Sélectionnez la section dans laquelle vous souhaitez faire votre recherche. The designs of a magnetic field integrator-transducer and nolinear transformer for programmed frequency control in the 7-Bev proton synchrotron are given. Désolé, un problème s'est produit lors de l'enregistrement de vos préférences en matière de cookies. (For preceding period see ANL-57l3.) Afficher ou modifier votre historique de navigation, Recyclage (y compris les équipements électriques et électroniques), Annonces basées sur vos centres d’intérêt. Acceleration elements are constructed in the form of drift tubes distributed in 11 compensating magnets.

The phase shift between any two channels does not exceed 30 deg . Variateurs de vitesse - fréquence Exemple de programmation Danfoss.
2. Measurements on end-effects were made on the 1/7-scale model magnet. A study is made of switching circuitry for capacitor energy storage apparatus, the flux concentrator idea, and the design of tape-wound coils. FREQUENCY PROGRAMMING (in Russian) Full Record; Other Related Research; Abstract. it is shown that almost certain charge sign identification is possible for tracks of over 2 mm length, for BETA =.7 in a field of 200 kilogauss. Nous utilisons des cookies et des outils similaires pour faciliter vos achats, fournir nos services, pour comprendre comment les clients utilisent nos services afin de pouvoir apporter des améliorations, et pour présenter des annonces.

Découvrez Nostalgia [Explicit] de Frequency Programming sur Amazon Music. An inverse momentum, qm, is calculated from these curvatures. Test data confirm the high-precision of the functional transformer. A plan view of a nviently driven to form a pile bent. This type of coil proves to be quite simple to build, very compact, and relatively easy to cool. The total power consumption is 400 kv. En passant une commande, vous acceptez nos. Veuillez réessayer. The variation in the effective magnetic end position as function of the central field value and also thc radial shape of the. Pump-down data for air in a 23-ft stanless stcel chamber with an Evaportion pump are tabulated. The measured distributions are: at 1 cm, q/sub m/ = 1.013 plus or minus .027 c/Bev and sigma =.227 c/Bev; and at2 cm, q/sub m/= 1.04 plus or minus .017 c/Bev and 0 =.15 c/ Bev. For 1 cm track lengths, q/sub 0/ = 1.07 c/Bev and sigma =.225 c/Bev; and for 2 cm track lengths, q/sub 0/ = 1.07 c/Bev and sigma =.15 c/Bev.

However, the flux concentrator is inefficient (~ 3%) when used with tape-wound primaries and long field pulse times. Two-hundred-thirty of these proton tracks are coordinate scanned and their curvatures measured.