1 / 114

LL-Ch.3 Collisions

LL-Ch.3 Collisions. JK LEE (Spring, 2006). Ch.3 Collisions ◎ Why do we need collisions? ◎ Types of Collisions 1)Elastic Collisions -Coul. Coll. (e-e, e-i, i-i ) -Polariz. Coll. (e-N, i-N) v 2)Inelastic Collisions(KE non-conserved)

yuki
Télécharger la présentation

LL-Ch.3 Collisions

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. LL-Ch.3 Collisions JK LEE (Spring, 2006)

  2. Ch.3 Collisions ◎Why do we need collisions? ◎Types of Collisions 1)Elastic Collisions -Coul. Coll. (e-e, e-i, i-i ) -Polariz. Coll. (e-N, i-N) v 2)Inelastic Collisions(KE non-conserved) -Ionization Coll. -Excitation Coll. (Meta stable Neutral) -Charge Transfer a +

  3. ◎Collisions in Argon •The mean free path for ionizing electrons is comparable to source dimensions. •The electron-neutral ionization rate is uniform. •The eedf is a Maxwellian, with Te uniform. •Argon is used as a reference, with second order rate constants Kiz, Kexc, and Kel, and Resonant charge transfer of on Ar exceeds elastic scattering. The combined ion cross section is Large , and

More Related