APS March Meeting 2012
Volume 57, Number 1
Monday–Friday, February 27–March 2 2012;
Boston, Massachusetts
Session T46: Invited Session: Keithley Award Session: Photoacoustic and Photothermal Measurement Science
2:30 PM–5:30 PM,
Wednesday, February 29, 2012
Room: 160AB
Sponsoring
Unit:
GIMS
Chair: Terrence Jach, National Institute of Standards and Technology
Abstract ID: BAPS.2012.MAR.T46.3
Abstract: T46.00003 : Photoacoustic and Photothermal Effects in Periodic Structures and Acoustic Resonators
3:42 PM–4:18 PM
Preview Abstract
Abstract
Author:
Gerald Diebold
(Brown University)
Laser excited photoacoustic and photothermal waves can be generated in
one-dimensional structures whose acoustic or thermal properties vary
sinusoidally in space. The wave equations describing the pressure or the
temperature in such structures can be shown to reduce to inhomogeneous
Mathieu equations. Solutions of the Mathieu equation are obtained based on
both the method of variation of parameters and expansion of the pressure or
temperature in a summation over eigenfunctions. The solutions for the
photoacoustic effect show the space equivalent of subharmonic generation
where resonances occur at one half of the period of the structure. The
positions of the band gaps and the dispersion relations for any modulation
depth of the acoustic properties of the structure can be found directly from
the Mathieu characteristic exponent. Since the photoacoustic effect is
governed by an inhomogeneous differential equation, excitation within
forbidden gaps is possible. For excitation within a finite region of the
structure, the Mathieu equation equivalent of Hankel functions are defined.
From these functions the properties of the photoacoustic waves excited
within or outside of the band gaps are found. For thermal waves, the
character of the waves and the dispersion relation can be found as well,
however no band gaps result from the periodicity of the thermal properties
of the structure. The generation of sound by continuous, unmodulated
irradiation of an absorbing gas in a resonant cavity is discussed. A
longitudinal resonance of the cavity is predicted to be excited since any
pressure increase from optical absorption is accompanied by a density
increase, the latter resulting in additional energy deposition by the laser
beam. Thus, on each return of the pressure pulse to the window of the
resonator where laser beam enters the acoustic signal is amplified.
Calculations show that for a strongly absorbing gas, the acoustic modes of
the resonator become mode locked.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2012.MAR.T46.3