Glow Discharge Calculations

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1 1 EECS 517 / NERS 578 FALL 2010 HOMEWORK #5 In this homework assignment, we will calculate the characteristics of a positive column glow discharge for realistic operating conditions. Use the following discharge circuit conditions A cylindrical discharge tube (length l, diameter d) is connected in series with a DC power supply (voltage V) and series ballast resistor (R B ohms). The gas pressure is 1 Torr at a gas temperature of 300 K (N = 9.654 10 18 P Torr /T K cm -3 ). Power Supply V d I R B Use the cross sections for the ideal molecule and M = 20 AMU. Assume that the only inelastic energy loss process is electron impact ionization, and that electron loss is dominated by ambipolar diffusion. You may assume that the ion temperature, T I is equal to the gas temperature. For these particular conditions, the plasma properties are obtained from the following: Electron Temperature: Obtained from the electron continuity equation: T e : n e t = 0, 0 2 e A e ion T D N T k (E/N): Obtained from the electron temperature equation: E N : i e m e i i e m e e B g e T Nk N T k N E T k m q m M k T T 2 2 2 2 3 2 Electron density: Obtained from the current density n e : N E T k m q n E d I j e m e e 2 2 2 Recall that collision frequencies are related to rate coefficients by i = k i N and that the ambipolar diffusion coefficient is I e I I e A T T T D T D 1 where T e Electron temperature (eV) k ion (T e ) Rate coefficient for ionization (cm 3 /s) k m (T e ) Rate coefficient for momentum transfer (cm 3 /s) k i (T e ), i Rate coefficient for inelastic process i with energy loss i (cm 3 /s, eV)

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Glow discharge calculations

Transcript of Glow Discharge Calculations

  • 1 1

    EECS 517 / NERS 578 FALL 2010 HOMEWORK #5 In this homework assignment, we will calculate the characteristics of a positive column glow discharge for realistic operating conditions. Use the following discharge circuit conditions A cylindrical discharge tube (length l, diameter d) is connected in series with a DC power supply (voltage V) and series ballast resistor (RB ohms). The gas pressure is 1 Torr at a gas temperature of 300 K (N = 9.654 1018 PTorr/TK cm-3 ).

    PowerSupply V

    d

    I

    RB

    Use the cross sections for the ideal molecule and M = 20 AMU. Assume that the only inelastic energy loss process is electron impact ionization, and that electron loss is dominated by ambipolar diffusion. You may assume that the ion temperature, TI is equal to the gas temperature. For these particular conditions, the plasma properties are obtained from the following: Electron Temperature: Obtained from the electron continuity equation:

    Te: ne t = 0, 02 eAeion

    TDNTk

    (E/N): Obtained from the electron temperature equation: EN :

    i em

    eii

    emeeBge TNk

    NTkNE

    Tkmq

    mM

    kTT

    2

    2

    2

    232

    Electron density: Obtained from the current density

    ne :

    NE

    TkmqnE

    dIj

    eme

    e2

    2

    2

    Recall that collision frequencies are related to rate coefficients by i = ki N and that the ambipolar diffusion coefficient is

    I

    eIIeA T

    TTDTD 1

    where Te Electron temperature (eV) kion(Te) Rate coefficient for ionization (cm3/s) km(Te) Rate coefficient for momentum transfer (cm3/s) ki(Te), i Rate coefficient for inelastic process i with energy loss i (cm3/s, eV)

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    DA(Te) Ambipolar diffusion coefficient (cm2/s) DI(TI) Ion diffusion coefficient (cm2/s)

    = d2

    2.405 Diffusion length for cylinder (cm)

    Tg Gas temperature (K) TI Ion temperature (K) kB Boltzmanns constant (1.6 x 10-12 erg/eV, 1.38 x 10-16 erg/K) N Gas density (cm3) M, me Gas atom mass, electron mass (g) q Elementary charge (c) j Current density (A/cm2) I Current (A) Conductivity (1/Ohm-cm) 1. Plot E/N, Te, I (total current), VDIS (voltage across the discharge tube) and ne for the following

    parameters. Use DI = 500 cm2

    s at a pressure of 1 Torr.

    L = 30 cm, j = 15 mA/cm2, 0.25 cm < d < 2.5 cm Discuss why each of E/N, Te, I, and VDIS change or does not change as the diameter of the

    discharge tube is changed. You may use values of rate coefficients you derived in previous homework assignments. You do not need to rederive the rate coefficients here.

    2. How will these values obtained in (1) change if j is increased to 25 mA/cm2? Sketch your

    answers. (No additional numerical work is required.) 3. How will the values in (1) change if L is increased to 60 cm? Sketch your answers. (No

    additional numerical work is required.) 4. Suppose we add an external source of ionization, Sion, so that

    ne t 0 = ne kION(Te)N

    Da(Te)2

    S ion

    The external source could be, for example, photo-ionization. How will Te, ne, E/N, VDIS and I change as S increases? Assume j remains a constant. (Explain your answer in words, no calculations are required.)