Pocketbook of Useful Formulæ and Memoranda
for Civil and Mechanical Engineers

Forfatter: Guilford L. Molesworth

Sider: 744

UDK: 600 (093)

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276 Molesworth’s pocket-book Waves. ■ A wave may travel without force to maintain its motion, provided it be long in proportion tu the depth of the fluid. 2. When the length of a wave is not greater than the depth of the water, the velocity of the wave depends (sensibly) only on its length, and is proportional to the square root of its length. 3. When the length is not less than 1000 times the depth of the water, the velocity depends only on the depth, and is the same as the velocity which a free body would acquire by falling throuo-h a height = half the depth of the water. 4. 1 or intermediate proportions, the velocity can only, be obtained by a general equation. Under no circumstances does an unbroken wave exceed 30 or 40 feet in height. A wave breaks when its height above the general level of the water is equal to the general depth.—Prof. Airev, ‘Encvdon Metrop.,’ “ Tides.” 1 V = Velocity of wave in feet per second. T = Time of wave in seconds. D = Depth of water in feet. II = Height of wave in feet. L = Length of wave in feet. when L is less than D. V = V 32-17 D when L exceeds 1000 D. — ^///32-17D (1 + 3^ j when the height of the wave bears a sensible proportion to the depth. T — -55 VL ) V = 1-818 a/L J