Lecture 16

1. Lecture 16 Electro-acoustics Microphones Amplifiers Tuners Loudspeakers Instructor: David Kirkby (dkirkby@uci.edu)Guest Lecturer: David Casper (dcasper@uci.edu)

2. The Need for Electro-acoustics • The intensity of sound decreases rapidly with distance, especially if the source radiates sound in all directions. • If a conductor normally hears a 100-voice choir from 3.2m away, it only sounds as loud as 10 voices from 10m away, and the same as just one voice from a distance of 32m. 32m0.01 DistanceIntensity 10m0.1 1m10.0 3.2m1.0 Physics of Music, Lecture 16, D. Casper

3. Transducers and “Pipelines” • A device that converts one form of energy into another is called a transducer. • The process of converting sound energy to electrical energy, modifying and amplifying the electrical signal, and then converting the electrical energy back to sound is called an audio pipeline, or sound reinforcement. SoundSources SoundOutput Effects,Equalizer Mixer Amplifier Transducer(Speaker) Effects Transducers(Microphones,Pickups) Physics of Music, Lecture 16, D. Casper

4. Sound and Analog Signals • Sound can be described as a superposition of waves: • At any time, a wave has an associated amplitude • A wave’s amplitude can be positive or negative • The sum of two waves is just the sum of their amplitudes • The electric currents in our audio pipeline have all the same properties! • In a purely “analog” sound system, we simply translate sound amplitudes into equivalent electric currents and (eventually) back again. • An ideal system where this works perfectly is said to be “linear” Sound wave Current Physics of Music, Lecture 16, D. Casper

5. Converting Sound to Electricity • A Microphone converts sound vibrations to electric signals. • The first microphone was part of Alexander Graham Bell’s telephone (1876) and used a liquid. • Two years later, the carbon microphone was invented. It is still used in some telephones today. • The ribbon microphone was developed for radio and is sometimes used for studio recording of vocals. Physics of Music, Lecture 16, D. Casper

6. Dynamic Microphones • The dynamic microphone is one of the most commonly used today. • It relies on the fact that a current is produced by moving a coil of wire in a magnetic field (“induction”). • The coil is attached to a diaphragm, which picks up vibrations in the air • Dynamic microphones are rugged and relatively inexpensive. They are also able to handle high sound volume. • Their frequency response is not as linear as condenser (or ribbon) microphones Physics of Music, Lecture 16, D. Casper

7. Condenser Microphone Basics • Condenser microphones are the other commonly used type. • Condenser microphones rely on electric forces rather than magnetic. • Parallel plates are charged by a battery; the incoming sound causes the distance between plates to change slightly, altering the amount of charge on the plates and creating a current. • Condenser microphones have more uniform frequency response, but are expensive and require a battery. They can also “pop” when very near the source. Physics of Music, Lecture 16, D. Casper

8. Omnidirectional and Cardioid Microphones • Not all microphones are equally sensitive to sound from all directions (“omnidirectional”). Omnidirectional mic’s have a diaphragm open only at the front. • The Cardioid microphone is so called because its directional sensitivity resembles a heart shape. Cardiod mic’s have a diaphragm exposed to air front and back. Vibrations from the back partially cancel those from the front. Physics of Music, Lecture 16, D. Casper

9. Directional Microphones • “Shotgun” or linear microphones are often used for recording video in noisy/crowded areas. • They use a tubular design which accepts sound coming along the direction of the tube, while sound from the side cancels. These microphones have a relatively limited frequency range. • Dish microphones are used to increase the total intensity of sound (up to 75 times) by focusing it with a parabolic reflector Physics of Music, Lecture 16, D. Casper

10. Converting Electricity to Sound • Loudspeakers are transducers which perform the opposite task of microphones – they convert electrical signals into sound. • Most home stereo systems use dynamic loudspeakers. • In their most basic version, a diaphragm vibrates to produce sound waves in the air. Physics of Music, Lecture 16, D. Casper

11. Dynamic Loudspeaker Operation • Dynamic speakers take the alternating electric current of the audio pipeline and use it to vibrate a diaphragm. • The principle is the opposite of the dynamic microphone: the electronic currents in a coil attached to the cone make it an alternating electromagnet, which is attracted and repulsed, in turn, by a stationary magnet. Physics of Music, Lecture 16, D. Casper

12. Baffles • When the wavelength of the signal is the same or larger than the diameter of the speaker cone, a dynamic speaker by itself does a very poor job of getting air moving. • Waves from the back of the cone interfere destructively with those from the front. • Even for a large 16” speaker, the wavelength equals the diameter at around 850 Hz. • Baffles prevent waves from back from reaching the front. Physics of Music, Lecture 16, D. Casper

13. Simple Enclosures • For lower tones, the efficiency of a speaker is greatly improved by enclosing it in a resonating cavity • In the closed baffle, or air suspension configuration, compression of the air trapped in the cavity adds to the restoring force on the speaker cone, allowing it to move further in and out. • This set-up allows good bass response from a relatively small speaker. Physics of Music, Lecture 16, D. Casper

14. Bass Reflex Speakers • Bass reflex speakers have a vent (hole) in the front, which allows vibrations from the back of the chamber to produce sound as well as the cone. • The result is lower power consumption than an air suspension speaker, and smoother, extended bass response. Physics of Music, Lecture 16, D. Casper

15. Efficiency of Dynamic Loudspeakers • Almost all the energy used to drive a dynamic loudspeaker is “wasted” – not converted to sound energy. • This inefficiency is due to the relative lightness of air – imagine trying to punch a handkerchief – you cannot transfer much energy to it. • Because dynamic speakers are very inefficient, they require a large amount of power (from an amplifier) to operate. • Their low efficiency also makes them poor choices for public address systems, where sound is to be projected over a very large area Physics of Music, Lecture 16, D. Casper

16. Horn Loudspeakers • Horn loudspeakers have a moving voice coil driving a membrane which resonates in a horn. • The horn results in far more efficient use of energy (40-50%) than a dynamic loudspeaker, hence these speakers are typically used for public-address and concert sound systems (also bullhorns) • The geometry of the horn must be chosen to match the wavelength of sound it will reproduce; for low frequency, folded or more complicated shapes are required Physics of Music, Lecture 16, D. Casper

17. Woofers, Tweeters and Midrange • To achieve the highest quality response over all frequencies, audio systems use two or more speakers of differing sizes. • A small horn speaker is often chosen as the “tweeter” for highest frequencies. • A large dynamic (or bass reflex) speaker serves as the “woofer” for bass. • An intermediate midrange is sometimes added. • The frequencies driving each speaker are controlled by a “cross-over unit” inside the speaker cabinet. Physics of Music, Lecture 16, D. Casper

18. Noise-Cancelling Headphones • Bose Corporation has invented a technology which uses the principle of superposition to reduce low-frequency noise • The headsets contain a small microphone that measures the ambient sound-level near your head and generates an inverted (out of phase) wave to cancel it before it reaches your ears. • The circumaural seal filters out higher frequencies. • Similar technology is now being used by some rock drummers to reduce ear damage in concert. Physics of Music, Lecture 16, D. Casper

19. Amplifiers • Amplifiers take low-power signals produced by microphones and other transducers and increase the power to levels sufficient to drive speakers. • Amplifiers work by using the low-power input signal to control a higher power output signal, like controlling a knob on a dial. • Transistors (or vacuum tubes) serve as the switches that make amplifiers work. They generate large amounts of heat in the process. • “Pre-amplifiers” are sometimes used in the pipeline, but they boost only voltage (to make the signal larger compared to noise introduced afterward), not power. Physics of Music, Lecture 16, D. Casper

20. Harmonic Distortion • If an amplifier is not linear, we say it introduces distortion. • Harmonic distortion occurs when the output pulse is clipped due to overloading some component. • In that case, higher harmonics of the original tone(s) are introduced. • If harmonic distortion is small, it may be unnoticeable, since most music contains several harmonics anyway. Physics of Music, Lecture 16, D. Casper

21. Intermodulation (IM) Distortion • When an amplifier is truly non-linear (not just overloaded), it introduces new frequencies in the waveform which are not harmonics of any already present. IM distortion is likely to be more noticeable. • Transient IM (TIM) distortion occurs when the amplifier cannot respond to rapid changes in the input signal, and has similar effects on sound quality. Physics of Music, Lecture 16, D. Casper

22. Radio Broadcasts • Two different methods are used to transmit commercial radio broadcasts • AM (Amplitude Modulation):Amplitude of a carrier wave (540-1600 kHz) is modulated with the signal. May only transmit frequencies up to 5000 Hz, limiting audio quality. • FM (Frequency Modulation): • Frequency of carrier wave(88-108 MHz) is modulated with signal. Due to higher frequency of carrier, better audio quality but shorter range. Physics of Music, Lecture 16, D. Casper

23. The Electromagnetic Spectrum • AM and FM radio broadcasts are electromagnetic radiation, in other words light. • Radio waves are a color of light that our eyes can’t see, like the rest of the electromagnetic spectrum. The wavelength of an FM wave is a few meters. The wavelength of an AM wave is a few hundreds of meters. Physics of Music, Lecture 16, D. Casper

24. Stereo Broadcasts • Broadcasts in FM stereo represent a challenge because two signals must be encoded, but the transmission must also be compatible with monaural reception by non-stereo devices. • The solution is to use one band of frequencies to store the L+R channel, and a different band to store the L-R. • L+R and L-R are picked up by all receivers; L-R channel is too high frequency to hear with mono. Stereo receivers reconstruct L and R for playback. Physics of Music, Lecture 16, D. Casper

25. Surround-Sound • Ever since Walt Disney’s Fantasia (1940), movie studios have tried to create a more 3-d listening experience in the theatre. • Today, many home stereo systems have 5+1-channel audio • (center, left, right, surround left, surround right plus bass). • Tricks like L+R, L-R (see below right) are no longer necessary since all channels are encoded on DVDs. • Both volume levels and phase differences can provide the convincing illusion of 3D. Physics of Music, Lecture 16, D. Casper