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	<id>http://wiki.hamtools.org/index.php?action=history&amp;feed=atom&amp;title=Piezoelectric_Effect</id>
	<title>Piezoelectric Effect - Revision history</title>
	<link rel="self" type="application/atom+xml" href="http://wiki.hamtools.org/index.php?action=history&amp;feed=atom&amp;title=Piezoelectric_Effect"/>
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	<updated>2026-05-02T04:03:21Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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	<entry>
		<id>http://wiki.hamtools.org/index.php?title=Piezoelectric_Effect&amp;diff=4685&amp;oldid=prev</id>
		<title>TimVK4YEH: reworded section and added diagram</title>
		<link rel="alternate" type="text/html" href="http://wiki.hamtools.org/index.php?title=Piezoelectric_Effect&amp;diff=4685&amp;oldid=prev"/>
		<updated>2010-11-20T01:22:42Z</updated>

		<summary type="html">&lt;p&gt;reworded section and added diagram&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 18:22, 19 November 2010&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l11&quot;&gt;Line 11:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 11:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==How the Piezoelectric Effect Works==&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==How the Piezoelectric Effect Works==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br/&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br/&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The piezoelectric effect occurs when the charge balance within the crystal lattice of a material is disturbed. When there is no applied stress on the material, the positive and negative charges are evenly distributed so there is no potential difference. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;When &lt;/del&gt;the lattice is &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;changed &lt;/del&gt;slightly&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;, &lt;/del&gt;the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;charge imbalance creates &lt;/del&gt;a potential difference&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;, often &lt;/del&gt;as high as several thousand volts&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;. However&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;the &lt;/del&gt;current &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;is extremely small and only causes a small electric shock&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;The converse piezoelectric &lt;/del&gt;effect &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;occurs when the electrostatic field created by an electrical current causes the atoms in the material to move slightly&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The piezoelectric effect occurs when the charge balance within the crystal lattice of a material is disturbed&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;.  In the diagram below, the left hand side illustrates an hexagonal crystalline structure. Such structures can be thought of as being made up of three matched pairs of ions distributed around a a regular hexagonal lattice&lt;/ins&gt;. When there is no applied stress on the material, the positive and negative charges are evenly distributed so there is no potential difference.  &lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;The right hand side of the diagram illustrates the situation when &lt;/ins&gt;the &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;crystalline structure is stressed physically. The &lt;/ins&gt;lattice is &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;distorted &lt;/ins&gt;slightly &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;and is no longer a regular hexagon. Pairs of positive ions on the left and pairs of negative ions on &lt;/ins&gt;the &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;right are forced to be closer together. The &amp;quot;squashed&amp;quot; hexagon essentially becomes a dipole with &lt;/ins&gt;a potential difference &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;between the two sides. This can be &lt;/ins&gt;as high as several thousand volts, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;accompanied by an extremely low &lt;/ins&gt;current.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[Image:PE &lt;/ins&gt;effect.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;jpg]]&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br/&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br/&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==Applications to ham radio==&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==Applications to ham radio==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>TimVK4YEH</name></author>
	</entry>
	<entry>
		<id>http://wiki.hamtools.org/index.php?title=Piezoelectric_Effect&amp;diff=4679&amp;oldid=prev</id>
		<title>TimVK4YEH: information transferred from old page</title>
		<link rel="alternate" type="text/html" href="http://wiki.hamtools.org/index.php?title=Piezoelectric_Effect&amp;diff=4679&amp;oldid=prev"/>
		<updated>2010-11-16T21:46:38Z</updated>

		<summary type="html">&lt;p&gt;information transferred from old page&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;wikipedia [http://en.wikipedia.org/wiki/Piezoelectricity article]&lt;br /&gt;
&lt;br /&gt;
==What is it?==&lt;br /&gt;
&lt;br /&gt;
The piezoelectric effect is the ability of some materials to produce electric current when they are exposed to physical stress. It also works in the opposite way, with the material deforming slightly when a small electric current is applied. Piezoelectricity was discovered more than one hundred years ago and has applications in electronic clocks, gas ovens, inkjet printers, and many other appliances. &lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The piezoelectric effect was first discovered in 1880 by brothers Pierre Curie and Jacques Curie. The Curie brothers only found that piezoelectric materials can produce electricity. The next development was the discovery by Gabriel Lippmann that electricity can deform piezoelectric materials. It was not until the early twentieth century that practical devices began to appear. Today, it is known that many materials such as quartz, topaz, cane sugar, Rochelle salt, and bone have this effect.&lt;br /&gt;
&lt;br /&gt;
==How the Piezoelectric Effect Works==&lt;br /&gt;
&lt;br /&gt;
The piezoelectric effect occurs when the charge balance within the crystal lattice of a material is disturbed. When there is no applied stress on the material, the positive and negative charges are evenly distributed so there is no potential difference. When the lattice is changed slightly, the charge imbalance creates a potential difference, often as high as several thousand volts. However, the current is extremely small and only causes a small electric shock. The converse piezoelectric effect occurs when the electrostatic field created by an electrical current causes the atoms in the material to move slightly.&lt;br /&gt;
&lt;br /&gt;
==Applications to ham radio==&lt;br /&gt;
&lt;br /&gt;
Quartz has a natural frequency that is ideal for creating the oscillations needed to maintain exact frequency or time. Hence Quartz is very useful in the construction of high stability [[Oscillator Design | oscillators]]&lt;br /&gt;
&lt;br /&gt;
{{electronics}}&lt;/div&gt;</summary>
		<author><name>TimVK4YEH</name></author>
	</entry>
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