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| author | priyanka | 2015-06-24 15:03:17 +0530 |
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| committer | priyanka | 2015-06-24 15:03:17 +0530 |
| commit | b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (patch) | |
| tree | ab291cffc65280e58ac82470ba63fbcca7805165 /1172/CH3/EX3.16.1/Example3_16a.sce | |
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initial commit / add all books
Diffstat (limited to '1172/CH3/EX3.16.1/Example3_16a.sce')
| -rwxr-xr-x | 1172/CH3/EX3.16.1/Example3_16a.sce | 11 |
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diff --git a/1172/CH3/EX3.16.1/Example3_16a.sce b/1172/CH3/EX3.16.1/Example3_16a.sce new file mode 100755 index 000000000..93ba623b5 --- /dev/null +++ b/1172/CH3/EX3.16.1/Example3_16a.sce @@ -0,0 +1,11 @@ +clc
+//Given that
+R = 1.097 // Rydberg’s constant
+n1 = 1 // transition state no
+n2 = 2 // transition state no
+//Sample Problem 16a page No. 142
+printf("\n\n\n # Problem 16a # \n")
+printf ("\n Standard formula Used \n For Lyman series 1/lambda = R*((1/2) ^2 - (1/n) ^2)")
+nu1 = R * (n2^2 - n1^2) / (n1^2 * n2^2) //calculation of frequency of first line of Lyman series
+lambda1 = 1/ nu1//calculation of Wavelength of first line of Lyman series
+printf ("\n Wavelength of first line of Lyman series is %f Angstrom. ", lambda1 *1000)
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