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<document xmlns="http://cnx.rice.edu/cnxml" xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:bib="http://bibtexml.sf.net/" id="Module.2004-02-06.2727">
  <name>Galileo and the Pendulum</name>
  <metadata>
  <md:version>1.3</md:version>
  <md:created>2004/05/11 14:08:40 GMT-5</md:created>
  <md:revised>2004/05/24 16:21:48.050 GMT-5</md:revised>
  <md:authorlist>
    <md:author id="helden">
      <md:firstname>Albert</md:firstname>
      
      <md:surname>Van Helden</md:surname>
      <md:email>helden@rice.edu</md:email>
    </md:author>
  </md:authorlist>

  <md:maintainerlist>
    <md:maintainer id="helden">
      <md:firstname>Albert</md:firstname>
      
      <md:surname>Van Helden</md:surname>
      <md:email>helden@rice.edu</md:email>
    </md:maintainer>
    <md:maintainer id="ahlfing">
      <md:firstname>Robert</md:firstname>
      
      <md:surname>Ahlfinger</md:surname>
      <md:email>ahlfing@rice.edu</md:email>
    </md:maintainer>
  </md:maintainerlist>
  
  <md:keywordlist>
    <md:keyword>Galileo</md:keyword>
    <md:keyword>Pendulum</md:keyword>
    <md:keyword>Science</md:keyword>
    <md:keyword>isochronism</md:keyword>
    <md:keyword>harmonic oscillator</md:keyword>
    <md:keyword>Vincenzo Viviani</md:keyword>
  </md:keywordlist>

  <md:abstract>A brief history of Galileo and the pendulum.</md:abstract>
</metadata>

  <content>
    <para id="para1">
      <figure id="fig1">
	<media type="image/gif" src="clock.gif"/>
	<caption>Pendulum Clock</caption>
      </figure>

      In Aristotelian physics, which was still the predominant way to
      explain the behavior of bodies near the Earth, a heavy body
      (that is, one in which the element earth predominated) sought
      its natural place, the center of the universe. The back and
      forth motion of a heavy body suspended from a rope was therefore
      not a phenomenon that could explain or illustrate much. It was
      outside the paradigm.
    </para>

    <para id="para2">
      Galileo was taught Aristotelian physics at the university of
      Pisa. But he quickly began questioning this approach. Where
      Aristotle had taken a qualitative and verbal approach, Galileo
      developed a quantitative and mathematical approach. Where the
      Aristotelians argued that heavier bodies fell faster than
      lighter ones in the same medium, Galileo, early in his career,
      came to believe that the difference in speed depended on the
      densities of the bodies. Where Aristotelians maintained that in
      the absence of the resisting force of a medium a body would
      travel infinitely fast and that a vacuum was therefore
      impossible, Galileo eventually came to believe that in a vacuum
      all bodies would fall with the same speed, and that this speed
      was proportional to the time of fall.
    </para>

    <para id="para3">
      Because of his mathematical approach to motion, Galileo was
      intrigued by the back and forth motion of a suspended
      weight. His earliest considerations of this phenomenon must be
      dated to his days before he accepted a teaching position at the
      university of Pisa. His first biographer, <cnxn document="">Vincenzo Viviani</cnxn>, states that he began his
      study of pendulums after he watched a suspended lamp swing back
      and forth in the cathedral of Pisa when he was still a student
      there. Galileo's first notes on the subject date from 1588, but
      he did not begin serious investigations until 1602.
    </para>

    <para id="para4">
      Galileo's discovery was that the period of swing of a pendulum
      is independent of its amplitude--the arc of the swing--the <term src="#isochronism">isochronism</term> of the pendulum.  
      <note type="footnote">
	Strictly speaking, a simple pendulum is not isochronous, the
	period does vary somewhat with the amplitude of the
	swing. This was shown by Christiaan Huygens, in the
	1650s. Huygens installed cycloidal "cheeks" near the
	suspension point of his pendulums and showed that as a result
	the bob now described a cycloidal arc. And he proved that when
	this is the case the pendulum is truly isochronous. In
	practice, the swing of the bob was kept very small and the
	amplitude as constant as possible, as in the long-case clock
	or our familiar grandfather clock. Under these conditions the
	simple pendulum is isochronous for all practical purposes.
      </note>
      Now this discovery had important implications for the
      measurement of time intervals. In 1602 he explained the
      isochronism of long pendulums in a letter to a friend, and a
      year later another friend, <cnxn document="">Santorio
      Santorio</cnxn>, a physician in Venice, began using a short
      pendulum, which he called "pulsilogium," to measure the pulse of
      his patients. The study of the pendulum, the first <term src="#harmonicoscillator">harmonic oscillator</term>, date from
      this period.
      <figure id="fig2">
	<media type="image/gif" src="brachistochron.gif"/>
	<caption>Harmonic Oscillator?</caption>
      </figure>
    </para>

    <para id="para5">
      The motion of the pendulum bob posed interesting problems. What
      was the fastest motion from a higher to a lower point, along a
      circular arc like a pendulum bob or along a straight line like
      on an inclined plane? Does the weight of the bob have an effect
      on the period? What is the relationship between the length and
      the period? Throughout his experimental work, the pendulum was
      never very far from Galileo's thought. But there was also the
      question of its practical use.
    </para>

    <para id="para6">
      A pendulum could be used for timing pulses or acting as a
      metronome for students of music: its swings measured out equal
      time intervals. Could the device also be used to improve clocks?
      The mechanical clock, using a heavy weight to provide the motive
      power, began displacing the much older water clock in the High
      Middle Ages. By incremental improvement, the device had become
      smaller and more reliable. But the accuracy of the best clocks
      was still so low that they were, for instance, useless for
      astronomical purposes. Not only did they gain or lose time, but
      they did so in an irregular and unpredictable manner. Could a
      pendulum be hooked up to the escape mechanism of a clock so as
      to regulate it?
    </para>

    <para id="para7">
      In 1641, at the age of 77, totally blind, Galileo turned his
      attention to this problem. <cnxn document="">Vincenzo
      Viviani</cnxn> describes the events as follows, as translated by
      <cite src="#drake1978">Stillman Drake</cite>:

      <quote type="block">
	One day in 1641, while I was living with him at his villa in
	Arcetri, I remember that the idea occurred to him that the
	pendulum could be adapted to clocks with weights or springs,
	serving in place of the usual <emphasis>tempo</emphasis>, he
	hoping that the very even and natural motions of the pendulum
	would correct all the defects in the art of clocks. But
	because his being deprived of sight prevented his making
	drawings and models to the desired effect, and his son
	Vincenzio coming one day from Florence to Arcetri, Galileo
	told him his idea and several discussions followed. Finally
	they decided on the scheme shown in the accompanying drawing,
	to be put in practice to learn the fact of those difficulties
	in machines which are usually not foreseen in simple
	theorizing.
      </quote>

      <cnxn document="">Viviani</cnxn> wrote this in 1659, seventeen
      years after Galileo's death and two years after the publication
      of Christiaan Huygens's <cite>Horologium</cite>, in which
      Huygens described his pendulum clock. It is from Huygens's
      construction that we date the practical development of the
      device.
    </para>
  </content>

  <glossary>
    <definition id="isochronism">
      <term>isochronous</term>
      <meaning>Equal or uniform in time</meaning>
    </definition>

    <definition id="harmonicoscillator">
      <term>harmonic oscillator</term>
      <meaning>Each oscillation has a frequency that is an integer multiple of the same basic frequency</meaning>
    </definition>
  </glossary>

  <bib:file>
    <bib:entry id="drake1978">
      <bib:book>
	<bib:author>Stillman Drake</bib:author>
	<bib:title>Galileo at Work: His Scientific Biography</bib:title>
	<bib:publisher>University of Chicago Press</bib:publisher>
	<bib:year>1978</bib:year>
	<bib:address>Chicago</bib:address>
	<bib:note>For explanations of how the pendulum figured in Galileo's experiments; quote from p. 419</bib:note>
      </bib:book>
    </bib:entry>

    <bib:entry id="bedini1991">
      <bib:book>
	<bib:author>Silvio A. Bedini</bib:author>
	<bib:title>The Pulse of Time: Galileo Galilei, the Determination of Longitude, and the Pendulum Clock</bib:title>
	<bib:publisher>Olschki</bib:publisher>
	<bib:year>1991</bib:year>
	<bib:address>Florence</bib:address>
	<bib:note>A useful recent treatment</bib:note>
      </bib:book>
    </bib:entry>

    <bib:entry id="bedini1967">
      <bib:book>
	<bib:author>Silvio A. Bedini</bib:author>
	<bib:title>Galileo and the Measure of Time</bib:title>
	<bib:publisher>Olschki</bib:publisher>
	<bib:year>1967</bib:year>
	<bib:address>Florence</bib:address>
      </bib:book>
    </bib:entry>

    <bib:entry id="settle1992">
      <bib:incollection>
	<bib:author>Thomas B. Settle</bib:author>
	<bib:title>Experimental Research and Galilean Mechanics</bib:title>
	<bib:booktitle>Galileo Scientist: His Years at Padua and Venice</bib:booktitle>
	<bib:publisher>Istituto Nazionale di Fisica Nucleare; Istituto Veneto di Scienze, Lettere ed Arti; Dipartimento di Fisica</bib:publisher>
	<bib:year>1992</bib:year>
	<bib:editor>Milla Baldo Ceolin</bib:editor>
	<bib:pages>39-57</bib:pages>
	<bib:address>Padua; Venice; Padua</bib:address>
	<bib:note>For explanations of how the pendulum figured in Galileo's experiment</bib:note>
      </bib:incollection>
    </bib:entry>
  </bib:file>
  
</document>
