(1) the fundamental frequency is inversely proportional to the length of the string. A stop is inserted under a point on the string, dividing the string into two segments.
(2) the fundamental frequency is directly proportional to the square root of the tension. Note the frequency of the thinner string with two kilograms of weight. Quadrupling the weight doubles the frequency, raising it one octave.
(3) the fundamental frequency is inversely proportional to the square root of the mass per unit length. The thicker string is about twice the diameter or four times the mass per unit length of the thinner string. With the same weight the pitch of the thicker string is about one octave lower. The thicker string must have about four times the tension (hanging mass) of the thinner string to make their fundamental frequencies the same.
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Demonstrate the origin of standing waves from one source and its reflection. Read More
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Illustrate resonance in an air column. Read More
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Demonstrates standing waves in a tube
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