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		<title>Oluschinski: Created page with &quot;{{Language_sel|LANG=ger|ARTIKEL=C-Bild-Technik}} {{PSM_Infobox}} &lt;span style=&quot;font-size:1.2em;font-weight:bold;&quot;&gt;C-scan technique&lt;/span&gt; __FORCETOC__  ==General information==  The C-scan is an ultrasonic testing and evaluation method for two-dimensional imaging of the acoustic properties of a test specimen volume. It is composed of A-scans that have been recorded using a grid of equidistant measuring points. A colour or gray v...&quot;</title>
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		<updated>2025-12-01T07:26:35Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;{{Language_sel|LANG=ger|ARTIKEL=C-Bild-Technik}} {{PSM_Infobox}} &amp;lt;span style=&amp;quot;font-size:1.2em;font-weight:bold;&amp;quot;&amp;gt;C-scan technique&amp;lt;/span&amp;gt; __FORCETOC__  ==General information==  The C-scan is an ultrasonic testing and evaluation method for two-dimensional imaging of the &lt;a href=&quot;/index.php/Acoustic_Properties&quot; title=&quot;Acoustic Properties&quot;&gt;acoustic properties&lt;/a&gt; of a test specimen volume. It is composed of &lt;a href=&quot;/index.php?title=A-Scan_Technique&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;A-Scan Technique (page does not exist)&quot;&gt;A-scans&lt;/a&gt; that have been recorded using a grid of equidistant measuring points. A colour or gray v...&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=C-Bild-Technik}}&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;C-scan technique&amp;lt;/span&amp;gt;&lt;br /&gt;
__FORCETOC__&lt;br /&gt;
&lt;br /&gt;
==General information==&lt;br /&gt;
&lt;br /&gt;
The C-scan is an ultrasonic testing and evaluation method for two-dimensional imaging of the [[Acoustic Properties|acoustic properties]] of a test specimen volume. It is composed of [[A-Scan Technique|A-scans]] that have been recorded using a grid of equidistant measuring points. A colour or gray value is assigned to the sum of the recorded amplitudes. This gives each [[A-Scan Technique|A-scan]] a pixel as a colour or gray value. In the C-scan, these pixels are assembled, and the colour values are graded relative to the scale of the colour palette used [1, 2]. The tests required for the C-scan can be performed using [[Air-Ultrasound|air ultrasound]], the [[Squirter Technique|squirter technique]], or in an [[Ultrasonic Immersion Bath Technique|immersion bath]]. If a moving test object is present, e.g., a passing sheet metal, then a fixed sensor array can be used; otherwise, the sensor (see: [[Ultrasonic Sensors|ultrasonic sensors]]) performs a meandering scanning movement on the stationary test object (&amp;#039;&amp;#039;&amp;#039;Fig. 1&amp;#039;&amp;#039;&amp;#039;). C-scans can also be recorded using [[Ultrasonic Phased Array Technique|ultrasonic phased array technique]].&lt;br /&gt;
&lt;br /&gt;
[[File:C-Scan-1.jpg|450px]]&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;|Schematic diagram of the passive (a) and active (b) scanning process on a plate to generate the C-scan&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
==Construction of a C-scan==&lt;br /&gt;
&lt;br /&gt;
A manipulator (scanner) scans the test piece to be examined according to the previously specified grid definition. The [[HF-Scan|HF-scans]] are recorded at the grid points. In order to generate a C-scan from the [[HF-Scan|HF-scans]], the amplitude values are used to generate an [[A-Scan Technique|A-scan]] (&amp;#039;&amp;#039;&amp;#039;Fig. 2&amp;#039;&amp;#039;&amp;#039;).&lt;br /&gt;
&lt;br /&gt;
The determined amplitude sums are arranged in a matrix according to the scanned grid (&amp;#039;&amp;#039;&amp;#039;Fig. 3a&amp;#039;&amp;#039;&amp;#039;). The sums are then colour-coded using a colour palette. The extremes of the selected colour palette are assigned the extreme values (maximum and minimum) of the sums, resulting in a relative assignment of the colour to the sum values of different scans (&amp;#039;&amp;#039;&amp;#039;Fig. 3b&amp;#039;&amp;#039;&amp;#039;). These values are often smoothed, as shown in &amp;#039;&amp;#039;&amp;#039;Fig. 3c&amp;#039;&amp;#039;&amp;#039;, to increase the resolution using a subpixel variant (see also: [[Colour|colour]]).&lt;br /&gt;
&lt;br /&gt;
[[File:C-Scan-2.jpg|450px]]&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. 2&amp;#039;&amp;#039;&amp;#039;: &lt;br /&gt;
|width=&amp;quot;600px&amp;quot;|A-scan of an ultrasonic signal on glass fibre-reinforced plastic (GFRP) (d = 15 mm)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
[[File:C_Bild-3.JPG|450px]]&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. 3&amp;#039;&amp;#039;&amp;#039;: &lt;br /&gt;
|width=&amp;quot;600px&amp;quot;|Example of a matrix of amplitude sums of the A-scans (a), colour-coded matrix (b), and smoothed presentation of the colour matrix (c)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
==Practical relevance of the C-scan==&lt;br /&gt;
&lt;br /&gt;
The C-scan is very important for testing near-surface defects in a [[Plastic Component|component]]. Its special feature compared to the volume scan is that it examines a test piece layer by layer. This allows, for example, impact damage to plates to be examined layer by layer in order to characterize the effects of impacts with different energy contents.&lt;br /&gt;
&lt;br /&gt;
[[File:C_Bild-4.JPG|450px]]&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. 4&amp;#039;&amp;#039;&amp;#039;: &lt;br /&gt;
|width=&amp;quot;600px&amp;quot;|Example of an ultrasonic examination of a glass fibre reinforced component damaged by three impacts; (a) surface and (b) rear wall&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
[[File:C_Bild-5.JPG|450px]]&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. 5&amp;#039;&amp;#039;&amp;#039;: &lt;br /&gt;
|width=&amp;quot;600px&amp;quot;|Example of an ultrasonic examination of sandwich components damaged by different energy levels&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Figure 4 shows the C-scans of the surface (a) and the back wall (b). This is made possible by selecting the appropriate time intervals of the response signal using apertures. The impact positions on the [[Surface|surface]] are clearly visible. &amp;#039;&amp;#039;&amp;#039;Fig. 4b&amp;#039;&amp;#039;&amp;#039; shows the typical impact behaviour of [[Short-fibre Reinforced Plastics|short-fibre reinforced composites]], where the damage spreads conically (impact trombe) towards the back wall and a closed damage area (delamination) can be seen (see also: [[Compression After Impact Test|compression after impact (CAI) test]]).&lt;br /&gt;
&lt;br /&gt;
In accordance with the different reflection properties on impact-damaged surfaces, the dependence of the amplitude values on the energy content of impacts can also be determined during the ultrasonic examinations while maintaining the test parameters (&amp;#039;&amp;#039;&amp;#039;Fig. 5&amp;#039;&amp;#039;&amp;#039;).&lt;br /&gt;
&lt;br /&gt;
==Other types of C-scan generation==&lt;br /&gt;
&lt;br /&gt;
The [[Ultrasonic Phased Array Sensors|phased array transducer]] generates the C-scan based on its [[B-Scan Technique|B-scan]] construction with a one-dimensional movement. The phased array transducer can be moved using a manipulator, whereby another option is to move the test object, as is the case with ultrasonic testing systems used in the production of sheet metal and strips [3]. In the phased array, individual [[Piezoelectric Ceramic Transducer|transducers]] are arranged equidistantly in the form of a line array, which can be addressed individually or in groups by the testing software or can be focused differently. The movement described above is simulated by a constant time offset.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
&lt;br /&gt;
* [[A-Scan Technique|A-scan technique]]&lt;br /&gt;
* [[B-Scan Technique|B-scan technique]]&lt;br /&gt;
* [[Imaging Ultrasonic Testing|Imaging ultrasonic testing]]&lt;br /&gt;
* [[D-Scan Technique|D-scan technique]]&lt;br /&gt;
* [[F-Scan Technique|F-scan technique]]&lt;br /&gt;
* [[HF-Scan|HF-scan]]&lt;br /&gt;
* [[Ultrasound Testing|Ultrasound testing]]&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;
|Matthies, K., Gohlke, D.: Der Ultraschall-Volumenscan als Werkzeug zur Prüfung komplizierter Geometrien und komplexer Gefüge. DGZfP-Jahrestagung 2007 &lt;br /&gt;
|-valign=&amp;quot;top&amp;quot;&lt;br /&gt;
|[2]&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;
|[3]&lt;br /&gt;
|John, M., Schlimper, R., Mudra, Chr.: Deformation and Failure Behaviour of Pre-damaged Foam-core Sandwich Structures in a Four-point Bending Configuration. ECCM17 – 17th European Conference on Composite Materials, Munich, Germany, 26-30th June 2016 &lt;br /&gt;
|-valign=&amp;quot;top&amp;quot;&lt;br /&gt;
|[4]&lt;br /&gt;
|http://www.karldeutsch.de/KD_GENERAL_DL_Contents_DE_M1.html (last access on 2.11.2025) &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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