{"id":2607,"date":"2016-11-06T14:19:49","date_gmt":"2016-11-06T14:19:49","guid":{"rendered":"http:\/\/www.raymaps.com\/?p=2607"},"modified":"2022-04-03T18:22:20","modified_gmt":"2022-04-03T18:22:20","slug":"knife-edge-diffraction-model","status":"publish","type":"post","link":"https:\/\/www.raymaps.com\/index.php\/knife-edge-diffraction-model\/","title":{"rendered":"Knife Edge Diffraction Model"},"content":{"rendered":"\n

What is Diffraction<\/strong><\/p>\n\n\n\n

Diffraction is a phenomenon where electromagnetic waves (such as light waves) bend around corners to reach places which are otherwise not reachable i.e. not in the line of sight. In technical jargon such regions are also called shadowed regions (the term again drawn from the physics of light). This phenomenon can be explained by Huygen’s principle which states that “as a plane wave propagates in a particular direction each new point along the wavefront is a source of secondary waves”. This can be understood by looking at the following figure. However one peculiarity of this principle is that it is unable to explain why the new point source transmits only in the forward direction.<\/p>\n\n\n\n

\"Image<\/figure><\/div>\n\n\n\n

Diffraction is Difficult to Model<\/strong><\/p>\n\n\n\n

The electromagnetic field in the shadowed region can be calculated by combining vectorially the contributions of all of these secondary sources, which is not an easy task. Secondly, the geometry is usually much more complicated than shown in the above figure. For example consider a telecom tower transmitting electromagnetic waves from a rooftop and a pedestrian using a mobile phone at street level. The EM waves usually reach the receiver at street level after more than one diffraction (not to mention multiple reflections). However, an approximation that works well in most cases is called knife edge diffraction, which assumes a single sharp edge (an edge with a thickness much smaller than the wavelength) separates the transmitter and receiver.<\/p>\n\n\n\n

Knife Edge Model<\/strong><\/p>\n\n\n\n

The path loss due to diffraction in the knife edge model is controlled by the Fresnel Diffraction Parameter which measures how deep the receiver is within the shadowed region. A negative value for the parameter shows that the obstruction is below the line of sight and if the value is below -1 there is hardly any loss. A value of 0 (zero) means that the transmitter, receiver and tip of the obstruction are all in line and the Electric Field Strength is reduced by half or the power is reduced to one fourth of the value without the obstruction i.e. a loss of 6dB.  As the value of the Fresnel Diffraction Parameter increases on the positive side the path loss rapidly increases reaching a value of 27 dB for a parameter value of 5. Sometimes the exact calculation is not needed and only an approximate calculation, as proposed by Lee in 1985, is sufficient.<\/p>\n\n\n\n

Fresnel Diffraction Parameter (v) is defined as:<\/p>\n\n\n\n

v=h\u221a(2(d1+d2)\/(\u03bb d1 d2))<\/p>\n\n\n\n

where<\/p>\n\n\n\n

d1 is the distance between the transmitter and the obstruction along the line of sight<\/p>\n\n\n\n

d2 is the distance between the receiver and the obstruction along the line of sight<\/p>\n\n\n\n

h is the height of the obstruction above the line of sight<\/p>\n\n\n\n

and \u03bb is the wavelength<\/p>\n\n\n\n

The electrical length of the path difference between a diffracted ray and a LOS ray is equal to \u03c6=(\u03c0\/2)(v\u00b2) and the normalized electric field produced at the receiver, relative to the LOS path is e-j\u03c6<\/sup>. Performing a summation of all the exponentials above the obstruction (from v to positive infinity) gives us the Fresnel Integral, F(v).<\/p>\n\n\n\n

\"\"<\/a>
Knife Edge Diffraction Model Using Huygens Principle<\/figcaption><\/figure><\/div>\n\n\n\n

Plot of Diffraction Loss<\/strong><\/p>\n\n\n\n

\"Diffraction<\/a><\/figure>\n\n\n\n

The MATLAB codes used to generate the above plots are given below (approximate method followed by the exact method). Feel free to use them in your simulations and if you have a question drop us a comment.<\/p>\n\n\n\n

MATLAB Code for Approximate Calculation of Diffraction Loss<\/h6>\n\n\n\n
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
% Calculation of the path loss based on the value of 
% Fresnel Diffraction Parameter as proposed by Lee 
% Lee W C Y Mobile Communications Engineering 1985 
% Copyright www.raymaps.com %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
clear all 
close all 
v=-5:0.01:5; 
for n=1:length(v)     
   if v(n) <= -1         
      G(n)=0;     
   elseif v(n) <= 0         
      G(n)=20*log10(0.5-0.62*v(n));     
   elseif v(n) <= 1         
      G(n)=20*log10(0.5*exp(-0.95*v(n)));     
   elseif v(n) <= 2.4         
      G(n)=20*log10(0.4-sqrt(0.1184-(0.38-0.1*v(n))^2));     
   else         
      G(n)=20*log10(0.225\/v(n));     
   end      
end 
plot(v, G, 'b') 
xlabel('Fresnel Diffraction Parameter') 
ylabel('Diffraction Loss (dB)') <\/pre>\n\n\n\n
MATLAB Code for Exact Calculation of Diffraction Loss<\/h6>\n\n\n\n
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
% Exact calculation of the path loss (in dB) 
% based on Fresnel Diffraction Parameter (v) 
% T S Rappaport Wireless Communications P&P 
% Copyright www.raymaps.com 
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
clear all 
close all 
v=-5:0.01:5; 
for n=1:length(v)          
   v_vector=v(n):0.01:v(n)+100;          
   F(n)=((1+1i)\/2)*sum(exp((-1i*pi*(v_vector).^2)\/2));      
end 
F=abs(F)\/(abs(F(1))); 
plot(v, 20*log10(F),'r') 
xlabel('Fresnel Diffraction Parameter') 
ylabel('Diffraction Loss (dB)') <\/pre>\n\n\n\n
We have used the following equations in the exact calculation of the Diffraction Loss [1] above. We did not want to scare you with the math so have saved it for the end.<\/p>\n\n\n\n
\"\"<\/a><\/figure><\/div>\n\n\n\n
Also please checkout this interesting video<\/a> explaining the phenomenon of diffraction.<\/p>\n\n\n\n
[1] http:\/\/www.waves.utoronto.ca<\/p>\n","protected":false},"excerpt":{"rendered":"
Diffraction is a phenomenon where electromagnetic waves (such as light waves) bend around corners to reach places which are otherwise not reachable i.e. not in the line of sight. In technical jargon such regions are also called shadowed regions (the term again drawn from the physics of light). This phenomenon can be explained by Huygen’s principle which states that “as a plane wave propagates in a particular direction each new point along the wavefront is a source of secondary waves”.<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[8,81],"tags":[129,123,130],"class_list":["post-2607","post","type-post","status-publish","format-standard","hentry","category-chanmod","category-fundamentals","tag-diffraction","tag-electromagnetic","tag-knife-edge"],"_links":{"self":[{"href":"https:\/\/www.raymaps.com\/index.php\/wp-json\/wp\/v2\/posts\/2607","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.raymaps.com\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.raymaps.com\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.raymaps.com\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.raymaps.com\/index.php\/wp-json\/wp\/v2\/comments?post=2607"}],"version-history":[{"count":29,"href":"https:\/\/www.raymaps.com\/index.php\/wp-json\/wp\/v2\/posts\/2607\/revisions"}],"predecessor-version":[{"id":4200,"href":"https:\/\/www.raymaps.com\/index.php\/wp-json\/wp\/v2\/posts\/2607\/revisions\/4200"}],"wp:attachment":[{"href":"https:\/\/www.raymaps.com\/index.php\/wp-json\/wp\/v2\/media?parent=2607"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.raymaps.com\/index.php\/wp-json\/wp\/v2\/categories?post=2607"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.raymaps.com\/index.php\/wp-json\/wp\/v2\/tags?post=2607"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}