Underwater Explosion Bubbles Iii the Effects of the Surface And the Bottom On T
Underwater Explosion Bubbles Iii the Effects of the Surface And the Bottom On T
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^ J a^(T) J For derivation, see, e. G. [2]. Experimental data indicate that Herring's formula predicts a too large migration, and the discrepancy is of the order of 50°/o for moderate explosions (300 lb. TNT), For bubbles in infinite water, bp 5, and b- < • This t^hows that our results are in qualitative agreement vrith experiraental data. In presence of boundaries, b„ -^ 0, and it dominates the third order corrootion. We shall estimate its effect hj computing b_ at « the time of the first minimum. In this estimate, we assume that b, is appreciable only during a short time interval near the first mini- mum of the bubble, and that the bubble radius, is during most of its m. Otion. Near its maximura. Then formulae (5«8) yield, approximately, at t = 2t m (7. 11) ] . , p^ ^ 12a;^^'T:A Here, M refers to data at the maximura, m, to data at the mini- k'2 m. Um of the bubble, and A is the average value of a^a . Both IX -33- • • t Pp and p^ are positive. Using the above estimate, we noi-j get (7.
What to read after Underwater Explosion Bubbles Iii the Effects of the Surface And the Bottom On T?
You can find similar books in the "Read Also" column, or choose other free books by Ignace I Kolodner to read online
To quickly assess the difficulty of the text, read a short excerpt:
^ J a^(T) J For derivation, see, e. G. [2]. Experimental data indicate that Herring's formula predicts a too large migration, and the discrepancy is of the order of 50°/o for moderate explosions (300 lb. TNT), For bubbles in infinite water, bp 5, and b- < • This t^hows that our results are in qualitative agreement vrith experiraental data. In presence of boundaries, b„ -^ 0, and it dominates the third order corrootion. We shall estimate its effect hj computing b_ at « the time of the first minimum. In this estimate, we assume that b, is appreciable only during a short time interval near the first mini- mum of the bubble, and that the bubble radius, is during most of its m. Otion. Near its maximura. Then formulae (5«8) yield, approximately, at t = 2t m (7. 11) ] . , p^ ^ 12a;^^'T:A Here, M refers to data at the maximura, m, to data at the mini- k'2 m. Um of the bubble, and A is the average value of a^a . Both IX -33- • • t Pp and p^ are positive. Using the above estimate, we noi-j get (7.
What to read after Underwater Explosion Bubbles Iii the Effects of the Surface And the Bottom On T?
You can find similar books in the "Read Also" column, or choose other free books by Ignace I Kolodner to read online
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