University Physics: Waves and Electricity Ch17. Longitudinal Waves Lecture 4 Dr.-Ing. Erwin Sitompul
4/2 January–April 2010University Physics: Wave and Electricity Homework 3: Standing Waves Two identical waves (except for direction of travel) oscillate through a spring and yield a superposition according to the equation (a)What are the amplitude and speed of the two waves? (b)What is the distance between nodes? (c)What is the transverse speed of a particle of the string at the position x = 1.5 cm when t = 9/8 s?
4/3 January–April 2010University Physics: Wave and Electricity Solution of Homework 3 (a)Identical except direction of travel ► standing waves: (b)Distance between nodes:
4/4 January–April 2010University Physics: Wave and Electricity Solution of Homework 3 (c)Transversal speed: At x = 1.5 cm = 15 mm and t = 9/8 s = 3/160 min,
4/5 January–April 2010University Physics: Wave and Electricity Sound Waves From previous chapter we know that mechanical waves are classified into transverse waves and longitudinal waves. In this class, a sound wave is defined roughly as a longitudinal waves. The figure above illustrates several ideas useful for the next discussions. Point S represents a tiny sound source, called a point source. It emits sound waves in all directions. Wavefronts are surfaces over which the oscillation due to the sound wave have the same value. Rays are directed lines perpendicular to the wavefronts that indicate the direction of travel of the wavefronts.
4/6 January–April 2010University Physics: Wave and Electricity Sound Waves As a longitudinal wave, sound wave travels through a medium (solid, liquid, or gas), involving oscillations parallel to the direction of wave travel. When a sound wave moves in time, the displacement of air molecules, the pressure, and the density vary sinusoidally with the frequency of the vibrating source.
4/7 January–April 2010University Physics: Wave and Electricity Interference Like transverse waves, sound waves can undergo interference. Now we will consider, in particular, the interference between two identical sound waves traveling in the same direction. Two point sources S 1 and S 2 emit sound waves that are in phase and of identical wavelength λ. Thus, as the waves emerge from the sources, their displacements are always identical. The waves travels through point P, with the distance L 1 or L 2 much greater than the distance between the sources, S 1 and S 2. The two sources can be approximated to travel in the same direction at P.
4/8 January–April 2010University Physics: Wave and Electricity Interference From the figure, the path L 2 traveled by the wave from S 2 is longer than the path L 1 traveled by the wave from S 1. The difference in path lengths means that the waves may not be in phase at point P. The phase difference Φ at P depends on their path length difference, The relation between phase difference to path length difference, as we recall from previous chapter, is:
4/9 January–April 2010University Physics: Wave and Electricity Fully constructive interference occurs when Φ is zero, 2π, or any integer multiple of 2π. Fully constructive interference Fully destructive interference occur when Φ is an odd multiple of π, Interference Fully destructive interference
4/10 January–April 2010University Physics: Wave and Electricity Interference Fully destructive, arrive “out of phase” Fully constructive, arrive “in phase”
4/11 January–April 2010University Physics: Wave and Electricity Example: Interference Two point sources S 1 and S 2, which are in phase and separated by distance D = 1.5λ, emit identical sound waves of wavelength λ. (a)What is the path length difference of the waves from S 1 and S 2 at point P 1, which lies on the perpendicular bisector of distance D, at a distance greater that D from the sources? What type of interference occurs at P 1 ? The waves undergo fully constructive interference at P 1
4/12 January–April 2010University Physics: Wave and Electricity Example: Interference (b)What are the path length difference and type of interference at point P2?P2? The waves undergo fully destructive interference at P 2
4/13 January–April 2010University Physics: Wave and Electricity Example: Interference (c) (c) The figure below shows a circle with a radius much greater than D, centered on the midpoint between sources S1 S1 and S 2. What is the number of points N around this circle at which the intereference is fully constructive? Using the symmetry, as we go around the circle, we will find 6 points where the interference is a fully constructive interference
4/14 January–April 2010University Physics: Wave and Electricity Homework 4: Two Speakers Two speakers separated by distance d 1 = 2 m are in phase. A listener observes at distance d 2 = 3.75 m directly in front of one speaker. Consider the full audible range for normal human hearing, 20 Hz to 20 kHz. Sound velocity is 343 m/s. (a)What is the lowest frequency f min,1 that gives minimum signal (destructive interference) at the listener’s ear? (b)What is the second lowest frequency f min,2 that gives minimum signal? (c)What is the lowest frequency f max,1 that gives maximum signal (constructive interference) at the listener’s ear? (d)What is the highest frequency f max,n that gives maximum signal?
4/15 January–April 2010University Physics: Wave and Electricity Homework 4: Other Two Speakers New Two loudspeakers, A and B, are driven by the same amplifier and emit sinusoidal waves in phase. Speaker B is 12 m to the right of speaker A. The frequency of the waves emitted by each speaker is 686 Hz. Sound velocity is 343 m/s. You are standing between the speakers, along the line connecting them, and are at a point of constructive interference. (a)How far must you walk toward speaker B to move to a point of destructive interference? (b)How far must you walk toward speaker B to move to another point of constructive interference?