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Radiofrequency and Microwave Discharges in Plasma Chemistry

The plasma temperature in the metallic cylindef can be expressed as (/ is ionization potential) [Pg.210]

Conductivity am strongly depends on temperature, whereas Tm and Xm are changing only slightly therefore, am a ihnf. Then, the Saha equation results in weak logarithmic dependence Tm(/o, )  [Pg.210]

The dependence of ICP power per unit length on solenoid current and frequency can be shown as [Pg.210]

Typical atmospheric pressure thermal RF-ICP discharge (/ = 13.6MHz, tube radius 3 cm) has a temperature of about 10,000 K, thermal conductivity Xm = T4 10 W/cm K, electric conductivity am 25 Ohm cm , and skin layer 5 0.27 cm. The electromag- [Pg.210]

ICP discharges at moderate to high pressures usually generate thermal plasma, whereas the RF-CCP discharges in the same conditions can generate non-thermal plasma. [Pg.211]


See other pages where Radiofrequency and Microwave Discharges in Plasma Chemistry is mentioned: [Pg.209]    [Pg.209]    [Pg.211]    [Pg.213]    [Pg.217]    [Pg.219]    [Pg.225]    [Pg.229]    [Pg.231]    [Pg.209]    [Pg.209]    [Pg.211]    [Pg.213]    [Pg.217]    [Pg.219]    [Pg.225]    [Pg.229]    [Pg.231]    [Pg.268]   


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And microwaves

Discharge chemistry

Microwave chemistry

Microwave discharge

Plasma discharge

Radiofrequency

Radiofrequency discharge

Radiofrequency plasmas

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