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| author | priyanka | 2015-06-24 15:03:17 +0530 |
|---|---|---|
| committer | priyanka | 2015-06-24 15:03:17 +0530 |
| commit | b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (patch) | |
| tree | ab291cffc65280e58ac82470ba63fbcca7805165 /3020/CH13/EX13.14/ex13_14.sce | |
| download | Scilab-TBC-Uploads-b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b.tar.gz Scilab-TBC-Uploads-b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b.tar.bz2 Scilab-TBC-Uploads-b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b.zip | |
initial commit / add all books
Diffstat (limited to '3020/CH13/EX13.14/ex13_14.sce')
| -rwxr-xr-x | 3020/CH13/EX13.14/ex13_14.sce | 16 |
1 files changed, 16 insertions, 0 deletions
diff --git a/3020/CH13/EX13.14/ex13_14.sce b/3020/CH13/EX13.14/ex13_14.sce new file mode 100755 index 000000000..9a8b45f86 --- /dev/null +++ b/3020/CH13/EX13.14/ex13_14.sce @@ -0,0 +1,16 @@ +clc;
+clear all;
+a = 1; // Lattice constant in meters suppose
+h1 = 1; //Miller indices of diffracted plane case1
+k1 = 0; //Miller indices of diffracted plane case1
+l1 = 0;// Miller indices of diffracted plane case1
+d1 = a/sqrt(h1^2+k1^2+l1^2);// Lattice constant
+h2 = 1; //Miller indices of diffracted plane case2
+k2 = 1; //Miller indices of diffracted plane case2
+l2 = 0;// Miller indices of diffracted plane case2
+d2 = a/sqrt(h2^2+k2^2+l2^2);// Lattice constant
+h3 = 1; //Miller indices of diffracted plane case3
+k3 = 1; //Miller indices of diffracted plane case3
+l3 = 1;// Miller indices of diffracted plane case3
+d3 = a/sqrt(h3^2+k3^2+l3^2);// Lattice constant
+disp(' ',[d1,d2,d3],'The ratio of d(1,0,0):d(1,1,0):d(1,1,1)) is')
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