1964
DOI: 10.1071/ph640307
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The Diffusion of Electrons in Dry, Carbon Dioxide Free Air

Abstract: SummaryValues of Townsend's energy factor kl for electrons in dry, carbon dioxide free air have been determined as a function of the parameter E Ip for 0 . 2 < E Ip < 40 at a temperature of 293°K. The results are first compared with those of other workers and are then utilized in a recomparison of the cross sections for electron attachment deduced from swarm and beam-type experiments.

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Cited by 16 publications
(11 citation statements)
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“…Figure 4 shows such a comparison between Buchel'nikova's data and the data from our experiments where the data have been analysed on the basis of a Maxwellian distribution, using the values of kl given in Table 1 * The values of c1a computed from data for aa/P for dry air and carbon dioxide by Rees (1964) and Rees and Jory (1964) are in error by 7%, the correct values being 7% higher than those quoted. This systematic error does not in any way affect the conclusions drawn from the compari- from a recalculation of these data using the newer data for kl and W is also shown.…”
Section: (4)mentioning
confidence: 91%
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“…Figure 4 shows such a comparison between Buchel'nikova's data and the data from our experiments where the data have been analysed on the basis of a Maxwellian distribution, using the values of kl given in Table 1 * The values of c1a computed from data for aa/P for dry air and carbon dioxide by Rees (1964) and Rees and Jory (1964) are in error by 7%, the correct values being 7% higher than those quoted. This systematic error does not in any way affect the conclusions drawn from the compari- from a recalculation of these data using the newer data for kl and W is also shown.…”
Section: (4)mentioning
confidence: 91%
“…Prasad and Craggs 1961;Rees 1964;Rees and Jory 1964) have shown discrepancies no greater than might be expected as a result of imprecise knowledge of the appropriate energy distributions, the comparisons for water vapour (Prasad and Craggs 1960) were a notable exception. For this gas, values of ua calculated from swarm experiments exceeded the corresponding values calculated from Buchel'nikova's data by a factor of 5 in some instances.…”
Section: Comparison Of Attachment Data From Beam and Swarm Experimentioning
confidence: 99%
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“…When comparisons are made between the results of swarm and beam experiments, values of Townsend's energy factor kl and of the drift velocity Ware employed as auxiliary data, and the accuracy of the comparisons depends markedly on the accuracy of the values used for kl (Rees and Jory 1964) and to a lesser extent on those used for W. The sensitivity of the comparisons to the accuracy of the data used for kl' arises from the fact that, particularly if kl increases slowly with E/p, a small error in kl can lead to a large error in the value of E/p (and hence also in lXa/P) attributed to a given mean energy E. It was thought to be worth while in the present work Table 1 and W data of Table 3. Curve C, swarm data of Schlumbohm (1962) using data of Tables 1 and 3.…”
Section: -mentioning
confidence: 99%
“…Hake and Phelps (1967) compared the transport coefficients of electrons in air measured by Townsend and Tizard (1913), Nielsen and Bradbury (1937), Riemann (1944), Crompton et al (1953), and Rees and Jory (1964) with coefficients deduced from the cross sections that they had shown to be compatible with measured transport coefficients for pure oxygen and nitrogen. They found the agreement for air to be significantly poorer than in the case of either oxygen or nitrogen on its own and concluded that a possible explanation was that the experimental data used in their analyses for one or more of the gases were in error.…”
mentioning
confidence: 99%