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Showing papers on "Shields published in 1968"


K. Obrien1, A. Reetz
01 Jan 1968
TL;DR: In this article, the authors present a method for calculating radiation penetration through protective shields in space radiation transport, spacecraft shielding design and advanced concepts, and methods for calculating the radiation penetration.
Abstract: Space radiation transport, spacecraft shielding design and advanced concepts, and methods for calculating radiation penetration through protective shields - conference

10 citations


01 Nov 1968
TL;DR: In this paper, the effects of shield spacing number, emissivity, lateral conductance, and targeting (high-emissivity coatings on annular rings of shields) on thermal performance were investigated.
Abstract: : Experiments were performed on multiple flat-disk shadow shields to determine the effects of shield spacing number, emissivity, lateral conductance, and targeting (high-emissivity coatings on annular rings of shields) on thermal performance. The experimental data, in general, agreed closely with an analytical model which assumed diffuse surfaces with nonuniform radiosity. A shadow-shield system for a hypothetical space vehicle was designed, scaled down, and tested. Results demonstrated: (1) a lightweight method of shield construction; (2) shield-support interactions: and (3) reduction of support heat leaks by shield location, attachment methods, and the use of high-emissivity coatings.

8 citations


Patent
Cramer Joseph F1, Rezek John R1
15 Jul 1968
TL;DR: In this paper, a miniature radio receiver operating at ultra-high frequency including coils and individual conductive shields forming helical resonators is described. And the coils are tuned at the low-impedance end by aluminum slugs providing low loss, and may be capacitively loaded at the high-impingance end.
Abstract: Tuner for miniature radio receiver operating at ultrahigh frequency including coils and individual conductive shields forming helical resonators The coils are tuned at the lowimpedance end by aluminum slugs providing low loss, and may be capacitively loaded at the high-impedance end Apertures in the shields provide coupling between the adjacent resonators, with the aperture in one shield being of the size to control the coupling and the aperture in the adjacent shield being larger so that it does not affect the coupling

7 citations



Patent
31 Dec 1968
TL;DR: In this paper, a radiation shield for furnaces is described, which is made of a removable ray protection element and a plurality of foil layers, and is used to protect furnaces from radiation.
Abstract: This invention relates to radiation shields for furnaces. Such shields are made of a removable ray protection element and a plurality of foil layers.

5 citations


Journal ArticleDOI
TL;DR: In this article, a simple formula for the minimum attenuation of incoming plane waves in spherical shields is presented for practical purposes, where the medium inside and outside the shield is air and the material is supposed to be well conducting.
Abstract: In this communication, a simple formula for the minimum attenuation of incoming plane waves in spherical shields is presented for practical purposes. This worst case condition is attained when the TM 011 resonance occurs in the room. The medium inside and outside the shield is air and the material is supposed to be well conducting.

5 citations


Journal ArticleDOI
TL;DR: The magnetic shield simulator (MAGSIM) as mentioned in this paper is an analog device that provides a simple means for directly measuring the forbidden volume or protective region produced by externally deflecting magnets, which can be employed to determine the protective volume for certain complex magnet configurations.
Abstract: Externally deflecting magnets provide a protective region around space vehicles which shields them from the hazardous space radiation. The magnetic shield simulator (MAGSIM) is an analog device that provides a simple means for directly measuring the forbidden volume or protective region produced by externally deflecting magnets. The MAG SIM has been employed to determine the protective volume for certain complex magnet configurations. These configurations include two coplanar coaxial current loops of different radii, and two quasihollow conductor configurations. In addition, the assumption of substituting an equivalent simple loop for a hollow conductor has been checked. In general, the simple-loop approximation predicts results in agreement with measurements with the hollow conductor magnet; however, the measured outward displacement of the forbidden volume from the center of the magnet is approximately 20% larger than that predicted by simple-loop theory. The ability to shape the forbidden region to match the shape of the vehicle is described.

4 citations


Patent
25 Oct 1968
TL;DR: In this paper, a tungsten dispenser cathode for a magnetron is described, which is provided with end shields in the form of solid graphite rings to improve suppression of undesirable electron emission.
Abstract: A tungsten dispenser cathode for a magnetron is described. The cathode is provided with end shields in the form of solid graphite rings to improve suppression of undesirable electron emission.

3 citations


01 Jan 1968
TL;DR: Inflatable solar shields for thermal protection of space vehicles utilizing cryogen propellants were used for the first time in this paper, where they were used to protect space vehicles from thermal degradation.
Abstract: Inflatable solar shields for thermal protection of space vehicles utilizing cryogen propellants

2 citations



Proceedings ArticleDOI
23 Jul 1968


01 Oct 1968
TL;DR: In this article, a direct algebraic approach for the design of Cassegrain light shields is proposed, where the surfaces of the mirrors are assumed to be plane surfaces and the main purpose of the shields is to avoid direct sky light falling on the image plane.
Abstract: A direct algebraic desigll oi Cassegraill light shields is proposed, usillg ollly the assul1lption that the mirror surfaces are fla t. lntrodllction During the design and construction of a Cassegrain or Ritchey-Chretien telescope, the design of an adequate shielding is required in order to avoid direct sky light falling on the focal planeo A sol ution to this problem has been worked out by means of a graphical method, using succesive approximationst, and later applied to electronic computers2. Recently, a different graphical solution has been explained, based also on succesive approximations3. Therefore, the possibility of a direct solution was studied. The final goal was reached using in this method only the approximation of considering the surfaces of the mirrors as plane surfaces. Parameters 01 a Cassegrain system. The main purpose of the shields in a Cassegrain system is to avoid direct sky light falling on the image planeo As the field increases the required shielding introduces two new problems, vignetting and central obscuration. The central obscuration is produced by the large size of the diameter of the shield at the secondary mirror and the vignetting is due to both shields. (See Fig. 2). Hence as it is pointed out by Young(2), these factors will set the conditions for the solution of the problem and will establish a compromise between the allowable field size and central obscuration.