. Acoustic scattering in the ocean. Project TRIDENT; Underwater acoustics; Sound-waves. III-24 liOOO r 1 1—r—I—Mill r 100 s = DAMPING CONSTANT .01 "< I I I I 11 » 1—I—I Mill 1—n—I—I I I I (0= BUBBLE RADIUS) a = .001. I L_J I I I II I I L_l I II I I I 100 f 1,000 f 10,000 1,000 RESONANCE RESONANCE J L_l I I I I I I L—ij I 1_L ? 100,000 + I RESONANCE RESONANCE I III ,000,000 0 = I cm 0 = .1 cm a = .01 cm f = FREQUENCY OF INCIDENT SOUND (cps) a = .001 cm FIGURE 111=8 DAMPING CONSTANT FOR FOUR TYPICAL BUBBLE SIZES AS A FUNCTION OF FREQUENCY S-7001-Q307. Please note that these images are ex


. Acoustic scattering in the ocean. Project TRIDENT; Underwater acoustics; Sound-waves. III-24 liOOO r 1 1—r—I—Mill r 100 s = DAMPING CONSTANT .01 "< I I I I 11 » 1—I—I Mill 1—n—I—I I I I (0= BUBBLE RADIUS) a = .001. I L_J I I I II I I L_l I II I I I 100 f 1,000 f 10,000 1,000 RESONANCE RESONANCE J L_l I I I I I I L—ij I 1_L ? 100,000 + I RESONANCE RESONANCE I III ,000,000 0 = I cm 0 = .1 cm a = .01 cm f = FREQUENCY OF INCIDENT SOUND (cps) a = .001 cm FIGURE 111=8 DAMPING CONSTANT FOR FOUR TYPICAL BUBBLE SIZES AS A FUNCTION OF FREQUENCY S-7001-Q307. Please note that these images are extracted from scanned page images that may have been digitally enhanced for readability - coloration and appearance of these illustrations may not perfectly resemble the original Meyer, R. F; Romberg, B. W; Arthur D. Little, Inc. Cambridge, Mass. : Arthur D. Little, Inc.


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