The probability of finding an electron in a region of space where its coordinates lie in the ranges r to r + dr, 0 to 0+ d0, and o to o + do is |y|²dr = [Rne(r)]² |Y™ (0, 0)|² r² sin 0 dr d0 dø 2πT [Rne(r)]² r² dr [²* * \Y?" (0, 6)²¹ sin0 d0 dó = [Rne(r)]² r² dr (We could perform the above simplification because the spherical harmonics are normalized.) (a) What are the values of n and l in Rne(r) for the ground-state of the H atom? (b) For the ground-state of H atom, the radial distribution function is given by 3/2 1=2(²) ¹/² Rn,e(r) = 2 e-Zr/a where Z is the atomic number. Find the probability that the electron in the ground-state H atom is less than a distance a from the nucleus. Standard Integral: 2.r ["* x² e¹² dx = eb² ( ²² - ² + ² ) b

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The probability of finding an electron in a region of space where its coordinates lie in the ranges r to r + dr, 0 to
0+ d0, and o to o + do is
|y|²dr = [Rne(r)]² |Y™ (0, 0)|² r² sin 0 dr d0 dø
2πT
[Rne(r)]² r² dr [²* * \Y?" (0, 6)²¹ sin0 d0 dó = [Rne(r)]² r² dr
(We could perform the above simplification because the spherical harmonics are normalized.)
(a) What are the values of n and l in Rne(r) for the ground-state of the H atom?
(b) For the ground-state of H atom, the radial distribution function is given by
3/2
1=2(²) ¹/²
Rn,e(r) = 2
e-Zr/a
where Z is the atomic number. Find the probability that the electron in the ground-state H atom is less than a
distance a from the nucleus.
Standard Integral:
2.r
["* a²eb¹² dx = eb² ( ²² - ² + ² )
b
Transcribed Image Text:The probability of finding an electron in a region of space where its coordinates lie in the ranges r to r + dr, 0 to 0+ d0, and o to o + do is |y|²dr = [Rne(r)]² |Y™ (0, 0)|² r² sin 0 dr d0 dø 2πT [Rne(r)]² r² dr [²* * \Y?" (0, 6)²¹ sin0 d0 dó = [Rne(r)]² r² dr (We could perform the above simplification because the spherical harmonics are normalized.) (a) What are the values of n and l in Rne(r) for the ground-state of the H atom? (b) For the ground-state of H atom, the radial distribution function is given by 3/2 1=2(²) ¹/² Rn,e(r) = 2 e-Zr/a where Z is the atomic number. Find the probability that the electron in the ground-state H atom is less than a distance a from the nucleus. Standard Integral: 2.r ["* a²eb¹² dx = eb² ( ²² - ² + ² ) b
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