<?xml version="1.0" encoding="utf-8" standalone="no"?>
<!DOCTYPE article SYSTEM "http://www.nonlin-processes-geophys.net/inc/npg/copernicus.dtd">
<article language="en">
	<journal>
		<journal_title>Nonlinear Processes  in Geophysics</journal_title>
		<journal_url>www.nonlin-processes-geophys.net</journal_url>
		<issn>1023-5809</issn>
		<eissn>1607-7946</eissn>
		<volume_number>3</volume_number>
		<issue_number>2</issue_number>
		<publication_year>1996</publication_year>
	</journal>
	<doi>10.5194/npg-3-89-1996</doi>
	<article_url>http://www.nonlin-processes-geophys.net/3/89/1996/</article_url>
	<abstract_html>http://www.nonlin-processes-geophys.net/3/89/1996/npg-3-89-1996.html</abstract_html>
	<fulltext_pdf>http://www.nonlin-processes-geophys.net/3/89/1996/npg-3-89-1996.pdf</fulltext_pdf>
	<start_page>89</start_page>
	<end_page>101</end_page>
	<publication_date>0000-00-00</publication_date>
	<article_title content_type="html">A new theoretical paradigm to describe hysteresis, discrete memory and nonlinear elastic wave propagation in rock</article_title>
	<authors>
		<author numeration="1" affiliations="1,2">
			<name>K. R. McCall</name>
		</author>
		<author numeration="2" affiliations="1,3">
			<name>R. A. Guyer</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Los Alamos National Laboratory, Los Alamos, New Mexiko</affiliation>
		<affiliation numeration="2" content_type="html">Present address Department of Physics, University of Nevada, Reno, Nevada</affiliation>
		<affiliation numeration="3" content_type="html">Present address Department of Physics and Astronomy, University of Massachusetts, Amherst, Massachusetts</affiliation>
	</affiliations>
	<abstract content_type="html">The  velocity of sound in  rock is  a
strong function
          of pressure, indicating that wave  propagation in rocks
is very nonlinear.  The quasistatic  elastic  properties of 
rocks  axe
          hysteretic, possessing  discrete memory.  In this  paper
a  new
          theory   is  developed,   placing  all   of  these  
properties (nonlinearity, hysteresis, and memory)  on equal 
footing. The
          starting  point of  the new theory  is closer  to a
microscopic
          description   of  a  rock   than  the  starting  point 
of  the
          traditional  five-constant  theory  of  nonlinear  
elasticity.
          However, this starting point (the  number density
&lt;I&gt;Ï?&lt;/I&gt;  of generic
          mechanical  elements  in  an  abstract  space) is 
deliberately
          independent of  a specific microscopic  model. No
prejudice  is
          imposed as  to the mechanism  causing nonlinear response
in the
          microscopic  mechanical  elements. The  new theory  (1)
relates
          suitable  stress-strain measurements  to the  number 
density &lt;I&gt;Ï?&lt;/I&gt;
          and  (2)  uses the  number density  &lt;I&gt;Ï?&lt;/I&gt; to  find
the behaviour of
          nonlinear  elastic waves. Thus  the new theory provides
for the
          synthesis of the full  spectrum of elastic behaviours of
a rock.
          Early  development  of  the  new  theory  is  sketched 
in this
          contribution.</abstract>
	<references>
	</references>
</article>

