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	<title>Inertial Load - Revision history</title>
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	<updated>2026-04-22T20:07:35Z</updated>
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	<entry>
		<id>https://en.wiki.polymerservice-merseburg.de/index.php?title=Inertial_Load&amp;diff=414&amp;oldid=prev</id>
		<title>Oluschinski: Created page with &quot;{{Language_sel|LANG=ger|ARTIKEL=Aufschlagimpuls}} {{PSM_Infobox}} &lt;span style=&quot;font-size:1.2em;font-weight:bold;&quot;&gt;Initial load, impact impulse or inertial force&lt;/span&gt; __FORCETOC__  ==Causes of inertial load==  The occurrence of an inertial load (also referred to as inertial force) caused by mass inertia, which is superimposed on the actual deformation behaviour, represents a measurement and evaluation problem in materials testing under dynamic load...&quot;</title>
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		<updated>2025-12-02T09:41:44Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;{{Language_sel|LANG=ger|ARTIKEL=Aufschlagimpuls}} {{PSM_Infobox}} &amp;lt;span style=&amp;quot;font-size:1.2em;font-weight:bold;&amp;quot;&amp;gt;Initial load, impact impulse or inertial force&amp;lt;/span&amp;gt; __FORCETOC__  ==Causes of inertial load==  The occurrence of an inertial load (also referred to as inertial force) caused by mass inertia, which is superimposed on the actual deformation behaviour, represents a measurement and evaluation problem in &lt;a href=&quot;/index.php/Materials_Testing&quot; title=&quot;Materials Testing&quot;&gt;materials testing&lt;/a&gt; under dynamic load...&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=Aufschlagimpuls}}&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;Initial load, impact impulse or inertial force&amp;lt;/span&amp;gt;&lt;br /&gt;
__FORCETOC__&lt;br /&gt;
&lt;br /&gt;
==Causes of inertial load==&lt;br /&gt;
&lt;br /&gt;
The occurrence of an inertial load (also referred to as inertial force) caused by mass inertia, which is superimposed on the actual deformation behaviour, represents a measurement and evaluation problem in [[Materials Testing|materials testing]] under dynamic loads. Due to the large differences in damping behaviour, the vibration problem is even more pronounced for [[Plastics|plastics]] than for metals.&lt;br /&gt;
&lt;br /&gt;
When the [[Stress|stress]] is applied suddenly during dynamic ([[Impact Loading Plastics|impact]]) tests, a complex reaction occurs in the entire coupled system, which consists of the following components:&lt;br /&gt;
&lt;br /&gt;
* Reaction forces of the test [[Specimen|specimen]],&lt;br /&gt;
* Acceleration forces,&lt;br /&gt;
* Signal vibrations caused by spring-mass forces,&lt;br /&gt;
* Signal vibrations caused by reflected body sound waves,&lt;br /&gt;
* High-frequency signal vibrations caused by downstream measuring electronics.&lt;br /&gt;
&lt;br /&gt;
==Relationship between inertial load and maximum load in ICIT==&lt;br /&gt;
&lt;br /&gt;
In an electronically recorded load–time or [[ICIT – Types of Impact Load–Deflection Diagrams|load–deflection diagram]] in the [[Instrumented Charpy Impact Test|instrumented Charpy impact test (ICIT)]], the mass inertia causes a reaction force to occur in the test specimen, the amplitude of which must always be considered in relation to the maximum load (force at the onset of unstable [[Crack Propagation|crack propagation]]). The vibration that occurs is referred to as inertial vibration. The inertial load is independent of the &amp;#039;&amp;#039;a&amp;#039;&amp;#039;/&amp;#039;&amp;#039;W&amp;#039;&amp;#039; ratio (&amp;#039;&amp;#039;a&amp;#039;&amp;#039; – [[Notching|notch depth]], &amp;#039;&amp;#039;W&amp;#039;&amp;#039; – specimen width) of the test [[Specimen|specimen]], but depends on stress parameters such as [[Velocity|velocity]] and temperature.&lt;br /&gt;
&lt;br /&gt;
==Criteria for determining the start of unstable crack propagation==&lt;br /&gt;
&lt;br /&gt;
The decisive factor in determining the point at which unstable [[Crack Propagation|crack propagation]] begins is that the maximum impact load &amp;#039;&amp;#039;F&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;max&amp;lt;/sub&amp;gt;&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;F_{max}\;&amp;gt;\;F_1&amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
must be greater than the inertial load &amp;#039;&amp;#039;F&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. To check this equation, the amplitude of the inertial force can be estimated using the equation&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;F_1\approx\frac{Z_1\,\cdot\,Z_2}{Z_1+Z_2} \cdot v_I&amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
must be greater than the inertial load &amp;#039;&amp;#039;F&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. To check this equation, the amplitude of the inertial force can be estimated using the equation&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;Z_{1{,}2}\,=\,c_{1{,}2} \cdot \rho_{1{,}2}&amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
where&lt;br /&gt;
&lt;br /&gt;
{|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;#039;&amp;#039;Z&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;1,2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|width=&amp;quot;15px&amp;quot; | &lt;br /&gt;
|spezific sound impedance of [[Specimen|specimen]] and/or pendulum &lt;br /&gt;
|-&lt;br /&gt;
|&amp;#039;&amp;#039;ρ&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;1,2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|[[Density]] of specimen and/or pendulum hammer material &lt;br /&gt;
|-&lt;br /&gt;
|&amp;#039;&amp;#039;c&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;1,2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|[[Sound Velocity|sound velocity]] of specimen and/or pendulum hammer&lt;br /&gt;
|-&lt;br /&gt;
|&amp;#039;&amp;#039;v&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;I&amp;lt;/sub&amp;gt; &lt;br /&gt;
|&lt;br /&gt;
|impact velocity according to ISO 13802&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
If the maximum impact load is greater than the inertial load, the [[Fracture Mechanics|fracture mechanics]] [[Material Parameter|parameters]] can be determined using static evaluation formulas.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
&lt;br /&gt;
* [[ICIT – Influence of Pendulum Hammer Velocity|ICIT– Influence of pendulum hammer velocity]]&lt;br /&gt;
* [[ICIT – Experimental Conditions|ICIT– Experimental conditions]]&lt;br /&gt;
* [[ICIT – Limits of Fracture Mechanics Evaluation|ICIT– Limits of fracture mechanics evaluation]]&lt;br /&gt;
* [[ICIT – Nonlinear Material Behaviour|ICIT– Nonlinear material behaviour]]&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;
* [[Grellmann, Wolfgang|Grellmann, W.]]: Bewertung der Zähigkeitseigenschaften durch bruchmechanische Kennwerte, In: Schmiedel, H. (Ed.): Handbuch der Kunststoffprüfung. Carl Hanser, Munich Vienna (1992), pp. 139–183, (ISBN 3-446-16336-0; see [[AMK-Büchersammlung|AMK-Library]] under A 3)&lt;br /&gt;
* [https://www.researchgate.net/profile/Wolfgang-Grellmann Grellmann, W.], [[Seidler, Sabine|Seidler, S. (eng.)]]: Kunststoffprüfung. Carl Hanser, Munich (2025) 4th Edition, pp. 256–261 (ISBN 978-3-446-44718-9; E-Book: ISBN 978-3-446-48105-3; see [[AMK-Büchersammlung|AMK-Library]] under A 23)&lt;br /&gt;
* ISO 13802 (2025-08): Plastics – Verification of Pendulum Impact-testing Machines – Charpy, Izod and Tensile Impact-testing&lt;br /&gt;
&lt;br /&gt;
[[category:Instrumented Impact Test]]&lt;/div&gt;</summary>
		<author><name>Oluschinski</name></author>
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