Download - 3P10-48

Transcript
  • 7/29/2019 3P10-48

    1/2

    Chemistry of Methane-Nitrogen in a dielectric barrier discharge at

    atmospheric pressure

    G. Scarduelli1, P. Franceschi1, G. Guella1, G. Dilecce2,3, S. De Benedictis3 and P. Tosi1

    P

    1P Department of Physics, University of Trento, via Sommarive 14, 38050 Povo, Trento, Italy

    P

    2P Istituto di Fotonica e Nanotecnologie - CNR, sede di Trento, via alla Cascata 56/C, 38050 Povo, Trento, Italy

    3Istituto di Metodologie Inorganiche e dei Plasmi - CNR, sede di Bari, via Orabona 4, 70126 Bari, Italy

    Methane is the principal component of natural gas, coal-bed methane and associated gas. The

    valorization of methane into higher hydrocarbons and oxygenates has been desired for several

    decades. Moreover the direct conversion of methane into more valuable chemicals and versatile

    fuels constitutes an important task. In this contribution we present a preliminary investigation of

    the liquid deposit obtained treating a methane-nitrogen mixture in a dielectric barrier discharge

    working at atmospheric pressure. The deposit was analyzed by means of various techniques

    (Nuclear Magnetic Resonance, Fourier Transform Infrared Spectroscopy and Matrix-Assisted

    Laser Desorption/Ionisation -Time Of Flight Mass Spectrometry), in order to explain its polymeric

    nature. Nevertheless its composition is at present not completely identified.

    1. Introduction

    Methane is the main component of gaseous/solid

    fossil fuel resources and constitutes one of the

    largest organic carbon reserves.

    The direct conversion of CH4 into more valuable

    chemicals is very attractive [1, 2]. However, there is

    still no practical technology for such conversion [3].

    Both thermal and nonthermal plasmas have been

    widely used for CH4 conversion. However

    nonthermal plasmas are the choice for chemical

    synthesis of higher hydrocarbons and oxygenatessince the electron temperature is high (up to 105 K),

    while the gas remains at room temperature.

    Most of products produced using corona,

    microwave and radio frequency discharges are small

    molecules, like ethylene, acetylene, hydrogen and

    carbon monoxide. Products can be more complex

    under the condition of dielectric barrier discharge

    including light hydrocarbons, liquid fuels, alcohols

    and acids [4]. The distribution of products depends

    on the different parameters, such as dielectric

    material, length, distance of discharge gap andelectrode configuration.

    In this contribution we present a preliminary

    investigation of CH4-N2 mixtures treated in a

    dielectric barrier discharge (DBD) working at

    atmospheric pressure. In particular, we have

    observed the deposition of a viscous liquid polymer.

    2. Experimental

    2. 1. Dielectric Barrier Discharge

    The methane-nitrogen mixtures are treated in a

    dielectric barrier discharge (DBD) working at

    atmospheric pressure. Different amounts of CH4

    were admitted in the plasma reactor and mixed with

    N2.

    Our DBD consists of a quartz tube ( = 10 mm)

    surrounded by a metal outer electrode (a spiral

    electrode). The internal electrode is a metallic rod

    embedded in a glass tube ( = 4 mm). The length of

    the plasma system is about 5 cm. Electrodes are

    powered at a frequency variable between 6 kHz and

    15 kHz by a variable high voltage transformer. The

    energy transferred to the plasma is evaluated by

    measuring both the applied voltage (with an HVprobe) and the charge (with a HV capacitor in series

    with the discharge) by the standard Manleys

    charge-voltage plot method [5]. The average power

    transmitted is ~10 W working at 16 kV with a

    frequency of 10 kHz. The reactor is vacuum sealed

    to allow control of the gas sample under treatment.

    2. 2. NMR

    Nuclear Magnetic Resonance (NMR) spectra were

    taken at 298.2 K by an Avance 400 Bruker

    spectrometer operating at 400.13 MHz for1

    H andequipped with a 5 mm inverse broad band (BBI)

    probe. Data were collected with XWINNMR

    (version 1.3) and processed using both Bruker

    TOPSPIN (version 1.3) and MestReC data

    processing software.

    2. 3. FT-IR

    Fourier Transform Infrared (FT-IR) Spectra were

    acquired by a spectrometer FT-IR EQUINOX 55

    Bruker Optics capable of 0.2 cm-1 maximum

    resolution, equipped with a DTGS detector and a

    Kbr beam splitter. Acquisitions have been

    performed with a resolution of 4 cm-1 by a Silver

    28 ICPIG, July 15-20, 2007, Prague, Czech Republicth Topic number: 10

    1001

  • 7/29/2019 3P10-48

    2/2

    Gate Reflection Attenuated Total Reflection (ATR)

    System.

    2. 4. MALDI-TOF MS

    Matrix-Assisted Laser Desorption/Ionisation -

    Time Of Flight (MALDI-TOF) spectra were takenby an Ultraflex II (Bruker Daltonics) spectrometer

    operating in reflectron mode with the following

    experimental parameters: delay time 0 ns, IS1 25 V,

    IS2 21.65 V, IS lens 10.5 V, laser energy (N 2, 337

    nm) 72.3 J.

    3. Preliminary results

    During DBD plasma treatment we have observed

    the formation of a liquid deposit on the surface of

    the plasma reactor. This material has been dissolved

    in a suitable solvent for NMR, FTIR and MALDI-

    TOF analysis.MALDI-TOF spectra (Fig. 1) of the deposit

    show, in the 200-1500 m/z region, the typical peak

    distribution of a polymeric compound. The repeated

    clusters of peaks present a constant mass difference,

    that is evaluated in 14 Da, as shown in Fig. 1. This

    value corresponds to a CH2 group.

    The polymeric nature of the deposit is confirmed

    also by broad signals in the 1H-NMR spectrum of

    the liquid deposit taken in acetone-d6, as shown in

    Fig. 2.

    In order to obtain further structural informationon the chemical functions present in the deposit, FT-

    IR measurements were also carried out. IR spectrum

    (Fig. 3) indicates the presence of CN groups

    possibly due to nitrogen containing impurities, and

    confirms the nature of polymer-like branched chain

    structure.

    Fig.1: MALDI-TOF spectra of the deposit obtained by

    DBD plasma on methane/N2 reacting system: in (a) we

    report the spectrum of the deposit dissolved in acetone,

    while in (b) we present the spectrum of the solution

    diluted 10 times.

    Fig.2: 1H-NMR spectrum of the liquid deposit taken in

    acetone-d6.

    Fig.3: FT-IR spectrum of the deposit obtained by DBD

    plasma on methane/N2 reacting system compared to FT-IR

    spectrum of the deposit obtained by DBD plasma on

    methane/Ar reacting system.

    Observations of the time evolution of the

    CN(B2+X2+) violet system emission during the

    DBD plasma treatment of a CH4-N2 mixture are

    presented in [6].

    4. References

    [1] J.H. Lunsford, Catal. Today 63 (2000) 165.[2] J.M. Fox, Catal. Rev., Sci. Eng. 35 (1993)

    169.

    [3] Y. Xu, X. Bao and L. Lin, J. Catal. 216

    (2003) 386.

    [4] Y. Zhang, Y. Li, Y. Wang, C. Liu and B.

    Eliasson, Fuel Process. Technol. 83 (2003) 101.

    [5] T. Manley, Trans. Electrochem. Soc. 84

    (1945) 83.

    [6] G. Scarduelli, P. Franceschi, G. Dilecce, S.

    De Benedictis and P. Tosi, ICPIG 2007, this book.

    28 ICPIG, July 15-20, 2007, Prague, Czech Republicth

    1002