Item | Explanation | Unit |
---|---|---|
ATTACHMENT-COEFFICIENT |
Attachment coefficient/pressure | 1/cm.Torr |
DRIFT-VELOCITY |
Drift velocity | cm/\μsec |
ION-DISSOCIATION |
Ion dissociation coefficient | 1/cm.Torr |
ION-MOBILITY |
Ion mobility | cm\²/\μsec.V |
LONGITUDINAL-DIFFUSION |
Longitudinal diffusion \√p | cm.\√Torr for 1\ cm |
LORENTZ-ANGLE |
Lorentz angle | degrees |
TOWNSEND-COEFFICIENT |
Townsend coefficient/pressure | 1/cm.Torr |
TRANSVERSE-DIFFUSION |
Transverse diffusion \√p | cm.\√Torr for 1\ cm |
Note that the same scalings have to be applied as for the TABLE.
Variable | Meaning | Unit |
---|---|---|
ANGLE_EB |
Angle between E and B | degrees |
ATTACHMENT |
Attachment coefficient / p | 1/cm.Torr |
B |
Magnetic field strength | Tesla |
BOLTZMANN |
Boltzmann constant | 1.380658 10\<SUP\>-23\</SUP\> J/K |
DISS |
Ion dissociation coefficient | 1/cm.Torr |
ECHARGE |
Electron charge | 1.60217733 10\<SUP\>-19\</SUP\> C |
EP |
Electric field / p | V/cm.Torr |
LORENTZ |
Lorentz angle | degrees |
MOBILITY |
Ion mobility | cm\²/\μsec.V |
P |
Pressure | Torr |
SIGMA_L |
Longitudinal diffusion \√ p | cm.\√Torr for 1\ cm |
SIGMA_T |
Transverse diffusion \√p | cm.\√Torr for 1\ cm |
T |
Temperature | K |
TOWNSEND |
Townsend coefficient / p | 1/cm.Torr |
VELOCITY |
Electron drift velocity | cm/\μsec |
The variable EP can always be used, ANGLE_EB and B can only be used in tables prepared for magnetic fields. The transport properties can be used only insofar as they have been entered already.
The E/p vector should in principle cover the entire range of the table. Values outside the range of the E/p vector are left untouched - no attempt is made to extrapolate. Since most items are initialised to values outside their permissible range, an error will in general be reported from the checks that are carried out while leaving the gas section. To avoid this, one can first set the item with an approximate function and then override in part with more precise values. This is illustrated here for He\<SUP\>+\</SUP\> in He:
// Experimental data Vector E_He_He K_He_He 0 10.5 6 10.3 8 10.2 10 10.2 12 10.1 15 10.0 20 9.90 25 9.74 30 9.60 40 9.28 50 8.97 60 8.67 80 8.12 100 7.67 120 7.25 150 6.78 200 6.12 250 5.60 300 5.19 400 4.58 500 4.17 600 3.81 700 3.57// Scaling from Td to V/cm.Torr and from V/cm\².sec to V/cm\².\μsec Global E_He_He = E_He_He/(0.010354*300) Global K_He_He = K_He_He*1e-6 // Fit an exponential to the shape Call fit_exponential(E_He_He,K_He_He,1e-8,p0,p1,p2,p3,ep0,ep1,ep2,ep3) // Provisionally set the mobility to the exponential function add ion-mobility exp({p0}+{p1}*ep+{p2}*ep^2+{p3}*ep^3) // Override the values that are in the range add ion-mobility K_He_He vs E_He_He
The E/p values in your vector do not have to coincide with the E/p values present in the table - your vectors will be interpolated at the values of the table and these interpolations are stored instead of the values from the vector.
When the data is smooth, a value of 2 (quadratic interpolation) is a good choice. This may however lead to intermediate points with a negative value in for instance Townsend coefficient tables that usually start at 0. For such tables, linear interpolation is advised.
Instead of ORDER 1, you may also type LINEAR. QUADRATIC is a synonym for ORDER 2, CUBIC for ORDER 3.
Formatted on 21/01/18 at 16:55.