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		<title>Oluschinski: Created page with &quot;{{Language_sel|LANG=ger|ARTIKEL=Schalldruck}} {{PSM_Infobox}} &lt;span style=&quot;font-size:1.2em;font-weight:bold;&quot;&gt;Sound pressure&lt;/span&gt; __FORCETOC__  ==Definition==  Sound pressure &#039;&#039;p&#039;&#039; is a physical measured variable (see also: material parameter) that is widely used in non-destructive polymer testing, particularly in acoustic resonance analysis and Ultrasound Testing|...&quot;</title>
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		<updated>2025-12-05T13:36:23Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;{{Language_sel|LANG=ger|ARTIKEL=Schalldruck}} {{PSM_Infobox}} &amp;lt;span style=&amp;quot;font-size:1.2em;font-weight:bold;&amp;quot;&amp;gt;Sound pressure&amp;lt;/span&amp;gt; __FORCETOC__  ==Definition==  Sound pressure &amp;#039;&amp;#039;p&amp;#039;&amp;#039; is a physical &lt;a href=&quot;/index.php/Measured_Variable&quot; title=&quot;Measured Variable&quot;&gt;measured variable&lt;/a&gt; (see also: &lt;a href=&quot;/index.php/Material_Parameter&quot; title=&quot;Material Parameter&quot;&gt;material parameter&lt;/a&gt;) that is widely used in &lt;a href=&quot;/index.php?title=Non-destructive_Polymer_Testing&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;Non-destructive Polymer Testing (page does not exist)&quot;&gt;non-destructive polymer testing&lt;/a&gt;, particularly in &lt;a href=&quot;/index.php/Resonance_Analysis&quot; title=&quot;Resonance Analysis&quot;&gt;acoustic resonance analysis&lt;/a&gt; and Ultrasound Testing|...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Language_sel|LANG=ger|ARTIKEL=Schalldruck}}&lt;br /&gt;
{{PSM_Infobox}}&lt;br /&gt;
&amp;lt;span style=&amp;quot;font-size:1.2em;font-weight:bold;&amp;quot;&amp;gt;Sound pressure&amp;lt;/span&amp;gt;&lt;br /&gt;
__FORCETOC__&lt;br /&gt;
&lt;br /&gt;
==Definition==&lt;br /&gt;
&lt;br /&gt;
Sound pressure &amp;#039;&amp;#039;p&amp;#039;&amp;#039; is a physical [[Measured Variable|measured variable]] (see also: [[Material Parameter|material parameter]]) that is widely used in [[Non-destructive Polymer Testing|non-destructive polymer testing]], particularly in [[Resonance Analysis|acoustic resonance analysis]] and [[Ultrasound Testing|ultrasound testing]], and is expressed in pascals (Pa). Because specifying sound pressure in pascals is rather impractical (it covers a very large range from 10&amp;lt;sup&amp;gt;-5&amp;lt;/sup&amp;gt; to 10&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; Pa), the logarithmic sound pressure level (abbreviated to sound level) is used. This is the logarithmic effective value of the sound pressure &amp;#039;&amp;#039;p&amp;#039;&amp;#039;, which is related to the sound pressure &amp;#039;&amp;#039;p&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; of the human hearing threshold at a frequency of 1 kHz. The specification of the level in dB (decibels) has been introduced and has proven itself in practice. The level is calculated from:&lt;br /&gt;
&lt;br /&gt;
{|&lt;br /&gt;
|-&lt;br /&gt;
|width=&amp;quot;20px&amp;quot;|&lt;br /&gt;
|width=&amp;quot;500px&amp;quot; | &amp;lt;math&amp;gt;L_p\,=\,20\, log\frac{p}{p_0}&amp;lt;/math&amp;gt; &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Here,&lt;br /&gt;
&lt;br /&gt;
{|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;#039;&amp;#039;p&amp;#039;&amp;#039;&lt;br /&gt;
|width=&amp;quot;15px&amp;quot; |&lt;br /&gt;
|is the sound pressure&lt;br /&gt;
|-&lt;br /&gt;
|&amp;#039;&amp;#039;p&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;	&lt;br /&gt;
|&lt;br /&gt;
| is the reference value for airborne sound (2 • 10&amp;lt;sup&amp;gt;-5&amp;lt;/sup&amp;gt; Pa).&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Normalisation to a reference value is necessary because the logarithm can only be calculated from a dimensionless number.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Reference&amp;#039;&amp;#039;&amp;#039;&lt;br /&gt;
&lt;br /&gt;
* Hertlin, Ingolf: Informationsschriften zur zerstörungsfreien Prüfung – ZfP kompakt und verständlich. Volume 5: Akustische Resonanzanalyse. Castell-Verlag GmbH, Wuppertal (2003)&lt;br /&gt;
&lt;br /&gt;
==Acoustic sound field variables==&lt;br /&gt;
&lt;br /&gt;
The sound pressure (more precisely: sound alternating pressure) &amp;#039;&amp;#039;p&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt; is a scalar quantity and describes the change in pressure in a medium as a function of place and time. Together with the normal pressure &amp;#039;&amp;#039;p&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; (= air pressure), it forms the total pressure:&lt;br /&gt;
&lt;br /&gt;
{|&lt;br /&gt;
|-&lt;br /&gt;
|width=&amp;quot;20px&amp;quot;|&lt;br /&gt;
|width=&amp;quot;500px&amp;quot; | &amp;lt;math&amp;gt;P\left(\vec r,t \right)\,=\,p_0\,+\,p_s\, \left(\vec r,t \right).&amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Sound pressure is of fundamental importance for calculating the [[Reflection Sound Waves|reflection]] or [[Transmission Sound Waves|transmission of sound waves]]. For example, the reflection coefficient is derived from the sound pressure ratio of the wave entering the [[Material &amp;amp; Werkstoff|material]] and the reflected wave.&lt;br /&gt;
&lt;br /&gt;
Due to HUYGENS&amp;#039; principle, the elementary waves in the environment of the [[Piezoelectric Ceramic|oscillator]] overlap until only one interference maximum is formed, which represents the beginning of the far field, in which the sound pressure decreases to ~1/z (see &amp;#039;&amp;#039;&amp;#039;Figure&amp;#039;&amp;#039;&amp;#039;).&lt;br /&gt;
&lt;br /&gt;
[[File:Schalldruck.JPG|600px]]&lt;br /&gt;
{| &lt;br /&gt;
|- valign=&amp;quot;top&amp;quot;&lt;br /&gt;
|width=&amp;quot;50px&amp;quot;|&amp;#039;&amp;#039;&amp;#039;Figure&amp;#039;&amp;#039;&amp;#039;: &lt;br /&gt;
|width=&amp;quot;600px&amp;quot; |Dependence of sound pressure on location in units of near-field length &amp;#039;&amp;#039;N&amp;#039;&amp;#039; on the acoustic axis (according to [1])&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The sound pressure in [[Ultrasound Testing|ultrasound testing]] is small compared to the total pressure, so that the [[Density|density]] in the medium through which the sound travels can be regarded as constant, thus simplifying the equations for calculating acoustic variables such as [[Sound Velocity|sound velocity]] and specific attenuation [2, 3].&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
&lt;br /&gt;
* [[Sound Power|Sound power]]&lt;br /&gt;
* [[Ultrasonic Birefringence|Ultrasonic birefringence]]&lt;br /&gt;
* [[Ultrasonic Standard Sensors|Ultrasonic standard sensors]]&lt;br /&gt;
* [[Absorption Sound Waves|Absorption sound waves]]&lt;br /&gt;
* [[Reflection Sound Waves|Reflection sound waves]]&lt;br /&gt;
* [[Transmission Sound Waves|Transmission sound waves]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;References&amp;#039;&amp;#039;&amp;#039;&lt;br /&gt;
&lt;br /&gt;
{|&lt;br /&gt;
|-valign=&amp;quot;top&amp;quot;&lt;br /&gt;
|[1]&lt;br /&gt;
|Deutsch, V.: Platte, M.; Vogt, M.: Ultraschallprüfung – Grundlagen und industrielle Anwendungen. Springer Verlag, Berlin Heidelberg (1997), (ISBN 3-540-62072-9; see [[AMK-Büchersammlung|AMK-Library]] under M 45) &lt;br /&gt;
|-valign=&amp;quot;top&amp;quot;&lt;br /&gt;
|[2]&lt;br /&gt;
|Matthies, K. u. a.: Dickenmessung mit Ultraschall. DGZfP, Deutsche Gesellschaft für zerstörungsfreie Prüfung, (Hrsg.), DVS-Verlag, Berlin (1998) 2nd expanded Edition (ISBN 3-87155-940-7; see [[AMK-Büchersammlung|AMK-Library]] under M 44) &lt;br /&gt;
|-valign=&amp;quot;top&amp;quot;&lt;br /&gt;
|[3]&lt;br /&gt;
|&amp;amp;Scaron;utilov, V. A.: Physik des Ultraschalls. Springer, Vienna New York (2012), ISBN 978-3-7091-8751-7; First Edition: Akademie Verlag, Berlin (1984)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
[[Category:Acoustic Test Methods_Ultrasonics]]&lt;/div&gt;</summary>
		<author><name>Oluschinski</name></author>
	</entry>
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