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Learn about the properties and varieties of mechanical waves, and how to calculate their speed and energy. Understand wave interference and analyze standing waves on a string.
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Chapter 15 Mechanical Waves Modifications by Mike Brotherton and Jim Verley
Goals for Slightly Abbreviated Chapter 15 • To study the properties and varieties of mechanical waves • To relate the speed, frequency, and wavelength of periodic waves • To interpret periodic waves mathematically • To calculate the speed of a wave on a string • To calculate the energy of mechanical waves • To understand the interference of mechanical waves • To analyze standing waves on a string
Introduction • Earthquake waves carry enormous power as they travel through the earth. • Other types of mechanical waves, such as sound waves or the vibration of the strings of a piano, carry far less energy. • Marvel’s Skye AKA Daisy Johnson AKA “Quake” has the power to amplify mechanical vibrations.
Types of mechanical waves • A mechanical wave is a disturbance traveling through a medium. • Figure 15.1 below illustrates transverse waves and longitudinal waves.
Periodic waves • For a periodic wave, each particle of the medium undergoes periodic motion. • The wavelength of a periodic wave is the length of one complete wave pattern. • The speed of any periodic wave of frequency f is v = f.
Periodic transverse waves • For the transverse waves shown here in Figures 15.3 and 15.4, the particles move up and down, but the wave moves to the right.
Periodic longitudinal waves • For the longitudinal waves shown here in Figures 15.6 and 15.7, the particles oscillate back and forth along the same direction that the wave moves. • Follow Example 15.1.
Mathematical description of a wave • The wave function, y(x,t), gives a mathematical description of a wave. In this function, y is the displacement of a particle at time t and position x. • The wave function for a sinusoidal wave moving in the +x-direction is y(x,t) = Acos(kx – t), where k = 2π/is called the wave number. • Figure 15.8 at the right illustrates a sinusoidal wave.
The speed of a wave on a string • Follow the first method using Figure 15.11 above. • Follow the second method using Figure 15.13 at the right. • The result is
Calculating wave speed • Follow Example 15.3 and refer to Figure 15.14 below.
Power in a wave • A wave transfers power along a string because it transfers energy. • The average power is proportional to the square of the amplitude and to the square of the frequency. This result is true for all waves. • Follow Example 15.4.
Wave intensity • The intensity of a wave is the average power it carries per unit area. • If the waves spread out uniformly in all directions and no energy is absorbed, the intensity I at any distance r from a wave source is inversely proportional to r2: I 1/r2. (See Figure 15.17 at the right.) • Follow Example 15.5.
Wave interference and superposition • Interference is the result of overlapping waves. • Principle of super-position:When two or more waves overlap, the total displacement is the sum of the displace-ments of the individual waves. • Study Figures 15.20 and 15.21 at the right.
Standing waves on a string • Waves traveling in opposite directions on a taut string interfere with each other. • The result is a standing wave pattern that does not move on the string. • Destructive interference occurs where the wave displacements cancel, and constructive interference occurs where the displacements add. • At the nodes no motion occurs, and at the antinodes the amplitude of the motion is greatest. • Figure 15.23 on the next slide shows photographs of several standing wave patterns.
Photos of standing waves on a string • Some time exposures of standing waves on a stretched string.
Chapter 16 Sound and Hearing Modifications by Mike Brotherton and Jim Verley
Goals for Abbreviated Chapter 16 • To describe sound waves in terms of particle displacements or pressure variations • To calculate the speed of sound in different materials • To calculate sound intensity • To find what determines the frequencies of sound from a pipe • To learn why motion affects pitch
Introduction • Most people prefer listening to music instead of noise. (Is that statement a no-brainer?) • We can think of a sound wave either in terms of the displace-ment of the particles or of the pressure it exerts. • How do humans actually perceive sound? • Why is the frequency of sound from a moving source different from that of a stationary source? • Beware Black Canary’s sonic scream!
Sound waves • Sound is simply any longitudinal wave in a medium. • The audible range of frequency for humans is between about 20 Hz and 20,000 Hz. • Ultrasonic sound waves have frequencies above human hearing and infrasonic waves are below. • Figure 16.1 at the right shows sinusoidal longitudinal wave.
Different ways to describe a sound wave • Sound can be described by a graph of displace-ment versus position, or by a drawing showing the displacements of individual particles, or by a graph of the pressure fluctuation versus position. • The pressure amplitude is pmax = BkA. • B is the bulk modulus from Ch. 11, which we skipped, where B=-p(x,t)/(dv/V)
Speed of sound waves • The speed of sound depends on the characteristics of the medium. Table 16.1 gives some examples. • The speed of sound:
The speed of sound in water and air • Follow Example 16.3 for the speed of sound in water, using Figure 16.8 below. • Follow Example 16.4 for the speed of sound in air.
Sound intensity • The intensity of a sinusoidal sound wave is proportional to the square of the amplitude, the square of the frequency, and the square of the pressure amplitude. • Study Problem-Solving Strategy 16.1. • Follow Examples 16.5, 16.6, and 16.7.
The decibel scale • The sound intensity level is = (10 dB) log(I/I0). • Table 16.2 shows examples for some common sounds.
Examples using decibels • Follow Example 16.8, which deals with hearing loss due to loud sounds. • Follow Example 16.9, using Figure 16.11 below, which investigates how sound intensity level depends on distance.
Standing sound waves and normal modes • The bottom figure shows displacement nodes and antinodes. • A pressure node is always a displace-ment antinode, and a pressure antinode is always a displacement node, as shown in the figure at the right.
The Doppler effect • The Doppler effect for sound is the shift in frequency when there is motion of the source of sound, the listener, or both. • Use Figure 16.27 below to follow the derivation of the frequency the listener receives.
The Doppler effect and wavelengths • Study Problem-Solving Strategy 16.2. • Follow Example 16.14 using Figure 16.29 below to see how the wavelength of the sound is affected.
The Doppler effect and frequencies • Follow Example 16.15 using Figure 16.30 below to see how the frequency of the sound is affected.
A moving listener • Follow Example 16.16 using Figure 16.31 below to see how the motion of the listener affects the frequency of the sound.