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Hearing Science

38 cards·by tala5760
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static pressure?
molecules moving about in the air; it is exerted on any material that is in contact with the air
The first of the two things that the pressure in static pressure depends on?
the density of the air (the more molecules there are per unit volumte, the greater the number of collisions and the greater the pressure)
The second of the two things that the pressure in static pressure depends on?
the temperature of the air (the higher the temperature the faster the air molecules move)
atmospheric pressure?
air molecules near the surface of the earth that have been squashed together to create a pressure of about 100,000 newtons per square meter
newtons per square meter?
N/(m squared)
condensation
vibrating obj. moves out; air molecules are pushed away + squeezed tog. creating increase in density and pressure
rarefaction
vibrating obj. moves in; air molecules spread out to fill space vacated + create decrease in density and pressure
sound waves
pressure variations; composed of alternating condensation and rarefaction; can propogatein all directions in 3dimensional space;longitudinal
speech of sound at atmospheric pressure
330 meters per second (m/s); 740 miles per hour
does sound travel through steel or vulcanized rubber faster?
steel (5200 m/s) because it is still. Rubber is dense and not still and sound travels at 54 m/s
what speed does sound travel through water?
1500 m/s even though water is denser than air (ususally slowing) it is much stiffer (accelerating)
the simplest sound wave is?
pure tone
pressure of a pure tone?
varies sinusoidally with time; x(t)= Asin(2(pie)ft+0)
pressure of a pure tone?
varies sinusoidally with time; x(t)= Asin(2(pie)ft+0)
x(t)= Asin(2(pie)ft+0)
x(t) is pressure variation over time; A is peak amplitute (or pressure); f is crequency and 0 is starting phase
sinusoidal function (sin)
produces a waveform taht varies up and down over time between plus and minus one
sound frequency
number of cycles of the pure tone (alternate condensation and rarefaction) that occur at a given location during a given length of time
high frequencies
treble; bright sounds
low grequencies
bass; warm sounds
hertz
the unit that measures the frequency of a sound. measured in cycles per second; Hz
frequency of a pure tone in Hz
corresponds to the # of times in each second the air pressure alternates between high and low (high freq often measured in kilohertz [kHz])
the period of a pure tone
inverse of frequency; it is the time taken for the pure tone to complete one cycle of alternative condensation + rarefaction
wavelength
physical distance that is covered by a complete cycle of the sound wave; simple function of the frequency of sound
wavelength (math)
speed of sound divided by the frequency of the sound wave; higher the frequency, the shorter the wavelength + vice versa
phase
phase of pure tone is the point reached on the pressure cycle at a particular time; covers range of 360 degrees or 2(pie) radians)
measurements of phase
are relative
positive zero crossing
when a waveform crosses zero and is rising
starting phase of zero
when a pure tone starts at a positive zero crossing
starting phase of (pie)/2
if a pure tone starts at a peak
amplitude of a soundwave
the magnitude of the pressure variations, measured with respect to the deviation from atmospheric pressure
amplitude often refers to?
the pressure at the peak of the waveform cycle
root mean squared (rms) pressure
the amplitude; the square root of the average over time of the individual pressure variations squared
rms for pure tone
is equal t the root of 2 (i.e. 0.707) times the peak pressure
velocity of a soundwave
depends on the distance the object has to move during each cycle + the # of times it has to make this movement every second
intensity of soundwaves
the sound energy passing through a unit area (e.g. a square meter of air) every second
power of soundwaves
the energy transmitted per second
units of intensity
watss (units of power) per square meter (W/m(squared))
intensity (math)
proportional to the square of rm pressure so that: I= kP (squared); I is intensity, P is rms pressure and k is a constant