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Superposition and Standing Waves EXAMPLES
Chapter 18 Superposition and Standing Waves EXAMPLES
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Chapter 18 Superposition and Standing Waves: EXAMPLES
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Example 18-1: Formation of a Standing Wave
Assume two waves are traveling in opposite direction to produce a standing wave y = (2A sinkx) cosωt = ymax cos ωt y1 = 4 sin(3x – 2t) and y2 = 4 sin(3x + 2t ) x and y in centimeters and t in seconds (A) Find the amplitude of the SHM (2A sinkx) of the element located at x = 2.3 cm A = 4 cm, k = 3 rad/cm, = 2 rad/s From the resultant wave will have: ymax = 2Asin(kx) = 8sin(kx) = 8 sin(3 · 2.3) = 4.6 cm
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Example 18-1: Formation of a Standing Wave, final
(B) Find the position of the nodes and antinodes if one end of the string is at x = 0 k = 3 rad/cm = 2/ = 2/3 cm Nodes: Antinodes: (C) Find ymax for an element located at an antinode An antinode occurs at a point of maximum displacement ymax = ±2A = ± 8.0 cm
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Example 18-2: Harmonics A middle “C” on a piano has a fundamental frequency of 262 Hz. What are the next two harmonics of this string? ƒ1 = 262 Hz ƒ2 = 2ƒ1 = 524 Hz ƒ3 = 3ƒ1 = 786 Hz
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Example 18-3: More About Harmonics
The first A above middle C has a fundamental frequency of 440 Hz. If both strings have the same linear mass density and length L, find the ratio between the two tensions.
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Example 18-4: Resonance If pendulum A is set into motion, the other pendulums begin to oscillate due to waves transmitted through the beam Pendulum C has a greater amplitude than B or D C’s length is closest to A’s and so C’s natural frequency is closest to the driving frequency from A
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Standing Wave on a String, Example Set-Up
One end of the string is attached to a vibrating blade. The other end passes over a pulley with a hanging mass attached to the end. This produces the tension in the string. The string is vibrating in its second harmonic. Section 18.3
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Material from the book to Study!!!
Material for the Midterm Material from the book to Study!!! Objective Questions: 1-6 Conceptual Questions: 1-2 Problems:
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