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Dr. Jie ZouPHY 13711 Chapter 18 Superposition and Standing Waves.

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Presentation on theme: "Dr. Jie ZouPHY 13711 Chapter 18 Superposition and Standing Waves."— Presentation transcript:

1 Dr. Jie ZouPHY 13711 Chapter 18 Superposition and Standing Waves

2 Dr. Jie ZouPHY 13712 Outline Superposition and interference Superposition principle Constructive and destructive interference Superposition of sinusoidal waves Interference of sound waves

3 Dr. Jie ZouPHY 13713 Superposition principle Superposition principle: If two or more traveling waves are moving through a medium, the resultant value of the wave function at any point is the algebraic sum of the values of the wave functions of the individual waves. Linear waves and nonlinear waves

4 Dr. Jie ZouPHY 13714 Superposition of two pulses Two traveling waves can pass through each other without being destroyed or even altered. Interference: The combination of separate waves in the same region of space to produce a resultant wave is called interference. Constructive interference Destructive interference

5 Dr. Jie ZouPHY 13715 Superposition of sinusoidal waves Two sinusoidal waves traveling in the same linear medium: y 1 = A sin(kx-  t) y 2 = A sin(kx-  t+  ) Resultant wave function: y = y 1 + y 2 = 2A cos(  /2)sin(kx-  t+  /2). If  = 0, 2 , 4  …, y 1 and y 2 are in phase and interfere constructively; y has an amplitude = 2A. If  = , 3  …, y 1 and y 2 are  rads out of phase and interfere destructively; y has an amplitude = 0. If 0 <  < , y has an amplitude between 0 and 2A.

6 Dr. Jie ZouPHY 13716 Interference of sound waves A phase difference may arise between two waves generated by the same source when they travel along paths of unequal lengths. Because a path difference of one wavelength corresponds to a phase angle of 2  rad,  /2  =  r/, or  r= (  /2  ). Conditions for constructive and destructive interference:  r = (2n) ( /2) for constructive interference  r = (2n+1) ( /2) for destructive interference Some definitions: Path length r: the distance along any path from speaker to receiver. Path difference  r = |r 2 – r 1 |

7 Dr. Jie ZouPHY 13717 Graphical example of interference of sound waves

8 Dr. Jie ZouPHY 13718 Example 18.1 A pair of speakers placed 3.00 m apart are driven by the same oscillator. A listener is originally at point O, which is located 8.00 m from the center of the line connecting the two speakers. The listener then walks to point P, which is a perpendicular distance 0.350 m from O, before reaching the first minimum in sound intensity. What is the frequency of the oscillator?

9 Dr. Jie ZouPHY 13719 Homework Ch. 18, Problems: #1, 5, 8, 11.


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