunc McGuiness |
doi_str_mv |
10.1109/ACCESS.2018.2866679 |
author2-role |
verfasserin |
title_sort |
parameter analysis in macro-scale molecular communications using advection-diffusion |
callnumber |
TK1-9971 |
title_auth |
Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion |
abstract |
Molecular communication (MC) is a method where the transmission of information involves the use of chemicals or molecules instead of electromagnetic waves. The study of MC to date has mostly focused on the nano (nm) to micro (μm) scale and there have been only a few experimental studies on the subject of macro-scale. In this paper properties of macro-scale MC are experimented and studied. These are signal flow (<i<q</i<), carrier flow (<i<Q</i<), and bit duration (<i<T</i<). A mass spectrometer with a quadrupole mass analyzer is used as the detector and an in-house-built odor generator is used as the chemical pulse generator. This paper has shown that the signal energy has a quadratic relation to signal flow whereas the carrier flow has a non-linear relation to both the signal amplitude and the signal energy. The bit duration has shown that the system reaches a saturation point as the bit duration is increased and this effect also occurs in the leftover chemical signal after bit transmission. Finally, a mathematical model is developed for the first time to explain the molecular transmission on the macro-scale using advection-diffusion equation. |
abstractGer |
Molecular communication (MC) is a method where the transmission of information involves the use of chemicals or molecules instead of electromagnetic waves. The study of MC to date has mostly focused on the nano (nm) to micro (μm) scale and there have been only a few experimental studies on the subject of macro-scale. In this paper properties of macro-scale MC are experimented and studied. These are signal flow (<i<q</i<), carrier flow (<i<Q</i<), and bit duration (<i<T</i<). A mass spectrometer with a quadrupole mass analyzer is used as the detector and an in-house-built odor generator is used as the chemical pulse generator. This paper has shown that the signal energy has a quadratic relation to signal flow whereas the carrier flow has a non-linear relation to both the signal amplitude and the signal energy. The bit duration has shown that the system reaches a saturation point as the bit duration is increased and this effect also occurs in the leftover chemical signal after bit transmission. Finally, a mathematical model is developed for the first time to explain the molecular transmission on the macro-scale using advection-diffusion equation. |
abstract_unstemmed |
Molecular communication (MC) is a method where the transmission of information involves the use of chemicals or molecules instead of electromagnetic waves. The study of MC to date has mostly focused on the nano (nm) to micro (μm) scale and there have been only a few experimental studies on the subject of macro-scale. In this paper properties of macro-scale MC are experimented and studied. These are signal flow (<i<q</i<), carrier flow (<i<Q</i<), and bit duration (<i<T</i<). A mass spectrometer with a quadrupole mass analyzer is used as the detector and an in-house-built odor generator is used as the chemical pulse generator. This paper has shown that the signal energy has a quadratic relation to signal flow whereas the carrier flow has a non-linear relation to both the signal amplitude and the signal energy. The bit duration has shown that the system reaches a saturation point as the bit duration is increased and this effect also occurs in the leftover chemical signal after bit transmission. Finally, a mathematical model is developed for the first time to explain the molecular transmission on the macro-scale using advection-diffusion equation. |
collection_details |
GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 |
title_short |
Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion |
url |
https://doi.org/10.1109/ACCESS.2018.2866679 https://doaj.org/article/7999bd5b71144f90a11d8edc3de19d26 https://ieeexplore.ieee.org/document/8445572/ https://doaj.org/toc/2169-3536 |
remote_bool |
true |
author2 |
Stamatios Giannoukos Alan Marshall Stephen Taylor |
author2Str |
Stamatios Giannoukos Alan Marshall Stephen Taylor |
ppnlink |
728440385 |
callnumber-subject |
TK - Electrical and Nuclear Engineering |
mediatype_str_mv |
c |
isOA_txt |
true |
hochschulschrift_bool |
false |
doi_str |
10.1109/ACCESS.2018.2866679 |
callnumber-a |
TK1-9971 |
up_date |
2024-07-03T14:15:56.382Z |
_version_ |
1803567661204897792 |
fullrecord_marcxml |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">DOAJ057813779</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230308220621.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230227s2018 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1109/ACCESS.2018.2866679</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)DOAJ057813779</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)DOAJ7999bd5b71144f90a11d8edc3de19d26</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="050" ind1=" " ind2="0"><subfield code="a">TK1-9971</subfield></datafield><datafield tag="100" ind1="0" ind2=" "><subfield code="a">Daniel Tunc McGuiness</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Parameter Analysis in Macro-Scale Molecular Communications Using Advection-Diffusion</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2018</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Molecular communication (MC) is a method where the transmission of information involves the use of chemicals or molecules instead of electromagnetic waves. The study of MC to date has mostly focused on the nano (nm) to micro (μm) scale and there have been only a few experimental studies on the subject of macro-scale. In this paper properties of macro-scale MC are experimented and studied. These are signal flow (<i<q</i<), carrier flow (<i<Q</i<), and bit duration (<i<T</i<). A mass spectrometer with a quadrupole mass analyzer is used as the detector and an in-house-built odor generator is used as the chemical pulse generator. This paper has shown that the signal energy has a quadratic relation to signal flow whereas the carrier flow has a non-linear relation to both the signal amplitude and the signal energy. The bit duration has shown that the system reaches a saturation point as the bit duration is increased and this effect also occurs in the leftover chemical signal after bit transmission. Finally, a mathematical model is developed for the first time to explain the molecular transmission on the macro-scale using advection-diffusion equation.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Molecular communication</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">mass spectrometry</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">macro-scale</subfield></datafield><datafield tag="653" ind1=" " ind2="0"><subfield code="a">Electrical engineering. Electronics. Nuclear engineering</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Stamatios Giannoukos</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Alan Marshall</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Stephen Taylor</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">In</subfield><subfield code="t">IEEE Access</subfield><subfield code="d">IEEE, 2014</subfield><subfield code="g">6(2018), Seite 46706-46717</subfield><subfield code="w">(DE-627)728440385</subfield><subfield code="w">(DE-600)2687964-5</subfield><subfield code="x">21693536</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:6</subfield><subfield code="g">year:2018</subfield><subfield code="g">pages:46706-46717</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doi.org/10.1109/ACCESS.2018.2866679</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doaj.org/article/7999bd5b71144f90a11d8edc3de19d26</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://ieeexplore.ieee.org/document/8445572/</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">https://doaj.org/toc/2169-3536</subfield><subfield code="y">Journal toc</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_DOAJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_213</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_230</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4249</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4306</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4307</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4322</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4367</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">6</subfield><subfield code="j">2018</subfield><subfield code="h">46706-46717</subfield></datafield></record></collection>
|
score |
7.398122 |