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	<id>https://en.wiki.polymerservice-merseburg.de/index.php?action=history&amp;feed=atom&amp;title=J-Integral_Concept</id>
	<title>J-Integral Concept - Revision history</title>
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	<updated>2026-04-22T19:41:11Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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	<entry>
		<id>https://en.wiki.polymerservice-merseburg.de/index.php?title=J-Integral_Concept&amp;diff=878&amp;oldid=prev</id>
		<title>Oluschinski at 06:12, 15 December 2025</title>
		<link rel="alternate" type="text/html" href="https://en.wiki.polymerservice-merseburg.de/index.php?title=J-Integral_Concept&amp;diff=878&amp;oldid=prev"/>
		<updated>2025-12-15T06:12:44Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
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				&lt;tr class=&quot;diff-title&quot; lang=&quot;en&quot;&gt;
				&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 08:12, 15 December 2025&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-l6&quot;&gt;Line 6:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 6:&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;==Energetic consideration of the fracture process==&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;==Energetic consideration of the fracture process==&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 &#039;&#039;J&#039;&#039;-integral introduced by Cherepanov [1] and Rice [2] has gained the greatest importance for [[Plastics | plastics]] due to the energetic consideration of the fracture process (see: [[Fracture Mechanics | &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Fracture &lt;/del&gt;mechanics]] and [[Fracture Types | types of fracture]]). The path-independent contour integral encloses the plastically deformed region and runs in the elastic deformed region with a closed integration path around the crack tip (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;).&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 &#039;&#039;J&#039;&#039;-integral introduced by Cherepanov [1] and Rice [2] has gained the greatest importance for [[Plastics | plastics]] due to the energetic consideration of the fracture process (see: [[Fracture Mechanics | &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;fracture &lt;/ins&gt;mechanics]] and [[Fracture Types | types of fracture]]). The path-independent contour integral encloses the plastically deformed region and runs in the elastic deformed region with a closed integration path around the crack tip (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;).&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;[[file:J-&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Integral&lt;/del&gt;.jpg|500px]]&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;[[file:J-&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;IntConcept-1&lt;/ins&gt;.jpg|500px]]&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;div&gt;{|  &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;{|  &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;div&gt;|- valign=&amp;quot;top&amp;quot;&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;|- valign=&amp;quot;top&amp;quot;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Oluschinski</name></author>
	</entry>
	<entry>
		<id>https://en.wiki.polymerservice-merseburg.de/index.php?title=J-Integral_Concept&amp;diff=437&amp;oldid=prev</id>
		<title>Oluschinski: Created page with &quot;{{Language_sel|LANG=ger|ARTIKEL=J-Integral-Konzept}} {{PSM_Infobox}} &lt;span style=&quot;font-size:1.2em;font-weight:bold;&quot;&gt;&#039;&#039;J&#039;&#039;-integral concept&lt;/span&gt; __FORCETOC__  ==Energetic consideration of the fracture process==  The &#039;&#039;J&#039;&#039;-integral introduced by Cherepanov [1] and Rice [2] has gained the greatest importance for  plastics due to the energetic consideration of the fracture process (see:  Fracture mechanics and Fracture Types | types...&quot;</title>
		<link rel="alternate" type="text/html" href="https://en.wiki.polymerservice-merseburg.de/index.php?title=J-Integral_Concept&amp;diff=437&amp;oldid=prev"/>
		<updated>2025-12-03T11:35:44Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;{{Language_sel|LANG=ger|ARTIKEL=J-Integral-Konzept}} {{PSM_Infobox}} &amp;lt;span style=&amp;quot;font-size:1.2em;font-weight:bold;&amp;quot;&amp;gt;&amp;#039;&amp;#039;J&amp;#039;&amp;#039;-integral concept&amp;lt;/span&amp;gt; __FORCETOC__  ==Energetic consideration of the fracture process==  The &amp;#039;&amp;#039;J&amp;#039;&amp;#039;-integral introduced by Cherepanov [1] and Rice [2] has gained the greatest importance for &lt;a href=&quot;/index.php/Plastics&quot; title=&quot;Plastics&quot;&gt; plastics&lt;/a&gt; due to the energetic consideration of the fracture process (see: &lt;a href=&quot;/index.php/Fracture_Mechanics&quot; title=&quot;Fracture Mechanics&quot;&gt; Fracture mechanics&lt;/a&gt; and Fracture Types | types...&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=J-Integral-Konzept}}&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;&amp;#039;&amp;#039;J&amp;#039;&amp;#039;-integral concept&amp;lt;/span&amp;gt;&lt;br /&gt;
__FORCETOC__&lt;br /&gt;
&lt;br /&gt;
==Energetic consideration of the fracture process==&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;J&amp;#039;&amp;#039;-integral introduced by Cherepanov [1] and Rice [2] has gained the greatest importance for [[Plastics | plastics]] due to the energetic consideration of the fracture process (see: [[Fracture Mechanics | Fracture mechanics]] and [[Fracture Types | types of fracture]]). The path-independent contour integral encloses the plastically deformed region and runs in the elastic deformed region with a closed integration path around the crack tip (&amp;#039;&amp;#039;&amp;#039;Figure 1&amp;#039;&amp;#039;&amp;#039;).&lt;br /&gt;
&lt;br /&gt;
[[file:J-Integral.jpg|500px]]&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;Fig. 1&amp;#039;&amp;#039;&amp;#039;: &lt;br /&gt;
|width=&amp;quot;600px&amp;quot; |Determination of the J-integral: path-independent contour integral with 1 – plastically deformed area (energy-dissipative zone) and 2 – elastically deformed area (a), experimentally determined load vs. load-line displacement curves of different crack lengths (b), energy determined by planimetrating the dependency &amp;#039;&amp;#039;F&amp;#039;&amp;#039; = &amp;#039;&amp;#039;F&amp;#039;&amp;#039;(&amp;#039;&amp;#039;v&amp;#039;&amp;#039;, &amp;#039;&amp;#039;f&amp;#039;&amp;#039;) dependence, related to the specimen thickness as a function of the crack length (c) and &amp;#039;&amp;#039;J&amp;#039;&amp;#039;-integral (d) determined by differentiating the curves (c) [3].&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The x- und y-components are defined by&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;J_x\,=\, \int_{R} \left( W \,dy-T_{ij} \cdot n_j \frac{\partial u}{\partial x}dR\right)&amp;lt;/math&amp;gt; und &lt;br /&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;J_y\,=\, \int_{R} \left( -W \,dx-T_{ij} \cdot n_j \frac{\partial u}{\partial x}dR\right)&amp;lt;/math&amp;gt;.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
with&lt;br /&gt;
{|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;#039;&amp;#039;W&amp;#039;&amp;#039;&lt;br /&gt;
|width=&amp;quot;15px&amp;quot; |&lt;br /&gt;
|elastic energy density&lt;br /&gt;
|-&lt;br /&gt;
|&amp;#039;&amp;#039;T&amp;#039;&amp;#039;&lt;br /&gt;
|&lt;br /&gt;
|stress tensor&lt;br /&gt;
|-&lt;br /&gt;
|&amp;#039;&amp;#039;n&amp;#039;&amp;#039;&lt;br /&gt;
|&lt;br /&gt;
|components oft the unit vector to R around the crack tip&lt;br /&gt;
|-&lt;br /&gt;
|&amp;#039;&amp;#039;u&amp;#039;&amp;#039;&lt;br /&gt;
|&lt;br /&gt;
|displacement vector components&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
==Experimental determination of J-values==&lt;br /&gt;
&lt;br /&gt;
The experimental determination is carried out according to &amp;#039;&amp;#039;&amp;#039;Fig. 1 b to d&amp;#039;&amp;#039;&amp;#039; by determining the deformation energy &amp;#039;&amp;#039;A&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;G&amp;lt;/sub&amp;gt; from the registered load vs. load line displacement curves with different notch depths by planimetry and displaying the ratio &amp;#039;&amp;#039;A&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;G&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;B&amp;#039;&amp;#039; as a function of &amp;#039;&amp;#039;a&amp;#039;&amp;#039;. The deformation energy &amp;#039;&amp;#039;A&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;G&amp;lt;/sub&amp;gt; is then determined by the graphical differentiation.&lt;br /&gt;
&lt;br /&gt;
Using graphical differentiation, the following results&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;J\,=\,\frac{1}{B} \frac{\partial A_G}{\partial a}&amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
as function of the load-line displacement resp. deflection.&lt;br /&gt;
&lt;br /&gt;
Since the effort to determine &amp;#039;&amp;#039;J&amp;#039;&amp;#039;-values according to this procedure is too high for practical [[Material Value | characteristic value]] determination, approximation formulas have been developed. The best-known procedures are:&lt;br /&gt;
&lt;br /&gt;
* Approximation method according to [[BEGLEY and LANDES – J-Integral Estimation Method | BEGLEY and LANDES]],&lt;br /&gt;
* Approximation method according to [[RICE, PARIS and MERKLE – J-Integral Estimation Method | RICE, PARIS and MERKLE]],&lt;br /&gt;
* Approximation method according to [[KANAZAWA – J-Integral Estimation Method | KANAZAWA ]],&lt;br /&gt;
* Approximation methods according to [[SUMPTER and TURNER – J-Integral Estimation Method | SUMPTER and TURNER]] and&lt;br /&gt;
* Approximation methods according to [[MERKLE and CORTEN – J-Integral Estimation Method | MERKLE and CORTEN]].&lt;br /&gt;
&lt;br /&gt;
==Correlations of the J-integral to the stress intensity factor and the crack opening displacement==&lt;br /&gt;
&lt;br /&gt;
For elastic material behaviour, the &amp;#039;&amp;#039;J&amp;#039;&amp;#039;-integral is identical to the [[Energy Release Rate | energy release rate &amp;#039;&amp;#039;G&amp;#039;&amp;#039;]]:&lt;br /&gt;
&lt;br /&gt;
{|&lt;br /&gt;
|-&lt;br /&gt;
|width=&amp;quot;20px&amp;quot;|&lt;br /&gt;
|width=&amp;quot;250px&amp;quot; | &amp;lt;math&amp;gt;J_I\,=\,G_I\,=\,\frac{{K_I}^2}{E}&amp;lt;/math&amp;gt;&lt;br /&gt;
|for ESZ resp.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&amp;lt;math&amp;gt;J_I\,=\,G_I\,=\,\frac{{K_I}^2}{E} \left(1- {\nu}^2 \right)&amp;lt;/math&amp;gt;&lt;br /&gt;
|for EDZ.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
These equations are to be used for the conversion of &amp;#039;&amp;#039;J&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;Ic&amp;lt;/sub&amp;gt; values into K&amp;lt;sub&amp;gt;Ic&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;J&amp;lt;/sup&amp;gt; values.&lt;br /&gt;
&lt;br /&gt;
The relationship between &amp;#039;&amp;#039;J&amp;#039;&amp;#039;-integral and [[Crack Tip Opening Displacement Concept (CTOD) | Crack tip opening displacement (CTOD)]] concept provides&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;J\,=\,m \cdot \sigma_y \cdot \delta_{Ic}&amp;lt;/math&amp;gt;,&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
where &amp;#039;&amp;#039;m&amp;#039;&amp;#039; is called the constraint factor according to [4, 5]. The critical &amp;#039;&amp;#039;J&amp;#039;&amp;#039;-values are geometry-independent, i.e. real [[Material Value | material values]], if the criterion&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;B{,}\ a{,}\ \left( W-a \right)\,\ge\,\varepsilon \frac{J}{\sigma_y}&amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
with&lt;br /&gt;
{|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;math&amp;gt;\varepsilon \!&amp;lt;/math&amp;gt; &lt;br /&gt;
|width=&amp;quot;15px&amp;quot; | &lt;br /&gt;
|material-dependent constant of the geometry criterion of the &amp;#039;&amp;#039;J&amp;#039;&amp;#039;-integral concept&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
is fulfilled.&lt;br /&gt;
&lt;br /&gt;
In [6], the relationship between the fracture mechanical [[Material Parameter | parameters]] determined according to the &amp;#039;&amp;#039;J&amp;#039;&amp;#039;-integral and the [[Crack Tip Opening Displacement Concept (CTOD) | CTOD concept]] is considered using the example of the temperature dependence of the toughness of unoriented and cold-rolled oriented polypropylene ([[Plastics – Symbols and Abbreviated Terms | abbreviation]]: PP). For the constraint factor, &amp;#039;&amp;#039;m&amp;#039;&amp;#039; = 0.7 is given for the examined PP material [7].&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
&lt;br /&gt;
*[[Fracture Mechanics | Fracture mechanics]]&lt;br /&gt;
*[[Fracture Types | Fracture types]]&lt;br /&gt;
*[[Crack Tip Opening Displacement Concept (CTOD) | Crack tip opening displacement concept (CTOD)]]&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;
|Cherepanov, G. P.: On Crack Propagation in Continuous Media. Applied Mechanics and Mathematics 31 (1967) 503&lt;br /&gt;
|-valign=&amp;quot;Top&amp;quot;&lt;br /&gt;
|[2]&lt;br /&gt;
|Rice, J. R.: A Path Independent Integral and the Approximate Analysis of Strain Concentration by Notches and Cracks. J. Appl. Mech. (1968) 379–386&lt;br /&gt;
|-valign=&amp;quot;Top&amp;quot;&lt;br /&gt;
|[3]&lt;br /&gt;
|[[Grellmann,_Wolfgang|Grellmann, W.]], [[Seidler,_Sabine|Seidler, S.]] (Eds.):Polymer Testing. Carl Hanser Verlag, Munich (2022) 3. Edition, p. 239–241 (ISBN 978-1-56990-806-8; E-Book ISBN: 878-1-56990-807-5; see [[AMK-Büchersammlung | AMK-Library]] under A 23)&lt;br /&gt;
|-valign=&amp;quot;Top&amp;quot;&lt;br /&gt;
|[4]&lt;br /&gt;
|[[Blumenauer, Horst|Blumenauer, H.]], Pusch, G.: Technische Bruchmechanik. Deutscher Verlag für Grundstoffindustrie, Leipzig Stuttgart (1993) 3. Auflage, (ISBN 3-342-00659-5; siehe [[AMK-Büchersammlung | AMK-Library]] under E 29-3)&lt;br /&gt;
|-valign=&amp;quot;Top&amp;quot;&lt;br /&gt;
|[5]&lt;br /&gt;
|Anderson, T. L.: Fracture Mechanics. Fundamentals and Applications. 2nd Ed., CRC Press, Boca Raton (1995) 2. Auflage, (ISBN 978-0849342608; siehe [[AMK-Büchersammlung | AMK-Library]] under E 8-1), DOI: [https://doi.org/10.1201/9781315370293]&lt;br /&gt;
|-valign=&amp;quot;Top&amp;quot;&lt;br /&gt;
|[6]&lt;br /&gt;
|[https://www.researchgate.net/profile/Wolfgang-Grellmann Grellmann, W.], Che, M.: Assessment of Temperature-dependent Fracture Behaviour with Different Fracture Mechanics Concepts on Example of Unoriented and Cold-rolled Polypropylene. J. Applied Polymer Science 66 (1997) 1237–1249; https://doi.org/10.1002/(SICI)1097-4628(19971114)66:7%3C1237::AID-APP4%3E3.0.CO;2-H&lt;br /&gt;
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|[7]&lt;br /&gt;
|Hille, E.: Untersuchungen zum Bruchverhalten des orientierten isotaktischen Polypropylen. Ph.D. Dissertation, [https://de.wikipedia.org/wiki/Technische_Hochschule_Leuna-Merseburg Technische Hochschule Leuna-Merseburg (1983)]&lt;br /&gt;
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[[Category:Fracture Mechanics]]&lt;br /&gt;
[[Category:Instrumented Impact Test]]&lt;/div&gt;</summary>
		<author><name>Oluschinski</name></author>
	</entry>
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