My WebLink
|
Help
|
About
|
Sign Out
Home
Browse
Search
WMOD00399
CWCB
>
Weather Modification
>
DayForward
>
WMOD00399
Metadata
Thumbnails
Annotations
Entry Properties
Last modified
7/28/2009 2:37:39 PM
Creation date
4/16/2008 11:05:22 AM
Metadata
Fields
Template:
Weather Modification
Title
WMO Training Workshop on Weather Modification for Meteorologists - Lecture Notes
Date
12/1/1979
Weather Modification - Doc Type
Report
Jump to thumbnail
< previous set
next set >
There are no annotations on this page.
Document management portal powered by Laserfiche WebLink 9 © 1998-2015
Laserfiche.
All rights reserved.
/
232
PDF
Print
Pages to print
Enter page numbers and/or page ranges separated by commas. For example, 1,3,5-12.
After downloading, print the document using a PDF reader (e.g. Adobe Reader).
Show annotations
View images
View plain text
<br />- 38 - <br /> <br />2.15 <br /> <br />1 <br /> <br />is used, the radar equation takes the fbrm <br /> <br />If the value Z <br /> <br />rr 3 C r Pt G :t r 8 2 ] I -I:z. <br />1024 i n 2 . "2 K r 2 <br />L A I <br />This is a more suitable form of notation for the radar e~uation in <br />which the radar's parameters are separated from those of the target. According to <br />this equation the assumed power can be expressed through the radar ref+ectivity <br />using the logarithmic relationship: <br />10 i g Pr = 101,9 Z - 201g r + c <br /> <br />Pr = Pt <br /> <br />; <br />where c is a constant determined by the radar's parameters. The log~rithmic <br />notation for the equation is useful because the variation range of IPr: and Z is <br />very wide. Usually Pr is measured in milliwatts, whilst the value 10 igPr is <br />the power in dBM (decibels in relation to one milliwatt); Z is measured in mm6/m3; <br />whilst the value 10 I, gZ is called the reflectivity in dBZ (decibels' in relation <br />to one mm6 / m3). <br /> <br />2.16 From the determination of Z it follows that this value;depends on <br />the drop-size distribution and, because of the sixth power relationshi~, is very <br />sensitive to the large-drop part of th~ distribution." Direct measurements of the <br />raindrop size ranges show that they have.a roughly exponential form of:distribution. <br />Marshall and Palmer were the firt to note that raindrop distributions, :except for <br />drops of the smallest dimensions, can be roughly described by the functions: <br /> <br />N ( D.) = No e - l). D 1 <br /> <br />in which the coefficient A depends only on the rain's intensity and is expressed <br />in the form 41 R 0.21 I <br />"A ( R) = <br /> <br />h .. -1 dR' <br />were A 1S 1n em ,an 1n <br />according to the Marshall-Palmer <br />the reflectivity is equal to <br /> <br />mm/hour. If the raindrops are distributed <br />law throughout the size range, it can Ibe shown that <br /> <br />Z = N 6! . R 1.47 <br />o (41)7 <br />This relationship is in good agreement with empirical data on the <br />in rain which can be approximated well by the relation: <br /> <br />Z = 200 R 1.6 <br /> <br />Z-R irelationship <br />! <br /> <br />2.17 <br />intensities <br /> <br />i <br />The following table shows the Z values for various precipitation <br />R calculated according this empirical relationship: i <br /> <br /> ~ <br />R (mm/hour) 0.1 1 10 100 <br />Z 6 3) 5 200 7950 316000 <br />(mm /mm <br />10 19 Z (dBZ) 7 23 39 ! 55 <br />
The URL can be used to link to this page
Your browser does not support the video tag.