Acoustical measurements Iiro Jantunen Nokia Research Center 19.4.2006 S-108.4010 Licentiate course in measurement science and technology 1 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Contents • Principles of acoustics • Acoustics measurements • Microphone • Sound pressure level measurements • Sound intensity measurements • Calibration • SoundField 2 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Principles of acoustics • Sound waves in gas or liquid • No shear forces → no transverse waves → purely longitudinal waves • Audible sound range 20 Hz – 20 kHz • Fully described by 3 variables • Pressure • Particle velocity • Density 3 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Wave equations of sound • Euler’s equation • Newton’s 2nd law (F=ma) applied to fluid • Continuity equation • Bringing extra air to a volume increases density • State equation • Relates pressure changes to density 4 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Wave equation of sound • Previous wave equations used pressure, density and particle velocity • Eliminating density and particle velocity the wave equation of sound is obtained • Two basic solutions: • Plane wave • Spherical wave 5 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Free field acoustics • Sound propagates to all directions without diffraction, reflection or absorption • Spherical waves • In principle, infinite, empty space without reflections • In practice, anechoic chamber, with near 100% absorptive walls 6 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Free field microphone • Intended to measure the sound pressure as it existed before the microphone was introduced • Microphone pointed to source • Microphone tip causes an increase in sound pressure • Taken care of by internal acoustical damping to achieve flat frequency response 7 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Diffuse field – random incidence microphone • Sound reflects from many directions → sound comes to microphone from every direction • In practice achieved in a reverberation room with 100% reflective and unparallel walls • Microphone diffracts the sound waves from different directions in different ways • Combined influence depends on directional distribution of sound waves • Standard distribution based on statistical considerations used for random incidence microphone 8 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Closed coupler • Chamber with small dimensions compared to sound wavelength • Special case: standing wave tube • Diameter smaller than sound wavelength • Source at the end • Possible to calculate the sound field • Used in calibration 9 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ • Used in microphone calibration Pressure microphone • Measuring the actual pressure on a wall • Typically used in closed coupler for calibration 10 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Microphone directionality • Directionality indicates the sensitiveness of a microphone to sound coming from different directions • No microphone is perfectly omnidirectional • Cardioid or hypercardioid commonly used to record vocals • Most ribbon microphones are bi-directional • Shotgun directionality used outdoors for TV/film production and wildlife recordings 11 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Parabolic microphone • Parabolic reflector used to collect sound waves to microphone • Very directional • For eavesdropping in e.g. spying 12 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Microphone transducers • Condenser microphones • Electret capacitor microphones • Dynamic microphones • Ribbon microphones • Carbon microphones • Piezoelectric microphones • Laser microphones 13 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Condenser microphone • Diaphragm and backplate form a plate capacitor • Charge kept constant → voltage varies as pressure actuates the diaphragm • External voltage supply or pre-charged diaphragm • Acoustical performance determined by physical dimensions 14 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Condenser microphone – cont • The larger the diaphragm, the more sensitive the microphone • Upper limit is defined by diaphragm touching the backplate • The smaller the microphone, the greater the frequency range • Increasing tension extends range but decreases sensitivity • Optimum size of a measurement microphone is (up to 20 kHz) is about 12.6 mm (1/2’’) • Damping effect of air reduced by drilling holes in the backplate 15 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Electret microphone • Invented at Bell Labs in 1962 by Gerhard Sessler and Jim West • Diaphragm permanently polarized the same way as permanent magnets magnetized (electrostatic magnet) • Once considered low price and low quality • Now most common microphone type 16 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Dynamic microphone • A movable coil is attached to the diaphragm • An unmovable magnet produces a magnetic field • Moving diaphragm moves the coil in the magnetic field, inducing a measurable current • Exactly same principle as in loudspeakers, only reversed • Poor low-frequency response → reduces handling noise • Robust, relatively inexpensive and resistant to moisture → widely used on-stage 17 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Ribbon microphones • Revolutionized recording and broadcast industry in the 30’s • Special type of dynamic microphones • Thin metal ribbon between poles of magnet • Voltage output typically low compared to normal dynamic microphones • Bidirectional • Very sensitive and accurate • Generally delicate and expensive 18 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Carbon microphones • Invented by David Hughes in 1878 • Very important in the history of telephone • Sound pressure (AP) presses the diaphragm (2) to a bed of carbon granules (1). Contact resistance depends on the pressure → resitance R changes • Also an amplifier • Extremely low-quality sound reproduction • Very limited frequency range • Very robust 19 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Piezo microphones • Piezoelectric material • Diaphragm moves the armature to bend piezoelectric crystal over a fulcrum • Small size, cheap, low quality • Have replaced carbon microphones • Often used as • contact microphones to sound instruments • underwater or other unusual environments 20 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Laser microphones • Window of a room acting as diaphragm • Reading with laser beam reflected from the window • Two laser beams for common mode rejection of large window movements and path disturbances • For eavesdropping • Works best with one-glass windows 21 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Sound level measurements • Measurement of sound pressure filtered by • frequency (A-weighting) • time-domain (RMS) • Mimics response of human ear to noise 22 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Human hearing frequency response A-weighting curve For subjective responses in special cases there are B-, C- and D-weighting curves •very high or low level •special noise, e.g., of aircraft 23 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Sound level measurements • IEC International Standard 651 ”Sound Level Meters” • Tolerances per frequency band defined for 4 classes of accuracy • Type 0: precision laboratory use • Type 1: general purpose • Type 2: low price • Type 3: not used in practice (too wide tolerances) 24 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Sound intensity measurements ISO Standard 3745 “Acoustics — Determination of sound power levels of noise sources — Precision method for anechoic and semi-anechoic rooms” no. 25 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ x/r y/r z/r 1 -0.99 0 0.15 2 0.5 -0.86 0.15 3 0.5 0.86 0.15 4 -0.45 0.77 0.45 5 -0.45 -0.77 0.45 6 0.89 0 0.45 7 0.33 0.57 0.75 8 -0.66 0 0.75 9 0.33 -0.57 0.75 10 0 0 1.00 Two-microphone probe • Measures the sound intensity in two directions • Pressure is mean of the two measured pressures • Air particle velocity calculated from the two pressures • All intensity is in radial direction, no intensity in perpendicular • Powerful tool to locate noise sources 26 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Calibration techniques • Reciprocity calibration method • Comparison or substitution methods • Pistonphone (closed coupler) • Sound pressure calibrator • Electrostatic actuation 27 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Reciprocity calibration method • Microphone can be used as a loudspeaker • Very accurate • Three test microphones measured against each other alternating the function • Requires well-controlled environment • As a result a set of 3 equations with microphone sensitivities as unknowns 28 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ • Rather tedious • Seldom used in practical situations Comparison/substitution methods • Microphone measured related to a reference microphone • Comparison method: microphone and reference at the same time • Substitution method: microphone put in the lace of the reference • Sound source stability 29 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Pistonphone • Closed coupler • Well-defined sound pressure level • Relatively simple mechanically, very stable • Used often as the sound source in comparison/subsitution calibration • Accuracy around 0.1 dB • Depends on • Volume of the coupler • Volume displacement • Barometric pressure • Humidity • Heat dissipation 30 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ Sound pressure calibrator • Small, self-contained • Comparison calibrator • Closed coupler • Small loudspeaker produces single-frequency signal • Reference microphone gives feedback signal 31 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ • Well-defined, provided that reference microphone and feedback gain are stable • For field-calibration of microphones • Normally not for laboratory calibrations Electrostatic calibration • Direct use of electrostatic actuator to drive the diaphragm • 800 V DC • 50-150 V AC signal • Generally used to measure frequency response of microphones 32 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ • Widely used as a convenient and accurate test method • For production and final calibration of measurement microphones SoundField microphone • 3D view of the sound with a single device • 4-channel measurement of sound: B-format • The spatial pattern can be decided later • Mono, stereo, 5.1, … • Fairly expensive, but replaces effectively a system of many microphones • http://www.soundfield.com 33 © 2006 Nokia Acoustical measurements.ppt / 2006-04-19 / IJ