In all microphones, sound waves (sound pressure) are translated into mechanical vibrations in a thin, flexible diaphragm. Then they are translated into electronic signals. There are varying ways that this is done, each with its particular strengths. Here are the main microphone types along with methods for using them.
In a capacitor microphone, also known as a condenser microphone, the diaphragm acts as one plate of a capacitor, and the distance changing vibrations produce changes in a voltage maintained across the capacitor plates. Capacitor microphones are not cheap and require an external power supply, called " Phantom Power," but give a high-quality sound signal and are the mics of choice in professional recording studios.
In the dynamic microphone a small movable induction coil, positioned in the magnetic field of a permanent magnet, is attached to the diaphragm. When the diaphragm vibrates, the coil moves in the magnetic field, producing a varying current in the coil (See electromagnetic induction). Dynamic microphones are robust and relatively inexpensive, and are used in a wide variety of applications. While their main use is on stage and live situations, they can also perform admirably in the studio.
A foil electret microphone is a relatively new type of condenser microphone invented at Bell laboratories in 1962, and often simply called an electret microphone. An electret is a dielectric material that has been permanently electrically charged or polarised. Electret microphones have existed since the 1920s but were considered impractical, but have now become the most common type of all, used in many applications from high-quality public address to built-in microphones in small sound recording devices. Unlike other condenser microphones they require no polarising voltage, but normally contain an integrated preamplifier which does require power (often incorrectly called polarising power). They are frequently phantom powered in sound reinforcement applications. They can be very small, and thus are often used as clip-on mics in shows.
In ribbon microphones a thin, corrugated metal ribbon is suspended in a magnetic field: vibration of the ribbon in the magnetic field generates a changing voltage. Ribbon microphones detect sound in a bidirectional pattern: this characteristic is useful in such applications as radio and television interviews, where it cuts out much extraneous sound.
A carbon microphone, formerly used in telephone handsets, is a capsule containing carbon granules pressed between two metal plates. A voltage is applied across the metal plates, causing a current to flow through the carbon. One of the plates, the diaphragm, vibrates in sympathy with incident sound waves, applying a varying pressure to the carbon. The changing pressure deforms the granules, causing the contact area between each pair of adjacent granules to change, and this causes the electrical resistance of the mass of granules to change (lose contact). Since the voltage across a conductor is proportional to its resistance, the voltage across the capsule varies according to the sound pressure. Do not forget a battery for the current flow.
A piezo microphone uses the phenomenon of piezoelectricity - the tendency of some materials to produce a voltage when subjected to pressure - to convert vibrations into an electrical signal. This type of microphone is often used to mic acoustic instruments for live performance, or to record sounds in unusual environments (underwater, for instance.)
Depending on various aspects of a microphone's construction, it may be nearly equally sensitive to sound coming in all directions (an omnidirectional microphone), or it may be more sensitive to sound coming from a particular direction (a unidirectional microphone). The most common of the unidirectional type is sometimes called a cardioid microphone, because the sensitivity pattern somewhat resembles the shape of a heart most vocal mikes are cardioid or hyper-cardioid (similar to cardioid but with a tighter area of front sensitivity and a tiny lobe of rear sensitivity.) Some microphones have more complex sensitivity patterns. Most ribbon microphones are bi-directional, receiving sound from both in front and back of the element. This type of response is also known as a figure-8 pattern, because of its shape.
Shotgun microphones, the most directional form of studio microphone, reserve most of their sensitivity for sounds directly in front of, and to a lesser extent, the rear of the microphone. Shotgun microphones also have small lobes of sensitivity to the left and right. This effect is a result of the microphone design, which generally involves placing the element inside of a tube with slots cut along the side wave-cancellation eliminates most of the off-axis noise.
A parabolic microphone uses a parabolic reflector to collect and focus sound waves onto a microphone receiver, in much the same way that a parabolic antenna (e.g. satellite dish) does with radio waves. Typical uses of this microphone, which has unusually focused front sensitivity and can pick up sounds from many meters away, include nature recording, eavesdropping, law enforcement, and even espionage. Parabolic microphones are not typically used for standard recording applications, because they tend to have poor low-frequency response as a side effect of their design.
A microphone with an omnidirectional characteristic is a pressure transducer: the output voltage is proportional to the air pressure at a given time. On the other hand, a figure-8 pattern is a pressure gradient transducer the output voltage is proportional to the difference in pressure on the front and on the back side. The result of this is that a sound wave coming from the back will lead to a signal with a sign opposite to that of an identical sound wave from the front. Moreover, shorter wavelengths (higher frequencies) are picked up more effectively than lower frequencies. A microphone with a cardioid directional characteristic is effectively a superposition of an omnidirectional and a figure-8 microphone for sound waves coming from the back, the negative signal from the figure-8 cancels the positive signal from the omnidirectional element, whereas for sound waves coming from the front, the two add to each other. A hypercardioid microphone is similar, but with a slightly larger figure-8 contribution.
Since directional microphones are (partially) pressure gradient transducers, their sensitivity is dependent from the distance to the sound source. This effect is known as proximity effect, a bass-boost at distances of a few centimeters.
There exist a number of well-developed microphone techniques used for miking musical, film, or voice sources. Choice of technique depends on a number of factors, including:
The collection of extraneous noise. This can be a concern, especially in amplified performances, where audio feedback can be a significant problem. Alternatively, it can be a desired outcome, in situations where ambient noise is useful (hall reverberation, audience reaction.)
Choice of a signal type: Mono, stereo or multi-channel.
Type of sound-source: Acoustic instruments produce a very different sound than electric instruments, which are again different from the human voice.
Processing: If the signal is destined to be heavily processed, or " mixed down" , a different type of input may be required.
There are several classes of microphone placement for recording and amplification.
In close miking, a directional microphone is placed relatively close to an instrument or sound-source. This serves to eliminate extraneous noise-- including room reverberation-- and is commonly used when attempting to record a number of separate instruments while keeping the signals separate, or when in order to avoid feedback in an amplified performance.
In ambient or distant miking, a sensitive microphone or microphone is placed at some distance from the sound source. The goal of this technique is to get a broader, natural mix of the sound source or sources, along with reverberation from the room or hall.
The X-Y technique involves the coincident placement of two directional microphones. When two directional microphones are placed coincidentally, typically at a 90+ degree angle to each other (typically with each microphone pointing to a side of the sound-stage), a stereo effect is achieved simply through intensity differences of the sound entering each microphone. Due to the lack of time-of-arrival stereo information, the stereo effect in X-Y recordings is somewhat unnatural, especially when listened to through headphones. The main advantage is that the signal is mono-compatible, i.e., the signal is suitable for playback on non-stereo devices such as radio.
The Mid-Side (M-S) technique is a special case of X-Y and uses a directional or omnidirectional microphone (M) and a bidirectional (figure-8) microphone (S), placed at a 90 degree angle to each other with the directional microphone facing the sound-stage. The outputs of these microphones are mixed in such a way as to generate sum and difference signals between the outputs. The S signal is added to the M for one channel, and is subtracted (by reversing phase and adding) to generate the other channel. M-S has two advantages: when the stereo signal is combined into mono, the signal from the S microphone cancels out entirely, leaving only the mono recording from the directional M microphone additionally, M-S recordings can be " remixed" after recording to alter or even remove the stereo spread. The M-S technique with an omnidirectional M microphone is equivalent to X-Y with two cardioids at a 180-degree angle.
Near-coincident recording is a variant of the X-Y technique and incorporates interchannel time delay by placing the microphones several inches apart. The ORTF stereo technique of the Office de Radiodiffusion Television Francaise = Radio France, calls for a pair of cardioid microphones placed 17 cm apart at an angle of 110 degrees. In the NOS stereo technique of the Nederlandse Omroep Stichting = Holland Radio, the angle is 90 degrees and the distance is 30 cm. The choice for one of the other dependens on the recording angle of the microphone system and not on the distance to and the width of the sound source. This technique leads to a realistic stereo effect and has a reasonable mono-compatibility. These signals have nothing to with interaural signals which come only from artifical head recordings.
The A-B technique uses two omnidirectional microphones at an especial distance to each other (20 centimeters up to some meters). Stereo information consists in large time-of-arrival distances and some sound level differences. On playback, with too large A-B the stereo image can be perceived as somewhat unnatural, as if the left and right channel are independent sound sources, without an even spread from left to right. A-B recordings are not so good for mono playback because the time-of-arrival differences can lead to certain frequency components being canceled out and other being amplified, the so-called comb-filtering effect, but the stereo sound can be really convincing. If you use wide A-B for big orchstras, you can fill the center with another microphone. Then you get a " Decca tree" , which brought us many good sounding recordings.
Binaural recording is a highly specific attempt to recreate the conditions of human hearing, reproducing the full three-dimensional sound-field. Most binaural recordings use model of a human head, with microphones placed where the ear canal could be. A sound source is then recorded with all of the stereo and spatial cues produced by the head and human pinnae with frequency dependent ILD (interaural level difference) and ITD (interaural time difference, max. 63 & micro sec) ear signals. A binaural recording is usually only somewhat successful, in addition to being highly inconvenient. For one thing, it tends to work well only when played back directly into the ear canal, via headphones (no speakers), as other methods of playback add additional spatial cues. Furthermore, as all heads and pinnae are different, a recording from one " pair of ears" will not always sound correct to another person. Also, headphones have a frequency response that compensates for the fact that the reflections from the pinnae, head and shoulders strongly affect the frequency spectrum, with the assumption that a recording is taken with a flat frequency spectrum. Introducing the spectral distortion already in the binaural recording results in an unnatural frequency spectrum, even when played through headphones. Finally, as visual cues are generally much more powerful than auditory cues when determining the source of a sound, binaural recordings are not always convincing to listeners.
This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article " Microphone"