Particle acceleration
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In a compressible sound transmission medium - mainly air - air particles get an accelerated motion: the particle acceleration or sound acceleration with the symbol a in metre/second². In acoustics or physics, acceleration (symbol: a) is defined as the rate of change (or time derivative) of velocity. It is thus a vector quantity with dimension length/time². In SI units, this is m/s².
To accelerate an object (air particle) is to change its velocity over a period of time. Acceleration is defined technically as "the rate of change of velocity of an object with respect to time" and is given by the equation
- [\mathbf = \over dt}]
- a is the acceleration vector
- v is the velocity vector expressed in m/s
- t is time expressed in seconds.
An alternative equation is:
- [\mathbf} = - \mathbf \over t}]
[\mathbf}] is the average acceleration (m/s²)
[\mathbf] is the initial velocity (m/s)
[\mathbf] is the final velocity (m/s)
[\mathbf] is the time interval (s)
Transverse acceleration (perpendicular to velocity) causes change in direction. If it is constant in magnitude and changing in direction with the velocity, we get a circular motion. For this centripetal acceleration we have
- [ \mathbf = - \frac \frac} = - \omega^2 \mathbf]
In classical mechanics, acceleration [ a \ ] is related to force [F \ ] and mass [m \ ] (assumed to be constant) by way of Newton's second law:
- [F = m \cdot a]
Equations in terms of other measurements
The Particle acceleration of the air particles a in m/s² of a plain sound wave is:
- [
| Symbol | Units | Meaning |
|---|---|---|
| a | m/s² | particle acceleration |
| v | m/s | particle velocity |
| ξ | m, meters | particle displacement |
| [\omega] = 2 · [\pi] · f | radians/s | angular frequency |
| f | Hz, hertz | frequency |
| p | Pa, pascals | sound pressure |
| Z | N·s/m³ | acoustic impedance |
| J | W/m² | sound intensity |
| E | W·s/m³ | sound energy density |
| Pac | W, watts | sound power or acoustic power |
| A | m² | area |
See also
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