US1625427A - Target for X-ray tubes - Google Patents
Target for X-ray tubes Download PDFInfo
- Publication number
- US1625427A US1625427A US601649A US60164922A US1625427A US 1625427 A US1625427 A US 1625427A US 601649 A US601649 A US 601649A US 60164922 A US60164922 A US 60164922A US 1625427 A US1625427 A US 1625427A
- Authority
- US
- United States
- Prior art keywords
- uranium
- target
- coherent
- ray
- ray tubes
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J35/00—X-ray tubes
- H01J35/02—Details
- H01J35/04—Electrodes ; Mutual position thereof; Constructional adaptations therefor
- H01J35/08—Anodes; Anti cathodes
Landscapes
- X-Ray Techniques (AREA)
Description
Patented Apr, 19, 1927.
' 1,625,42? raiser caries.
HARVEY CLAYTON RENTSOHLER AND JOHN WESLEY MARDEN, OF EAST ORANGE, NEW'JERSEY; .ASSIGNORS TO WESTINGZ-ICUSE LAMP COMPANY, CORPORATION OF PENNSYLVANIA.
No Drawing. Original applicationfiled December 21, 1920, Serial No. 432,326. Divided and this application filed November 17, 1922, Serial No. 601,649. Renewed December 6, 1926.
The present application is a division of our application for an improvement in targets for X-ray tubes, Serial I No. 432,326, filed Dec. 21, 1920, and assigned to the Westinghouse Lamp Company.
This invention relates to'Rontgen or X- ray tubes and, more particularly, to the targets or anticathodes employed in such devices.
It has been recognized for a long time that the intensity of the X rays generated in devices of this character is dependent upon the atomic weight of the anticathode or target. It is well known that the greater the atomic weight of the target, the greater is the intensity of the X-rays emanating from the target. Kaye has arranged the metals having high atomic weights and which are suitable for X-ray targets on the basis of 100 for platinum as follows, the values for uranium and thorium being calculated:
Uranium 125 Thorium 120 Gold 101 Platinum 100 Iridium 98 Osmium 97 Tungsten 91 Tantalum 90 Of these metals, gold is unsuitable owing to its low melting point. Platinum, iridium and osmium are practically eliminated on account of the scarcity of these metals. Uranium has not been used heretofore because it has been impossible to prepare the same in a condition suitable for anticathodes.
Many attempts have been made to produce the heavier rare metals, such as uranium, in dense, coherent, metallic form suitable for targets and for other purposes, but such efforts have uniformly been unsuccessful. So far as we are aware, no one hitherto has succeeded in producing uranium in dense, coherent, metallic form, although the powder of this metal is well known. Owing to the readiness with which uranium oxidizes in the air and the great ease with which it interacts with gases, such as oxygen, hydrogen, water vapor, and the like, it is especially diflicult to obtain metallic uranium in the pure, coherent form.
We have recently discovered that various refractory metals, such as uranium, may be ed Jan. 8, 192 1, on furnaces, and assigned to the Westinghouse Lamp. Company. The
method employed in the production of such coherent metals and the products obtained thereby are described and claimed in our 00- pending application, Serial No. 432,325, filed December 21, 1920, on a method of sintering metals, and assigned to the Westinghouse Lamp Company.
In accordance with the method set forth, we generally prefer to mold or compress a disk or pellet of metal powder, such as uranium, and place the same in a crucible or on a sheet of molybdenum or tungsten which is inserted within a closely wound coil in an evacuated chamber. High-frequency currentis passed through the coil which acts as a primary, inducing secondary currents in the crucible or sheet and the pressed disk of metal powder, sintering the same and forming dense, coherent, metallic uranium.
Uranium has the highest atomic weight of any metal known, namely 238.5. The intensity of emission of X-rays from this metal is in the neighborhood of 20% to 25% greater than the intensity of emission of rays from-platinum. We believe that we are the first ,to have obtained satisfactory X-ray targets which have atomic weights above 200.
We are aware of a patent which claims the use of metallic uranium for X-ray targets but it is not apparent from the description of said patent that the inventor had dense, coherent, metallic uranium. Further- -more, so far as we know, no process had been devised prior to the date of that patent which would. produce substantially pure, coherent uranium, although, as heretofore stated, it was appreciated that this metal m Mimi possesses certain properties which are clesiruble in I l-ray targets.
rrn Iii-ray target oi uranium is eminently suitable for my emission since its melting point is eon'lpz'u'zitivel t' high and its atomic weight the highest known. It is tar superior to the metal tungsten ln'e'v'iously in eonnnon use.
\Ve tlO not; wish to restrict ourselves to the use of the pure .nietzils alone as I l-ray target's, but we may use alloys or mixtures of uranium with thorium or with other metals.
let desired, the I l-ray tulle may he tilled with an inert gas, such ttS argon, helium, and the like.
Vi e claim {15; our invention:
1. ln en I l-ray tube, a target of dense, coherent metallic uranium.
In on X-rey tube, Ft target of substantially pure, coherent, metallic uranium.
3. An zintieatthotle comprisingcoherent, metallic uranium.
meme? 4-. An antieuthode comprising substantially pure, coherent, metallic uranium.
A. target for X-ray tubes and the like consisting; partly of substantially pure, co herent uranium.
(5. A target for X-ray tubes and the like consisting wholl; of substantially pure, cm herent uranium.
7. In an X- 'ny tube, 21 target in a dense, coherentlorm and containing uranium in such proportion that the major portion of X-ruy emission is due to the uranium.
8. A target for an X-rey tube containing COl'lGlQllt uranium in such proportion that the major portion of X-rziy emission is clue to the uranium.
In testimony whereof, We have hereunto subscribed our names this sixteenth day of November, 1922.
HARVEY CLAYTON RENTSCHLER. JGHN WESLEY MARDEN.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US601649A US1625427A (en) | 1920-12-21 | 1922-11-17 | Target for X-ray tubes |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US432326A US1625426A (en) | 1920-12-21 | 1920-12-21 | Target for x-ray tubes |
US601649A US1625427A (en) | 1920-12-21 | 1922-11-17 | Target for X-ray tubes |
Publications (1)
Publication Number | Publication Date |
---|---|
US1625427A true US1625427A (en) | 1927-04-19 |
Family
ID=27029451
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US601649A Expired - Lifetime US1625427A (en) | 1920-12-21 | 1922-11-17 | Target for X-ray tubes |
Country Status (1)
Country | Link |
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US (1) | US1625427A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2464591A (en) * | 1944-04-04 | 1949-03-15 | Mallory & Co Inc P R | Method of bonding a tungsten member to a backing member |
US3689795A (en) * | 1970-06-02 | 1972-09-05 | Schwarzkopf Dev Co | Boron-containing rotating x-ray target |
-
1922
- 1922-11-17 US US601649A patent/US1625427A/en not_active Expired - Lifetime
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2464591A (en) * | 1944-04-04 | 1949-03-15 | Mallory & Co Inc P R | Method of bonding a tungsten member to a backing member |
US3689795A (en) * | 1970-06-02 | 1972-09-05 | Schwarzkopf Dev Co | Boron-containing rotating x-ray target |
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