1973
DOI: 10.1002/ctpp.19730130104
|View full text |Cite
|
Sign up to set email alerts
|

Bestimmung des UV‐Strahlungsflusses im Ar‐Hg‐Plasma

Abstract: Bei 57 hämolysierenden aus menschlichem Untersuchungsmaterial isolierten Stämmen von Escherichia coli wurde das Resistenzspektrum bestimmt. Drei Stämme konnten neben dem R‐Plasmid auch das Hämolysinbildungsvermögen auf eine nalidixinsäureresistente Mutante von E. coli K‐12 konjugativ übertragen. Die Übertragung der Plasmide erfolgte unabhängig voneinander. Von den restlichen 54 Stämmen konjugierten 44 ebenfalls mit E. coli K‐12, wie sich durch die R‐Plasmidübertragungen nachweisen ließ, die Hämolysinbildung gi… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

1973
1973
1990
1990

Publication Types

Select...
4
1

Relationship

4
1

Authors

Journals

citations
Cited by 5 publications
(1 citation statement)
references
References 12 publications
0
1
0
Order By: Relevance
“…These balance equations for the excited states are then numerically solved simultaneously with the discharge current equation i = eorcR2nn,pobe(E/po) (6) and the stationary, quasi-homogeneous Boltzmann equation According to this relation the power input from the electric field to the electrons is dissipated primarily by the output of resonance radiation (first two terms on the r.h.s. of (9)) and, to a minor extent, by elastic collisions of electrons with Ar and Hg atoms, by collisional transitions from the levels g, q, r, s, p to the non-balanced levels u, t and to the ionization continuum i and finally by all inelastic collisions of electrons with Ar atoms (denoted in equation (9) by flAr).…”
Section: --_mentioning
confidence: 99%
“…These balance equations for the excited states are then numerically solved simultaneously with the discharge current equation i = eorcR2nn,pobe(E/po) (6) and the stationary, quasi-homogeneous Boltzmann equation According to this relation the power input from the electric field to the electrons is dissipated primarily by the output of resonance radiation (first two terms on the r.h.s. of (9)) and, to a minor extent, by elastic collisions of electrons with Ar and Hg atoms, by collisional transitions from the levels g, q, r, s, p to the non-balanced levels u, t and to the ionization continuum i and finally by all inelastic collisions of electrons with Ar atoms (denoted in equation (9) by flAr).…”
Section: --_mentioning
confidence: 99%