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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 /1016/CH4 | |
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Diffstat (limited to '1016/CH4')
-rwxr-xr-x | 1016/CH4/EX4.10/ex4_10.sce | 20 | ||||
-rwxr-xr-x | 1016/CH4/EX4.11/ex4_11.sce | 14 | ||||
-rwxr-xr-x | 1016/CH4/EX4.13/ex4_13.sce | 22 | ||||
-rwxr-xr-x | 1016/CH4/EX4.2/ex4_2.sce | 13 | ||||
-rwxr-xr-x | 1016/CH4/EX4.3/ex4_3.sce | 15 | ||||
-rwxr-xr-x | 1016/CH4/EX4.4/ex4_4.sce | 14 |
6 files changed, 98 insertions, 0 deletions
diff --git a/1016/CH4/EX4.10/ex4_10.sce b/1016/CH4/EX4.10/ex4_10.sce new file mode 100755 index 000000000..c071a32d1 --- /dev/null +++ b/1016/CH4/EX4.10/ex4_10.sce @@ -0,0 +1,20 @@ +clc;clear;
+//Example 4.10
+
+//given data
+r=1.746;//atomic radius in angstrom
+
+//calulations
+a=4*r/sqrt(2);
+//for (i)
+h=2;k=0;l=0;
+d=a/sqrt(h^2+k^2+l^2);
+disp(d,'distace for (200) in A.U');
+//for (ii)
+h=2;k=2;l=0;
+d=a/sqrt(h^2+k^2+l^2);
+disp(d,'distace for (220) in A.U ')
+//for (iii)
+h=1;k=1;l=1;
+d=a/sqrt(h^2+k^2+l^2);
+disp(d,'distace for (111) in A.U')
\ No newline at end of file diff --git a/1016/CH4/EX4.11/ex4_11.sce b/1016/CH4/EX4.11/ex4_11.sce new file mode 100755 index 000000000..6f1f49d53 --- /dev/null +++ b/1016/CH4/EX4.11/ex4_11.sce @@ -0,0 +1,14 @@ +clc;clear;
+//Example 4.11
+
+//calculations
+//for (i)
+l=1;m=0;n=0;
+p=0;q=1;r=0;
+d=acosd((l*p+m*q+n*r)/(sqrt(l^2+m^2+n^2)*sqrt(p^2+q^2+r^2)));
+disp(d,'angle b/w pair of miller incdices in (i)');
+//for (ii)
+l=1;m=2;n=1;
+p=1;q=1;r=1;
+d=acosd((l*p+m*q+n*r)/(sqrt(l^2+m^2+n^2)*sqrt(p^2+q^2+r^2)));
+disp(d,'angle b/w pair of miller incdices in (ii)')
\ No newline at end of file diff --git a/1016/CH4/EX4.13/ex4_13.sce b/1016/CH4/EX4.13/ex4_13.sce new file mode 100755 index 000000000..a3c9177ec --- /dev/null +++ b/1016/CH4/EX4.13/ex4_13.sce @@ -0,0 +1,22 @@ +clc;clear;
+//Example 4.13
+
+//given data
+a=3.61*10^-7;//lattice constant in mm
+
+//calcualtions
+//for (i) plane (100)
+SA=a*a;
+tamc=2;//total atoms included according to sketch
+ans=tamc/SA;
+disp(ans,'atoms per mm^2 for (i)');
+//for (ii) plane (110)
+A=a*(sqrt(2)*a);
+tamc=2;//total atoms included according to sketch
+ans=tamc/A;
+disp(ans,'atoms per mm^2 for (ii)');
+//for (iii) plane (111)
+A=0.866*a*a;
+tamc=2;//total atoms included according to sketch
+ans=tamc/A;
+disp(ans,'atoms per mm^2 for (iii)')
\ No newline at end of file diff --git a/1016/CH4/EX4.2/ex4_2.sce b/1016/CH4/EX4.2/ex4_2.sce new file mode 100755 index 000000000..f24cae4ef --- /dev/null +++ b/1016/CH4/EX4.2/ex4_2.sce @@ -0,0 +1,13 @@ +clc;clear;
+//Example 4.2
+
+//given data
+d=2180;//density of NaCl
+M=23.5+35.5;//Molecular weight
+Na=6.02*10^26;//Avgraodo no. in 1/kg mole
+n=4;//for f.c.c
+
+//calculations
+a=(n*M/(Na*d))^(1/3);
+d=a/2;
+disp((d*10^10),'distance between to adajcent atoms in angstrom')
\ No newline at end of file diff --git a/1016/CH4/EX4.3/ex4_3.sce b/1016/CH4/EX4.3/ex4_3.sce new file mode 100755 index 000000000..d2ae52ca0 --- /dev/null +++ b/1016/CH4/EX4.3/ex4_3.sce @@ -0,0 +1,15 @@ +clc;clear;
+//Example 4.3
+
+//given data
+d=2.163;//density in gm/cm^3
+M=58.45;
+Na=6.02*10^23;//Avgraodo no. in 1/gm mole
+
+//calcualtions
+n=Na/M;//no. of molecules/gram
+n=n*d;//no. of molecules/cm^3
+n=2*n;//no. of atom/cm^3;
+n=n^(1/3);//no. of atoms in a row 1cm long
+d1=1/n;
+disp((d1*10^8),'Spacing in angstrom')
\ No newline at end of file diff --git a/1016/CH4/EX4.4/ex4_4.sce b/1016/CH4/EX4.4/ex4_4.sce new file mode 100755 index 000000000..992c5d020 --- /dev/null +++ b/1016/CH4/EX4.4/ex4_4.sce @@ -0,0 +1,14 @@ +clc;clear;
+//Example 4.4
+
+//given data
+r=1.278;//radius in A.U
+n=4;//structure is f.c.c
+M=63.54;
+Na=6.02*10^23;//Avgraodo no. in 1/gm mole
+
+//calculations
+a=4*r/(sqrt(2));
+V=a^3;
+d=n*M/(Na*V);
+disp((d*(10^8)^3),'Density in g/cm^3')
\ No newline at end of file |