The Effect of Surface Modification on the Photo-Electric Threshold of Mercury

<p>This work is a continuation of that of Kazda, who found the long wavelength limit of a mercury surface cleansed of impurities by means of a constant overflow.</p> <p>Kazda's value of 2735A for the threshold of clean mercury is checked. When the surface flow is allowed t...

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Main Author: Dunn, Hugh Kenneth
Format: Others
Published: 1925
Online Access:https://thesis.library.caltech.edu/2708/1/Dunn_hk_1925.pdf
Dunn, Hugh Kenneth (1925) The Effect of Surface Modification on the Photo-Electric Threshold of Mercury. Dissertation (Ph.D.), California Institute of Technology. doi:10.7907/Z0D9-RW50. https://resolver.caltech.edu/CaltechETD:etd-06242004-094823 <https://resolver.caltech.edu/CaltechETD:etd-06242004-094823>
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spelling ndltd-CALTECH-oai-thesis.library.caltech.edu-27082019-10-04T03:07:09Z The Effect of Surface Modification on the Photo-Electric Threshold of Mercury Dunn, Hugh Kenneth <p>This work is a continuation of that of Kazda, who found the long wavelength limit of a mercury surface cleansed of impurities by means of a constant overflow.</p> <p>Kazda's value of 2735A for the threshold of clean mercury is checked. When the surface flow is allowed to stop in a high vacuum, some impurity attacks the surface, quickly raising the threshold to 2850A. If liquid air is not used this impurity is present in larger amounts and attacks the running surface. Indications are that a surface film is formed and maintained in spite of the flow when liquid air is not used, or requires two hours or more of flow for removal if liquid air is used. This impurity cannot be one of the gases with extremely low melting points. It is not water, but may be a component of the stopcock grease. When the surface is left standing several days in a high vacuum its threshold falls to 2680A. If liquid air is not used the standing surface has a limit of 2560A. All of these values are closely reproducible. Pure hydrogen in contact with the surface does not change the photoelectric behavior. When the mercury is condensed in the presence of hydrogen, some of the gas is dissolved in the metal. This does not change the characteristic threshold of the mercury. It does, however, have the effect of greatly impeding the action of other impurities that form on the surface. This is indicated by the fact that over two hours is required for the change from the threshold of 2735A for the clean surface to the maximum of 2850A, as compared with 13 minutes for this change when hydrogen is not present.</p> 1925 Thesis NonPeerReviewed application/pdf https://thesis.library.caltech.edu/2708/1/Dunn_hk_1925.pdf https://resolver.caltech.edu/CaltechETD:etd-06242004-094823 Dunn, Hugh Kenneth (1925) The Effect of Surface Modification on the Photo-Electric Threshold of Mercury. Dissertation (Ph.D.), California Institute of Technology. doi:10.7907/Z0D9-RW50. https://resolver.caltech.edu/CaltechETD:etd-06242004-094823 <https://resolver.caltech.edu/CaltechETD:etd-06242004-094823> https://thesis.library.caltech.edu/2708/
collection NDLTD
format Others
sources NDLTD
description <p>This work is a continuation of that of Kazda, who found the long wavelength limit of a mercury surface cleansed of impurities by means of a constant overflow.</p> <p>Kazda's value of 2735A for the threshold of clean mercury is checked. When the surface flow is allowed to stop in a high vacuum, some impurity attacks the surface, quickly raising the threshold to 2850A. If liquid air is not used this impurity is present in larger amounts and attacks the running surface. Indications are that a surface film is formed and maintained in spite of the flow when liquid air is not used, or requires two hours or more of flow for removal if liquid air is used. This impurity cannot be one of the gases with extremely low melting points. It is not water, but may be a component of the stopcock grease. When the surface is left standing several days in a high vacuum its threshold falls to 2680A. If liquid air is not used the standing surface has a limit of 2560A. All of these values are closely reproducible. Pure hydrogen in contact with the surface does not change the photoelectric behavior. When the mercury is condensed in the presence of hydrogen, some of the gas is dissolved in the metal. This does not change the characteristic threshold of the mercury. It does, however, have the effect of greatly impeding the action of other impurities that form on the surface. This is indicated by the fact that over two hours is required for the change from the threshold of 2735A for the clean surface to the maximum of 2850A, as compared with 13 minutes for this change when hydrogen is not present.</p>
author Dunn, Hugh Kenneth
spellingShingle Dunn, Hugh Kenneth
The Effect of Surface Modification on the Photo-Electric Threshold of Mercury
author_facet Dunn, Hugh Kenneth
author_sort Dunn, Hugh Kenneth
title The Effect of Surface Modification on the Photo-Electric Threshold of Mercury
title_short The Effect of Surface Modification on the Photo-Electric Threshold of Mercury
title_full The Effect of Surface Modification on the Photo-Electric Threshold of Mercury
title_fullStr The Effect of Surface Modification on the Photo-Electric Threshold of Mercury
title_full_unstemmed The Effect of Surface Modification on the Photo-Electric Threshold of Mercury
title_sort effect of surface modification on the photo-electric threshold of mercury
publishDate 1925
url https://thesis.library.caltech.edu/2708/1/Dunn_hk_1925.pdf
Dunn, Hugh Kenneth (1925) The Effect of Surface Modification on the Photo-Electric Threshold of Mercury. Dissertation (Ph.D.), California Institute of Technology. doi:10.7907/Z0D9-RW50. https://resolver.caltech.edu/CaltechETD:etd-06242004-094823 <https://resolver.caltech.edu/CaltechETD:etd-06242004-094823>
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