Thank you for the clarification.
HERE IS THE ANSWER:
Sound is a compression wave in a medium (air) which can be
represented as an Ideal Gas. Here is a animated picture of that:
http://www.glenbrook.k12.il.us/gbssci/phys/Class/sound/u11l1c.html
Variables density and compression modulus (or bulk modulus)
depend on temmperature and determine "speed of sound" v ,
and "impedance of the medium Z". Basic material constant is gamma,
about 1.44 for air (a mixture of diatomic gases), which is defined here:
http://hypertextbook.com/physics/waves/sound/
Quick look on the Efffect of T on speed v (same as c here) is here:
http://encyclopedia.thefreedictionary.com/Speed of sound
Detailed, 35 pages long, technical description is here:
http://www.mech.soton.ac.uk/mh/ME318/Compressed_notes_mh.pdf
Salient points are this: The compression is adiabatic (i.e.so fast
that there is no thermal equilibration),
(this seems to be different then view expressed in the comment)
and quantities in the Hooks law: strain * K = stress are
strain .. dimensionless (=change of density / density)
stress .. pressure (Pascals - N /m. m )
K = bulk modulus is in Pa and equals gamma*P
This is consequence of Ideal Gas equation od state for adiabatic compression
as explained on page 11 here:
http://fisicanet.terra.com.br/cursos/msu/m202.pdf
So , combining all that: to get your answer you
first get P amplitude of the pressure vawe, from SPL (which is Lp
here) using this equation
Lp= 20 * log(P/P0),
which explained here:
http://physics.mtsu.edu/~wmr/log_3.htm
From that and K you get you get your strain amplitude. K is
proportional to P which is proportional to absolute temperature T.
Strain is a dimensionless number.(A surface wave measures displacement
in microns, but compression wave masures strain in percents. Even the
loudest sound (meaning at treshold of pain) is less then 3%.)
So, the same pressure amplitude, at lower temperature, will produce
slightly larger strain (=cold air is stiffer).
Let's say, in summer T = 273K and in winter T=253K. Then strain for
very loud sound, (a dimensionless number) would be 9/273 and 9/253
respectively.
So, what is the displacement of particles in microns? During load
sound three percent of particles must escape the volume defined by the
wavelength. The actual speed of the particles is comparable to the
speed of sound. The sound is just changing counts of particles
arriving and leaving the volumes of compressions and rarefications.
hedgie
hedgie |