Mosaic crystal - Revision history

BrianMcMahon: Tidied translations and added German and Spanish (U. Mueller)

2017-11-16T13:06:05Z

Tidied translations and added German and Spanish (U. Mueller)

BrianMcMahon: Edits to align with printed edition

2017-05-15T17:11:06Z

Edits to align with printed edition

MassimoNespolo: Ja

2015-03-20T13:24:00Z

BrianMcMahon at 12:20, 18 June 2014

2014-06-18T12:20:04Z

MassimoNespolo at 18:41, 21 December 2008

2008-12-21T18:41:19Z

New page

Cristal à mosaique (''Fr''). Cristallo a mosaico (''It'').

The [[mosaic crystal]] is a simplified model of real crystals proposed by C.G. Darwin. In this model, a real crystal is described as a mosaic of crystalline blocks with dimensions of 10-5 cm, tilted to each other by fractions of a minute of arc. Each block is separated from the surrounding blocs by faults and cracks.

In a [[diffraction]] experiment, [[interference]] between waves only occurs inside a bloc, whose dimensions satisfy the theoretical conditions of applicability of the kinematical theory. Because of the loss of coherence between the waves diffracted from different blocks, the diffracted intensity from the whole crystal is equal to the sum of the intensities diffracted by every block.

[[Category:X-rays]]

← Older revision		Revision as of 13:06, 16 November 2017
Line 1:		Line 1:
−	<~~Font~~ color="blue">Cristal à mosaique</~~Font~~> (''Fr''). <~~Font~~ color="black">Cristallo a mosaico</~~Font~~> (''It'').　<~~Font~~ color="purple">モザイク結晶</~~Font~~> (''Ja'').	+	<font color="blue">Cristal à mosaique</font> (''Fr''). <font color="red">Mosaikkristall, Mosaikstruktur</font> (''Ge''). <font color="black">Cristallo a mosaico</font> (''It''). <font color="purple">モザイク結晶</font> (''Ja''). <font color="green">Estructura de mosaico</font> (''Sp'').

@@ Line 1: / Line 1: @@
-<Font color="blue">Cristal à mosaique</Font> (''Fr''). <Font color="black">Cristallo a mosaico</Font> (''It'').　<Font color="purple">モザイク結晶</Font> (''Ja'')
+<Font color="blue">Cristal à mosaique</Font> (''Fr''). <Font color="black">Cristallo a mosaico</Font> (''It'').　<Font color="purple">モザイク結晶</Font> (''Ja'').
-The [[mosaic crystal]] is a simplified model of real crystals proposed by C. G. Darwin. In this model, a real crystal is described as a mosaic of crystalline blocks with dimensions of 10<sup>-5</sup> cm, tilted to each other by fractions of a minute of arc. Each block is separated from the surrounding blocks by faults and cracks.
+In a [[diffraction]] experiment, [[interference]] between waves only occurs inside a block, whose dimensions satisfy the theoretical conditions of applicability of the kinematical theory. Because of the loss of coherence between the waves diffracted from different blocks, the diffracted intensity from the whole crystal is equal to the sum of the intensities diffracted by every block. If the blocks are not small
-In a [[diffraction]] experiment, [[interference]] between waves only occurs inside a block, whose dimensions satisfy the theoretical conditions of applicability of the kinematical theory. Because of the loss of coherence between the waves diffracted from different blocks, the diffracted intensity from the whole crystal is equal to the sum of the intensities diffracted by every block.
+== See also ==
 [[Category:X-rays]]

← Older revision		Revision as of 13:24, 20 March 2015
Line 1:		Line 1:
−	<Font color="blue">Cristal à mosaique</Font> (''Fr''). <Font color="black">Cristallo a mosaico</Font> (''It'').	+	<Font color="blue">Cristal à mosaique</Font> (''Fr''). <Font color="black">Cristallo a mosaico</Font> (''It'').　<Font color="purple">モザイク結晶</Font> (''Ja'')

@@ Line 3: / Line 3: @@
-The [[mosaic crystal]] is a simplified model of real crystals proposed by C.G. Darwin. In this model, a real crystal is described as a mosaic of crystalline blocks with dimensions of 10<sup>-5</sup> cm, tilted to each other by fractions of a minute of arc. Each block is separated from the surrounding blocs by faults and cracks.
+The [[mosaic crystal]] is a simplified model of real crystals proposed by C. G. Darwin. In this model, a real crystal is described as a mosaic of crystalline blocks with dimensions of 10<sup>-5</sup> cm, tilted to each other by fractions of a minute of arc. Each block is separated from the surrounding blocks by faults and cracks.
-In a [[diffraction]] experiment, [[interference]] between waves only occurs inside a bloc, whose dimensions satisfy the theoretical conditions of applicability of the kinematical theory. Because of the loss of coherence between the waves diffracted from different blocks, the diffracted intensity from the whole crystal is equal to the sum of the intensities diffracted by every block.
+In a [[diffraction]] experiment, [[interference]] between waves only occurs inside a block, whose dimensions satisfy the theoretical conditions of applicability of the kinematical theory. Because of the loss of coherence between the waves diffracted from different blocks, the diffracted intensity from the whole crystal is equal to the sum of the intensities diffracted by every block.
 [[Category:X-rays]]