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Sound pressure p (acoustic pressure) is the measurement in pascals of the average sound wave pressure variations of a sound wave passing by a fixed point. The symbol for pressure is the lower case p. (The upper case P is the symbol for power. Often you find this misprinted.)
p = \frac{F}{A} \ \mathrm{ \ or \ } \ \frac{F}{S} <math>
The SI unit is pascal with the symbol Pa. One pascal equals a pressure of one newton per cm2
1 \ \mathrm{ Pa = 1 \frac{N}{\, m^{2}} } = 1 \mathrm{ \frac{kg}{\, m \cdot s^{2}} }\;<math>
The amplitude of sound pressure decreases in the free field (direct field) with 1/r of the distance of a point source.
The sound pressure level is calculated in dB as:
L_p=20\, \log_{10}\left(\frac{p_1}{p_0}\right)\mathrm{dB} <math>
Reference sound pressure is: p0 = 2 · 10-5 Pa = 20 µPa
Sound pressure p in N/m2 or Pa is:
p = Z \cdot v = \frac{J}{v} = \sqrt{J \cdot Z} <math>
Notice: The often used term "intensity of sound pressure" is not correct. Think it over. Use "magnitude", "strength", "amplitude", or "level" instead. "Intensity" is the quadratic sound energy value, but "pressure" is a linear sound field value. Intensity is not pressure.
The sound pressure p is connected to particle displacement or particle amplitude ξ, in m, by:
\xi = \frac{v}{2 \cdot \pi \cdot f} = \frac{v}{\omega} = \frac{p}{Z \cdot \omega} = \frac{p}{Z \cdot 2 \cdot \pi \cdot f} <math>
where:
Sound pressure p:
p = \rho \cdot c \cdot \omega \cdot \xi = Z \cdot \omega \cdot \xi = {\xi \cdot Z \cdot 2 \cdot \pi \cdot f} = \frac{a \cdot Z}{\omega} = c \cdot \sqrt{\rho \cdot E} = \sqrt{\frac{P_{ac} \cdot Z}{A}} <math> normally in units of N/m2 = Pa.
where:
See also: Sound pressure level