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In a two-dimensional rectangular coordinate system, the image of a single variable function can be drawn, and what is obtained is a curve; in a three-dimensional rectangular coordinate system, the image of a function of two variables can be drawn, and the obtained surface is a curved surface
.
In the three-dimensional rectangular coordinate system, the image of the wave function Ψ(x, y, z) with three variables cannot be drawn
.
In the spherical coordinate system, the wave function is expressed as Ψ(r,θ,Φ)=R(r)Y(θ,Φ), and its image cannot be drawn in three-dimensional space
1.
Radial probability distribution plot
From Figure 5-4, we can understand the changing trend of |Ψ| 2 -r
.
For 1s electrons, the probability density |Ψ| 2 decreases as r increases
If we consider the variation of the probability of electrons in a thin-layer spherical shell per unit thickness with r, the probability that the thickness of the thin-layer spherical shell at the distance r from the core is △r can be found (Figure 5-6)
.
Figure 5-6 Image of 1s electron
(a)|R| 2 changes with r; (b) electron cloud: (c) spherical shells of unit thickness with unequal radii
The area of the sphere at the distance r from the core is 4πr 2 , and the volume of the thin spherical shell is approximately 4πr 2 △r
.
Considering only the change of |Ψ| 2 with r, the radial probability density |R| 2 can be used instead of |Ψ| 2
w=4πr 2 △r|R| 2
The probability of electrons appearing in unit spherical shell thickness is
D(r) is called the radial distribution function, which represents the probability of electrons appearing in a spherical shell of unit thickness from the core r
.
By plotting D(r) against r, the radial probability distribution diagrams of electrons in various states can be obtained (Figure 5-7)
According to the radial probability distribution diagram, 1s has 1 probability peak, 2s has 2 probability peaks.
.
.
Figure 5-7 Radial probability distribution diagram
There is a nodal plane with a probability density of 0 between the two peaks, and the number of nodal planes with a probability density of 0 for each state of electron movement is
N section surface = nl-1