Air-kerma rate constant - Revision history

Karen Clement at 17:31, 12 September 2019

2019-09-12T17:31:24Z

Intern at 17:47, 6 June 2019

2019-06-06T17:47:48Z

Intern at 17:47, 6 June 2019

2019-06-06T17:47:14Z

Chris Clement at 03:11, 27 March 2019

2019-03-27T03:11:29Z

Intern at 20:04, 7 March 2019

2019-03-07T20:04:41Z

Intern at 14:43, 7 March 2019

2019-03-07T14:43:44Z

Intern at 14:40, 7 March 2019

2019-03-07T14:40:58Z

Admin: 1 revision imported

2019-03-05T17:23:54Z

1 revision imported

icrpaedia>Clement at 14:15, 23 February 2019

2019-02-23T14:15:39Z

New page

__NOTOC__
A characteristic constant for a radionuclide, which is defined in terms of an ideal point source, as , where is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance l in a vacuum from a point source of the radionuclide of activity A.

(Adapted from [http://www.icrp.org/publication.asp?id=ICRP%20Publication%20107 ICRP ''Publication 107''])

''[[ICRP Glossary]] entry - 22 February 2019''

==<span class="mw-collapsible-headline">Previous Versions</span>==

<div id="collapse01" class="mw-collapsible mw-collapsed">
<div class="mw-collapsible-toggle">
<div class="mw-collapsible-toggle-row">
<div class="mw-collapsible-toggle"><span style="color:#ffffff;">[see more/less]</span></div>
</div>
</div>
<br />

<div class="mw-collapsible-content">

[http://www.icrp.org/publication.asp?id=ICRP%20Publication%20107 '''ICRP''' '''''Publication 107'''''] Glossary (Ann. ICRP 38(3), 2008)

<blockquote>This constant, a characteristic of a radionuclide, is defined in terms of an ideal point source as where is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance l in a vacuum from a point source of the radionuclide of activity A.</blockquote>

</div> </div>

@@ Line 1: / Line 1: @@
-__NOTOC__
+A characteristic constant for a radionuclide, which is defined in terms of an ideal point source, as <math>   \Gamma _\delta =</math> <math>\frac{\iota^2\ \dot{K}_\delta}{A} </math> , where <math> \dot{K}_\delta</math>is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance <math>\iota</math> in a vacuum from a point source of the radionuclide of activity A. (Adapted from [[ICRP Publication 107]])
-''[[ICRP Glossary]] entry - 22 February 2019''
+''ICRP Glossary entry - 22 February 2019''
-<div id="collapse01" class="mw-collapsible mw-collapsed">
+'''Return to [[ICRP Glossary|Glossary]]'''

@@ Line 1: / Line 1: @@
 __NOTOC__
-A characteristic constant for a radionuclide, which is defined in terms of an ideal point source, as <math>   \Gamma _\delta =</math> <math>\frac{\iota^2\ \dot{K}_\delta}{A} </math> , where <math> \dot{K}_\delta</math>is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance <math>\iota</math> in a vacuum from a point source of the radionuclide of activity A.
+A characteristic constant for a radionuclide, which is defined in terms of an ideal point source, as <math>   \Gamma _\delta =</math> <math>\frac{\iota^2\ \dot{K}_\delta}{A} </math> , where <math> \dot{K}_\delta</math>is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance <math>\iota</math> in a vacuum from a point source of the radionuclide of activity A.(adaoted from [[ICRP Publication 107]])
 ''[[ICRP Glossary]] entry - 22 February 2019''

← Older revision		Revision as of 17:47, 6 June 2019
Line 3:		Line 3:


−	(~~Adapted from~~ [~~http://www.icrp.org/publication.asp?id=ICRP%20Publication%20107~~ ICRP ''Publication 107''])	+	([[ICRP Publication 107]])

	''[[ICRP Glossary]] entry - 22 February 2019''		''[[ICRP Glossary]] entry - 22 February 2019''

← Older revision		Revision as of 03:11, 27 March 2019
Line 1:		Line 1:
	__NOTOC__		__NOTOC__
−	A characteristic constant for a radionuclide, which is defined in terms of an ideal point source, as <math> \Gamma _\delta =</math> <math>\frac{\iota^2\ \dot{K}_\delta}{A} </math> , where <math> \dot{K}_\delta</math>is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance l in a vacuum from a point source of the radionuclide of activity A.	+	A characteristic constant for a radionuclide, which is defined in terms of an ideal point source, as <math> \Gamma _\delta =</math> <math>\frac{\iota^2\ \dot{K}_\delta}{A} </math> , where <math> \dot{K}_\delta</math>is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance <math>\iota</math> in a vacuum from a point source of the radionuclide of activity A.

← Older revision		Revision as of 14:43, 7 March 2019
Line 1:		Line 1:
	__NOTOC__		__NOTOC__
−	A characteristic constant for a radionuclide, which is defined in terms of an ideal point source, a <math> \Gamma _\delta =</math> <math>\frac{\iota^2\ \dot{K}_\delta}{A} </math> , where <math> \dot{K}_\delta</math>is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance l in a vacuum from a point source of the radionuclide of activity A.	+	A characteristic constant for a radionuclide, which is defined in terms of an ideal point source, as <math> \Gamma _\delta =</math> <math>\frac{\iota^2\ \dot{K}_\delta}{A} </math> , where <math> \dot{K}_\delta</math>is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance l in a vacuum from a point source of the radionuclide of activity A.

@@ Line 21: / Line 21: @@
 [http://www.icrp.org/publication.asp?id=ICRP%20Publication%20107 '''ICRP''' '''''Publication 107'''''] Glossary (Ann. ICRP 38(3), 2008)
-<blockquote>This constant, a characteristic of a radionuclide, is defined in terms of an ideal point source as where is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance l in a vacuum from a point source of the radionuclide of activity A.</blockquote>
+<blockquote>This constant, a characteristic of a radionuclide, is defined in terms of an ideal point source, as <math>   \Gamma _\delta =</math> <math>\frac{\iota^2\ \dot{K}_\delta}{A} </math> , where <math> \dot{K}_\delta</math> is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance l in a vacuum from a point source of the radionuclide of activity A.</blockquote>
 </div> </div>

@@ Line 1: / Line 1: @@
 __NOTOC__
-A characteristic constant for a radionuclide, which is defined in terms of an ideal point source, as , where is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance l in a vacuum from a point source of the radionuclide of activity A.
+A characteristic constant for a radionuclide, which is defined in terms of an ideal point source, a <math>   \Gamma _\delta =</math> <math>\frac{\iota^2\ \dot{K}_\delta}{A} </math> , where <math> \dot{K}_\delta</math>is the air-kerma rate due to photons (gamma and x rays) of energy greater than δ at a distance l in a vacuum from a point source of the radionuclide of activity A.
 (Adapted from [http://www.icrp.org/publication.asp?id=ICRP%20Publication%20107 ICRP ''Publication 107''])

← Older revision	Revision as of 17:23, 5 March 2019
(No difference)