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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 /296/CH2 | |
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 '296/CH2')
-rwxr-xr-x | 296/CH2/EX2.1/eg2_1.sce | 4 |
1 files changed, 4 insertions, 0 deletions
diff --git a/296/CH2/EX2.1/eg2_1.sce b/296/CH2/EX2.1/eg2_1.sce new file mode 100755 index 000000000..d83d6b4bd --- /dev/null +++ b/296/CH2/EX2.1/eg2_1.sce @@ -0,0 +1,4 @@ +//j=complex(0,1);
+//psi = A*exp(j*k*x);
+disp("px = h_cross*k(x)");
+disp("If we try to evaluate these integrals directly, we run into the problem that both numerator and denominator tend to infinity, because an ideal plane wave is strictly not a normalizable wave function. The trick to use is to choose the limits of integration from, say, -L/2 to +L/2 in a region of length L.The factor L cancels out in the numerator and denominator. Then we can consider L approaches infinity. For wave functions that are normalizable, such a mathematical trickdoes not have to be used.")
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