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Diffstat (limited to '1172/CH3/EX3.16.2')
-rwxr-xr-x | 1172/CH3/EX3.16.2/3_16b.txt | 5 | ||||
-rwxr-xr-x | 1172/CH3/EX3.16.2/Example3_16b.sce | 11 |
2 files changed, 16 insertions, 0 deletions
diff --git a/1172/CH3/EX3.16.2/3_16b.txt b/1172/CH3/EX3.16.2/3_16b.txt new file mode 100755 index 000000000..ce00d1377 --- /dev/null +++ b/1172/CH3/EX3.16.2/3_16b.txt @@ -0,0 +1,5 @@ + # Problem 16b #
+
+ Standard formula Used
+ For Lyman series 1/lambda = R*((1/2)^2 -(1/n)^2)
+ Wavelength of first line of Lyman series is 1025 Angstrom.
diff --git a/1172/CH3/EX3.16.2/Example3_16b.sce b/1172/CH3/EX3.16.2/Example3_16b.sce new file mode 100755 index 000000000..4151748f2 --- /dev/null +++ b/1172/CH3/EX3.16.2/Example3_16b.sce @@ -0,0 +1,11 @@ +clc
+//Given that
+R = 1.097 // Rydberg’s constant
+n1 = 1 // transition state no
+n2 = 3 // transition state no
+//Sample Problem 16b page No. 142
+printf("\n\n\n # Problem 16b # \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 second line of Lyman series is %d Angstrom. ", lambda1 *1000 )
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