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authorEugeniy Mikhailov <evgmik@gmail.com>2011-07-07 21:49:36 -0400
committerEugeniy Mikhailov <evgmik@gmail.com>2011-07-07 21:49:36 -0400
commit7029af4187e83db0aff57fccf1b8ef61fadab268 (patch)
tree495d3e4cade512cf29c846cd2d5bf77960bfe9d2
parent789728cddc88718d500127cd30076ab4017a6934 (diff)
downloadwgmr-7029af4187e83db0aff57fccf1b8ef61fadab268.tar.gz
wgmr-7029af4187e83db0aff57fccf1b8ef61fadab268.zip
reflection coefficient according to Fresnel equation
-rw-r--r--fresnel_reflection.m26
1 files changed, 26 insertions, 0 deletions
diff --git a/fresnel_reflection.m b/fresnel_reflection.m
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+function [R, theta_t] = fresnel_reflection(n1, n2, theta_i)
+%% calculates intensity reflection coefficient for s and p polarizations
+%% for light travelling from material with index of refraction n1 to material with n2
+%% theta_i - incident index of refraction
+%% R - coefficients of reflection array [Rs, Rp]
+
+ %% see http://en.wikipedia.org/wiki/Fresnel_equations
+ %% refracstion angle or angle of transmitted beam with respect to normal
+ sin_theta_t=n1/n2*sin(theta_i);
+
+ if ( abs(sin_theta_t) >= 1)
+ %% total internal reflection
+ R = [1, 1];
+ theta_t=sign(theta_i)*pi/2;
+ return;
+ end
+
+ theta_t = asin(sin_theta_t); % angle of refraction or transmitted beam
+
+ cos_theta_t = cos( theta_t );
+ cos_theta_i = cos( theta_i );
+
+ Rs = ( ( n1*cos_theta_i - n2*cos_theta_t ) / ( n1*cos_theta_i + n2*cos_theta_t ) ).^2;
+ Rp = ( ( n1*cos_theta_t - n2*cos_theta_i ) / ( n1*cos_theta_t + n2*cos_theta_i ) ).^2;
+ R = [Rs,Rp];
+end